Changes
On November 28, 2024 at 1:05:31 PM UTC, admin:
-
Set author of Finite size data for U_q[OSp(3|2)] quantum chains with quantum group invariant boundaries to Frahm, Holger (previously Holger Frahm)
-
Updated description of Finite size data for U_q[OSp(3|2)] quantum chains with quantum group invariant boundaries from
Bethe ansatz data (roots, finite size energies and conformal weights) for low energy states of the integrable $U_q[OSp(3|2)]$-invariant superspin chain. For details see Holger Frahm and Márcio J. Martins: "$U_q[OSp(3|2)]$ quantum chains with quantum group invariant boundaries", arXiv:2307.09412
toBethe ansatz data (roots, finite size energies and conformal weights) for low energy states of the integrable $U_q[OSp(3|2)]$-invariant superspin chain. For details see Holger Frahm and Márcio J. Martins: "$U_q[OSp(3|2)]$ quantum chains with quantum group invariant boundaries", Nucl. Phys. B __995__ (2023) 116329 [arXiv:2307.09412]
-
Changed value of field
source_metadata_modified
to2024-08-09T13:57:11.370325
in Finite size data for U_q[OSp(3|2)] quantum chains with quantum group invariant boundaries -
Changed value of field
extra_authors
to[{'extra_author': 'Martins, Márcio J.', 'familyName': 'Martins', 'givenName': 'Márcio J.'}]
in Finite size data for U_q[OSp(3|2)] quantum chains with quantum group invariant boundaries -
Added resource Nucl. Phys. B 995 (2023) 116329 to Finite size data for U_q[OSp(3|2)] quantum chains with quantum group invariant boundaries
-
Set format of resource preprint arXiv:2307.09412 to HTML in Finite size data for U_q[OSp(3|2)] quantum chains with quantum group invariant boundaries
f | 1 | { | f | 1 | { |
n | 2 | "author": "Holger Frahm", | n | 2 | "author": "Frahm, Holger", |
3 | "author_email": "frahm@itp.uni-hannover.de", | 3 | "author_email": "frahm@itp.uni-hannover.de", | ||
n | n | 4 | "citation": [], | ||
4 | "creator_user_id": "17755db4-395a-4b3b-ac09-e8e3484ca700", | 5 | "creator_user_id": "17755db4-395a-4b3b-ac09-e8e3484ca700", | ||
5 | "doi": "10.25835/ypipefbz", | 6 | "doi": "10.25835/ypipefbz", | ||
6 | "doi_date_published": "2023-08-07", | 7 | "doi_date_published": "2023-08-07", | ||
7 | "doi_publisher": "LUIS", | 8 | "doi_publisher": "LUIS", | ||
8 | "doi_status": "true", | 9 | "doi_status": "true", | ||
9 | "domain": "https://data.uni-hannover.de", | 10 | "domain": "https://data.uni-hannover.de", | ||
10 | "extra_authors": [ | 11 | "extra_authors": [ | ||
11 | { | 12 | { | ||
n | 12 | "extra_author": " M\u00e1rcio J. Martins" | n | 13 | "extra_author": "Martins, M\u00e1rcio J.", |
14 | "familyName": "Martins", | ||||
15 | "givenName": "M\u00e1rcio J." | ||||
13 | } | 16 | } | ||
14 | ], | 17 | ], | ||
n | n | 18 | "familyName": "Frahm", | ||
19 | "givenName": "Holger", | ||||
15 | "groups": [], | 20 | "groups": [], | ||
16 | "have_copyright": "Yes", | 21 | "have_copyright": "Yes", | ||
17 | "id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 22 | "id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
18 | "isopen": false, | 23 | "isopen": false, | ||
19 | "license_id": "CC-BY-3.0", | 24 | "license_id": "CC-BY-3.0", | ||
20 | "license_title": "CC-BY-3.0", | 25 | "license_title": "CC-BY-3.0", | ||
21 | "maintainer": "Holger Frahm", | 26 | "maintainer": "Holger Frahm", | ||
22 | "maintainer_email": "", | 27 | "maintainer_email": "", | ||
23 | "metadata_created": "2023-08-14T00:00:16.044079", | 28 | "metadata_created": "2023-08-14T00:00:16.044079", | ||
n | 24 | "metadata_modified": "2023-08-14T00:00:16.044085", | n | 29 | "metadata_modified": "2024-11-28T13:05:31.292708", |
25 | "name": "luh-u_q-osp-3-2-invariant-quantum-chains", | 30 | "name": "luh-u_q-osp-3-2-invariant-quantum-chains", | ||
26 | "notes": "Bethe ansatz data (roots, finite size energies and | 31 | "notes": "Bethe ansatz data (roots, finite size energies and | ||
27 | conformal weights) for low energy states of the integrable | 32 | conformal weights) for low energy states of the integrable | ||
28 | $U_q[OSp(3|2)]$-invariant superspin chain.\r\n\r\nFor details see | 33 | $U_q[OSp(3|2)]$-invariant superspin chain.\r\n\r\nFor details see | ||
29 | Holger Frahm and M\u00e1rcio J. Martins: \"$U_q[OSp(3|2)]$ quantum | 34 | Holger Frahm and M\u00e1rcio J. Martins: \"$U_q[OSp(3|2)]$ quantum | ||
n | 30 | chains with quantum group invariant boundaries\", | n | 35 | chains with quantum group invariant boundaries\", Nucl. Phys. B |
31 | arXiv:2307.09412\r\n", | 36 | __995__ (2023) 116329 [arXiv:2307.09412]\r\n", | ||
32 | "num_resources": 13, | 37 | "num_resources": 14, | ||
33 | "num_tags": 4, | 38 | "num_tags": 4, | ||
34 | "organization": { | 39 | "organization": { | ||
35 | "approval_status": "approved", | 40 | "approval_status": "approved", | ||
36 | "created": "2021-10-14T10:15:55.193734", | 41 | "created": "2021-10-14T10:15:55.193734", | ||
37 | "description": "https://www.itp.uni-hannover.de/agfrahm.html", | 42 | "description": "https://www.itp.uni-hannover.de/agfrahm.html", | ||
38 | "id": "5bb3488c-e223-4283-a276-5697b2c526e9", | 43 | "id": "5bb3488c-e223-4283-a276-5697b2c526e9", | ||
