{"status":"ok","message-type":"work-list","message-version":"1.0.0","message":{"facets":{},"total-results":12305,"items":[{"indexed":{"date-parts":[[2022,6,23]],"date-time":"2022-06-23T23:43:29Z","timestamp":1656027809957},"reference-count":13,"publisher":"Stichting SciPost","issue":"7","license":[{"start":{"date-parts":[[2022,6,22]],"date-time":"2022-06-22T00:00:00Z","timestamp":1655856000000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"We investigate the production of CP-odd Higgs boson\nA^0<\/jats:tex-math>A<\/mml:mi>0<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nassociated with a real \\gamma<\/jats:tex-math>\u03b3<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nin e^+e^-<\/jats:tex-math>e<\/mml:mi>+<\/mml:mo><\/mml:msup>e<\/mml:mi>\u2212<\/mml:mo><\/mml:msup><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\ncollisions. Because of the properties of A^0<\/jats:tex-math>A<\/mml:mi>0<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\ncoupling to the other fields, the main contribution comes from the\ntop-quark triangle loop diagrams. We obtain the \u201ctimelike\u201d transition\nform factor which describes the production amplitude of\nA^0<\/jats:tex-math>A<\/mml:mi>0<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nin the e^+e^-<\/jats:tex-math>e<\/mml:mi>+<\/mml:mo><\/mml:msup>e<\/mml:mi>\u2212<\/mml:mo><\/mml:msup><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\ncollisions. This timelike transition form factor is related to the\nspacelike transition form factor relevant for the\nA^0<\/jats:tex-math>A<\/mml:mi>0<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nproduction in e^-\\gamma<\/jats:tex-math>e<\/mml:mi>\u2212<\/mml:mo><\/mml:msup>\u03b3<\/mml:mi><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\ncollisions. It turns out that the possible extra contributions from\nchargino-sneutrino and neutralino-selectron box diagrams do not give\nsizable effects.<\/jats:p>","DOI":"10.21468\/scipostphysproc.7.044","type":"journal-article","created":{"date-parts":[[2022,6,22]],"date-time":"2022-06-22T08:11:46Z","timestamp":1655885506000},"update-policy":"http:\/\/dx.doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":0,"title":["Timelike transition form factor for CP-odd Higgs boson production"],"prefix":"10.21468","author":[{"given":"Ken","family":"Sasaki","sequence":"first","affiliation":[{"name":"Yokohama National University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Tsuneo","family":"Uematsu","sequence":"additional","affiliation":[{"name":"Kyoto University"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2022,6,22]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2012.08.020"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2012.08.021"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.106\/j.physletb.2013.08.010"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.106\/j.physletb.2013.08.026"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.110.081803"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2013.11.051"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.90.033015"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2018.04.005"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.22323\/1.375.0021"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1016\/S0550-3213(96)00711-0"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1093\/ptep\/ptaa104"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(79)90234-7"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2017.10.044"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.7.044\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.7.044\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,6,22]],"date-time":"2022-06-22T08:11:48Z","timestamp":1655885508000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.7.044"}},"issued":{"date-parts":[[2022,6,22]]},"references-count":13,"journal-issue":{"issue":"7","published-online":{"date-parts":[[2022]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.7.044","archive":["CLOCKSS"],"ISSN":["2666-4003"],"issn-type":[{"value":"2666-4003","type":"electronic"}],"published":{"date-parts":[[2022,6,22]]},"article-number":"044"},{"indexed":{"date-parts":[[2022,6,22]],"date-time":"2022-06-22T08:43:22Z","timestamp":1655887402973},"reference-count":30,"publisher":"Stichting SciPost","issue":"7","license":[{"start":{"date-parts":[[2022,6,22]],"date-time":"2022-06-22T00:00:00Z","timestamp":1655856000000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"We study the non-linear background field redefinitions arising at the\nquantum level in a spontaneously broken effective gauge field theory.\nThe non-linear field redefinitions are crucial for the symmetric\n(i.e.\u00a0fulfilling all the relevant functional identities of the theory)\nrenormalization of gauge-invariant operators. In a general\nR_\\xi<\/jats:tex-math>R<\/mml:mi>\u03be<\/mml:mi><\/mml:msub><\/mml:math><\/jats:alternatives><\/jats:inline-formula>-gauge\nthe classical background-quantum splitting is also non-linearly deformed\nby radiative corrections. In the Landau gauge these deformations vanish\nto all orders in the loop expansion.<\/jats:p>","DOI":"10.21468\/scipostphysproc.7.045","type":"journal-article","created":{"date-parts":[[2022,6,22]],"date-time":"2022-06-22T08:22:24Z","timestamp":1655886144000},"update-policy":"http:\/\/dx.doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":0,"title":["Background field method and generalized field redefinitions in effective field theories"],"prefix":"10.21468","author":[{"given":"Andrea","family":"Quadri","sequence":"first","affiliation":[{"name":"National Institute for Nuclear Physics"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2022,6,22]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(86)90262-2"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP10(2010)085"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.23731\/CYRM-2017-002"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1016\/j.physrep.2018.11.002"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1016\/0370-1573(94)00112-G"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1007\/BF01090719"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(71)90297-5"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(96)00132-0"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1007\/BF02730284"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1016\/0370-2693(74)90058-6"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1088\/1126-6708\/2004\/11\/019"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRev.162.1195"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.12.482"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(81)90371-0"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(83)90337-1"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(95)00037-S"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.1016\/S0550-3213(99)00457-5"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(96)00017-X"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.1006\/aphy.2001.6198"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.120.251801"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.101.013005"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhys.10.6.144"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.93.065034"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.1140\/epjp\/s13360-021-01665-9"},{"key":"ref25","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP05(2020)141"},{"key":"ref26","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP09(2019)032"},{"key":"ref27","doi-asserted-by":"publisher","DOI":"10.1140\/epjc\/s10052-020-8349-0"},{"key":"ref28","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.73.065024"},{"key":"ref29","doi-asserted-by":"publisher","DOI":"10.1142\/S0217751X17500890"},{"key":"ref30","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP04(2018)050"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.7.045\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.7.045\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,6,22]],"date-time":"2022-06-22T08:22:27Z","timestamp":1655886147000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.7.045"}},"issued":{"date-parts":[[2022,6,22]]},"references-count":30,"journal-issue":{"issue":"7","published-online":{"date-parts":[[2022]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.7.045","archive":["CLOCKSS"],"ISSN":["2666-4003"],"issn-type":[{"value":"2666-4003","type":"electronic"}],"published":{"date-parts":[[2022,6,22]]},"article-number":"045"},{"indexed":{"date-parts":[[2023,9,30]],"date-time":"2023-09-30T16:43:39Z","timestamp":1696092219499},"reference-count":41,"publisher":"Stichting