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Multi-Repository Metadata Assessment
type: Dataset
description: The metadata of energy-related datasets from the following repositories is used in this multi-repository assessment of conformance of metadata with [OEMetadata v2](https://github.com/OpenEnergyPlatform/oemetadata): - Energy Data eXchange: https://edx.netl.doe.gov/ - EU Open Data Portal: https://data.europa.eu/data/datasets - Eurostat: https://ec.europa.eu/eurostat - FfE Open Data Portal: https://opendata.ffe.de/ - Inspire-HEP: https://inspirehep.net - Open Energy Data Initiative: https://data.openei.org/ - Open Energy Platform: https://openenergyplatform.org/database/ - OpenAIRE: https://explore.openaire.eu/ - Open Power System Data (OPSD): https://open-power-system-data.org/ - Open Access Power-Grid Frequency Database: https://osf.io/m43tg/ Unfortunately, we cannot share the scripts that we used for downloading the metadata from these repositories. However, we are sharing our preprocessing scripts for the repositories which needed preprocessing before mapping them to OEMetadata. These scripts would be executed directly after retrieving the metadata from the repository. In order to map the raw metadata (see `metadata_raw`) to the OEMetadata, execute ```bash pip install -r requirements.txt python parser.py ``` The transformed metadata is then stored in a directory called `metadata_mapped`. To fix some reporting issues with nested fields, execute the cleanup script for the OEP: ```bash python cleanup_oep.py ``` Now you are ready to reproduce our report by running ```bash python report.py ``` The reports for each of the repositories is then stored in the directory `report`.
issued: 2025-12-13T09:51:22.924113
modified: 2025-12-13T10:00:55.139764
contact point: Organization
  fn: Philipp D. Rohde
creator: Agent
creator: creator
keyword: OEMetadata
keyword: Metadata Quality

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Metadata Assessment
type: Distribution
description: All files required to reproduce the reported results, including raw metadata, mappings, and scripts
format: ZIP
access URL: https://service.tib.eu/ldm_nfdi4energy/ldmservice/dataset/fe4c4894-1015-4120-b416-4130a2afa2fe/resource/7f77ecf7-4ff4-43b8-b984-2c4ae3ac92ca/download/metadataassessment.zip
byte size: 161652102.0
media type: application/zip

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Table 1
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Table 1
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Table 1
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Measurement of multi-particle azimuthal correlations in $pp$, $p$+Pb and low-multiplicity Pb+Pb collisions with the ATLAS detector
type: Dataset
description: CERN-LHC. Multi-particle cumulants and corresponding Fourier harmonics are measured for azimuthal angle distributions of charged particles in pp collisions at $\sqrt{s}$ = 5.02 and 13 TeV and in p+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV, and compared to the results obtained for low-multiplicity Pb+Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV. These measurements aim to assess the collective nature of particle production. The measurements of multi-particle cumulants confirm the evidence for collective phenomena in p+Pb and low-multiplicity Pb+Pb collisions. On the other hand, the pp results for four-particle cumulants do not demonstrate collective behaviour, indicating that they may be biased by contributions from non-flow correlations. A comparison of multi-particle cumulants and derived Fourier harmonics across different collision systems is presented as a function of the charged-particle multiplicity. For a given multiplicity, the measured Fourier harmonics are largest in Pb+Pb, smaller in p+Pb and smallest in pp collisions. The pp results show no dependence on the collision energy, nor on the multiplicity.
issued: 2025-11-17T17:13:40.884506
language: Deutsch
modified: 2025-11-17T17:13:40.884506
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Table 26
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Table 69
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Table 11
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Table 410
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Searches for heavy $ZZ$ and $ZW$ resonances in the $\ell\ell qq$ and $\nu\nu qq$ final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC, ATLAS. Acceptance times efficiency Basic event selection: - Additional selection: Signal region (SR): - Control Region (CR): - Validation Region (VR): -
issued: 2025-11-17T17:13:41.169764
language: Deutsch
modified: 2025-11-17T17:13:41.169764
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 6
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Table 149
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Table 166
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Search for the decay of the Higgs boson to a $Z$ boson and a light pseudoscalar particle decaying to two photons
type: Dataset
description: A search for the decay of the Higgs boson to a Z boson and a light, pseudoscalar particle, a, decaying respectively to two leptons and to two photons is reported. The search uses the full LHC Run 2 proton-proton collision data at sqrt(s)=13 TeV, corresponding to 139 fb-1 collected by the ATLAS detector. This is one of the first searches for this specific decay mode of the Higgs boson, and it probes unexplored parameter space in models with axion-like particles (ALPs) and extended scalar sectors. The mass of the a particle is assumed to be in the range 0.1-33 GeV. The data are analysed in two categories: a merged category where the photons from the a decay are reconstructed in the ATLAS calorimeter as a single cluster, and a resolved category in which two separate photons are detected. The main background processes are from Standard Model Z boson production in association with photons or jets. The data are in agreement with the background predictions, and upper limits on the branching ratio of the Higgs boson decay to Za times the branching ratio a->yy are derived at the 95% confidence level and they range from 0.08% to 2% depending on the mass of the a particle. The results are also interpreted in the context of ALP models.
issued: 2025-11-17T17:13:40.824187
language: Deutsch
modified: 2025-11-17T17:13:40.824187
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 1
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Table 417
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Table 12
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Table 6
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A search for $B-L$ $R$-parity-violating top squarks in $\sqrt{s} = 13$ TeV $pp$ collisions with the ATLAS experiment
type: Dataset
description: No description
issued: 2025-11-17T17:13:40.957112
language: English
modified: 2025-11-17T17:13:40.957112
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Table 25
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Table 20
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Table 207
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access URL: https://doi.org/10.17182/hepdata.77891.v1/t207

Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector
type: Dataset
description: No description
issued: 2025-11-17T17:13:41.381675
language: Deutsch
modified: 2025-11-17T17:13:41.381675
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 6
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Table 17
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Table 1
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Table 25
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Table 33
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Table 35
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Table 25
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Table 33
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Table 21
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Table 2
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Table 288
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Table 2
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Table 19
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Table 17
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Table 405
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Table 10
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Table 35
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Table 12
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Table 24
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Table 42
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Table 3
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Table 28
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Table 1
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Table 50
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Table 413
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Table 3
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Table 43
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Table 16
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Table 10
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Table 32
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Table 33
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Table 18
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Search for a new scalar decaying into new spin-1 bosons in four-lepton final states with the ATLAS detector
type: Dataset
description: A search is conducted for a new scalar boson $S$, with a mass distinct from that of the Higgs boson, decaying promptly into four leptons ($\ell =$ $e$, $\mu$) via an intermediate state containing two on-shell, promptly decaying new spin-1 bosons $Z_{d}$: $S \rightarrow Z_{d}Z_{d} \rightarrow 4\ell$, where the $Z_{d}$ boson has a mass between 15 and 300 GeV, and the $S$ boson has a mass between either 30 and 115 GeV or 130 and 800 GeV. The search uses proton-proton collision data collected with the ATLAS detector at the Large Hadron Collider with an integrated luminosity of 139 fb$^{-1}$ at a centre-of-mass energy of $\sqrt{s}=13$ TeV. No significant excess above the Standard Model background expectation is observed. Upper limits at 95% confidence level are set on the production cross-section times branching ratio, $\sigma(gg \rightarrow S) \times \mathcal{B}(S\rightarrow Z_{d}Z_{d} \rightarrow 4\ell)$, as a function of the mass of both particles, $S$ and $m_{Z_{d}}$.
issued: 2025-11-17T17:13:41.293225
language: Deutsch
modified: 2025-11-17T17:13:41.293225
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 196
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Table 6
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Table 13
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Table 21
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Table 5
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Table 41
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access URL: https://doi.org/10.17182/hepdata.79165.v1/t41

Table 2
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Table 423
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Table 335
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Table 57
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Table 156
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Table 51
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Table 4
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Table 53
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Table 219
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Table 37
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Table 481
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Table 87
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Table 37
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Table 60
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Table 137
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Table 250
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Table 43
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Table 43
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Table 11
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Table 19
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Table 291
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Table 2
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Table 8
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Table 36
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Table 3
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Table 70
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Table 154
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Table 238
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Table 520
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Table 22
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Table 17
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Table 202
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Table 271
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Search for heavy resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $q\bar{q}^{(\prime)}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
type: Dataset
description: No description
issued: 2025-11-17T17:13:41.188652
language: Deutsch
modified: 2025-11-17T17:13:41.188652
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 81
type: Distribution
access URL: https://doi.org/10.17182/hepdata.151814.v1/t81

Table 1
type: Distribution
access URL: https://doi.org/10.17182/hepdata.78375.v2/t1

Table 73
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Table 81
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Table 329
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Table 650
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Table 41
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Table 41
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Table 8
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access URL: https://doi.org/10.17182/hepdata.114363.v1/t8

Table 263
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Table 31
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Table 35
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Table 16
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Table 101
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Table 496
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Table 18
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Table 33
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Table 95
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Table 15
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access URL: https://doi.org/10.17182/hepdata.141286.v1/t15

Table 262
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Table 222
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Table 53
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Table 31
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access URL: https://doi.org/10.17182/hepdata.77891.v6/t31

Table 164
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Table 635
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Table 353
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Table 13
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Table 14
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Table 174
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Table 63
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access URL: https://doi.org/10.17182/hepdata.84154.v1/t63

Table 30
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Search for dark matter produced in association with a Standard Model Higgs boson decaying into $b$-quarks using the full Run 2 dataset from the ATLAS detector
type: Dataset
description: CERN-LHC, ATLAS. Limits on the production of dark matter candidates in association with a SM Higgs boson decaying to a bottom-quark pair in two Higgs doublet models with a vector or pseudoscalar mediator.
issued: 2025-11-17T17:13:41.663315
language: Deutsch
modified: 2025-11-17T17:13:41.663315
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

Table 29
type: Distribution
access URL: https://doi.org/10.17182/hepdata.75197.v1/t29

Table 9
type: Distribution
access URL: https://doi.org/10.17182/hepdata.18108.v1/t9

Table 31
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access URL: https://doi.org/10.17182/hepdata.77491.v2/t31

Table 6
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access URL: https://doi.org/10.17182/hepdata.140529.v1/t6

Table 28
type: Distribution
access URL: https://doi.org/10.17182/hepdata.75330.v1/t28