39 | "image_url": "", | 44 | "image_url": "", | ||
40 | "is_organization": true, | 45 | "is_organization": true, | ||
41 | "name": "ag-frahm", | 46 | "name": "ag-frahm", | ||
42 | "state": "active", | 47 | "state": "active", | ||
43 | "title": "AG Frahm", | 48 | "title": "AG Frahm", | ||
44 | "type": "organization" | 49 | "type": "organization" | ||
45 | }, | 50 | }, | ||
46 | "owner_org": "5bb3488c-e223-4283-a276-5697b2c526e9", | 51 | "owner_org": "5bb3488c-e223-4283-a276-5697b2c526e9", | ||
47 | "private": false, | 52 | "private": false, | ||
48 | "relationships_as_object": [], | 53 | "relationships_as_object": [], | ||
49 | "relationships_as_subject": [], | 54 | "relationships_as_subject": [], | ||
50 | "repository_name": "Leibniz University Hannover", | 55 | "repository_name": "Leibniz University Hannover", | ||
51 | "resources": [ | 56 | "resources": [ | ||
52 | { | 57 | { | ||
53 | "cache_last_updated": null, | 58 | "cache_last_updated": null, | ||
54 | "cache_url": null, | 59 | "cache_url": null, | ||
n | n | 60 | "created": "2023-08-25T11:09:36.492637", | ||
61 | "description": "$U_q[OSp(3|2)]$ quantum chains with quantum | ||||
62 | group invariant boundaries, Holger Frahm, M\u00e1rcio J. | ||||
63 | Martins\r\n\r\nAbstract: Based on the finite-size analysis of the | ||||
64 | spectrum of the quantum group invariant deformation of the OSp(3|2) | ||||
65 | superspin chain we identify the operator content of the conformal | ||||
66 | field theory describing the model in its scaling limit. We find that | ||||
67 | the macroscopic degeneracy of the conformal weights observed in the | ||||
68 | thermodynamic limit of the isotropic superspin chain is lifted by the | ||||
69 | deformation.\r\n", | ||||
70 | "format": "HTML", | ||||
71 | "hash": "", | ||||
72 | "id": "23f31999-8f8b-42b4-a887-988ed90db8d3", | ||||
73 | "last_modified": null, | ||||
74 | "metadata_modified": "2024-11-28T13:05:31.298826", | ||||
75 | "mimetype": null, | ||||
76 | "mimetype_inner": null, | ||||
77 | "name": "Nucl. Phys. B 995 (2023) 116329", | ||||
78 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||||
79 | "position": 0, | ||||
80 | "resource_type": null, | ||||
81 | "size": null, | ||||
82 | "state": "active", | ||||
83 | "url": "https://doi.org/10.1016/j.nuclphysb.2023.116329", | ||||
84 | "url_type": "" | ||||
85 | }, | ||||
86 | { | ||||
87 | "cache_last_updated": null, | ||||
88 | "cache_url": null, | ||||
55 | "created": "2023-07-18T08:03:36.505748", | 89 | "created": "2023-07-18T08:03:36.505748", | ||
56 | "description": "$U_q[OSp(3|2)]$ quantum chains with quantum | 90 | "description": "$U_q[OSp(3|2)]$ quantum chains with quantum | ||
57 | group invariant boundaries, Holger Frahm, M\u00e1rcio J. | 91 | group invariant boundaries, Holger Frahm, M\u00e1rcio J. | ||
58 | Martins\r\n\r\nAbstract: Based on the finite-size analysis of the | 92 | Martins\r\n\r\nAbstract: Based on the finite-size analysis of the | ||
59 | spectrum of the quantum group invariant deformation of the OSp(3|2) | 93 | spectrum of the quantum group invariant deformation of the OSp(3|2) | ||
60 | superspin chain we identify the operator content of the conformal | 94 | superspin chain we identify the operator content of the conformal | ||
61 | field theory describing the model in its scaling limit. We find that | 95 | field theory describing the model in its scaling limit. We find that | ||
62 | the macroscopic degeneracy of the conformal weights observed in the | 96 | the macroscopic degeneracy of the conformal weights observed in the | ||
63 | thermodynamic limit of the isotropic superspin chain is lifted by the | 97 | thermodynamic limit of the isotropic superspin chain is lifted by the | ||
64 | deformation. ", | 98 | deformation. ", | ||
n | 65 | "format": "", | n | 99 | "format": "HTML", |
66 | "hash": "", | 100 | "hash": "", | ||
67 | "id": "42a38b4c-d057-4e1c-913f-0fa1677197a6", | 101 | "id": "42a38b4c-d057-4e1c-913f-0fa1677197a6", | ||
68 | "last_modified": null, | 102 | "last_modified": null, | ||
n | 69 | "metadata_modified": "2023-08-14T00:00:16.013275", | n | 103 | "metadata_modified": "2024-11-28T13:05:31.299000", |
70 | "mimetype": null, | 104 | "mimetype": null, | ||
71 | "mimetype_inner": null, | 105 | "mimetype_inner": null, | ||
72 | "name": "preprint arXiv:2307.09412", | 106 | "name": "preprint arXiv:2307.09412", | ||
73 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 107 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 74 | "position": 0, | n | 108 | "position": 1, |
75 | "resource_type": null, | 109 | "resource_type": null, | ||
76 | "size": null, | 110 | "size": null, | ||
77 | "state": "active", | 111 | "state": "active", | ||
78 | "url": "https://arxiv.org/abs/2307.09412", | 112 | "url": "https://arxiv.org/abs/2307.09412", | ||
79 | "url_type": "" | 113 | "url_type": "" | ||
80 | }, | 114 | }, | ||
81 | { | 115 | { | ||
82 | "cache_last_updated": null, | 116 | "cache_last_updated": null, | ||
83 | "cache_url": null, | 117 | "cache_url": null, | ||
84 | "created": "2023-07-18T09:58:50.670718", | 118 | "created": "2023-07-18T09:58:50.670718", | ||