SciPost","issue":"13","license":[{"start":{"date-parts":[[2023,9,29]],"date-time":"2023-09-29T00:00:00Z","timestamp":1695945600000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"The scientific achievements of the Pierre Auger Collaboration cover diverse and complementary fields of research. The search for the origin of ultra-high energy cosmic rays (UHECRs) is based on the measurement of the energy spectrum and mass composition of the primaries, on studies of multi-messengers, and on extensive anisotropy searches. With the collected data it is also possible to explore the characteristics of hadronic interactions at energies unreachable at human-made accelerators, and to assess the existence of non-standard physics effects. A selection of the latest results is presented and the emerging picture is discussed.<\/jats:p>","DOI":"10.21468\/scipostphysproc.13.034","type":"journal-article","created":{"date-parts":[[2023,9,29]],"date-time":"2023-09-29T14:59:43Z","timestamp":1695999583000},"update-policy":"http:\/\/dx.doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":0,"title":["Astroparticle and particle physics at ultra-high energy: Results from the Pierre Auger Observatory"],"prefix":"10.21468","author":[{"given":"Antonella","family":"Castellina","sequence":"first","affiliation":[{"name":"INFN Sezione di Torino"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2023,9,29]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1016\/j.nima.2015.06.058"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.22323\/1.358.0231"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1126\/science.aan4338"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.3847\/1538-4357\/aae689"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.3847\/1538-4357\/ab7236"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.92.063014"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.3847\/2041-8213\/abf11e"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.3847\/1538-4357\/ac7d4e"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0375"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0308"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1140\/epjc\/s10052-021-09700-w"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.90.122006"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.96.122003"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.22323\/1.358.0440"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0387"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0321"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0337"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1051\/epjconf\/201921001009"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.1088\/1475-7516\/2019\/10\/022"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.3847\/1538-4357\/ac7393"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.1088\/1475-7516\/2019\/11\/004"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.3847\/1538-4357\/abb476"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0968"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0973"},{"key":"ref25","doi-asserted-by":"publisher","DOI":"10.1088\/1475-7516\/2017\/04\/038"},{"key":"ref26","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0311"},{"key":"ref27","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.125.121106"},{"key":"ref28","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.109.062002"},{"key":"ref29","doi-asserted-by":"publisher","DOI":"10.22323\/1.236.0401"},{"key":"ref30","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.91.032003"},{"key":"ref31","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.117.192001"},{"key":"ref32","doi-asserted-by":"publisher","DOI":"10.1140\/epjc\/s10052-020-8055-y"},{"key":"ref33","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.92.019903"},{"key":"ref34","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.96.122003"},{"key":"ref35","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.126.152002"},{"key":"ref36","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0310"},{"key":"ref37","doi-asserted-by":"publisher","DOI":"10.1088\/1475-7516\/2022\/01\/023"},{"key":"ref38","doi-asserted-by":"publisher","DOI":"10.22323\/1.395.0340"},{"key":"ref39","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.130.061001"},{"key":"ref40","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.107.042002"},{"key":"ref41","doi-asserted-by":"publisher","DOI":"10.1051\/epjconf\/201921006002"}],"container-title":["SciPost 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Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.13.034\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.13.034\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2023,9,29]],"date-time":"2023-09-29T14:59:46Z","timestamp":1695999586000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.13.034"}},"issued":{"date-parts":[[2023,9,29]]},"references-count":41,"journal-issue":{"issue":"13","published-online":{"date-parts":[[2023]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.13.034","archive":["CLOCKSS"],"ISSN":["2666-4003"],"issn-type":[{"value":"2666-4003","type":"electronic"}],"published":{"date-parts":[[2023,9,29]]},"article-number":"034"},{"indexed":{"date-parts":[[2022,7,12]],"date-time":"2022-07-12T07:42:06Z","timestamp":1657611726232},"reference-count":15,"publisher":"Stichting SciPost","issue":"8","license":[{"start":{"date-parts":[[2022,7,12]],"date-time":"2022-07-12T00:00:00Z","timestamp":1657584000000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"A new method is suggested for the extraction of\nu<\/jats:tex-math>u<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>-quark\nand d<\/jats:tex-math>d<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>-quark\ntransversity distributions, using single spin asymmetry (SSA) data in\nsemi-inclusive deep inelastic scattering (SIDIS) processes, where they\ncouple to the Collins or the di-hadron fragmentation functions. We\ndiscuss a recent suggestion to extract the transversity distribution\nusing the concept of difference asymmetries and their ratios, which\navoids the requirement of Collins function. We suggest new measurements,\ninvolving ratios of polarized cross-sections, that would directly probe\nthe ratio h_1^{d_v}\/h_1^{u_v}<\/jats:tex-math>h<\/mml:mi>1<\/mml:mn>d<\/mml:mi>v<\/mml:mi><\/mml:msub><\/mml:msubsup>\/<\/mml:mi>h<\/mml:mi>1<\/mml:mn>u<\/mml:mi>v<\/mml:mi><\/mml:msub><\/mml:msubsup><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>.\nWe also show some numerical estimates.