Table 217
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Table 94
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Table 424
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Table 2
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access URL: https://doi.org/10.17182/hepdata.95967.v1/t2

Table 5
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Table 292
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Table 29
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access URL: https://doi.org/10.17182/hepdata.71339.v1/t29

Table 193
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Table 16
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access URL: https://doi.org/10.17182/hepdata.76541.v1/t16

Table 10
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access URL: https://doi.org/10.17182/hepdata.135471.v1/t10

Table 327
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Table 389
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Table 316
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Table 53
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Table 5
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access URL: https://doi.org/10.17182/hepdata.77891.v3/t5

Table 14
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Table 21
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Table 217
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Table 112
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Table 15
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Table 82
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Table 80
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Table 32
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Table 567
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Table 11
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Table 20
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Table 188
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Table 36
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Table 244
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Table 304
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Table 36
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Table 6
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access URL: https://doi.org/10.17182/hepdata.72491.v1/t6

Table 44
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access URL: https://doi.org/10.17182/hepdata.79165.v1/t44

Table 211
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Table 10
type: Distribution
access URL: https://doi.org/10.17182/hepdata.71195.v1/t10

Table 7
type: Distribution
access URL: https://doi.org/10.17182/hepdata.72491.v1/t7

Table 4
type: Distribution
access URL: https://doi.org/10.17182/hepdata.95748.v1/t4

Table 84
type: Distribution
access URL: https://doi.org/10.17182/hepdata.127994.v1/t84

Table 73
type: Distribution
access URL: https://doi.org/10.17182/hepdata.76542.v1/t73

Table 45
type: Distribution
access URL: https://doi.org/10.17182/hepdata.76542.v2/t45

Table 4
type: Distribution
access URL: https://doi.org/10.17182/hepdata.77891.v2/t4

Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
issued: 2025-11-17T17:13:41.626278
language: Deutsch
modified: 2025-11-17T17:13:41.626278
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 24
type: Distribution
access URL: https://doi.org/10.17182/hepdata.140529.v1/t24

Measurements of $Z\gamma$ and $Z\gamma\gamma$ production in $pp$ collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. The production of $Z$ bosons with one or two isolated high-energy photons is studied using $pp$ collisions at $\sqrt{s}$ = 8 TeV. The analyses use a data sample with an integrated luminosity of 20.3 fb$^{-1}$ collected by the ATLAS detector during the 2012 LHC data taking. The $Z\gamma$ and $Z\gamma\gamma$ production cross sections are measured with leptonic ($e^{+}e^{-}$, $\mu^{+}\mu^{-}$, $\nu\bar{\nu}$) decays of the $Z$ boson, in extended fiducial regions defined in terms of the lepton and photon acceptance. They are then compared to cross-section predictions from the Standard Model, where the sources of the photons are radiation off initial-state quarks and radiative $Z$-boson decay to charged leptons, and from fragmentation of final-state quarks and gluons into photons. The yields of events with photon transverse energy $E_{\mathrm{T}} >$ 250 GeV from $\ell^{+}\ell^{-}\gamma$ events and with $E_{\mathrm{T}} >$ 400 GeV from $\nu\bar{\nu}\gamma$ events are used to search for anomalous triple gauge-boson couplings $ZZ\gamma$ and $Z\gamma\gamma$. The yields of events with diphoton invariant mass $m_{\gamma\gamma} >$ 200 GeV from $\ell^{+}\ell^{-}\gamma\gamma$ events and with $m_{\gamma\gamma} > $ 300 GeV from $\nu\bar{\nu}\gamma\gamma$ events are used to search for anomalous quartic gauge-boson couplings $ZZ\gamma\gamma$ and $Z\gamma\gamma\gamma$. No deviations from Standard Model predictions are observed and limits are placed on parameters used to describe anomalous triple and quartic gauge-boson couplings.
issued: 2025-11-17T17:13:40.804372
language: Deutsch
modified: 2025-11-17T17:13:40.804372
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

Table 21
type: Distribution
access URL: https://doi.org/10.17182/hepdata.78375.v2/t21

Table 27
type: Distribution
access URL: https://doi.org/10.17182/hepdata.76542.v2/t27

Table 106
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access URL: https://doi.org/10.17182/hepdata.84154.v1/t106

Table 14
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access URL: https://doi.org/10.17182/hepdata.74004.v1/t14

Table 279
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Table 115
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Table 17
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Table 16
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access URL: https://doi.org/10.17182/hepdata.76843.v1/t16

Table 189
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Table 261
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Table 125
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Table 184
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Table 40
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Table 27
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Table 320
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Table 221
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Table 9
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Table 44
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Table 2
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Table 35
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Table 11
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Table 544
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Table 420
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Table 11
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Table 26
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Table 196
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Table 26
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Table 308
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Table 258
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Table 15
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Table 83
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Table 135
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Table 24
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Table 20
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Table 204
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Table 1
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Table 63
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Table 70
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Table 83
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Table 2
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Table 207
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Table 56
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Table 35
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Table 36
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Table 15
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Table 164
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Table 275
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Table 138
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Table 412
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Table 411
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Table 182
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Table 175
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Table 40
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Table 19
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Table 5
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access URL: https://doi.org/10.17182/hepdata.95748.v1/t5

Table 388
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access URL: https://doi.org/10.17182/hepdata.77891.v4/t388

Table 117
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Table 46
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Table 151
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Table 2
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Table 268
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Table 1
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access URL: https://doi.org/10.17182/hepdata.76728.v1/t1

Table 28
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access URL: https://doi.org/10.17182/hepdata.76541.v1/t28

Table 37
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Table 13
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Table 40
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access URL: https://doi.org/10.17182/hepdata.78375.v5/t40

Search for pair-produced scalar and vector leptoquarks decaying into third-generation quarks and first- or second-generation leptons in pp collisions with the ATLAS detector
type: Dataset
description: No description
issued: 2025-11-17T17:13:40.925013
language: Deutsch
modified: 2025-11-17T17:13:40.925013
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 212
type: Distribution
access URL: https://doi.org/10.17182/hepdata.77891.v3/t212

Table 33
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access URL: https://doi.org/10.17182/hepdata.79165.v1/t33

Table 263
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access URL: https://doi.org/10.17182/hepdata.87144.v1/t263

Table 3
type: Distribution
access URL: https://doi.org/10.17182/hepdata.78375.v3/t3

Table 98
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access URL: https://doi.org/10.17182/hepdata.77891.v3/t98

Table 702
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access URL: https://doi.org/10.17182/hepdata.87144.v1/t702

Table 323
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access URL: https://doi.org/10.17182/hepdata.77891.v6/t323

Table 129
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Table 98
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Table 132
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Table 487
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Table 58
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Table 130
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access URL: https://doi.org/10.17182/hepdata.77891.v6/t130

Table 222
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access URL: https://doi.org/10.17182/hepdata.87144.v1/t222

Measurement of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ meson production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. The production of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ charmed mesons has been measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV at the LHC, using data corresponding to an integrated luminosity of $280\,$nb$^{-1}$. The charmed mesons have been reconstructed in the range of transverse momentum $3.5<p_{\rm T}(D)<100$ GeV and pseudorapidity $|\eta(D)|<2.1$. The differential cross sections as a function of transverse momentum and pseudorapidity were measured for $D^{*\pm}$ and $D^\pm$ production. The next-to-leading-order QCD predictions are consistent with the data in the visible kinematic region within the large theoretical uncertainties. Using the visible $D$ cross sections and an extrapolation to the full kinematic phase space, the strangeness-suppression factor in charm fragmentation, the fraction of charged non-strange $D$ mesons produced in a vector state, and the total cross section of charm production at $\sqrt{s}=7$ TeV were derived.
issued: 2025-11-17T17:13:40.947941
language: Deutsch
modified: 2025-11-17T17:13:40.947941
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 27
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Table 420
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Measurement of the Inelastic Proton-Proton Cross Section at $\sqrt{s} = 13$ TeV with the ATLAS Detector at the LHC
type: Dataset
description: CERN-LHC. Measurement of the inelastic proton-proton cross section at a centre-of-mass energy of 13 TeV. The data set has a total integrated luminosity of 60 $\mu$b$^{-1}$. Scintillation counters in the forward region were used to select inelastic events. Results are given for a cut off of $M(X)^{2}/S > 1*10^{-6}$, equivalent to $M_X > 13$ GeV at 13 TeV and also extrapolated to the full range $M(P)^{2}/S$.
issued: 2025-11-17T17:13:40.618295
language: English
modified: 2025-11-17T17:13:40.618295
contact point: Organization
  fn: M. Aaboud
creator: Agent
creator: creator

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Table 24
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Table 37
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Measurement of event-shape observables in $Z \to \ell^{+} \ell^{-}$ events in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector at the LHC
type: Dataset
description: CERN-LHC. Event-shape observables measured using charged particles in inclusive Z-Boson events are presented, using the electron and muon decay modes of the Z-bosons. The measurements are based on an integrated luminosity of $ 1.1 {\rm fb}^{-1}$ of proton--proton collisions recorded by the ATLAS detector at the LHC at a centre-of-mass energy $\sqrt{s}=7$ TeV. Charged-particle distributions, excluding the lepton--antilepton pair from the Z-boson decay, are measured in different ranges of transverse momentum of the Z-boson. Distributions include multiplicity, scalar sum of transverse momenta, beam thrust, transverse thrust, spherocity, and $\mathcal{F}$ -parameter, which are in particular sensitive to properties of the underlying event at small values of the Z-boson transverse momentum.
issued: 2025-11-17T17:13:41.212975
language: Deutsch
modified: 2025-11-17T17:13:41.212975
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