85 | "description": "Bethe roots and finite size spectral data for | 119 | "description": "Bethe roots and finite size spectral data for | ||
86 | the lowest states with spin j=0,1,2,3 of the quantum group invariant | 120 | the lowest states with spin j=0,1,2,3 of the quantum group invariant | ||
87 | U_q[SU(2)] spin chain with gamma=2pi/9.\r\n\r\nNote that the Bethe | 121 | U_q[SU(2)] spin chain with gamma=2pi/9.\r\n\r\nNote that the Bethe | ||
88 | roots are rescaled by a factor gamma as compared to the notation in | 122 | roots are rescaled by a factor gamma as compared to the notation in | ||
89 | the paper.", | 123 | the paper.", | ||
90 | "format": "ZIP", | 124 | "format": "ZIP", | ||
91 | "hash": "", | 125 | "hash": "", | ||
92 | "id": "9ccfd1fe-c7f5-476d-a2e2-e33b5d0c38a6", | 126 | "id": "9ccfd1fe-c7f5-476d-a2e2-e33b5d0c38a6", | ||
93 | "last_modified": "2023-07-18T14:13:10.259021", | 127 | "last_modified": "2023-07-18T14:13:10.259021", | ||
n | 94 | "metadata_modified": "2023-08-14T00:00:16.014567", | n | 128 | "metadata_modified": "2024-11-28T13:05:31.299119", |
95 | "mimetype": "application/zip", | 129 | "mimetype": "application/zip", | ||
96 | "mimetype_inner": null, | 130 | "mimetype_inner": null, | ||
97 | "name": "XXZ1: L odd", | 131 | "name": "XXZ1: L odd", | ||
98 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 132 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 99 | "position": 1, | n | 133 | "position": 2, |
100 | "resource_type": null, | 134 | "resource_type": null, | ||
101 | "size": 95258, | 135 | "size": 95258, | ||
102 | "state": "active", | 136 | "state": "active", | ||
103 | "url": | 137 | "url": | ||
104 | esource/9ccfd1fe-c7f5-476d-a2e2-e33b5d0c38a6/download/xxz1_l-odd.zip", | 138 | esource/9ccfd1fe-c7f5-476d-a2e2-e33b5d0c38a6/download/xxz1_l-odd.zip", | ||
105 | "url_type": "" | 139 | "url_type": "" | ||
106 | }, | 140 | }, | ||
107 | { | 141 | { | ||
108 | "cache_last_updated": null, | 142 | "cache_last_updated": null, | ||
109 | "cache_url": null, | 143 | "cache_url": null, | ||
110 | "created": "2023-07-18T11:02:35.372726", | 144 | "created": "2023-07-18T11:02:35.372726", | ||
111 | "description": "Bethe roots and finite size spectral data for | 145 | "description": "Bethe roots and finite size spectral data for | ||
112 | the first excitation with spin j=0 of the quantum group invariant | 146 | the first excitation with spin j=0 of the quantum group invariant | ||
113 | U_q[SU(2)] spin chain with even length and gamma=2pi/9, 2pi/7, 9pi/25, | 147 | U_q[SU(2)] spin chain with even length and gamma=2pi/9, 2pi/7, 9pi/25, | ||
114 | 3pi/7, pi/2.\r\n\r\nNote that the Bethe roots are rescaled by a factor | 148 | 3pi/7, pi/2.\r\n\r\nNote that the Bethe roots are rescaled by a factor | ||
115 | gamma as compared to the notation in the paper.", | 149 | gamma as compared to the notation in the paper.", | ||
116 | "format": "ZIP", | 150 | "format": "ZIP", | ||
117 | "hash": "", | 151 | "hash": "", | ||
118 | "id": "865ee3e3-de1a-440c-a37a-760f8ccfad67", | 152 | "id": "865ee3e3-de1a-440c-a37a-760f8ccfad67", | ||
119 | "last_modified": "2023-07-18T14:13:41.753566", | 153 | "last_modified": "2023-07-18T14:13:41.753566", | ||
n | 120 | "metadata_modified": "2023-08-14T00:00:16.015798", | n | 154 | "metadata_modified": "2024-11-28T13:05:31.299224", |
121 | "mimetype": "application/zip", | 155 | "mimetype": "application/zip", | ||
122 | "mimetype_inner": null, | 156 | "mimetype_inner": null, | ||
123 | "name": "XXZ1: spin j=0, first excitation, L even", | 157 | "name": "XXZ1: spin j=0, first excitation, L even", | ||
124 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 158 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 125 | "position": 2, | n | 159 | "position": 3, |
126 | "resource_type": null, | 160 | "resource_type": null, | ||
127 | "size": 24054, | 161 | "size": 24054, | ||
128 | "state": "active", | 162 | "state": "active", | ||
129 | "url": | 163 | "url": | ||
130 | /865ee3e3-de1a-440c-a37a-760f8ccfad67/download/xxz1_j0_x2_l-even.zip", | 164 | /865ee3e3-de1a-440c-a37a-760f8ccfad67/download/xxz1_j0_x2_l-even.zip", | ||
131 | "url_type": "" | 165 | "url_type": "" | ||
132 | }, | 166 | }, | ||
133 | { | 167 | { | ||
134 | "cache_last_updated": null, | 168 | "cache_last_updated": null, | ||
135 | "cache_url": null, | 169 | "cache_url": null, | ||
136 | "created": "2023-07-18T14:31:02.539603", | 170 | "created": "2023-07-18T14:31:02.539603", | ||
137 | "description": "Bethe roots (in bfbfb grading) and finite size | 171 | "description": "Bethe roots (in bfbfb grading) and finite size | ||
138 | spectral data for the ground state of the quantum group invariant | 172 | spectral data for the ground state of the quantum group invariant | ||
139 | U_q[OSp(3|2)] quantum chain with odd length and | 173 | U_q[OSp(3|2)] quantum chain with odd length and | ||
140 | gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled by a factor | 174 | gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled by a factor | ||
