Changes
On August 4, 2023 at 8:46:29 AM UTC, admin:
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Set author of Finite size data for the q-deformed OSp(3|2) superspin chain to Holger Frahm (previously Holger Frahm, Konstantin Hobuß, Márcio J. Martins)
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from resource SEC00_state_0_twist.zip in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource SEC01.zip in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource SEC11.zip in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource SEC20.zip in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource SEC21.zip in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource preprint arXiv:1906.00655 in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource SEC02.zip in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource SEC22.zip in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource OSP32q_repository.pdf in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource SEC12.zip in Finite size data for the q-deformed OSp(3|2) superspin chain -
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from resource Nucl. Phys. B 946 (2019) 114697 in Finite size data for the q-deformed OSp(3|2) superspin chain
f | 1 | { | f | 1 | { |
n | 2 | "author": "Holger Frahm, Konstantin Hobu\u00df, M\u00e1rcio J. | n | 2 | "author": "Holger Frahm", |
3 | Martins", | ||||
4 | "author_email": "frahm@itp.uni-hannover.de", | 3 | "author_email": "frahm@itp.uni-hannover.de", | ||
5 | "creator_user_id": "17755db4-395a-4b3b-ac09-e8e3484ca700", | 4 | "creator_user_id": "17755db4-395a-4b3b-ac09-e8e3484ca700", | ||
6 | "doi": "10.25835/0064330", | 5 | "doi": "10.25835/0064330", | ||
7 | "doi_date_published": "2019-06-03", | 6 | "doi_date_published": "2019-06-03", | ||
8 | "doi_publisher": "LUIS", | 7 | "doi_publisher": "LUIS", | ||
9 | "doi_status": "true", | 8 | "doi_status": "true", | ||
10 | "domain": "https://data.uni-hannover.de", | 9 | "domain": "https://data.uni-hannover.de", | ||
n | n | 10 | "extra_authors": [ | ||
11 | { | ||||
12 | "extra_author": " Konstantin Hobu\u00df" | ||||
13 | }, | ||||
14 | { | ||||
15 | "extra_author": " M\u00e1rcio J. Martins" | ||||
16 | } | ||||
17 | ], | ||||
11 | "groups": [], | 18 | "groups": [], | ||
12 | "have_copyright": "Yes", | 19 | "have_copyright": "Yes", | ||
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15 | "license_id": "CC-BY-3.0", | 22 | "license_id": "CC-BY-3.0", | ||
16 | "license_title": "CC-BY-3.0", | 23 | "license_title": "CC-BY-3.0", | ||
17 | "maintainer": "Konstantin Hobu\u00df", | 24 | "maintainer": "Konstantin Hobu\u00df", | ||
18 | "maintainer_email": "", | 25 | "maintainer_email": "", | ||
19 | "metadata_created": "2021-10-14T10:15:57.324224", | 26 | "metadata_created": "2021-10-14T10:15:57.324224", | ||
n | 20 | "metadata_modified": "2021-10-14T10:15:57.324229", | n | 27 | "metadata_modified": "2023-08-04T08:46:29.865536", |
21 | "name": | 28 | "name": | ||
22 | "luh-finite-size-data-for-the-q-deformed-osp-3-2-superspin-chain", | 29 | "luh-finite-size-data-for-the-q-deformed-osp-3-2-superspin-chain", | ||
23 | "notes": "Bethe ansatz data (roots, finite size energies, scaling | 30 | "notes": "Bethe ansatz data (roots, finite size energies, scaling | ||
24 | dimensions and conformal spin) for low energy states of the integrable | 31 | dimensions and conformal spin) for low energy states of the integrable | ||
25 | $U_q[OSp(3|2)]$ superspin chain.\r\n\r\nsee Holger Frahm, Konstantin | 32 | $U_q[OSp(3|2)]$ superspin chain.\r\n\r\nsee Holger Frahm, Konstantin | ||
26 | Hobu\u00df, M\u00e1rcio J. Martins: \"On the critical behaviour of the | 33 | Hobu\u00df, M\u00e1rcio J. Martins: \"On the critical behaviour of the | ||
27 | integrable $q$-deformed $OSp(3|2)$ superspin chain\", Nucl. Phys. B | 34 | integrable $q$-deformed $OSp(3|2)$ superspin chain\", Nucl. Phys. B | ||
28 | __946__ (2019) 114697, arXiv:1906.00655", | 35 | __946__ (2019) 114697, arXiv:1906.00655", | ||
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33 | "created": "2021-10-14T10:15:55.193734", | 40 | "created": "2021-10-14T10:15:55.193734", | ||