Table 26
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Search for triboson $W^{\pm}W^{\pm}W^{\mp}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. Measurements on the triboson W+-W+-W-+ production cross-section using two decay channels fully-leptonic W+-W+-W-+ -> l+-nu l+-nu l-+nu and semi-leptonic W+-W+-W-+ -> l+-nu l+-nu jj (with l=e,mu) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWWW anomalous quartic gauge couplings. The fully-leptonic channel (W+-W+-W-+ -> l+-nu l+-nu l-+nu ) is defined as (the exact definition is given in table 1 of the preprint): - Exactly 3 leptons electrons or muons with pT(Lepton)>25 GeV and |eta(Leptons)|<=2.5 - If there are 2 Same Flavor Opposite Signe (SFOS) pairs, MET>55 GeV, if there is 1 SFOS, MET>45 GeV, and if there is 0 SFOS pairs no requirement is applied on the MET. - If there is no SFOS pairs the invariant mass between any lepton paires mll > 20 GeV. No such requirements is applied in the presence of 1 or 2 SFOS pairs. - The angle between the trilepton system and the pTMiss must be |phi_3l-phi_met|>2.5 - If there is no SFOS pairs, |mee-mZ|>15 GeV, if there is one SFOS pair mZ-mSFOS>35 Gev or mSFOS-mZ>20 GeV, and if there are two SFOS pairs mSFOS-mZ|>20 GeV. - There should be at most 1 jet with pT>25 GeV and |eta|<4.5 - DeltaR(l,l)>0.1 The semi-leptonic channel (W+-W+-W-+ -> l+-nu l+-nu jj) is defined as (the exact definition is given in table 2 of the preprint): - Exactly 2 same-charge leptons electrons or muons with pT(Lepton)>30 GeV and |eta(Leptons)|<=2.5 - Veto the presence of any third lepton with pT>6 GeV and |\eta|<2.5 GeV. - In the ee final state mee<80 GeV or mee>100 GeV. - The lepton pair should satisfy mll>40 GeV. - There should be at least 2 jets with pT(j1)>30 GeV , pT(j2)>30 GeV and |eta|<2.5 - The dijet system should satisfy 65 GeV<mjj< 105 GeV and |Delta_Eta(jj)|<1.5 - If there is at least one electron in the events, MET>55 GeV. - DeltaR(l,l)>0.1 and DeltaR(l,j)>0.3
issued: 2025-11-17T17:13:41.335243
language: Deutsch
modified: 2025-11-17T17:13:41.335243
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

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Table 35
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Table 12
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Table 526
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Table 1
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Table 54
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Table 25
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Table 65
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Table 24
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Table 4
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Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector
type: Dataset
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
issued: 2025-11-17T17:13:40.850169
language: Deutsch
modified: 2025-11-17T17:13:40.850169
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Table 130
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Table 2
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Table 36
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Table 2
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Table 17
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Table 30
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Table 334
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Table 16
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Table 113
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Table 1
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Table 360
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Table 42
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Table 13
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Table 329
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Table 30
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Table 92
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Table 171
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Table 54
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Table 53
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Table 67
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Table 47
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Table 312
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Table 18
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Table 26
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Table 50
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Table 35
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Table 130
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Table 34
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Table 10
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Table 2
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Table 55
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Table 7
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Table 11
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Table 23
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Table 676
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Table 357
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Table 35
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Table 30
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Table 42
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Table 12
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Table 542
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Table 108
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Table 78
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Table 359
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Table 323
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Table 23
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Table 48
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Table 10
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Table 26
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Table 7
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Table 28
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Table 349
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Table 81
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Table 6
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Table 92
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Table 93
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Table 54
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Table 134
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Table 670
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Table 9
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Table 25
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Table 45
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Table 105
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Table 24
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Table 310
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Measurement of the cross-section for electroweak production of dijets in association with a $Z$ boson in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. Measurement of the cross-section for electroweak production of dijets in association with a Z boson in pp collisions at a centre-of-mass energy of 13 TeV with the ATLAS detector. The measurement was made using the 3.2 fb^-1 of data collected in 2015.
issued: 2025-11-17T17:13:41.619686
language: Deutsch
modified: 2025-11-17T17:13:41.619686
contact point: Organization
  fn: M. Aaboud
creator: Agent
creator: creator

Table 232
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access URL: https://doi.org/10.17182/hepdata.84154.v2/t232

Table 43
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access URL: https://doi.org/10.17182/hepdata.77891.v2/t43

Table 665
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Table 256
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Table 52
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access URL: https://doi.org/10.17182/hepdata.104702.v1/t52

Table 8
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Table 11
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Table 49
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Table 663
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Table 74
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Table 34
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Table 255
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Table 28
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Table 151
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Table 134
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Table 290
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Table 140
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Table 343
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Table 23
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Table 464
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Table 34
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Table 251
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Search for new phenomena in high-mass final states with a photon and a jet from $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
type: Dataset
description: A search is performed for new phenomena in events with a high-transverse momentum photon and jets collected in 36.7/fb of pp collisions at a centre-of-mass energy of 13 TeV recorded with the ATLAS detector at the Large Hadron Collider. The invariant mass distribution of the leading photon and jet is examined to look for a resonant production of new particles or the presence of new high-mass states beyond the Standard Model. No significant deviation is observed in the mass distribution from the background-only hypothesis and cross section limits for generic Gaussian-shaped resonances are extracted. Excited quarks hypothesized in the quark compositeness model and high-mass states predicted in the quantum black hole models with extra dimensions are also examined in the analysis. The observed data exclude, at 95% confidence level, mass range below 5.3 TeV for the excited quarks and 7.1 TeV (4.4 TeV) for the quantum black holes with six (one) extra dimensions in the Arkani-Hamed-Dimopoulos-Dvali (Randall-Sundrum) model.
issued: 2025-11-17T17:13:41.209408
language: Deutsch
modified: 2025-11-17T17:13:41.209408
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 355
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Table 60
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Table 9
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access URL: https://doi.org/10.17182/hepdata.75330.v1/t9

Table 418
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Table 5
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Table 3
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Table 173
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Table 402
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Fiducial, total and differential cross-section measurements of $t$-channel single top-quark production in $pp$ collisions at 8 TeV using data collected by the ATLAS detector
type: Dataset
description: - CERN-LHC. Detailed measurements of $t$-channel single top-quark production are presented. They use $20.2~\mathrm{fb}^{-1}$ of data collected by the ATLAS experiment in proton--proton collisions at a centre-of-mass energy of 8 TeV at the LHC. Total, fiducial and differential cross-sections are measured for both top-quark and top-antiquark production. The fiducial cross-section is measured with a precision of $5.8~\%$ (top quark) and $7.8~\%$ (top antiquark), respectively. The total cross-sections are measured to be $\sigma_\mathrm{tot}(tq) = 56.7^{+4.3}_{-3.8}\;\mathrm{pb}$ for top-quark production and $\sigma_\mathrm{tot}(\bar{t} q) = 32.9^{+3.0}_{-2.7}\;\mathrm{pb}$ for top-antiquark production, in agreement with the Standard Model prediction. In addition, the ratio of top-quark to top-antiquark production cross-sections is determined to be $R_t=1.72 \pm 0.09$. The differential cross-sections as a function of the transverse momentum and rapidity of both the top quark and the top antiquark are measured at both the parton and particle levels. The transverse momentum and rapidity differential cross-sections of the accompanying jet from the $t$-channel scattering are measured at particle level. All measurements are compared to various Monte Carlo predictions as well as to fixed-order QCD calculations where available.
issued: 2025-11-17T17:13:41.588365
language: Deutsch
modified: 2025-11-17T17:13:41.588365
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

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Studies of new Higgs boson interactions through nonresonant $HH$ production in the $b\bar{b}\gamma\gamma$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
type: Dataset
description: A search for nonresonant Higgs boson pair production in the $b\bar{b}\gamma\gamma$ final state is performed using 140 fb$^{-1}$ of proton--proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. This analysis supersedes and expands upon the previous nonresonant ATLAS results in this final state based on the same data sample. The analysis strategy is optimised to probe anomalous values not only of the Higgs ($H$) boson self-coupling modifier $\kappa_\lambda$ but also of the quartic $HHVV$ ($V=W,Z$) coupling modifier $\kappa_{2V}$. No significant excess above the expected background from Standard Model processes is observed. An observed upper limit $\mu_{HH}<4.0$ is set at 95% confidence level on the Higgs boson pair production cross-section normalised to its Standard Model prediction. The 95% confidence intervals for the coupling modifiers are $-1.4<\kappa_\lambda<6.9$ and $-0.5<\kappa_{2V}<2.7$, assuming all other Higgs boson couplings except the one under study are fixed to the Standard Model predictions. The results are interpreted in the Standard Model effective field theory and Higgs effective field theory frameworks in terms of constraints on the couplings of anomalous Higgs boson (self-)interactions
issued: 2025-11-17T17:13:41.388779
language: Deutsch
modified: 2025-11-17T17:13:41.388779
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

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Precision measurement and interpretation of inclusive $W^+$, $W^-$ and $Z/\gamma^*$ production cross sections with the ATLAS detector
type: Dataset
description: CERN-LHC. High-precision measurements by the ATLAS Collaboration are presented of inclusive $W^+\to\ell^+\nu$, $W^-\to\ell^-\bar{\nu}$ and $Z/\gamma^*\to\ell\ell$ ($\ell=e,\mu$) Drell--Yan production cross sections at the LHC. The data were collected in proton--proton collisions at $\sqrt{s} = 7$ TeV with an integrated luminosity of 4.6 fb$^{-1}$. Differential $W^+$ and $W^-$ cross sections are measured in a lepton pseudorapidity range $|\eta_{\ell}| = 2.5$. Differential $Z/\gamma^*$ cross sections are measured as a function of the absolute dilepton rapidity, for $|y_{\ell\ell}| < 3.6$, for three intervals of dilepton mass, $m_{\ell\ell}$, extending from 46 to 150 GeV. The integrated and differential electron- and muon-channel cross sections are combined and compared to theoretical predictions using recent sets of parton distribution functions. The data, together with the final inclusive $e^{\pm}p$ scattering cross-section data from H1 and ZEUS, are interpreted in a next-to-next-to-leading-order QCD analysis, and a new set of parton distribution functions, ATLAS-epWZ16, is obtained. The ratio of strange-to-light sea-quark densities in the proton is determined more accurately than in previous determinations based on collider data only, and is established to be close to unity in the sensitivity range of the data. A new measurement of the CKM matrix element $|V_{cs}|$ is also provided. The differential cross sections are provided in two forms, a version with summarised uncertainties as in the paper tables and as "attached resource" files in HerAverager/xFitter format detailing all sources of correlated uncertainties separately. In addition to the experimental results, detailed information on the theoretical predictions are provided as required to reproduce the interpretation.
issued: 2025-11-17T17:13:40.780270
language: Deutsch
modified: 2025-11-17T17:13:40.780270
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