141 | gamma as compared to the notation in the paper.", | 175 | gamma as compared to the notation in the paper.", | ||
142 | "format": "ZIP", | 176 | "format": "ZIP", | ||
143 | "hash": "", | 177 | "hash": "", | ||
144 | "id": "ea79b1ac-8f7b-4cd0-9b74-d13af76bf299", | 178 | "id": "ea79b1ac-8f7b-4cd0-9b74-d13af76bf299", | ||
145 | "last_modified": "2023-07-18T14:31:02.484858", | 179 | "last_modified": "2023-07-18T14:31:02.484858", | ||
n | 146 | "metadata_modified": "2023-08-14T00:00:16.017327", | n | 180 | "metadata_modified": "2024-11-28T13:05:31.299329", |
147 | "mimetype": "application/zip", | 181 | "mimetype": "application/zip", | ||
148 | "mimetype_inner": null, | 182 | "mimetype_inner": null, | ||
149 | "name": "U_q[OSp(3|2)]: sector (0;1/2), L odd", | 183 | "name": "U_q[OSp(3|2)]: sector (0;1/2), L odd", | ||
150 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 184 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 151 | "position": 3, | n | 185 | "position": 4, |
152 | "resource_type": null, | 186 | "resource_type": null, | ||
153 | "size": 75126, | 187 | "size": 75126, | ||
154 | "state": "active", | 188 | "state": "active", | ||
155 | "url": | 189 | "url": | ||
156 | -d13af76bf299/download/o32q_p00-q05_bfbfb_gs_l-odd_gamma022222pi.zip", | 190 | -d13af76bf299/download/o32q_p00-q05_bfbfb_gs_l-odd_gamma022222pi.zip", | ||
157 | "url_type": "" | 191 | "url_type": "" | ||
158 | }, | 192 | }, | ||
159 | { | 193 | { | ||
160 | "cache_last_updated": null, | 194 | "cache_last_updated": null, | ||
161 | "cache_url": null, | 195 | "cache_url": null, | ||
162 | "created": "2023-07-18T14:33:24.717461", | 196 | "created": "2023-07-18T14:33:24.717461", | ||
163 | "description": "Bethe roots (in bfbfb grading) and finite size | 197 | "description": "Bethe roots (in bfbfb grading) and finite size | ||
164 | spectral data for some low energy states in the sector (p;q)=(0;1) of | 198 | spectral data for some low energy states in the sector (p;q)=(0;1) of | ||
165 | the quantum group invariant U_q[OSp(3|2)] quantum chain with even | 199 | the quantum group invariant U_q[OSp(3|2)] quantum chain with even | ||
166 | length and gamma=2pi/9, 2pi/7 and 4Pi/7.\r\n\r\nNote that the Bethe | 200 | length and gamma=2pi/9, 2pi/7 and 4Pi/7.\r\n\r\nNote that the Bethe | ||
167 | roots are rescaled by a factor gamma as compared to the notation in | 201 | roots are rescaled by a factor gamma as compared to the notation in | ||
168 | the paper.", | 202 | the paper.", | ||
169 | "format": "ZIP", | 203 | "format": "ZIP", | ||
170 | "hash": "", | 204 | "hash": "", | ||
171 | "id": "ab3fbd24-4a20-4b6e-96be-deeba3d11d23", | 205 | "id": "ab3fbd24-4a20-4b6e-96be-deeba3d11d23", | ||
172 | "last_modified": "2023-08-08T08:08:11.087215", | 206 | "last_modified": "2023-08-08T08:08:11.087215", | ||
n | 173 | "metadata_modified": "2023-08-14T00:00:16.022683", | n | 207 | "metadata_modified": "2024-11-28T13:05:31.299433", |
174 | "mimetype": "application/zip", | 208 | "mimetype": "application/zip", | ||
175 | "mimetype_inner": null, | 209 | "mimetype_inner": null, | ||
176 | "name": "U_q[OSp(3|2)]: sector (0;1), L even", | 210 | "name": "U_q[OSp(3|2)]: sector (0;1), L even", | ||
177 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 211 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 178 | "position": 4, | n | 212 | "position": 5, |
179 | "resource_type": null, | 213 | "resource_type": null, | ||
180 | "size": 2194552, | 214 | "size": 2194552, | ||
181 | "state": "active", | 215 | "state": "active", | ||
182 | "url": | 216 | "url": | ||
183 | 4-4a20-4b6e-96be-deeba3d11d23/download/o32q_p00-q10_bfbfb_l-even.zip", | 217 | 4-4a20-4b6e-96be-deeba3d11d23/download/o32q_p00-q10_bfbfb_l-even.zip", | ||
184 | "url_type": "" | 218 | "url_type": "" | ||
185 | }, | 219 | }, | ||
186 | { | 220 | { | ||
187 | "cache_last_updated": null, | 221 | "cache_last_updated": null, | ||
188 | "cache_url": null, | 222 | "cache_url": null, | ||
189 | "created": "2023-07-18T14:52:41.791193", | 223 | "created": "2023-07-18T14:52:41.791193", | ||
190 | "description": "Bethe roots (in bfbfb grading) and finite size | 224 | "description": "Bethe roots (in bfbfb grading) and finite size | ||
191 | spectral data for some low energy states in the sector (p;q)=(0;3/2) | 225 | spectral data for some low energy states in the sector (p;q)=(0;3/2) | ||
192 | of the quantum group invariant U_q[OSp(3|2)] quantum chain with odd | 226 | of the quantum group invariant U_q[OSp(3|2)] quantum chain with odd | ||
193 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | 227 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | ||
194 | by a factor gamma as compared to the notation in the paper.", | 228 | by a factor gamma as compared to the notation in the paper.", | ||
195 | "format": "ZIP", | 229 | "format": "ZIP", | ||
196 | "hash": "", | 230 | "hash": "", | ||
197 | "id": "e2e0e48c-5978-49da-a965-ae6edf83e410", | 231 | "id": "e2e0e48c-5978-49da-a965-ae6edf83e410", | ||
198 | "last_modified": "2023-07-18T14:52:41.727459", | 232 | "last_modified": "2023-07-18T14:52:41.727459", | ||