<\/jats:p>","DOI":"10.21468\/scipostphysproc.8.052","type":"journal-article","created":{"date-parts":[[2022,7,12]],"date-time":"2022-07-12T07:09:39Z","timestamp":1657609779000},"update-policy":"http:\/\/dx.doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":0,"title":["A new method to extract the valence transversity distributions"],"prefix":"10.21468","author":[{"given":"Mauro","family":"Anselmino","sequence":"first","affiliation":[{"name":"University of Turin"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Raj","family":"Kishore","sequence":"additional","affiliation":[{"name":"Indian Institute of Technology Bombay"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Asmita","family":"Mukherjee","sequence":"additional","affiliation":[{"name":"Indian Institute of Technology Bombay"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2022,7,12]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(93)90262-N"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.75.054032"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1016\/j.nuclphysbps.2009.03.117"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.87.094019"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.93.014009"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.107.012001"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP03(2013)119"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP05(2015)123"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1088\/1126-6708\/2007\/02\/093"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.83.114019"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.102.096012"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.99.114004"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1140\/epjc\/s10052-009-1072-5"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.91.014035"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.63.094005"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.052\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.052\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,7,12]],"date-time":"2022-07-12T07:09:40Z","timestamp":1657609780000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.052"}},"issued":{"date-parts":[[2022,7,12]]},"references-count":15,"journal-issue":{"issue":"8","published-online":{"date-parts":[[2022]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.8.052","archive":["CLOCKSS"],"ISSN":["2666-4003"],"issn-type":[{"value":"2666-4003","type":"electronic"}],"published":{"date-parts":[[2022,7,12]]},"article-number":"052"},{"indexed":{"date-parts":[[2022,7,13]],"date-time":"2022-07-13T15:11:05Z","timestamp":1657725065887},"reference-count":13,"publisher":"Stichting SciPost","issue":"8","license":[{"start":{"date-parts":[[2022,7,13]],"date-time":"2022-07-13T00:00:00Z","timestamp":1657670400000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"The amount of data collected by the CMS experiment at the CERN LHC in the second data taking period provides the possibility to study absolute and differential cross sections of top quark interaction processes with high precision. Utilizing these results, fundamental standard model parameters such as the top quark mass are extracted. Moreover, given standard model measurements are interpreted in the context of beyond the standard model theories.\nRecent results on top quark properties and rare or anomalous top quark interactions by CMS are presented in these proceedings. 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Proc."],"abstract":"The Tile Calorimeter (TileCal) is a sampling calorimeter that forms the central region of the hadronic calorimeter of the ATLAS experiment. This sub-detector is to undergo its Phase-II upgrade during long-shutdown 3, in the years from 2025 to mid 2027, in preparation for the start of operation of the High Luminosity Large Hadron Collider (HL-LHC) in 2027. In this proceeding, an overview of the TileCal HL-LHC on-detector electronics upgrade is provided. The detectors Run-II performance in the cases of EM scale calibration, calorimeter response, cell energy distribution and noise as well as a portion of the 2015-2018 Test-beam campaigns results are examined.<\/jats:p>","DOI":"10.21468\/scipostphysproc.8.171","type":"journal-article","created":{"date-parts":[[2022,7,14]],"date-time":"2022-07-14T13:57:26Z","timestamp":1657807046000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":0,"title":["The ATLAS Tile Calorimeter performance and its upgrade towards the High Luminosity Large Hadron Collider"],"prefix":"10.21468","author":[{"given":"Ryan","family":"Mckenzie","sequence":"first","affiliation":[{"name":"University of the Witwatersrand"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2022,7,14]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1088\/1748-0221\/3\/08\/s08003"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1140\/epjc\/s10052-021-09292-5"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1016\/S0168-9002(03)01368-8"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.171\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.171\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,7,14]],"date-time":"2022-07-14T13:57:28Z","timestamp":1657807048000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.171"}},"issued":{"date-parts":[[2022,7,14]]},"references-count":3,"journal-issue":{"issue":"8","published-online":{"date-parts":[[2022]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.8.171","archive":["CLOCKSS"],"ISSN":["2666-4003"],"issn-type":[{"type":"electronic","value":"2666-4003"}],"published":{"date-parts":[[2022,7,14]]},"article-number":"171"},{"indexed":{"date-parts":[[2025,2,21]],"date-time":"2025-02-21T23:40:27Z","timestamp":1740181227466,"version":"3.37.3"},"reference-count":10,"publisher":"Stichting SciPost","issue":"8","license":[{"start":{"date-parts":[[2022,7,11]],"date-time":"2022-07-11T00:00:00Z","timestamp":1657497600000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/100000015","name":"United States Department of Energy","doi-asserted-by":"publisher","award":["DE-SC0013393"],"award-info":[{"award-number":["DE-SC0013393"]}],"id":[{"id":"10.13039\/100000015","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"Transverse single spin asymmetries of particles produced in\np+p^{\\uparrow}<\/jats:tex-math>p<\/mml:mi>+<\/mml:mo>p<\/mml:mi>\u2191<\/mml:mo><\/mml:msup><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\ncollisions provide insight on the partonic spin and momentum structure\nof hadrons; heavy flavor electrons provide access to initial state\nspin-momentum correlations of gluons in the proton, while charged pions\nprovide access to initial and final state transverse spin effects.\nCharged particles are measured at midrapidity at PHENIX using the\nsilicon vertex detector and central arm spectrometer, made of an\nelectromagnetic calorimeter, a ring-imaging Cherenkov detector, and\ndrift and pad chambers. Recent results for both electron and charged\npion measurements from the 2015 running period will be presented.<\/jats:p>","DOI":"10.21468\/scipostphysproc.8.012","type":"journal-article","created":{"date-parts":[[2022,7,11]],"date-time":"2022-07-11T06:48:16Z","timestamp":1657522096000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":0,"title":["Transverse Single Spin Asymmetries of Heavy Flavor Electrons and Charged Pions in 200 GeV $p+p^{\\uparrow}$ Collisions at Midrapidity"],"prefix":"10.21468","author":[{"given":"Dillon","family":"Fitzgerald","sequence":"first","affiliation":[{"name":"University of Michigan\u2013Ann Arbor"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2022,7,11]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.95.112001"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.41.1689"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.85.655"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.98.012006"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1142\/S0217751X16300490"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1007\/s00601-014-0929-9"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.103.052009"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.95.202001"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.82.112008"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.78.114013"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.012\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.012\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,7,11]],"date-time":"2022-07-11T06:48:18Z","timestamp":1657522098000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.012"}},"issued":{"date-parts":[[2022,7,11]]},"references-count":10,"journal-issue":{"issue":"8","published-online":{"date-parts":[[2022]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.8.012","archive":["CLOCKSS"],"ISSN":["2666-4003"],"issn-type":[{"type":"electronic","value":"2666-4003"}],"published":{"date-parts":[[2022,7,11]]},"article-number":"012"},{"indexed":{"date-parts":[[2025,9,27]],"date-time":"2025-09-27T07:52:29Z","timestamp":1758959549433,"version":"3.37.3"},"reference-count":11,"publisher":"Stichting