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Measurement of jet substructure in boosted $t\bar{t}$ events with the ATLAS detector using 140 fb$^{-1}$ of 13 TeV $pp$ collisions
type: Dataset
description: Particle level differential cross-section measurements for top-pair production, in event with at least an hadronically decaying top-quark, as a function of substructure of the boosted top-quark. Only charged particles are used to build the substructure. Two topologies, $l$+jets and all-hadronic, are considered. The study was performed using data from pp collisions at centre-of-mass energy of 13 TeV collected in Run2 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of 140 fb$^{−1}$. Due to the large cross-section at the LHC, such measurements allow a detailed study of the properties top-quark substructure, enabling precision tests of several Monte Carlo generators. The Monte Carlo predictions for measures of the broadness, and also the two-body structure, of the top-quark jets are found to be in good agreement with the measurements, while variables sensitive to the three-body structure of the top-quark jets exhibit some tension with the measured distributions .
issued: 2025-11-17T17:13:40.584079
language: Deutsch
modified: 2025-11-17T17:13:40.584079
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

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https://service.tib.eu/dataset/ca9d7282-d4d9-494b-9ab8-937d2c1761af
type: Dataset
description: CERN-LHC. Observables sensitive to the anomalous production of events containing hadronic jets and missing momentum in the plane transverse to the proton beams at the Large Hadron Collider are presented. The observables are defined as a ratio of cross sections, for events containing jets and large missing transverse momentum to events containing jets and a pair of charged leptons from the decay of a $Z/\gamma^\ast$ boson. This definition minimises experimental and theoretical systematic uncertainties in the measurements. This ratio is measured differentially with respect to a number of kinematic properties of the hadronic system in two phase-space regions; one inclusive single-jet region and one region sensitive to vector-boson-fusion topologies. The data are found to be in agreement with the Standard Model predictions and used to constrain a variety of theoretical models for dark-matter production, including simplified models, effective field theory models, and invisible decays of the Higgs boson. The measurements use 3.2 fb${}^{-1}$ of proton-proton collision data recorded by the ATLAS experiment at a centre-of-mass energy of 13 TeV and are fully corrected for detector effects, meaning that the data can be used to constrain new-physics models beyond those shown in this paper. Numerator and denominator ($\geq 1$ jet): - $p_\text{T}^\text{miss} > 200$ GeV - no additional electron or muon with $p_\text{T}$(lepton)>7 GeV and |$\eta$(lepton)|<2.5 - |$y$(jet)|<4.5 and $p_\text{T}$(jet)>25 GeV - $\Delta\phi$(jet,$p_\text{T}^\text{miss}$) > 0.4 for the four leading jets with $p_\text{T}$(jet)>30 GeV - leading $p_\text{T}$(jet)>120 GeV and |$\eta$(jet)|<2.4 Numerator and denominator (VBF): - $p_\text{T}^\text{miss} > 200$ GeV - no additional electron or muon with $p_\text{T}$(lepton)>7 GeV and |$\eta$(lepton)|<2.5 - |$y$(jet)|<4.5 and $p_\text{T}$(jet)>25 GeV - $\Delta\phi$(jet,$p_\text{T}^\text{miss}$) > 0.4 for the four leading jets with $p_\text{T}$(jet)>30 GeV - leadin…
issued: 2025-11-17T17:13:41.583255
language: Deutsch
modified: 2025-11-17T17:13:41.583255
title: Measurement of detector-corrected observables sensitive to the anomalous production of events with jets and large missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV using the ATLAS detector
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

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Studies of $Z\gamma$ production in association with a high-mass dijet system in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. Measurements of the cross-section of the electroweak production in Zy final state in association with two jets, using two decay channels Z -> l+ l- and Z -> nu nu~ (with l=e,mu and nu=e/mu/tau neutrinos and nu~=e/mu/tau anti-neutrinos and y=photons) in proton-proton collision data corresponding to an integrated luminosity of 20.2 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWZy/ZZZy/ZyZy/yyZy anomalous quartic gauge couplings. The charged-leptonic channel Zyjj electroweak process cross sections are measured in two regions, one of which is constructed with maximized sensitivity to Zyjj electroweak process (SR) and the other region is defined as the Zyjj QCD process control region (CR). A further optimized region with higher Et photon cut applied is used to probe the anomalous quartic couplings (aQGC). The neutrino channel is probed in a region used to further improve the sensitivity to aQGC and combined with charged leptonic channel. The detailed definitions are summarized as follows. The charged-leptonic channel (Z -> l+ l- ) is defined as (the exact definition is given in table 5 of the preprint): - 2 Same Flavor Opposite Sign (SFOS) leptons (electrons or muons) with pT(Lepton)>25 GeV and |eta(Lepton)|<=2.5 - 1 isolated photon with ET(Photon)>15 GeV and |eta(Photon)|<=2.37 - 2 jets with pT(Jet)>30 GeV and |eta(Jet)|<4.5 - |m(LeptonLepton) + m(LeptonLeptonPhoton)| > 182 GeV, |m(LeptonLepton)|>40 GeV - DeltaR(Lepton, Photon)>0.4, DeltaR(Jet, Photon)>0.4, DeltaR(Jet, Lepton)>0.3 - SR is defined with |m(JetJet)|>500 GeV - CR is defined with 500 GeV>|m(JetJet)|>150 GeV - aQGC search region is defined on top of SR with ET(Photon)>250 GeV - Requirement of Photon isolation (particle level only): ET(isolation)/ET(Photon) < 0.5. The photon isolation energy is taken as the energy of the jet matching the photon (DeltaR(Jet, Photon)<0.3), with the photon energy subtracted. The neutrino channel …
issued: 2025-11-17T17:13:41.022256
language: Deutsch
modified: 2025-11-17T17:13:41.022256
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

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A statistical combination of ATLAS Run 2 searches for charginos and neutralinos at the LHC
type: Dataset
description: Statistical combinations of searches for charginos and neutralinos using various decay channels are performed using $139\,$fb$^{-1}$ of pp collision data at $\sqrt{s}$=13 TeV with the ATLAS detector at the Large Hadron Collider. Searches targeting pure-wino chargino pair production, pure-wino chargino-neutralino production, or higgsino production decaying via Standard Model W, Z, or h bosons are combined to extend the mass reach to the produced SUSY particles by 30-100 GeV. The depth of the sensitivity of the original searches is also improved by the combinations, lowering the 95% CL cross-section upper limits by 15%-40%.
issued: 2025-11-17T17:13:40.915791
language: English
modified: 2025-11-17T17:13:40.915791
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

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Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV $pp$ collision data
type: Dataset
description: No description
issued: 2025-11-17T17:13:41.300813
language: English
modified: 2025-11-17T17:13:41.300813
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

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Measurement of forward-backward multiplicity correlations in lead-lead, proton-lead, and proton-proton collisions with the ATLAS detector
type: Dataset
description: No description
issued: 2025-11-17T17:13:41.421706
language: Deutsch
modified: 2025-11-17T17:13:41.421706
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

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Measurements of top-quark pair to $Z$-boson cross-section ratios at $\sqrt s = 13, 8, 7$TeV with the ATLAS detector
type: Dataset
description: CERN-LHC, ATLAS. Measurements of the fiducial and total cross sections for Z production using the electron and muon final states in proton-proton collisions at a centre-of-mass energy of 13 TeV with 3.2 fb^-1 of data collected in 2015. Measurements of single and double fiducial and total cross-section ratios for ttbar and Z production at 13, 8, and 7TeV.
issued: 2025-11-17T17:13:41.373162
language: Deutsch
modified: 2025-11-17T17:13:41.373162
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

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Search for Resonant Production of Dark Quarks in the Dijet Final State with the ATLAS Detector
type: Dataset
description: This paper presents a search for a new $Z^\prime$ resonance decaying into a pair of dark quarks which hadronise into dark hadrons before promptly decaying back to Standard Model particles. This analysis is based on proton-proton collision data recorded at $\sqrt{s}=13$ TeV with the ATLAS detector at the Large Hadron Collider between 2015 and 2018, corresponding to an integrated luminosity of 139 fb$^{-1}$. After selecting events containing large-radius jets with high track multiplicity, the invariant mass distribution of the two leading jets is scanned to look for an excess above a data-driven estimate of the Standard Model multi-jet background. No significant excess of events is observed and the results are thus used to set $95 \%$ confidence-level upper limits on the production cross-section times branching ratio of the $Z^\prime$ to dark quarks as a function of the $Z^\prime$ mass for various dark-quark scenarios.
issued: 2025-11-17T17:13:41.543695
language: English
modified: 2025-11-17T17:13:41.543695
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 72
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INSPIRE
type: Organization

Measurement of the forward-backward asymmetries in the production of $\Xi$ and $\Omega$ baryons in $p \bar{p}$ collisions
type: Dataset
description: Numbers taken from table 1 of arXiv:1605.03513v1.
issued: 2025-11-17T17:13:41.323307
language: English
modified: 2025-11-17T17:13:41.323307
contact point: Organization
  fn: Victor Mukhamedovich Abazov
creator: creator
creator: Agent

Table 130
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Table 5
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Table 1
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Table 59
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Table 36
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Measurement and interpretation of same-sign $W$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
type: Dataset
description: This paper presents the measurement of fiducial and differential cross sections for both the inclusive and electroweak production of a same-sign $W$-boson pair in association with two jets ($W^\pm W^\pm jj$) using $139\,\mathrm{fb}^{-1}$ of proton--proton collision data recorded at a centre-of-mass energy of $\sqrt{s}=13$ TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity difference. The measured fiducial cross sections for electroweak and inclusive $W^\pm W^\pm jj$ production are $2.92 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb and $3.38 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95\%\ confidence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons \(H^{\pm\pm}\) that are produced in vector-boson fusion processes and decay into a same-sign $W$ boson pair is performed. The largest deviation from the Standard Model occurs for an \(H^{\pm\pm}\) mass near $450\,\mathrm{GeV}$, with a global significance of 2.5 standard deviations.
issued: 2025-11-17T17:13:41.050890
language: Deutsch
modified: 2025-11-17T17:13:41.050890
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