n | 199 | "metadata_modified": "2023-08-14T00:00:16.023909", | n | 233 | "metadata_modified": "2024-11-28T13:05:31.299534", |
200 | "mimetype": "application/zip", | 234 | "mimetype": "application/zip", | ||
201 | "mimetype_inner": null, | 235 | "mimetype_inner": null, | ||
202 | "name": "U_q[OSp(3|2)]: sector (0;3/2), L odd", | 236 | "name": "U_q[OSp(3|2)]: sector (0;3/2), L odd", | ||
203 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 237 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 204 | "position": 5, | n | 238 | "position": 6, |
205 | "resource_type": null, | 239 | "resource_type": null, | ||
206 | "size": 356061, | 240 | "size": 356061, | ||
207 | "state": "active", | 241 | "state": "active", | ||
208 | "url": | 242 | "url": | ||
209 | e2e0e48c-5978-49da-a965-ae6edf83e410/download/o32q_p00-q15_l-odd.zip", | 243 | e2e0e48c-5978-49da-a965-ae6edf83e410/download/o32q_p00-q15_l-odd.zip", | ||
210 | "url_type": "" | 244 | "url_type": "" | ||
211 | }, | 245 | }, | ||
212 | { | 246 | { | ||
213 | "cache_last_updated": null, | 247 | "cache_last_updated": null, | ||
214 | "cache_url": null, | 248 | "cache_url": null, | ||
215 | "created": "2023-07-18T15:05:29.305343", | 249 | "created": "2023-07-18T15:05:29.305343", | ||
216 | "description": "Bethe roots (in bfbfb grading) and finite size | 250 | "description": "Bethe roots (in bfbfb grading) and finite size | ||
217 | spectral data for some low energy states in the sector (p;q)=(0;2) of | 251 | spectral data for some low energy states in the sector (p;q)=(0;2) of | ||
218 | the quantum group invariant U_q[OSp(3|2)] quantum chain with even | 252 | the quantum group invariant U_q[OSp(3|2)] quantum chain with even | ||
219 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | 253 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | ||
220 | by a factor gamma as compared to the notation in the paper.", | 254 | by a factor gamma as compared to the notation in the paper.", | ||
221 | "format": "ZIP", | 255 | "format": "ZIP", | ||
222 | "hash": "", | 256 | "hash": "", | ||
223 | "id": "7687bc13-fa39-488b-ac45-1ed4a691b310", | 257 | "id": "7687bc13-fa39-488b-ac45-1ed4a691b310", | ||
224 | "last_modified": "2023-07-18T15:05:29.228820", | 258 | "last_modified": "2023-07-18T15:05:29.228820", | ||
n | 225 | "metadata_modified": "2023-08-14T00:00:16.025275", | n | 259 | "metadata_modified": "2024-11-28T13:05:31.299636", |
226 | "mimetype": "application/zip", | 260 | "mimetype": "application/zip", | ||
227 | "mimetype_inner": null, | 261 | "mimetype_inner": null, | ||
228 | "name": "U_q[OSP(3|2)]: sector (0;2), L even", | 262 | "name": "U_q[OSP(3|2)]: sector (0;2), L even", | ||
229 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 263 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 230 | "position": 6, | n | 264 | "position": 7, |
231 | "resource_type": null, | 265 | "resource_type": null, | ||
232 | "size": 115262, | 266 | "size": 115262, | ||
233 | "state": "active", | 267 | "state": "active", | ||
234 | "url": | 268 | "url": | ||
235 | 687bc13-fa39-488b-ac45-1ed4a691b310/download/o32q_p00-q20_l-even.zip", | 269 | 687bc13-fa39-488b-ac45-1ed4a691b310/download/o32q_p00-q20_l-even.zip", | ||
236 | "url_type": "" | 270 | "url_type": "" | ||
237 | }, | 271 | }, | ||
238 | { | 272 | { | ||
239 | "cache_last_updated": null, | 273 | "cache_last_updated": null, | ||
240 | "cache_url": null, | 274 | "cache_url": null, | ||
241 | "created": "2023-07-20T11:34:55.175246", | 275 | "created": "2023-07-20T11:34:55.175246", | ||
242 | "description": "Bethe roots (in fbbbf grading) and finite size | 276 | "description": "Bethe roots (in fbbbf grading) and finite size | ||
243 | spectral data for some low energy states in the sector (p;q)=(1;1/2) | 277 | spectral data for some low energy states in the sector (p;q)=(1;1/2) | ||
244 | of the quantum group invariant U_q[OSp(3|2)] quantum chain with even | 278 | of the quantum group invariant U_q[OSp(3|2)] quantum chain with even | ||
245 | length and gamma=2pi/9.\r\nAs an example of the finite size data for | 279 | length and gamma=2pi/9.\r\nAs an example of the finite size data for | ||
246 | \\gamma>pi/2 this dataset also includes the ground state for | 280 | \\gamma>pi/2 this dataset also includes the ground state for | ||
247 | gamma=4pi/7.\r\n\r\nNote that the Bethe roots are rescaled by a factor | 281 | gamma=4pi/7.\r\n\r\nNote that the Bethe roots are rescaled by a factor | ||
248 | gamma as compared to the notation in the paper.", | 282 | gamma as compared to the notation in the paper.", | ||
249 | "format": "ZIP", | 283 | "format": "ZIP", | ||
250 | "hash": "", | 284 | "hash": "", | ||
251 | "id": "7da23271-1614-4171-9ccb-acd56c52f921", | 285 | "id": "7da23271-1614-4171-9ccb-acd56c52f921", | ||
252 | "last_modified": "2023-08-07T13:24:04.887687", | 286 | "last_modified": "2023-08-07T13:24:04.887687", | ||
n | 253 | "metadata_modified": "2023-08-14T00:00:16.026608", | n | 287 | "metadata_modified": "2024-11-28T13:05:31.299737", |
254 | "mimetype": "application/zip", | 288 | "mimetype": "application/zip", | ||
255 | "mimetype_inner": null, | 289 | "mimetype_inner": null, | ||