SciPost","issue":"8","license":[{"start":{"date-parts":[[2022,7,14]],"date-time":"2022-07-14T00:00:00Z","timestamp":1657756800000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/501100007175","name":"Centre National de la Recherche Scientifique","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100007175","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100006489","name":"Commissariat \u00e0 l'\u00c9nergie Atomique et aux \u00c9nergies Alternatives","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100006489","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100004007","name":"Instituto Nazionale di Fisica Nucleare","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100004007","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100012190","name":"Ministry of Science and Higher Education of the Russian Federation","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100012190","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100003725","name":"National Research Foundation of Korea","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100003725","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/100000001","name":"National Science Foundation","doi-asserted-by":"publisher","id":[{"id":"10.13039\/100000001","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100000271","name":"Science and Technology Facilities Council","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100000271","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/100000015","name":"United States Department of Energy","doi-asserted-by":"publisher","award":["DE-AC05-06OR23177"],"award-info":[{"award-number":["DE-AC05-06OR23177"]}],"id":[{"id":"10.13039\/100000015","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"High precision measurements of the polarized electron beam-spin\nasymmetry in SIDIS from the proton have been performed using a 10.6 GeV\nincident electron beam and the CLAS12 spectrometer at Jefferson Lab. The\nproceeding reports a multidimensional study of the structure function\nratio F^{sin\\phi}_{LU}\/F_{UU}<\/jats:tex-math>F<\/mml:mi>L<\/mml:mi>U<\/mml:mi><\/mml:mrow>s<\/mml:mi>i<\/mml:mi>n<\/mml:mi>\u03d5<\/mml:mi><\/mml:mrow><\/mml:msubsup>\/<\/mml:mi>F<\/mml:mi>U<\/mml:mi>U<\/mml:mi><\/mml:mrow><\/mml:msub><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nextracted from single pion (\\pi^{+}<\/jats:tex-math>\u03c0<\/mml:mi>+<\/mml:mo><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>,\n\\pi^{-}<\/jats:tex-math>\u03c0<\/mml:mi>\u2212<\/mml:mo><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>,\n\\pi^{0}<\/jats:tex-math>\u03c0<\/mml:mi>0<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>)\nSIDIS data over a large kinematic range in\nz<\/jats:tex-math>z<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>,\nx_{B}<\/jats:tex-math>x<\/mml:mi>B<\/mml:mi><\/mml:msub><\/mml:math><\/jats:alternatives><\/jats:inline-formula>,\nP_{T}<\/jats:tex-math>P<\/mml:mi>T<\/mml:mi><\/mml:msub><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nand virtualities Q^{2}<\/jats:tex-math>Q<\/mml:mi>2<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nranging from 1~GeV^2<\/jats:tex-math>2<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nup to 7~GeV^2<\/jats:tex-math>2<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>.\nF^{sin\\phi}_{LU}<\/jats:tex-math>F<\/mml:mi>L<\/mml:mi>U<\/mml:mi><\/mml:mrow>s<\/mml:mi>i<\/mml:mi>n<\/mml:mi>\u03d5<\/mml:mi><\/mml:mrow><\/mml:msubsup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nis a twist-3 quantity that can reveal novel properties of quark-gluon\ncorrelations within the nucleon.<\/jats:p>","DOI":"10.21468\/scipostphysproc.8.149","type":"journal-article","created":{"date-parts":[[2022,7,14]],"date-time":"2022-07-14T09:12:57Z","timestamp":1657789977000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":1,"title":["Multidimensional, high precision beam spin asymmetry measurements of semi-inclusive pion production off the proton with CLAS12"],"prefix":"10.21468","author":[{"given":"Stefan","family":"Diehl","sequence":"first","affiliation":[{"name":"University of Giessen"},{"name":"University of Connecticut"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2022,7,14]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1016\/j.physrep.2018.03.002"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1146\/annurev-nucl-011720-042725"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2005.05.037"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1088\/1126-6708\/2007\/02\/093"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1016\/j.ppnp.2016.08.003"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2018.11.033"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1016\/0370-2693(94)91391-9"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1016\/j.ppnp.2020.103806"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1016\/j.nima.2020.163419"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.128.062005"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.89.072011"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.149\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.149\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,7,14]],"date-time":"2022-07-14T09:13:02Z","timestamp":1657789982000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.149"}},"issued":{"date-parts":[[2022,7,14]]},"references-count":11,"journal-issue":{"issue":"8","published-online":{"date-parts":[[2022]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.8.149","archive":["CLOCKSS"],"ISSN":["2666-4003"],"issn-type":[{"type":"electronic","value":"2666-4003"}],"published":{"date-parts":[[2022,7,14]]},"article-number":"149"},{"indexed":{"date-parts":[[2026,4,1]],"date-time":"2026-04-01T12:22:05Z","timestamp":1775046125975,"version":"3.50.1"},"reference-count":29,"publisher":"Stichting SciPost","issue":"5","license":[{"start":{"date-parts":[[2018,11,5]],"date-time":"2018-11-05T00:00:00Z","timestamp":1541376000000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/501100002347","name":"Bundesministerium f\u00fcr Bildung und Forschung","doi-asserted-by":"publisher","award":["05P12VHCTG"],"award-info":[{"award-number":["05P12VHCTG"]}],"id":[{"id":"10.13039\/501100002347","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100001659","name":"Deutsche Forschungsgemeinschaft","doi-asserted-by":"publisher","award":["SFB 1225"],"award-info":[{"award-number":["SFB 1225"]}],"id":[{"id":"10.13039\/501100001659","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100001659","name":"Deutsche Forschungsgemeinschaft","doi-asserted-by":"publisher","award":["STA 283\/16-2"],"award-info":[{"award-number":["STA 283\/16-2"]}],"id":[{"id":"10.13039\/501100001659","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys."],"abstract":"\n One of the main challenges in simulations on Lefschetz thimbles is\nthe computation of the relative weights of contributing thimbles. In\nthis paper we propose a solution to that problem by means of computing\nthose weights using a reweighting procedure. Besides we present recipes\nfor finding parametrizations of thimbles and anti-thimbles for a given\ntheory. Moreover, we study some approaches to combine the Lefschetz\nthimble method with the Complex Langevin evolution. Our numerical\ninvestigations are carried out by using toy models among which we\nconsider a one-site\n \n \n z^4<\/jats:tex-math>\n \n \n z<\/mml:mi>\n 4<\/mml:mn>\n <\/mml:msup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n model as well as a\n \n \n U(1)<\/jats:tex-math>\n \n \n U<\/mml:mi>\n (<\/mml:mo>\n 1<\/mml:mn>\n )<\/mml:mo>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n one-link model.