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Table 390
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Table 13
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Table 691
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Table 1
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Table 62
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Search for new resonances in events with one lepton and missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. A search for $W^\prime$ bosons in events with one lepton (electron or muon) and missing transverse momentum is presented. The search uses 3.2 fb$^{-1}$ of $pp$ collision data collected at $\sqrt{s} = 13$ TeV by the ATLAS experiment at the LHC in 2015. The transverse mass distribution is examined and no significant excess of events above the level expected from Standard Model processes is observed. Upper limits on the $W^\prime$ boson cross-section times branching ratio to leptons are set as a function of the $W^\prime$ mass. Assuming a $W^\prime$ boson as predicted by the Sequential Standard Model, $W^\prime$ masses below 4.07 TeV are excluded at the 95% confidence level. This extends the limit set using LHC data at $\sqrt{s}=8$ TeV by around 800 GeV.
issued: 2025-11-17T17:13:41.714401
language: Deutsch
modified: 2025-11-17T17:13:41.714401
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 36
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Table 10
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Table 419
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Table 606
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Table 406
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Table 387
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Table 33
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Table 51
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Table 33
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Table 2
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Table 2
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Table 47
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Table 28
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Table 2
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Table 20
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Table 113
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Table 37
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Table 20
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Table 10
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Table 20
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Table 17
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Table 17
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Table 8
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Table 2
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Table 4
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Table 1
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Table 108
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Table 116
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Table 2
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Table 19
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Table 26
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Table 37
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Table 78
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Table 38
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Table 32
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Table 8
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Table 41
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Table 13
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Table 299
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Table 75
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Table 173
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Table 61
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Table 7
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Table 15
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Table 26
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Table 2
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Table 83
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Table 64
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Table 2
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Table 3
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Table 88
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Table 84
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Table 453
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Table 85
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Table 51
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Table 30
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Table 57
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Table 92
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Table 7
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Table 19
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Table 59
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Table 240
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Table 17
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Table 7
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Table 44
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Table 40
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Table 396
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Table 228
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Table 33
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Table 78
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Table 61
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Table 19
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Table 101
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Table 16
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Table 53
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Table 689
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Table 39
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Table 9
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Table 59
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Table 86
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Table 20
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Table 39
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Table 57
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Table 330
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Table 44
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Table 20
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Table 19
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Table 322
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Table 32
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Table 214
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Table 60
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Table 5
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Table 11
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Table 244
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Table 225
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Table 26
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Table 20
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Table 54
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Table 50
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Table 33
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Table 19
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Table 300
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Table 17
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Table 31
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Table 21
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Table 56
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Table 423
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Table 32
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Table 93
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Table 154
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Table 8
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Table 243
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Table 29
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Table 50
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Table 425
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Table 201
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Table 14
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Table 229
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Table 73
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Table 240
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Table 657
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Table 71
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Table 263
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Table 13
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Table 2
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Table 619
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Table 19
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Table 532
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Table 22
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Table 34
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Table 23
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Table 209
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Table 34
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Table 32
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Table 386
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Table 24
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Table 24
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Table 142
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Table 33
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Table 159
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Table 13
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Table 1
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Table 99
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Table 4
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Table 35
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Table 10
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Table 11
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Table 92
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Table 40
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Table 204
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Table 192
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Table 213
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Table 237
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Table 474
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Table 152
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Table 138
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Table 89
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Table 25
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Table 371
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Table 48
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Table 88
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Table 355
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Table 20
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Table 672
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Table 20
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Table 108
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Table 109
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Table 84
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Table 17
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Table 65
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Table 32
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Table 16
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Table 377
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Table 211
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Table 42
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Table 43
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Table 327
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Table 14
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Table 18
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Table 80
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Table 22
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Table 383
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Table 299
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Table 1
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Table 103
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Table 58
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Table 29
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Table 46
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Table 1
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access URL: https://doi.org/10.17182/hepdata.76542.v2/t1

Table 26
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Table 77
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Table 32
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Table 27
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Table 17
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Table 18
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Table 8
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Table 35
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Table 37
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Table 44
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Table 3
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Table 100
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Table 9
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access URL: https://doi.org/10.17182/hepdata.76505.v1/t9

Table 94
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Table 7
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Table 172
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Table 29
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Table 257
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Table 288
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Table 28
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Table 47
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Search for resonances decaying into a weak vector boson and a Higgs boson in the fully hadronic final state produced in proton$-$proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
type: Dataset
description: No description
issued: 2025-11-17T17:13:40.932026
language: Deutsch
modified: 2025-11-17T17:13:40.932026
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

Table 39
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Table 70
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Table 30
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Table 49
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Constraining the Higgs boson self-coupling from single- and double-Higgs production with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV
type: Dataset
description: Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the bbbb, bb$\tau\tau$ and bb$\gamma\gamma$ decay channels with single-Higgs boson analyses targeting the $\gamma\gamma$, $ZZ^{∗}$, $WW^{∗}$, $\tau\tau$ and bb decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton−proton collisions at 13 TeV and correspond to an integrated luminosity of 126−139 fb$^{-1}$ . The combination of the double-Higgs analyses sets an upper limit of $\mu_{HH} < 2.4$ at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling ($\lambda_{HHH}$), values outside the interval $-0.4< \kappa_\lambda < 6.3$ are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles.
issued: 2025-11-17T17:13:40.574772
language: Deutsch
modified: 2025-11-17T17:13:40.574772
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 489
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Table 102
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Table 146
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Table 11
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access URL: https://doi.org/10.17182/hepdata.76730.v1/t25

Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV p+Pb collisions measured by the ATLAS experiment
type: Dataset
description: CERN-LHC. Measurements of the per-event charged-particle yield as a function of the charged-particle transverse momentum and rapidity are performed using $p+$Pb collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of $\sqrt{s_{NN}}=5.02$ TeV. Charged particles are reconstructed over pseudorapidity $|\eta|<2.3$ and transverse momentum between $0.1$ GeV and $22$ GeV in a dataset corresponding to an integrated luminosity of $1$ $\mu b^{-1}$. The results are presented in the form of charged-particle nuclear modification factors, where the $p+$Pb charged-particle multiplicities are compared between central and peripheral $p+$Pb collisions as well as to charged-particle cross sections measured in pp collisions. The $p+$Pb collision centrality is characterized by the total transverse energy measured in $-4.9<\eta<-3.1$, which is in the direction of the outgoing lead beam. Three different estimations of the number of nucleons participating in the $p+$Pb collision are carried out using the Glauber model and two Glauber-Gribov colour-fluctuation extensions to the Glauber model. The values of the nuclear modification factors are found to vary significantly as a function of rapidity and transverse momentum. A broad peak is observed for all centralities and rapidities in the nuclear modification factors for charged-particle transverse momentum values around $3$ GeV. The magnitude of the peak increases for more central collisions as well as rapidity ranges closer to the direction of the outgoing lead nucleus.
issued: 2025-11-17T17:13:41.340523
language: Deutsch
modified: 2025-11-17T17:13:41.340523
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

Table 47
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creator
agent: Agent
name: James P Agnew
name: Nicola Abraham
name: Henso Abreu
name: Ricardo Abreu
name: Yiming Abulaiti
name: Andrew Warren Askew
name: Ovsat Abdinov
name: Kira Abeling
name: Georgiy D Alkhazov
name: Maris Abolins
name: Dale Charles Abbott
name: Bobby Samir Acharya
name: Bannanje Sripath Acharya
name: Dale Abbott
name: Ossama Abouzeid
name: Baptiste Abeloos
name: Asmaa Aboulhorma
name: Adam Abed Abud
name: Mark Raymond Adams
name: Rosemarie Aben
name: Chen-hsun Chan
name: Enrique Iglesias
name: D.C. Abbott
name: Guennadi D Alexeev
name: Deshan Kavishka Abhayasinghe
name: Georges Aad
name: Todd Adams
name: Braden Keim Abbott
name: Haider Abidi
name: Jalal Abdallah
name: A.C. Abusleme Hoffman
name: Ossama AbouZeid
name: Halina Abramowicz
name: Nils Julius Abicht
name: Chi Lung Cheng
name: Erlend Aakvaag
name: Hass Abouzeid
name: Angel Abusleme
name: O.S. AbouZeid
name: Andrew K Alton
name: Yulian Budagov
name: Syed Haider Abidi
name: Brad Abbott

Table 76
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Table 1
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Search for long-lived charginos based on a disappearing-track signature in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. This paper presents a search for direct electroweak gaugino or gluino pair production with a chargino nearly mass-degenerate with a stable neutralino. It is based on an integrated luminosity of 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV collected by the ATLAS experiment at the LHC. The final state of interest is a disappearing track accompanied by at least one jet with high transverse momentum from initial-state radiation or by four jets from the gluino decay chain. The use of short track segments reconstructed from the innermost tracking layers significantly improves the sensitivity to short chargino lifetimes. The results are found to be consistent with Standard Model predictions. Exclusion limits are set at 95% confidence level on the mass of charginos and gluinos for different chargino lifetimes. For a pure wino with a lifetime of about 0.2 ns, chargino masses up to 460 GeV are excluded. For the strong production channel, gluino masses up to 1.65 TeV are excluded assuming a chargino mass of 460 GeV and lifetime of 0.2 ns. For the strong production channel, gluino masses up to 1.65 TeV are excluded assuming a chargino mass of 460 GeV and lifetime of 0.2 ns.
issued: 2025-11-17T17:13:41.226093
language: Deutsch
modified: 2025-11-17T17:13:41.226093
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 42
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Search for magnetic monopoles and stable particles with high electric charges in $\sqrt{s}=$13 TeV $pp$ collisions with the ATLAS detector
type: Dataset
description: CERN-LHC. We present a search for magnetic monopoles and high-electric-charge objects using LHC Run 2 $\sqrt{s}$ = 13 TeV proton–proton collisions recorded by the ATLAS detector. A total integrated luminosity of 138 fb$^{−1}$ was collected by a specialized trigger and analyzed.No highly ionizing particle candidate was observed. Considering the Drell-Yan and photon-fusion pair production mechanisms as benchmark models, lowest to-date cross-section upper limits are presented for spin-0 and spin-$\frac{1}{2}$ magnetic monopoles of charge 1$g_{D}$ and 2$g_{D}$ and high-electric-charge objects of charge $20\le|z|\le100$, for masses between 200 and 4000 GeV.
issued: 2025-11-17T17:13:41.156203
language: Deutsch
modified: 2025-11-17T17:13:41.156203
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 5
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Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector
type: Dataset
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered. The fiducial region of the $e\tau$ channel is defined as: - Opposite-sign electron-muon pair - $p_{\mathrm{T}}(e)$ > 27 GeV - $p_{\mathrm{T}}(\mu)$ > 10 GeV - $p_{\mathrm{T}}(e)$ > $p_{\mathrm{T}}(\mu)$ - Veto on 1.37 < $|\eta(e)|$ < 1.52 - $\Delta R(e,\mu)$ > 0.1 - $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ > 1 - Visible mass $m_{\mathrm{vis}}(e,\mu)$ > 40 GeV - No $b$-jets - Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ < 35 GeV The fiducial region of the $\mu\tau$ channel is defined as: - Opposite-sign electron-muon pair - $p_{\mathrm{T}}(e)$ > 15 GeV - $p_{\mathrm{T}}(\mu)$ > 27 GeV - $p_{\mathrm{T}}(\mu)$ > $p_{\mathrm{T}}(e)$ - Veto on 1.37 < $|\eta(e)|$ < 1.52 - $\Delta R(e,\mu)$ > 0.1 - $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ > 1 - Visible mass $m_{\mathrm{vis}}(e,\mu)$ > 40 GeV - No $b$-jets - Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ < 35 GeV
issued: 2025-11-17T17:13:41.045874
language: Deutsch
modified: 2025-11-17T17:13:41.045874
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