256 | "name": "U_q[OSp(3|2)]: sector (1;1/2), L even", | 290 | "name": "U_q[OSp(3|2)]: sector (1;1/2), L even", | ||
257 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 291 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 258 | "position": 7, | n | 292 | "position": 8, |
259 | "resource_type": null, | 293 | "resource_type": null, | ||
260 | "size": 854536, | 294 | "size": 854536, | ||
261 | "state": "active", | 295 | "state": "active", | ||
262 | "url": | 296 | "url": | ||
263 | da23271-1614-4171-9ccb-acd56c52f921/download/o32q_p10-q05_l-even.zip", | 297 | da23271-1614-4171-9ccb-acd56c52f921/download/o32q_p10-q05_l-even.zip", | ||
264 | "url_type": "" | 298 | "url_type": "" | ||
265 | }, | 299 | }, | ||
266 | { | 300 | { | ||
267 | "cache_last_updated": null, | 301 | "cache_last_updated": null, | ||
268 | "cache_url": null, | 302 | "cache_url": null, | ||
269 | "created": "2023-07-20T12:01:48.486114", | 303 | "created": "2023-07-20T12:01:48.486114", | ||
270 | "description": "Bethe roots (in fbbbf grading) and finite size | 304 | "description": "Bethe roots (in fbbbf grading) and finite size | ||
271 | spectral data for some low energy states in the (atypical) sector | 305 | spectral data for some low energy states in the (atypical) sector | ||
272 | (p;q)=(1;1) of the quantum group invariant U_q[OSp(3|2)] quantum chain | 306 | (p;q)=(1;1) of the quantum group invariant U_q[OSp(3|2)] quantum chain | ||
273 | with odd length for gamma=2pi/9 and 2pi/7.\r\n\r\nNote that the Bethe | 307 | with odd length for gamma=2pi/9 and 2pi/7.\r\n\r\nNote that the Bethe | ||
274 | roots are rescaled by a factor gamma as compared to the notation in | 308 | roots are rescaled by a factor gamma as compared to the notation in | ||
275 | the paper.", | 309 | the paper.", | ||
276 | "format": "ZIP", | 310 | "format": "ZIP", | ||
277 | "hash": "", | 311 | "hash": "", | ||
278 | "id": "96ed04cf-ca05-423a-9e7d-898a55fcb258", | 312 | "id": "96ed04cf-ca05-423a-9e7d-898a55fcb258", | ||
279 | "last_modified": "2023-07-20T12:01:48.422343", | 313 | "last_modified": "2023-07-20T12:01:48.422343", | ||
n | 280 | "metadata_modified": "2023-08-14T00:00:16.027863", | n | 314 | "metadata_modified": "2024-11-28T13:05:31.299838", |
281 | "mimetype": "application/zip", | 315 | "mimetype": "application/zip", | ||
282 | "mimetype_inner": null, | 316 | "mimetype_inner": null, | ||
283 | "name": "U_q[OSp(3|2)]: sector (1;1), L odd", | 317 | "name": "U_q[OSp(3|2)]: sector (1;1), L odd", | ||
284 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 318 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 285 | "position": 8, | n | 319 | "position": 9, |
286 | "resource_type": null, | 320 | "resource_type": null, | ||
287 | "size": 129014, | 321 | "size": 129014, | ||
288 | "state": "active", | 322 | "state": "active", | ||
289 | "url": | 323 | "url": | ||
290 | 96ed04cf-ca05-423a-9e7d-898a55fcb258/download/o32q_p10-q10_l-odd.zip", | 324 | 96ed04cf-ca05-423a-9e7d-898a55fcb258/download/o32q_p10-q10_l-odd.zip", | ||
291 | "url_type": "" | 325 | "url_type": "" | ||
292 | }, | 326 | }, | ||
293 | { | 327 | { | ||
294 | "cache_last_updated": null, | 328 | "cache_last_updated": null, | ||
295 | "cache_url": null, | 329 | "cache_url": null, | ||
296 | "created": "2023-07-20T12:02:48.026959", | 330 | "created": "2023-07-20T12:02:48.026959", | ||
297 | "description": "Bethe roots (in fbbbf grading) and finite size | 331 | "description": "Bethe roots (in fbbbf grading) and finite size | ||
298 | spectral data for some low energy states in the (atypical) sector | 332 | spectral data for some low energy states in the (atypical) sector | ||
299 | (p;q)=(1;1) of the quantum group invariant U_q[OSp(3|2)] quantum chain | 333 | (p;q)=(1;1) of the quantum group invariant U_q[OSp(3|2)] quantum chain | ||
300 | with even length for gamma=2pi/9 and 2pi/7.\r\n\r\nNote that the Bethe | 334 | with even length for gamma=2pi/9 and 2pi/7.\r\n\r\nNote that the Bethe | ||
301 | roots are rescaled by a factor gamma as compared to the notation in | 335 | roots are rescaled by a factor gamma as compared to the notation in | ||
302 | the paper.", | 336 | the paper.", | ||
303 | "format": "ZIP", | 337 | "format": "ZIP", | ||
304 | "hash": "", | 338 | "hash": "", | ||
305 | "id": "f2fe3eaa-6795-44f1-82d8-23370b1727dd", | 339 | "id": "f2fe3eaa-6795-44f1-82d8-23370b1727dd", | ||
306 | "last_modified": "2023-07-20T12:02:47.947704", | 340 | "last_modified": "2023-07-20T12:02:47.947704", | ||
n | 307 | "metadata_modified": "2023-08-14T00:00:16.029114", | n | 341 | "metadata_modified": "2024-11-28T13:05:31.299937", |
308 | "mimetype": "application/zip", | 342 | "mimetype": "application/zip", | ||
309 | "mimetype_inner": null, | 343 | "mimetype_inner": null, | ||
310 | "name": "U_q[OSp(3|2)]: sector (1;1), L even", | 344 | "name": "U_q[OSp(3|2)]: sector (1;1), L even", | ||
311 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 345 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 312 | "position": 9, | n | 346 | "position": 10, |
313 | "resource_type": null, | 347 | "resource_type": null, | ||