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40 | "title": "AG Frahm", | 47 | "title": "AG Frahm", | ||
41 | "type": "organization" | 48 | "type": "organization" | ||
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54 | "description": "\"On the critical behaviour of the integrable | 60 | "description": "\"On the critical behaviour of the integrable | ||
55 | q-deformed OSp(3|2) superspin chain\", Holger Frahm, Konstantin | 61 | q-deformed OSp(3|2) superspin chain\", Holger Frahm, Konstantin | ||
56 | Hobu\u00df, and M\u00e1rcio J. Martins\r\n\r\nAbstract:\r\nThis paper | 62 | Hobu\u00df, and M\u00e1rcio J. Martins\r\n\r\nAbstract:\r\nThis paper | ||
57 | is concerned with the investigation of the massless regime of an | 63 | is concerned with the investigation of the massless regime of an | ||
58 | integrable spin chain based on the quantum group deformation of the | 64 | integrable spin chain based on the quantum group deformation of the | ||
59 | OSp(3|2) superalgebra. The finite-size properties of the eigenspectra | 65 | OSp(3|2) superalgebra. The finite-size properties of the eigenspectra | ||
60 | are computed by solving the respective Bethe ansatz equations for | 66 | are computed by solving the respective Bethe ansatz equations for | ||
61 | large system sizes allowing us to uncover the low-lying critical | 67 | large system sizes allowing us to uncover the low-lying critical | ||
62 | exponents. We present evidences that critical exponents appear to be | 68 | exponents. We present evidences that critical exponents appear to be | ||
63 | built in terms of composites of anomalous dimensions of two Coulomb | 69 | built in terms of composites of anomalous dimensions of two Coulomb | ||
64 | gases with distinct radii and the exponents associated to Z(2) degrees | 70 | gases with distinct radii and the exponents associated to Z(2) degrees | ||
65 | of freedom. This view is supported by the fact that the S = 1 XXZ | 71 | of freedom. This view is supported by the fact that the S = 1 XXZ | ||
66 | integrable chain spectrum is present in some of the sectors of our | 72 | integrable chain spectrum is present in some of the sectors of our | ||
67 | superspin chain at a particular value of the deformation parameter. We | 73 | superspin chain at a particular value of the deformation parameter. We | ||
68 | find that the fine structure of finite-size effects is very rich for a | 74 | find that the fine structure of finite-size effects is very rich for a | ||
69 | typical anisotropic spin chain. In fact, we argue on the existence of | 75 | typical anisotropic spin chain. In fact, we argue on the existence of | ||
70 | a family of states with the same conformal dimension whose lattice | 76 | a family of states with the same conformal dimension whose lattice | ||
71 | degeneracies are apparently lifted by logarithmic corrections. On the | 77 | degeneracies are apparently lifted by logarithmic corrections. On the | ||
72 | other hand we also report on states of the spectrum whose finite-size | 78 | other hand we also report on states of the spectrum whose finite-size | ||
73 | corrections seem to be governed by a power law behaviour. We finally | 79 | corrections seem to be governed by a power law behaviour. We finally | ||
74 | observe that under toroidal boundary conditions the ground state | 80 | observe that under toroidal boundary conditions the ground state | ||
75 | dependence on the twist angle has two distinct analytical | 81 | dependence on the twist angle has two distinct analytical | ||
76 | structures.\r\n", | 82 | structures.\r\n", | ||
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99 | "description": "\"On the critical behaviour of the integrable | 103 | "description": "\"On the critical behaviour of the integrable | ||
100 | q-deformed OSp(3|2) superspin chain\",\r\nHolger Frahm, Konstantin | 104 | q-deformed OSp(3|2) superspin chain\",\r\nHolger Frahm, Konstantin | ||
101 | Hobu\u00df, M\u00e1rcio J. Martins\r\n\r\nAbstract:\r\nThis paper is | 105 | Hobu\u00df, M\u00e1rcio J. Martins\r\n\r\nAbstract:\r\nThis paper is | ||