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type: Catalog
language: en
modified: 2025-12-13T10:00:55.139764

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Measurements of electroweak $Wjj$ production and constraints on anomalous gauge couplings with the ATLAS detector
type: Dataset
description: CERN-LHC. Measurements of the electroweak production of a $W$ boson in association with two jets at high dijet invariant mass are performed using $\sqrt{s} = 7$ and 8 TeV proton--proton collision data produced by the Large Hadron Collider, corresponding respectively to 4.7 and 20.2 fb${}^{-1}$ of integrated luminosity collected by the ATLAS detector. The measurements are sensitive to the production of a $W$ boson via a triple-gauge-boson vertex and include both the fiducial and differential cross sections of the electroweak process. Preselection: - Lepton $p_\text{T} > 25$ GeV - Lepton $|\eta| < 2.5$ - $E_\text{T}^\text{miss} > 25$ GeV - $m_\text{T} > 40$ GeV - $p_\text{T}^{j_1} > 80$ GeV - $p_\text{T}^{j_2} > 60$ GeV - Jet $|y| < 4.4$ - $M_{jj} > 500$ GeV - $\Delta y(j_1, j_2) > 2$ - $\Delta R(j,\ell) > 0.3$ Inclusive regions: - $M_{jj} > 0.5$ TeV, 1 TeV, 1.5 TeV, or 2 TeV Forward-lepton/central-jet region: - $N^\text{cen}_\text{lepton} = 0$, $N^\text{cen}_\text{jets} \geq 1$ Forward-lepton control region: - $N^\text{cen}_\text{lepton} = 0$, $N^\text{cen}_\text{jets} = 0$ Central-jet validation region: - $N^\text{cen}_\text{lepton} = 1$, $N^\text{cen}_\text{jets} \geq 1$ Signal region: - $N^\text{cen}_\text{lepton} = 1$, $N^\text{cen}_\text{jets} = 0$ High-mass signal region: - $M_{jj} > 1$ TeV, $N^\text{cen}_\text{lepton} = 1$, $N^\text{cen}_\text{jets} = 0$
issued: 2025-11-17T17:13:40.994721
language: Deutsch
modified: 2025-11-17T17:13:40.994721
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

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Measurement of the dependence of transverse energy production at large pseudorapidity on the hard-scattering kinematics of proton-proton collisions at $\sqrt{s} = 2.76$ TeV with ATLAS
type: Dataset
description: CERN-LHC. The relationship between jet production in the central region and the underlying-event activity in a pseudorapidity-separated region is studied in 4.0 pb$^{-1}$ of $\sqrt{s} = 2.76$ TeV $pp$ collision data recorded with the ATLAS detector at the LHC. The underlying event is characterised through measurements of the average value of the sum of the transverse energy at large pseudorapidity downstream of one of the protons, which are reported here as a function of hard-scattering kinematic variables. The hard scattering is characterised by the average transverse momentum and pseudorapidity of the two highest transverse momentum jets in the event. The dijet kinematics are used to estimate, on an event-by-event basis, the scaled longitudinal momenta of the hard-scattered partons in the target and projectile beam-protons moving toward and away from the region measuring transverse energy, respectively. Transverse energy production at large pseudorapidity is observed to decrease with a linear dependence on the longitudinal momentum fraction in the target proton and to depend only weakly on that in the projectile proton. The results are compared to the predictions of various Monte Carlo event generators, which qualitatively reproduce the trends observed in data but generally underpredict the overall level of transverse energy at forward pseudorapidity.
issued: 2025-11-17T17:13:40.907794
language: Deutsch
modified: 2025-11-17T17:13:40.907794
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

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Search for new phenomena in a lepton plus high jet multiplicity final state with the ATLAS experiment using $\sqrt{s}$ = 13 Tev proton-proton collision data
type: Dataset
description: CERN-LHC. A search for new phenomena in final states characterized by high jet multiplicity, an isolated lepton (electron or muon) and either zero or at least three b-tagged jets is presented. The search uses 36.1 fb-1 of sqrt(s) = 13 TeV proton-proton collision data collected by the ATLAS experiment at the Large Hadron Collider in 2015 and 2016. The dominant sources of background are estimated using parameterized extrapolations, based on observables at medium jet multiplicity, to predict the b-tagged jet multiplicity distribution at the higher jet multiplicities used in the search. No significant excess over the Standard Model expectation is observed and 95% confidence-level limits are extracted constraining four simplified models of R-parity-violating supersymmetry that feature either gluino or top-squark pair production. The exclusion limits reach as high as 2.1 TeV in gluino mass and 1.2 TeV in top-squark mass in the models considered. In addition, an upper limit is set on the cross-section for Standard Model tttt production of 60 fb (6.5 times the Standard Model prediction) at 95% confidence level. Finally, model-independent limits are set on the contribution from new phenomena to the signal-region yields.
issued: 2025-11-17T17:13:41.268137
language: English
modified: 2025-11-17T17:13:41.268137
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Table 11
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Table 90
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Table 23
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Table 16
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Table 305
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Table 530
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Table 24
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Table 7
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Table 96
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Table 37
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Measurement of the inclusive isolated prompt photon cross section in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. Measurement of the inclusive isolated prompt photon cross section in pp collisions at 8 TeV with the ATLAS detector. The prompt photon fiducial region is defined as: - ET(Photon) range: 25 < ET(Photon) < 1500 GeV - |EtaPhoton|: 0-0.6, 0.6-1.37, 1.56-1.81, 1.81-2.37 - Photon Isolation in DeltaR-Cone of 0.4: ETIso < 4.8 GeV + 4.2x10^{-3} ET(Photon). At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons.
issued: 2025-11-17T17:13:41.711026
language: Deutsch
modified: 2025-11-17T17:13:41.711026
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 224
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Combination of searches for resonant Higgs boson pair production using $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
type: Dataset
description: A combination of searches for resonant Higgs boson pair production is presented, using up to 139 $fb^{-1}$ of $pp$ collision data at $\sqrt{s}$ = 13 TeV recorded with the ATLAS detector at the LHC. The combination includes searches performed in three decay channels: bbbb, bb$\tau\tau$, bb$\gamma\gamma$. No excess above the expected background is observed and upper limits are set at the 95% confidence level on the production cross section of Higgs boson pairs originating from the decay of a narrow scalar resonance with mass in the range 251 GeV-5 TeV. The observed (expected) limits are in the range 0.96-600 fb (1.2-390 fb). The limits are interpreted in the Type-I Two-Higgs-Doublet Model and the Minimimal Supersymmetric Standard Model, and constrain parameter space not previously excluded by other searches.
issued: 2025-11-17T17:13:41.418641
language: Deutsch
modified: 2025-11-17T17:13:41.418641
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

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High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. Measurements of the cross section for prompt photon plus jet production in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.2/fb of data collected in 2012. The photon is required to have a transverse energy above 130 GeV and absolute value of pseudorapity |etaGamma|<2.37, excluding the region 1.37<|etaGamma|<1.56. The photon isolation is ensured by requiring the transverse energy around a cone of radius R=0.4 around the photon to be less than 10 GeV. At particle level it is the sum of transverse energy from all particles, except for muons, neutrinos and the photon itself. At parton level it is the sum of energy from all coloured partons. Jets are reconstructed using the anti-kt algorithm with radius parameter R=0.6 and required to have the jet rapidity in the range |yjet|<4.4 and the distance between the jet and the photon DeltaR(gamma jet)>1. The requirements on the jet transverse momenta depend on the sample and are as follows. Photon+1jet sample (tables 1 and 2): pTjet1 > 100 GeV. Photon+1jet sample (tables 3 to 13): pTjet1 > 100 GeV, |yjet1| < 2.37, |costhetastar| < 0.83 and |etaGamma + yjet1| < 2.37 and mgammajet1 > 467 GeV. Photon+2jet sample (tables 14 to 17): pTjet1 > 100 GeV and pTjet2 > 65 GeV. Photon+2jet sample (tables 18 and 20): pTjet1 > 100 GeV, pTjet2 > 65 GeV and 130 < ETGamma < 300 GeV. Photon+2jet sample (tables 19 and 21): pTjet1 > 100 GeV, pTjet2 > 65 GeV and ETGamma > 300 GeV. Photon+2jet sample (table 22): pTjet1 > 130 GeV, pTjet2 > 50 GeV, Delta R(gamma jet1) > 3, 1 < Delta R(jet1 jet2) < 1.5 and |etajet1| < 2.37. Photon+2jet sample (table 23): pTjet1 > 130 GeV, pTjet2 > 50 GeV, Delta R(gamma jet1) > 3, 1 < Delta R(gamma jet2) < 1.5, |etajet1| < 2.37 and pTjet2 < ETGamma. Photon+2jet sample (table 24): ratio of cross sections in tables 22 and 23. Photon+3jet sample (tables 25 to 29): pTjet1 > 100 GeV, pTjet2 > 65 GeV and pTjet3 > 50 GeV. Photon+3jet sample (tables 30, 32 and 34): pTjet1 > 100 GeV, pTjet2 > 65 GeV…
issued: 2025-11-17T17:13:41.030346
language: Deutsch
modified: 2025-11-17T17:13:41.030346
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