\n <\/jats:p>","DOI":"10.21468\/scipostphys.5.5.044","type":"journal-article","created":{"date-parts":[[2018,11,5]],"date-time":"2018-11-05T03:56:48Z","timestamp":1541390208000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":17,"title":["Reweighting Lefschetz Thimbles"],"prefix":"10.21468","volume":"5","author":[{"given":"Stefan","family":"Bluecher","sequence":"first","affiliation":[{"name":"Heidelberg University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Jan M.","family":"Pawlowski","sequence":"additional","affiliation":[{"name":"ExtreMe Matter Institute"},{"name":"Heidelberg University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Manuel","family":"Scherzer","sequence":"additional","affiliation":[{"name":"Heidelberg University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Mike","family":"Schlosser","sequence":"additional","affiliation":[{"name":"Heidelberg University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Ion-Olimpiu","family":"Stamatescu","sequence":"additional","affiliation":[{"name":"Heidelberg University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Sebastian","family":"Syrkowski","sequence":"additional","affiliation":[{"name":"Heidelberg University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Felix","family":"Ziegler","sequence":"additional","affiliation":[{"name":"Heidelberg University"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2018,11,5]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2015.11.011"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.113.072001"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.22323\/1.091.0010"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.22323\/1.214.0016"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.22323\/1.187.0002"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.22323\/1.251.0016"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.66.074507"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1016\/S0550-3213(02)00626-0"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.67.014505"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1016\/S0370-2693(02)01583-6"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.90.094502"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1088\/1126-6708\/2008\/09\/018"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2014.01.019"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.86.074506"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.88.051501"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.89.114505"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.97.014503"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1051\/epjconf\/201817507015"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.22323\/1.256.0076"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.93.014504"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP03(2015)044"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.117.081602"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP10(2017)100"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.96.111501"},{"key":"ref25","doi-asserted-by":"publisher","DOI":"10.1093\/ptep\/ptx191"},{"key":"ref26","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.97.094510"},{"key":"ref27","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP10(2014)159"},{"key":"ref28","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP06(2017)023"},{"key":"ref29","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP03(2013)073"}],"container-title":["SciPost Physics"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.5.5.044\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.5.5.044\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2018,11,5]],"date-time":"2018-11-05T03:56:50Z","timestamp":1541390210000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.5.5.044"}},"issued":{"date-parts":[[2018,11,5]]},"references-count":29,"journal-issue":{"issue":"5","published-online":{"date-parts":[[2018]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphys.5.5.044","archive":["CLOCKSS"],"relation":{"has-review":[{"id-type":"doi","id":"10.21468\/SciPost.Report.524","asserted-by":"object"},{"id-type":"doi","id":"10.21468\/SciPost.Report.551","asserted-by":"object"}]},"published":{"date-parts":[[2018,11,5]]},"article-number":"044"},{"indexed":{"date-parts":[[2026,4,1]],"date-time":"2026-04-01T12:42:56Z","timestamp":1775047376921,"version":"3.50.1"},"reference-count":24,"publisher":"Stichting SciPost","issue":"3","license":[{"start":{"date-parts":[[2020,2,27]],"date-time":"2020-02-27T00:00:00Z","timestamp":1582761600000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/501100002261","name":"Russian Foundation for Basic Research","doi-asserted-by":"publisher","award":["19-02-00079a"],"award-info":[{"award-number":["19-02-00079a"]}],"id":[{"id":"10.13039\/501100002261","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"\n We study deuteron- proton elastic scattering in the deuteron energy\nrange between 500 MeV and 2\u00a0GeV at the cms scattering angle\n \n \n \\theta^*\\ge 140^\\circ<\/jats:tex-math>\n \n \n \n \u03b8<\/mml:mi>\n *<\/mml:mo>\n <\/mml:msup>\n \u2265<\/mml:mo>\n \n 140<\/mml:mn>\n \u2218<\/mml:mo>\n <\/mml:msup>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n .\nThe reaction is considered in the relativistic multiple scattering\nexpansion framework. The four reaction mechanisms are included into\nconsideration: one-nucleon exchange, single scattering, double\nscattering, and the term corresponding to the delta excitation in the\nintermediate state.\n <\/jats:p>\n \n The model is applied to describe the angular dependence of the\ndifferential cross section at the deuteron energies of between 880 and\n1300 MeV. Also the energy dependence of the differential cross section\nand polarisation observables such as tensor analyzing power\n \n \n T_{20}<\/jats:tex-math>\n \n \n T<\/mml:mi>\n 20<\/mml:mn>\n <\/mml:msub>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n and polarization transfer from the deuteron to proton\n \n \n \\varkappa<\/jats:tex-math>\n \n \ud835\udf18<\/mml:mo>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n are considered at the scattering angle equal to\n180\n \n \n ^\\circ<\/jats:tex-math>\n \n \n \n \u2218<\/mml:mo>\n <\/mml:msup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n .\nContributions of the different reaction mechanisms into the reaction\namplitude are demonstrated in comparison with the existing experimental\ndata.\n <\/jats:p>","DOI":"10.21468\/scipostphysproc.3.053","type":"journal-article","created":{"date-parts":[[2020,2,27]],"date-time":"2020-02-27T06:32:30Z","timestamp":1582785150000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":2,"title":["Study of deuteron-proton backward elastic scattering at intermediate energies"],"prefix":"10.21468","author":[{"given":"Nadezhda","family":"Ladygina","sequence":"first","affiliation":[{"name":"Joint Institute for Nuclear