314 | "size": 185015, | 348 | "size": 185015, | ||
315 | "state": "active", | 349 | "state": "active", | ||
316 | "url": | 350 | "url": | ||
317 | 2fe3eaa-6795-44f1-82d8-23370b1727dd/download/o32q_p10-q10_l-even.zip", | 351 | 2fe3eaa-6795-44f1-82d8-23370b1727dd/download/o32q_p10-q10_l-even.zip", | ||
318 | "url_type": "" | 352 | "url_type": "" | ||
319 | }, | 353 | }, | ||
320 | { | 354 | { | ||
321 | "cache_last_updated": null, | 355 | "cache_last_updated": null, | ||
322 | "cache_url": null, | 356 | "cache_url": null, | ||
323 | "created": "2023-07-20T12:11:21.529521", | 357 | "created": "2023-07-20T12:11:21.529521", | ||
324 | "description": "Bethe roots (in fbbbf grading) and finite size | 358 | "description": "Bethe roots (in fbbbf grading) and finite size | ||
325 | spectral data for some low energy states in the sector (p;q)=(1;3/2) | 359 | spectral data for some low energy states in the sector (p;q)=(1;3/2) | ||
326 | of the quantum group invariant U_q[OSp(3|2)] quantum chain with even | 360 | of the quantum group invariant U_q[OSp(3|2)] quantum chain with even | ||
327 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | 361 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | ||
328 | by a factor gamma as compared to the notation in the paper.", | 362 | by a factor gamma as compared to the notation in the paper.", | ||
329 | "format": "ZIP", | 363 | "format": "ZIP", | ||
330 | "hash": "", | 364 | "hash": "", | ||
331 | "id": "f41e7d23-9e71-4d56-8688-9154dc1594d5", | 365 | "id": "f41e7d23-9e71-4d56-8688-9154dc1594d5", | ||
332 | "last_modified": "2023-07-20T12:11:21.456395", | 366 | "last_modified": "2023-07-20T12:11:21.456395", | ||
n | 333 | "metadata_modified": "2023-08-14T00:00:16.030379", | n | 367 | "metadata_modified": "2024-11-28T13:05:31.300040", |
334 | "mimetype": "application/zip", | 368 | "mimetype": "application/zip", | ||
335 | "mimetype_inner": null, | 369 | "mimetype_inner": null, | ||
336 | "name": "U_q[OSp(3|2)]: sector (1;3/2), L even", | 370 | "name": "U_q[OSp(3|2)]: sector (1;3/2), L even", | ||
337 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 371 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 338 | "position": 10, | n | 372 | "position": 11, |
339 | "resource_type": null, | 373 | "resource_type": null, | ||
340 | "size": 216398, | 374 | "size": 216398, | ||
341 | "state": "active", | 375 | "state": "active", | ||
342 | "url": | 376 | "url": | ||
343 | 41e7d23-9e71-4d56-8688-9154dc1594d5/download/o32q_p10-q15_l-even.zip", | 377 | 41e7d23-9e71-4d56-8688-9154dc1594d5/download/o32q_p10-q15_l-even.zip", | ||
344 | "url_type": "" | 378 | "url_type": "" | ||
345 | }, | 379 | }, | ||
346 | { | 380 | { | ||
347 | "cache_last_updated": null, | 381 | "cache_last_updated": null, | ||
348 | "cache_url": null, | 382 | "cache_url": null, | ||
349 | "created": "2023-07-20T12:18:29.514351", | 383 | "created": "2023-07-20T12:18:29.514351", | ||
350 | "description": "Bethe roots (in fbbbf grading) and finite size | 384 | "description": "Bethe roots (in fbbbf grading) and finite size | ||
351 | spectral data for some low energy states in the sector (p;q)=(2;1/2) | 385 | spectral data for some low energy states in the sector (p;q)=(2;1/2) | ||
352 | of the quantum group invariant U_q[OSp(3|2)] quantum chain with odd | 386 | of the quantum group invariant U_q[OSp(3|2)] quantum chain with odd | ||
353 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | 387 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | ||
354 | by a factor gamma as compared to the notation in the paper.", | 388 | by a factor gamma as compared to the notation in the paper.", | ||
355 | "format": "ZIP", | 389 | "format": "ZIP", | ||
356 | "hash": "", | 390 | "hash": "", | ||
357 | "id": "3d7da05c-91cb-4cc0-9eb5-0fd3b09b526a", | 391 | "id": "3d7da05c-91cb-4cc0-9eb5-0fd3b09b526a", | ||
358 | "last_modified": "2023-08-07T13:28:50.492951", | 392 | "last_modified": "2023-08-07T13:28:50.492951", | ||
n | 359 | "metadata_modified": "2023-08-14T00:00:16.031624", | n | 393 | "metadata_modified": "2024-11-28T13:05:31.300139", |
360 | "mimetype": "application/zip", | 394 | "mimetype": "application/zip", | ||
361 | "mimetype_inner": null, | 395 | "mimetype_inner": null, | ||
362 | "name": "U_q[OSp(3|2)]: sector (2;1/2), L odd", | 396 | "name": "U_q[OSp(3|2)]: sector (2;1/2), L odd", | ||
363 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 397 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 364 | "position": 11, | n | 398 | "position": 12, |
365 | "resource_type": null, | 399 | "resource_type": null, | ||
366 | "size": 112705, | 400 | "size": 112705, | ||
367 | "state": "active", | 401 | "state": "active", | ||
368 | "url": | 402 | "url": | ||
369 | 3d7da05c-91cb-4cc0-9eb5-0fd3b09b526a/download/o32q_p20-q05_l-odd.zip", | 403 | 3d7da05c-91cb-4cc0-9eb5-0fd3b09b526a/download/o32q_p20-q05_l-odd.zip", | ||
370 | "url_type": "" | 404 | "url_type": "" | ||
371 | }, | 405 | }, | ||
372 | { | 406 | { | ||
373 | "cache_last_updated": null, | 407 | "cache_last_updated": null, | ||