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Table 7
type: Distribution
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Table 362
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Table 24
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Table 150
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Table 417
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Table 11
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Table 72
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Table 24
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Table 191
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Table 30
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Table 6
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Table 178
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Table 159
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Table 47
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Table 7
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Table 404
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Table 34
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Table 18
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Table 56
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Table 8
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Table 48
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Table 156
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Table 137
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Table 114
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Table 12
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Table 402
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Table 75
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Table 2
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Table 2
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Table 127
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Table 310
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Table 20
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Table 5
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Table 2
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Table 538
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Performance of the missing transverse momentum triggers for the ATLAS detector during Run-2 data taking
type: Dataset
description: No description
issued: 2025-11-17T17:13:41.645275
language: Deutsch
modified: 2025-11-17T17:13:41.645275
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 14
type: Distribution
access URL: https://doi.org/10.17182/hepdata.72792.v1/t14

Search for squarks and gluinos in events with hadronically decaying tau leptons, jets and missing transverse momentum in proton-proton collisions at $\sqrt{s}=13$ TeV recorded with the ATLAS detector
type: Dataset
description: CERN-LHC. A search for supersymmetry in events with large missing transverse momentum, jets, and at least one hadronically decaying tau lepton has been performed using 3.2 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=13$ TeV recorded by the ATLAS detector at the Large Hadron Collider in 2015. Two exclusive final states are considered, with either exactly one or at least two tau leptons. No excess over the Standard Model prediction is observed in the data. Results are interpreted in the context of gauge-mediated supersymmetry breaking and a simplified model of gluino pair production with tau-rich cascade decays, substantially improving on previous limits. In the GMSB model considered, supersymmetry-breaking scale ($\Lambda$) values below 92 TeV are excluded at the 95% confidence level, corresponding to gluino masses below 2000 GeV. For large values of $\tan\beta$, values of $\Lambda$ up to 107 TeV and gluino masses up to 2300 GeV are excluded. In the simplified model, gluino masses are excluded up to 1570 GeV for neutralino masses around 100 GeV. Neutralino masses up to 700 GeV are excluded for all gluino masses between 800 GeV and 1500 GeV, while the strongest exclusion of 750 GeV is achieved for gluino masses around 1400 GeV.
issued: 2025-11-17T17:13:41.611720
language: Deutsch
modified: 2025-11-17T17:13:41.611720
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 385
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Table 1
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Table 79
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Table 43
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Table 25
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Table 19
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Table 14
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Table 32
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Table 14
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Table 10
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Table 5
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Table 24
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Table 99
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Table 82
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Table 13
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Table 123
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Table 2
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Table 110
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Table 73
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Table 95
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Table 48
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Table 185
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Table 3
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Table 14
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Table 289
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Table 7
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Table 319
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Table 19
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Table 278
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Table 636
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Table 71
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Table 21
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Table 1
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Table 212
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Table 59
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Table 4
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Table 10
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Table 399
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access URL: https://doi.org/10.17182/hepdata.77891.v2/t399

Search for invisible particles produced in association with single top quarks in proton-proton collisions at $\sqrt{s}$=13 TeV with the ATLAS detector
type: Dataset
description: A search for events with one top quark and missing transverse momentum in the final state is presented. The fully hadronic decay of the top quark is explored by selecting events with a reconstructed boosted top-quark topology produced in association with large missing transverse momentum. The analysis uses 139 fb$^{-1}$ of proton--proton collision data at a centre-of-mass energy of $\sqrt{s} =13$ TeV recorded during 2015-2018 by the ATLAS detector at the Large Hadron Collider. The results are interpreted in terms of simplified models for Dark Matter particle production and the single production of a vector-like $T$ quark.
issued: 2025-11-17T17:13:40.845064
language: Deutsch
modified: 2025-11-17T17:13:40.845064
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 39
type: Distribution
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Table 22
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access URL: https://doi.org/10.17182/hepdata.78376.v2/t22

Table 401
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Table 30
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Table 145
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Table 401
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Table 309
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Table 643
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Table 289
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Table 116
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Table 116
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access URL: https://doi.org/10.17182/hepdata.77893.v1/t116

Table 12
type: Distribution
access URL: https://doi.org/10.17182/hepdata.78375.v1/t12

Table 16
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access URL: https://doi.org/10.17182/hepdata.79797.v1/t16

Table 355
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Table 43
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Table 103
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Table 63
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Table 130
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Table 12
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access URL: https://doi.org/10.17182/hepdata.76843.v1/t12

Measurement of the $t\bar{t}\gamma$ production cross section in proton-proton collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC-ATLAS. Measurements of the cross section for $t\bar{t}\gamma$ production using the single lepton (e or mu) channel in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.2 fb^-1 of data collected in 2012. The fiducial region is defined as: - 1 electron or muon, 1 photon, at least 4 jets, at least 1 b-jet - ptLepton > 25 GeV, |etaLepton| < 2.5 - ptPhoton > 15 GeV, |etaPhoton| < 2.37 - ptJet > 25 GeV, |etaJet| < 2.5 - min(DeltaR(lepton,photon)) > 0.7 - min(DeltaR(jet,photon)) > 0.5
issued: 2025-11-17T17:13:41.607862
language: Deutsch
modified: 2025-11-17T17:13:41.607862
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Table 226
type: Distribution
access URL: https://doi.org/10.17182/hepdata.77891.v5/t226

Table 120
type: Distribution
access URL: https://doi.org/10.17182/hepdata.84154.v1/t120

Table 3
type: Distribution
access URL: https://doi.org/10.17182/hepdata.78375.v4/t3

Table 67
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Table 14
type: Distribution
access URL: https://doi.org/10.17182/hepdata.78376.v2/t14

Table 25
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access URL: https://doi.org/10.17182/hepdata.75197.v1/t25

Table 44
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Table 379
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Table 69
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Table 79
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Table 29
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Table 52
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Table 17
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Table 3
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Table 56
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Table 281
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Table 6
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Table 28
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Table 6
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Table 3
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Table 16
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Table 113
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Table 45
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Table 482
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Table 3
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Table 36
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Table 63
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Table 444
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Table 28
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Table 219
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Table 38
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Table 25
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Table 690
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Table 2
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Table 83
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Table 373
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Table 331
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Table 4
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Table 134
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Table 5
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Table 316
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Table 10
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Table 14
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Table 120
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Table 7
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Table 20
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Table 2
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Table 367
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Table 52
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Table 6
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Table 94
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Table 87
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Table 23
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Table 1
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Table 24
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Table 52
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Table 347
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Table 69
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Table 63
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Table 6
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Table 651
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Table 62
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Table 54
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Table 8
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Table 68
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Table 70
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Table 2
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Table 306
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Table 319
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Table 86
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Table 13
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Table 10
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Table 21
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Table 90
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Table 379
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Table 83
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Table 50
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Table 68
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Table 120
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Search for new phenomena with large jet multiplicities and missing transverse momentum using large-radius jets and flavour-tagging at ATLAS in 13 TeV $pp$ collisions
type: Dataset
description: CERN-LHC. A search is presented for particles that decay producing a large jet multiplicity and invisible particles. The event selection applies a veto on the presence of isolated electrons or muons and additional requirements on the number of $b$-tagged jets and the scalar sum of masses of large-radius jets. Having explored the full ATLAS 2015--2016 dataset of LHC proton--proton collisions at $\sqrt{s}$=13 TeV, which corresponds to 36.1~fb$^{-1}$ of integrated luminosity, no evidence is found for physics beyond the Standard Model.The results are interpreted in the context of simplified models inspired by R-parity-conserving and R-parity-violating supersymmetry, where gluinos are pair-produced. More generic models within the phenomenological minimal supersymmetric Standard Model are also considered.
issued: 2025-11-17T17:13:41.097710
language: English
modified: 2025-11-17T17:13:41.097710
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

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Search for heavy, long-lived, charged particles with large ionisation energy loss in $pp$ collisions at $\sqrt{s} = 13~\text{TeV}$ using the ATLAS experiment and the full Run 2 dataset
type: Dataset
description: This paper presents a search for hypothetical massive, charged, long-lived particles with the ATLAS detector at the LHC using an integrated luminosity of $139 \mathrm{fb^{-1}}$ of proton--proton collisions at $\sqrt{s}=13 \text{TeV}$. These particles are expected to move significantly slower than the speed of light and should be identifiable by their high transverse momenta and anomalously large specific ionisation losses, $dE/dx$. Trajectories reconstructed solely by the inner tracking system and a $dE/dx$ measurement in the pixel detector layers provide sensitivity to particles with lifetimes down to ${\cal O}(1) \text{ns}$ with a mass, measured using the Bethe--Bloch relation, ranging from $100 \text{GeV}$ to 3 $\text{TeV}$. Interpretations for pair-production of $R$-hadrons, charginos and staus in scenarios of supersymmetry compatible with these particles being long-lived are presented, with mass limits extending considerably beyond those from previous searches in broad ranges of lifetime.
issued: 2025-11-17T17:13:41.398605
language: English
modified: 2025-11-17T17:13:41.398605
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

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Search for new phenomena in dijet events using 37 fb$^{-1}$ of $pp$ collision data collected at $\sqrt{s}=$13 TeV with the ATLAS detector
type: Dataset
description: No description
issued: 2025-11-17T17:13:40.952035
language: Deutsch
modified: 2025-11-17T17:13:40.952035
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 35
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Search for dark matter in association with an energetic photon in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
type: Dataset
description: CERN-LHC, ATLAS. A search for dark matter is conducted in final states containing a photon and missing transverse momentum in proton-proton collisions at 13 TeV. The data, collected during 2015-2018 by the ATLAS experiment at the CERN LHC, correspond to an integrated luminosity of 139 fb$^{-1}$. No deviations are observed relative to the predictions of the Standard Model. The results are interpreted as exclusion limits in models where weakly interacting dark-matter candidates are pair-produced via an axial-vector or a vector mediator in the s-channel. Results are also expressed in terms of 95% confidence level limits on the parameters of a model with an axion-like particle produced in association with a photon.
issued: 2025-11-17T17:13:41.631895
language: Deutsch
modified: 2025-11-17T17:13:41.631895
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