Research"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2020,2,27]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1016\/0370-1573(95)00085-2"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.96.064001"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.16.944"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.17.827"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRev.180.1483"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.67.034001"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.68.024005"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1134\/S1063778808120053"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1140\/epja\/i2009-10852-0"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1140\/epja\/i2016-16199-5"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1016\/S0370-1573(87)80002-9"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.63.024001"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1016\/0370-2693(81)90659-6"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.24.1073"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.27.438"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.1016\/0370-1573(93)90037-E"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.1016\/0375-9474(86)90158-2"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.6.2010"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.4.1261"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.24.236"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.6.457"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.39.1253"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.1016\/0375-9474(84)90272-0"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.1016\/0370-2693(95)00344-K"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.3.053\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.3.053\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2020,2,27]],"date-time":"2020-02-27T06:32:32Z","timestamp":1582785152000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.3.053"}},"issued":{"date-parts":[[2020,2,27]]},"references-count":24,"journal-issue":{"issue":"3","published-online":{"date-parts":[[2020]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.3.053","archive":["CLOCKSS"],"relation":{"has-review":[{"id-type":"doi","id":"10.21468\/SciPost.Report.1503","asserted-by":"object"}]},"ISSN":["2666-4003"],"issn-type":[{"value":"2666-4003","type":"electronic"}],"published":{"date-parts":[[2020,2,27]]},"article-number":"053"},{"indexed":{"date-parts":[[2026,3,30]],"date-time":"2026-03-30T16:37:20Z","timestamp":1774888640444,"version":"3.50.1"},"reference-count":11,"publisher":"Stichting SciPost","issue":"8","license":[{"start":{"date-parts":[[2022,7,13]],"date-time":"2022-07-13T00:00:00Z","timestamp":1657670400000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/100000015","name":"United States Department of Energy","doi-asserted-by":"publisher","award":["DE-SC0004286"],"award-info":[{"award-number":["DE-SC0004286"]}],"id":[{"id":"10.13039\/100000015","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys. Proc."],"abstract":"The small-x<\/jats:tex-math>x<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nquark helicity evolution equations at double-logarithmic order, with the\nkernel \\sim\\alpha_s\\ln^2(1\/x)<\/jats:tex-math>\u223c<\/mml:mo>\u03b1<\/mml:mi>s<\/mml:mi><\/mml:msub>ln<\/mml:mo>2<\/mml:mn><\/mml:msup>(<\/mml:mo>1<\/mml:mn>\/<\/mml:mi>x<\/mml:mi>)<\/mml:mo><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>,\nhave been derived previously. In this\nwork, we derive the single-logarithmic corrections to the equations, to\norder \\alpha_s\\ln(1\/x)<\/jats:tex-math>\u03b1<\/mml:mi>s<\/mml:mi><\/mml:msub>ln<\/mml:mo>(<\/mml:mo>1<\/mml:mn>\/<\/mml:mi>x<\/mml:mi>)<\/mml:mo><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nof the evolution kernel. The new equations include the effects of the\nrunning coupling and the unpolarized\nsmall-x<\/jats:tex-math>x<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nevolution, both of which are parametrically significant at\nsingle-logarithmic order. The large-N_c<\/jats:tex-math>N<\/mml:mi>c<\/mml:mi><\/mml:msub><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nand large-N_c\\ N_f<\/jats:tex-math>N<\/mml:mi>c<\/mml:mi><\/mml:msub>N<\/mml:mi>f<\/mml:mi><\/mml:msub><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\napproximations to the equation are computed. (Here,\nN_c<\/jats:tex-math>N<\/mml:mi>c<\/mml:mi><\/mml:msub><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nand N_f<\/jats:tex-math>N<\/mml:mi>f<\/mml:mi><\/mml:msub><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nare the numbers of quark colors and flavors, respectively.) Their\nsolutions will provide more precise estimates of the quark helicity\ndistribution at small x<\/jats:tex-math>x<\/mml:mi><\/mml:math><\/jats:alternatives><\/jats:inline-formula>,\ncontributing to the resolution of the proton spin puzzle.<\/jats:p>","DOI":"10.21468\/scipostphysproc.8.103","type":"journal-article","created":{"date-parts":[[2022,7,13]],"date-time":"2022-07-13T08:29:59Z","timestamp":1657700999000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":1,"title":["Single-Logarithmic Corrections to Small-$x$ Helicity Evolution"],"prefix":"10.21468","author":[{"given":"Yossathorn","family":"Tawabutr","sequence":"first","affiliation":[{"name":"The Ohio State University"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2022,7,13]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP03(2022)184"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(90)90506-9"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP10(2017)198"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.99.054032"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP01(2016)072"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.118.052001"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.75.014001"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1016\/j.nuclphysa.2006.10.075"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1016\/j.physletb.2017.06.032"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP08(2020)014"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.104.L031501"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.103\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.103\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,7,13]],"date-time":"2022-07-13T08:30:01Z","timestamp":1657701001000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.8.103"}},"issued":{"date-parts":[[2022,7,13]]},"references-count":11,"journal-issue":{"issue":"8","published-online":{"date-parts":[[2022]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.8.103","archive":["CLOCKSS"],"ISSN":["2666-4003"],"issn-type":[{"value":"2666-4003","type":"electronic"}],"published":{"date-parts":[[2022,7,13]]},"article-number":"103"},{"indexed":{"date-parts":[[2025,12,31]],"date-time":"2025-12-31T16:00:09Z","timestamp":1767196809214,"version":"build-2238731810"},"update-to":[{"DOI":"10.21468\/scipostphys.16.2.057","type":"correction","label":"Correction","source":"publisher","updated":{"date-parts":[[2024,2,27]],"date-time":"2024-02-27T00:00:00Z","timestamp":1708992000000}}],"reference-count":0,"publisher":"Stichting SciPost","content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys."],"DOI":"10.21468\/scipostphys.16.2.057-update-1","type":"journal-article","created":{"date-parts":[[2024,2,27]],"date-time":"2024-02-27T11:00:01Z","timestamp":1709031601000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":0,"title":["Correction: The Virasoro minimal string"],"prefix":"10.21468","author":[{"given":"Scott","family":"Collier","sequence":"first","affiliation":[{"id":[{"id":"https:\/\/ror.org\/042nb2s44","id-type":"ROR","asserted-by":"publisher"}],"name":"Massachusetts Institute of Technology"},{"id":[{"id":"https:\/\/ror.org\/00hx57361","id-type":"ROR","asserted-by":"publisher"}],"name":"Princeton University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Lorenz","family":"Eberhardt","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/00f809463","id-type":"ROR","asserted-by":"publisher"}],"name":"Institute for Advanced Study"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Beatrix","family":"Muehlmann","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/01pxwe438","id-type":"ROR","asserted-by":"publisher"}],"name":"McGill University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Victor A.","family":"Rodriguez","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/00hx57361","id-type":"ROR","asserted-by":"publisher"}],"name":"Princeton University"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2024,2,27]]},"container-title":["SciPost