102 | concerned with the investigation of the massless regime of an | 106 | concerned with the investigation of the massless regime of an | ||
103 | integrable spin chain based on the quantum group deformation of the | 107 | integrable spin chain based on the quantum group deformation of the | ||
104 | OSp(3|2) superalgebra. The finite-size properties of the eigenspectra | 108 | OSp(3|2) superalgebra. The finite-size properties of the eigenspectra | ||
105 | are computed by solving the respective Bethe ansatz equations for | 109 | are computed by solving the respective Bethe ansatz equations for | ||
106 | large system sizes allowing us to uncover the low-lying critical | 110 | large system sizes allowing us to uncover the low-lying critical | ||
107 | exponents. We present evidences that critical exponents appear to be | 111 | exponents. We present evidences that critical exponents appear to be | ||
108 | built in terms of composites of anomalous dimensions of two Coulomb | 112 | built in terms of composites of anomalous dimensions of two Coulomb | ||
109 | gases with distinct radii and the exponents associated to Z(2) degrees | 113 | gases with distinct radii and the exponents associated to Z(2) degrees | ||
110 | of freedom. This view is supported by the fact that the S=1 XXZ | 114 | of freedom. This view is supported by the fact that the S=1 XXZ | ||
111 | integrable chain spectrum is present in some of the sectors of our | 115 | integrable chain spectrum is present in some of the sectors of our | ||
112 | superspin chain at a particular value of the deformation parameter. We | 116 | superspin chain at a particular value of the deformation parameter. We | ||
113 | find that the fine structure of finite-size effects is very rich for a | 117 | find that the fine structure of finite-size effects is very rich for a | ||
114 | typical anisotropic spin chain. In fact, we argue on the existence of | 118 | typical anisotropic spin chain. In fact, we argue on the existence of | ||
115 | a family of states with the same conformal dimension whose lattice | 119 | a family of states with the same conformal dimension whose lattice | ||
116 | degeneracies are apparently lifted by logarithmic corrections. On the | 120 | degeneracies are apparently lifted by logarithmic corrections. On the | ||
117 | other hand we also report on states of the spectrum whose finite-size | 121 | other hand we also report on states of the spectrum whose finite-size | ||
118 | corrections seem to be governed by a power law behaviour. We finally | 122 | corrections seem to be governed by a power law behaviour. We finally | ||
119 | observe that under toroidal boundary conditions the ground state | 123 | observe that under toroidal boundary conditions the ground state | ||
120 | dependence on the twist angle has two distinct analytical structures. | 124 | dependence on the twist angle has two distinct analytical structures. | ||
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169 | dimensions for the studied states in the $(n_1, n_2) = (0, 0)$ sector | 169 | dimensions for the studied states in the $(n_1, n_2) = (0, 0)$ sector | ||
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456 | "name": "superspin chains", | 438 | "name": "superspin chains", | ||
457 | "state": "active", | 439 | "state": "active", | ||
458 | "vocabulary_id": null | 440 | "vocabulary_id": null | ||
459 | } | 441 | } | ||
460 | ], | 442 | ], | ||
461 | "terms_of_usage": "Yes", | 443 | "terms_of_usage": "Yes", | ||
462 | "title": "Finite size data for the q-deformed OSp(3|2) superspin | 444 | "title": "Finite size data for the q-deformed OSp(3|2) superspin | ||
463 | chain", | 445 | chain", | ||
464 | "type": "vdataset", | 446 | "type": "vdataset", | ||
465 | "url": | 447 | "url": | ||
466 | /dataset/finite-size-data-for-the-q-deformed-osp-3-2-superspin-chain", | 448 | /dataset/finite-size-data-for-the-q-deformed-osp-3-2-superspin-chain", | ||
467 | "version": "" | 449 | "version": "" | ||
468 | } | 450 | } |