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Measurement of $W^{\pm}$ and $Z$-boson production cross sections in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC, ATLAS. Measurements of the fiducial and total cross sections and ratios for W+/-, Z production using the electron and muon final states in proton-proton collisions at a centre-of-mass energy of 13 TeV with 81 pb^-1 of data collected in 2015. Where there are two systematic uncertainties, the first is experimental (omitting luminosity) and the second uncertainty is that of luminosity.
issued: 2025-11-17T17:13:41.182049
language: Deutsch
modified: 2025-11-17T17:13:41.182049
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 596
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Study of ordered hadron chains with the ATLAS detector
type: Dataset
description: Study of 2-particle correlations in the context of coherent particle emission, test of the model of quantized fragmentation of a helical QCD string. Low intensity minimum bias pp data collected at centre-of-mass energy of 7 TeV. Acceptance region pT>100 MeV and |eta|<2.5. Non-identified particles, treated as pions.
issued: 2025-11-17T17:13:41.377722
language: Deutsch
modified: 2025-11-17T17:13:41.377722
contact point: Organization
  fn: M. Aaboud
creator: Agent
creator: creator

Table 42
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Table 1
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Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. A search for heavy neutral Higgs bosons and $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016. The 1l1tau_h channel fiducial region is defined as: - 1e+>=1tau_h or 1mu+>=1tau_h - ptLepton > 30 GeV - |etaMuon| < 2.4, |etaEle| < 2.47 (excluding 1.37 < |etaEle| < 1.52) - ptTauVis > 25 GeV - |etaTauVis| < 2.3 (excluding 1.37 < |etaTauVis| < 1.52) - No events with more than 1 electron (ptEle > 15 GeV) or muon (ptMuon > 7 GeV, |etaMuon|<2.5) - If multiple tau_h exist, the leading visible pt one is chosen - l and tau_h opposite electric charge - |DeltaPhi(l,tau_h)| > 2.4 rad - mT(l,MET) < 40 GeV - veto 80 < m(l,tau_h) < 110 in 1e1tau_h channel The 2tau_h channel fiducial region is defined as: - >=2tau_h - ptTauVis > 65 GeV (at least one with ptTauVis > 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data) - No events with an electron or muon, ptLepton > 7 (15) GeV for muons (electrons), |etaMuon| < 2.5, |etaEle| < 2.47 (excluding 1.37 < |etaEle| < 1.52) - If more than two tau_h exist, the two leading visible pt ones are chosen - The two tau_h have opposite electric charge - |DeltaPhi(tau1_h,tau2_h)| > 2.7 rad For Higgs interpretations events entering the fiducial region of each channel are categorised as: - "b-tag: if they contain a b-quark initiated jet (ptJet > 20 GeV, |etaJet|<2.5)" - "b-veto: otherwise"
issued: 2025-11-17T17:13:40.621037
language: Deutsch
modified: 2025-11-17T17:13:40.621037
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Search for supersymmetry at $\sqrt{s}=13$ TeV in final states with jets and two same-sign leptons or three leptons with the ATLAS detector
type: Dataset
description: CERN-LHC. A search for strongly produced supersymmetric particles is conducted using signatures involving multiple energetic jets and either two isolated leptons ($e$ or $\mu$) with the same electric charge or at least three isolated leptons. The search also utilises $b$-tagged jets, missing transverse momentum and other observables to extend its sensitivity. The analysis uses a data sample of proton-proton collisions at $\sqrt{s}=13$ TeV recorded with the ATLAS detector at the Large Hadron Collider in 2015 corresponding to a total integrated luminosity of 3.2 fb$^{-1}$. No significant excess over the Standard Model expectation is observed. The results are interpreted in several simplified supersymmetric models and extend the exclusion limits from previous searches. In the context of exclusive production and simplified decay modes, gluino masses are excluded at 95% confidence level up to 1.1-1.3 TeV for light neutralinos (depending on the decay channel), and bottom squark masses are also excluded up to 540 GeV. In the former scenarios, neutralino masses are also excluded up to 550-850 GeV for gluino masses around 1 TeV.
issued: 2025-11-17T17:13:41.175027
language: Deutsch
modified: 2025-11-17T17:13:41.175027
contact point: Organization
  fn: Georges Aad
creator: Agent
creator: creator

Table 258
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Table 138
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Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC. Search for new phenomena in high-mass diphoton final states using 37 fb^−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are 2 photons. The fiducial region for the spin-0 resonance search is defined as: - 2 photons - E_T > 0.4 m_gamgam for the photon with leading E_T, and E_T > 0.3 m_gamgam for the photon with sub-leading E_T - |eta_gam| < 2.37 - An isolation requirement using all particles with lifetime greater than 10 ps at the generator level in a cone of Delta_R = 0.4 around the photon direction: E^iso_T< 0.05 E_T+ 6 GeV. For the spin-2 resonance search, the acceptance and efficiencies are assumed to be those obtained from MC simulation of KK graviton decays.
issued: 2025-11-17T17:13:40.638160
language: Deutsch
modified: 2025-11-17T17:13:40.638160
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Table 1
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Table 42
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Search for pair production of higgsinos in events with two Higgs bosons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions at the ATLAS experiment
type: Dataset
description: This paper presents a search for pair production of higgsinos, the supersymmetric partners of the Higgs bosons, in scenarios with gauge-mediated supersymmetry breaking. Each higgsino is assumed to decay into a Higgs boson and a nearly-massless gravitino. The search targets the decay of the two Higgs bosons to $b\bar{b}$, leading to a reconstructed final state with at least three energetic $b$-jets and missing transverse momentum. Two complementary analysis channels are used, with each channel specifically targeting either low or high values of the higgsino mass. The low (high) mass channel exploits 126 (139) fb$^{-1}$ of $\sqrt{s}=13$ TeV data collected by the ATLAS detector during Run 2 of the Large Hadron Collider. No significant excess above the Standard Model prediction is found. At 95% confidence level, masses up to 940 GeV are excluded for higgsinos decaying exclusively to Higgs bosons. Exclusion limits as a function of the higgsino decay branching ratio to a Higgs boson are also reported.
issued: 2025-11-17T17:13:41.142539
language: English
modified: 2025-11-17T17:13:41.142539
contact point: Organization
  fn: Georges Aad
creator: creator
creator: Agent

Table 206
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Table 1
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Measurement of charged-particle distributions sensitive to the underlying event in $\sqrt{s} = 13$ TeV proton-proton collisions with the ATLAS detector at the LHC
type: Dataset
description: We present charged-particle distributions sensitive to the underlying event, measured by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV, in low-luminosity Large Hadron Collider fills corresponding to an integrated luminosity of 1.6 nb$^{-1}$. The distributions were constructed using charged particles with absolute pseudorapidity less than 2.5 and with transverse momentum greater than 500 MeV, in events with at least one such charged particle with transverse momentum above 1 GeV. These distributions characterise the angular distribution of energy and particle flows with respect to the charged particle with highest transverse momentum, as a function of both that momentum and of charged-particle multiplicity. The results have been corrected for detector effects and are compared to the predictions of various Monte Carlo event generators, experimentally establishing the level of underlying-event activity at LHC Run 2 energies and providing inputs for the development of event generator modelling. The current models in use for UE modelling typically describe this data to 5% accuracy, compared with data uncertainties of less than 1%.
issued: 2025-11-17T17:13:40.795423
language: Deutsch
modified: 2025-11-17T17:13:40.795423
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 17
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Table 95
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Table 1
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Table 323
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Table 2
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Table 18
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Table 23
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Table 385
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Search for squarks and gluinos in final states with jets and missing transverse momentum using 36 fb$^{-1}$ of $\sqrt{s}$=13 TeV $pp$ collision data with the ATLAS detector
type: Dataset
description: CERN-LHC. A search for the supersymmetric partners of quarks and gluons (squarks and gluinos) in final states containing hadronic jets and missing transverse momentum, but no electrons or muons, is presented. The data used in this search were recorded in 2015 and 2016 by the ATLAS experiment in $\sqrt{s}=13\mathrm{\ Te\kern -0.1em V}$ proton--proton collisions at the Large Hadron Collider, corresponding to an integrated luminosity of 36.1 fb$^{-1}$. The results are interpreted in the context of various models where squarks and gluinos are pair-produced and the neutralino is the lightest supersymmetric particle. An exclusion limit at the 95% confidence level on the mass of the gluino is set at 2.03$\mathrm{\ Te\kern -0.1em V}$ for a simplified model incorporating only a gluino and the lightest neutralino, assuming the lightest neutralino is massless. For a simplified model involving the strong production of mass-degenerate first- and second-generation squarks, squark masses below 1.55$\mathrm{\ Te\kern -0.1em V}$ are excluded if the lightest neutralino is massless. These limits substantially extend the region of supersymmetric parameter space previously excluded by searches with the ATLAS detector.
issued: 2025-11-17T17:13:41.718044
language: Deutsch
modified: 2025-11-17T17:13:41.718044
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Table 80
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Table 1
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Table 1
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Table 1
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Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
type: Dataset
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
issued: 2025-11-17T17:13:40.828126
language: Deutsch
modified: 2025-11-17T17:13:40.828126
contact point: Organization
  fn: Morad Aaboud
creator: creator
creator: Agent

Table 59
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Table 14
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Table 127
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Table 22
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Table 26
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Table 15
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Table 23
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Table 250
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Table 11
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Table 56
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Table 18
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Table 68
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Table 7
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Table 370
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Table 411
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Table 30
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Table 47
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Table 26
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Table 11
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Table 121
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Table 3
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access URL: https://doi.org/10.17182/hepdata.71339.v1/t3

Table 46
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Table 47
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Search for supersymmetry in events with $b$-tagged jets and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
type: Dataset
description: No description
issued: 2025-11-17T17:13:41.548534
language: Deutsch
modified: 2025-11-17T17:13:41.548534
contact point: Organization
  fn: Morad Aaboud
creator: Agent
creator: creator

Table 68
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Table 365
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Table 310
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Table 191
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Table 43
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Table 360
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Table 4
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Table 1
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access URL: https://doi.org/10.17182/hepdata.76843.v1/t1

Table 125
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Table 8
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Table 469
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access URL: https://doi.org/10.17182/hepdata.87144.v1/t469