374 | "cache_url": null, | 408 | "cache_url": null, | ||
375 | "created": "2023-07-20T12:23:34.137241", | 409 | "created": "2023-07-20T12:23:34.137241", | ||
376 | "description": "Bethe roots (in fbbbf grading) and finite size | 410 | "description": "Bethe roots (in fbbbf grading) and finite size | ||
377 | spectral data for some low energy states in the sector (p;q)=(2;1) of | 411 | spectral data for some low energy states in the sector (p;q)=(2;1) of | ||
378 | the quantum group invariant U_q[OSp(3|2)] quantum chain with even | 412 | the quantum group invariant U_q[OSp(3|2)] quantum chain with even | ||
379 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | 413 | length and gamma=2pi/9.\r\n\r\nNote that the Bethe roots are rescaled | ||
380 | by a factor gamma as compared to the notation in the paper.", | 414 | by a factor gamma as compared to the notation in the paper.", | ||
381 | "format": "ZIP", | 415 | "format": "ZIP", | ||
382 | "hash": "", | 416 | "hash": "", | ||
383 | "id": "0d506f76-9ddb-4fe8-802f-a8622e2cef68", | 417 | "id": "0d506f76-9ddb-4fe8-802f-a8622e2cef68", | ||
384 | "last_modified": "2023-07-20T12:23:34.051594", | 418 | "last_modified": "2023-07-20T12:23:34.051594", | ||
n | 385 | "metadata_modified": "2023-08-14T00:00:16.032860", | n | 419 | "metadata_modified": "2024-11-28T13:05:31.300239", |
386 | "mimetype": "application/zip", | 420 | "mimetype": "application/zip", | ||
387 | "mimetype_inner": null, | 421 | "mimetype_inner": null, | ||
388 | "name": "U_q[OSp(3|2)]: sector (2;1), L even", | 422 | "name": "U_q[OSp(3|2)]: sector (2;1), L even", | ||
389 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | 423 | "package_id": "59947bde-e1bf-47b7-ac68-527f1ce27a80", | ||
n | 390 | "position": 12, | n | 424 | "position": 13, |
391 | "resource_type": null, | 425 | "resource_type": null, | ||
392 | "size": 92037, | 426 | "size": 92037, | ||
393 | "state": "active", | 427 | "state": "active", | ||
394 | "url": | 428 | "url": | ||
395 | d506f76-9ddb-4fe8-802f-a8622e2cef68/download/o32q_p20-q10_l-even.zip", | 429 | d506f76-9ddb-4fe8-802f-a8622e2cef68/download/o32q_p20-q10_l-even.zip", | ||
396 | "url_type": "" | 430 | "url_type": "" | ||
397 | } | 431 | } | ||
398 | ], | 432 | ], | ||
399 | "services_used_list": "", | 433 | "services_used_list": "", | ||
400 | "source_metadata_created": "2023-07-18T08:02:31.540779", | 434 | "source_metadata_created": "2023-07-18T08:02:31.540779", | ||
t | 401 | "source_metadata_modified": "2023-08-11T09:54:56.209315", | t | 435 | "source_metadata_modified": "2024-08-09T13:57:11.370325", |
402 | "state": "active", | 436 | "state": "active", | ||
403 | "tags": [ | 437 | "tags": [ | ||
404 | { | 438 | { | ||
405 | "display_name": "Bethe ansatz", | 439 | "display_name": "Bethe ansatz", | ||
406 | "id": "236a2df8-c82e-46cb-9c3a-797353c800c3", | 440 | "id": "236a2df8-c82e-46cb-9c3a-797353c800c3", | ||
407 | "name": "Bethe ansatz", | 441 | "name": "Bethe ansatz", | ||
408 | "state": "active", | 442 | "state": "active", | ||
409 | "vocabulary_id": null | 443 | "vocabulary_id": null | ||
410 | }, | 444 | }, | ||
411 | { | 445 | { | ||
412 | "display_name": "finite-size data", | 446 | "display_name": "finite-size data", | ||
413 | "id": "66baf9c7-21c6-43e9-8bd4-cc3ba6869816", | 447 | "id": "66baf9c7-21c6-43e9-8bd4-cc3ba6869816", | ||
414 | "name": "finite-size data", | 448 | "name": "finite-size data", | ||
415 | "state": "active", | 449 | "state": "active", | ||
416 | "vocabulary_id": null | 450 | "vocabulary_id": null | ||
417 | }, | 451 | }, | ||
418 | { | 452 | { | ||
419 | "display_name": "quantum group symmetry", | 453 | "display_name": "quantum group symmetry", | ||
420 | "id": "9c065147-8501-4b50-a319-4c33b5cb723b", | 454 | "id": "9c065147-8501-4b50-a319-4c33b5cb723b", | ||
421 | "name": "quantum group symmetry", | 455 | "name": "quantum group symmetry", | ||
422 | "state": "active", | 456 | "state": "active", | ||
423 | "vocabulary_id": null | 457 | "vocabulary_id": null | ||
424 | }, | 458 | }, | ||
425 | { | 459 | { | ||
426 | "display_name": "superspin chains", | 460 | "display_name": "superspin chains", | ||
427 | "id": "98058706-37c4-4b7a-970d-e0297ce7b3db", | 461 | "id": "98058706-37c4-4b7a-970d-e0297ce7b3db", | ||
428 | "name": "superspin chains", | 462 | "name": "superspin chains", | ||
429 | "state": "active", | 463 | "state": "active", | ||
430 | "vocabulary_id": null | 464 | "vocabulary_id": null | ||
431 | } | 465 | } | ||
432 | ], | 466 | ], | ||
433 | "terms_of_usage": "Yes", | 467 | "terms_of_usage": "Yes", | ||
434 | "title": "Finite size data for U_q[OSp(3|2)] quantum chains with | 468 | "title": "Finite size data for U_q[OSp(3|2)] quantum chains with | ||
435 | quantum group invariant boundaries", | 469 | quantum group invariant boundaries", | ||
436 | "type": "vdataset", | 470 | "type": "vdataset", | ||
437 | "url": | 471 | "url": | ||
438 | ://data.uni-hannover.de/dataset/u_q-osp-3-2-invariant-quantum-chains", | 472 | ://data.uni-hannover.de/dataset/u_q-osp-3-2-invariant-quantum-chains", | ||
439 | "version": "" | 473 | "version": "" | ||
440 | } | 474 | } |