Physics"],"deposited":{"date-parts":[[2024,2,27]],"date-time":"2024-02-27T11:00:03Z","timestamp":1709031603000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.16.2.057-update-1"}},"issued":{"date-parts":[[2024,2,27]]},"references-count":0,"URL":"https:\/\/doi.org\/10.21468\/scipostphys.16.2.057-update-1","ISSN":["2542-4653"],"issn-type":[{"value":"2542-4653","type":"electronic"}],"published":{"date-parts":[[2024,2,27]]}},{"indexed":{"date-parts":[[2026,3,18]],"date-time":"2026-03-18T16:47:51Z","timestamp":1773852471629,"version":"3.50.1"},"reference-count":99,"publisher":"Stichting SciPost","issue":"5","license":[{"start":{"date-parts":[[2022,5,3]],"date-time":"2022-05-03T00:00:00Z","timestamp":1651536000000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/501100000781","name":"European Research Council","doi-asserted-by":"publisher","award":["771536"],"award-info":[{"award-number":["771536"]}],"id":[{"id":"10.13039\/501100000781","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/100009566","name":"Foundational Questions Institute","doi-asserted-by":"publisher","award":["FQXi-IAF19-03-S2"],"award-info":[{"award-number":["FQXi-IAF19-03-S2"]}],"id":[{"id":"10.13039\/100009566","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100004329","name":"Javna Agencija za Raziskovalno Dejavnost RS","doi-asserted-by":"publisher","award":["N1-0109"],"award-info":[{"award-number":["N1-0109"]}],"id":[{"id":"10.13039\/501100004329","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100003825","name":"Magyar Tudom\u00e1nyos Akad\u00e9mia","doi-asserted-by":"publisher","award":["\u00daNKP-21-5"],"award-info":[{"award-number":["\u00daNKP-21-5"]}],"id":[{"id":"10.13039\/501100003825","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100011019","name":"Nemzeti Kutat\u00e1si, Fejleszt\u00e9si \u00e9s Innov\u00e1ci\u00f3s Hivatal","doi-asserted-by":"publisher","award":["K 138606"],"award-info":[{"award-number":["K 138606"]}],"id":[{"id":"10.13039\/501100011019","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100011019","name":"Nemzeti Kutat\u00e1si, Fejleszt\u00e9si \u00e9s Innov\u00e1ci\u00f3s Hivatal","doi-asserted-by":"publisher","award":["SNN139581"],"award-info":[{"award-number":["SNN139581"]}],"id":[{"id":"10.13039\/501100011019","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys."],"abstract":"We study inhomogeneous quantum quenches in the attractive regime of the sine--Gordon model. In our protocol, the system is prepared in an inhomogeneous initial state in finite volume by coupling the topological charge density operator to a Gaussian external field. After switching off the external field, the subsequent time evolution is governed by the homogeneous sine--Gordon Hamiltonian. Varying either the interaction strength of the sine--Gordon model or the amplitude of the external source field, an interesting transition is observed in the expectation value of the soliton density. This affects both the initial profile of the density and its time evolution and can be summarised as a steep transition between behaviours reminiscent of the Klein--Gordon, and the free massive Dirac fermion theory with initial external fields of high enough magnitude. The transition in the initial state is also displayed by the classical sine--Gordon theory and hence can be understood by semi-classical considerations in terms of the presence of small amplitude field configurations and the appearance of soliton excitations, which are naturally associated with bosonic and fermionic excitations on the quantum level, respectively. Features of the quantum dynamics are also consistent with this correspondence and comparing them to the classical evolution of the density profile reveals that quantum effects become markedly pronounced during the time evolution. These results suggest a crossover between the dominance of bosonic and fermionic degrees of freedom whose precise identification in terms of the fundamental particle excitations can be rather non-trivial. Nevertheless, their interplay is expected to influence the sine--Gordon dynamics in arbitrary inhomogeneous settings.<\/jats:p>","DOI":"10.21468\/scipostphys.12.5.144","type":"journal-article","created":{"date-parts":[[2022,5,3]],"date-time":"2022-05-03T03:16:43Z","timestamp":1651547803000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":25,"title":["Inhomogeneous quantum quenches in the sine-Gordon theory"],"prefix":"10.21468","volume":"12","author":[{"given":"David","family":"Horvath","sequence":"first","affiliation":[{"name":"INFN Trieste"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Spyros","family":"Sotiriadis","sequence":"additional","affiliation":[{"name":"Freie Universit\u00e4t Berlin"},{"name":"University of Ljubljana"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"M\u00e1rton","family":"Kormos","sequence":"additional","affiliation":[{"name":"Budapest University of Technology and Economics"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Gabor","family":"Takacs","sequence":"additional","affiliation":[{"name":"Budapest University of Technology and 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dependent Yukawa interactions.\nIn contrast to the previously studied models, the random Yukawa couplings are sampled from a collection of Gaussian ensembles whose variances follow a continuous distribution rather than being fixed to a constant.\nBy tuning the analytic behaviour of the distribution, we could control the fermion incoherence to systematically examine various normal states ranging from the Fermi liquid to non-Fermi liquids that are different from the conformal solution of the SYK model with a constant variance.\nUsing the linearised Eliashberg theory, we show that the onset of the unconventional spin-triplet pairing is preferred with the spin-dependent interactions while all pairing channels show instabilities with the spin-independent interactions.\nAlthough the interactions shorten the lifetime of the fermions in the non-Fermi liquid, the same interactions also dress the bosons to strengthen the tendency to pair the incoherent fermions.\nAs a consequence, the onset temperature\n \n \n T_c<\/jats:tex-math>\n \n \n T<\/mml:mi>\n c<\/mml:mi>\n <\/mml:msub>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n of the pairing is enhanced in the non-Fermi liquid compared to the case of the Fermi liquid.\n <\/jats:p>","DOI":"10.21468\/scipostphys.12.5.151","type":"journal-article","created":{"date-parts":[[2022,5,9]],"date-time":"2022-05-09T03:21:31Z","timestamp":1652066491000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":10,"title":["Pairing instabilities of the Yukawa-SYK models with controlled fermion incoherence"],"prefix":"10.21468","volume":"12","author":[{"given":"Wonjune","family":"Choi","sequence":"first","affiliation":[{"name":"Munich Center for Quantum Science and Technology"},{"name":"Technical University of Munich"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Omid","family":"Tavakol","sequence":"additional","affiliation":[{"name":"University of Toronto"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Yong Baek","family":"Kim","sequence":"additional","affiliation":[{"name":"University of Toronto"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2022,5,9]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.78.17"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.84.1383"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1209\/epl\/i2001-00266-0"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1038\/nature06480"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1038\/nature14165"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1088\/1361-6633\/80\/1\/014503"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1146\/annurev-conmatphys-070909-103925"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.73.174501"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1038\/srep22715"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.95.165137"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1088\/0034-4885\/66\/8\/202"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.92.045118"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.80.155129"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.80.165102"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.82.045121"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.82.075127"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.82.075128"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.123.066601"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.91.115111"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.102.024524"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.102.024525"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.80.035117"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.70.3339"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevX.8.031024"},{"key":"ref25","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.119.216601"},{"key":"ref26","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.124.017002"},{"key":"ref27","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.103.195108"},{"key":"ref28","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevResearch.2.033084"},{"key":"ref29","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevResearch.3.013250"},{"key":"ref30","doi-asserted-by":"publisher","DOI":"10.3367\/ufne.2020.06.038805"},{"key":"ref31","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.95.205105"},{"key":"ref32","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.104.L020509"},{"key":"ref33","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevResearch.2.033025"},{"key":"ref34","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.100.115132"},{"key":"ref35","doi-asserted-by":"publisher","DOI":"10.1016\/j.aop.2020.168120"},{"key":"ref36","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevResearch.2.013301"},{"key":"ref37","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.101.125112"},{"key":"ref38","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.102.085134"},{"key":"ref39","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.104.125120"}],"container-title":["SciPost Physics"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.12.5.151\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.12.5.151\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,5,9]],"date-time":"2022-05-09T03:21:33Z","timestamp":1652066493000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.12.5.151"}},"issued":{"date-parts":[[2022,5,9]]},"references-count":39,"journal-issue":{"issue":"5","published-online":{"date-parts":[[2022]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphys.12.5.151","archive":["CLOCKSS"],"relation":{"has-review":[{"id-type":"doi","id":"10.21468\/SciPost.Report.3998","asserted-by":"object"},{"id-type":"doi","id":"10.21468\/SciPost.Report.3792","asserted-by":"object"}]},"ISSN":["2542-4653"],"issn-type":[{"value":"2542-4653","type":"electronic"}],"published":{"date-parts":[[2022,5,9]]},"article-number":"151"},{"indexed":{"date-parts":[[2026,3,24]],"date-time":"2026-03-24T04:28:50Z","timestamp":1774326530346,"version":"3.50.1"},"reference-count":39,"publisher":"Stichting SciPost","issue":"5","license":[{"start":{"date-parts":[[2021,11,12]],"date-time":"2021-11-12T00:00:00Z","timestamp":1636675200000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/100000001","name":"National Science Foundation","doi-asserted-by":"publisher","award":["DMR-1906325"],"award-info":[{"award-number":["DMR-1906325"]}],"id":[{"id":"10.13039\/100000001","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/100000015","name":"United States Department of Energy","doi-asserted-by":"publisher","award":["DE-SC-0019274"],"award-info":[{"award-number":["DE-SC-0019274"]}],"id":[{"id":"10.13039\/100000015","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys."],"abstract":"Majorana zero modes are expected to arise in\nsemiconductor-superconductor hybrid systems, with potential topological\nquantum computing applications. One limitation of this approach is the\nneed for a relatively high external magnetic field that should also\nchange direction at the nanoscale. This proposal considers devices that\nincorporate micromagnets to address this challenge. We perform numerical\nsimulations of stray magnetic fields from different micromagnet\nconfigurations, which are then used to solve for Majorana wavefunctions.\nSeveral devices are proposed, starting with the basic four-magnet design\nto align magnetic field with the nanowire and scaling up to nanowire\nT-junctions. The feasibility of the approach is assessed by performing\nmagnetic imaging of prototype patterns.<\/jats:p>","DOI":"10.21468\/scipostphys.11.5.090","type":"journal-article","created":{"date-parts":[[2021,11,12]],"date-time":"2021-11-12T10:58:06Z","timestamp":1636714686000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":16,"title":["Integrating micromagnets and hybrid nanowires for topological quantum computing"],"prefix":"10.21468","volume":"11","author":[{"given":"Malcolm","family":"Jardine","sequence":"first","affiliation":[{"name":"University of Pittsburgh"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"John","family":"Stenger","sequence":"additional","affiliation":[{"name":"University of Pittsburgh"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Yifan","family":"Jiang","sequence":"additional","affiliation":[{"name":"University of Pittsburgh"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Eline J.","family":"de Jong","sequence":"additional","affiliation":[{"name":"Eindhoven University of Technology"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Wenbo","family":"Wang","sequence":"additional","affiliation":[{"name":"University of California, Santa Barbara"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Ania C.","family":"Bleszynski Jayich","sequence":"additional","affiliation":[{"name":"University of California, Santa Barbara"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Sergey","family":"Frolov","sequence":"additional","affiliation":[{"name":"University of Pittsburgh"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2021,11,12]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.105.177002"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.105.077001"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1038\/npjqi.2015.1"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevX.6.031016"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1126\/science.1222360"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1038\/nature17162"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1126\/science.aaf3961"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1038\/nnano.2013.267"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1038\/s41567-020-01107-w"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1038\/s41567-020-0925-6"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.109.236801"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevX.3.011008"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.85.020503"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1038\/s41563-019-0457-6"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevApplied.12.034048"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.102.224501"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.102.125425"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevApplied.10.054071"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.1021\/acs.nanolett.9b04187"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.1038\/s41567-020-1017-3"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhys.10.5.108"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.103.165301"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.103.134506"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevMaterials.5.064606"},{"key":"ref25","doi-asserted-by":"publisher","DOI":"10.1063\/1.4899186"},{"key":"ref26","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.98.085407"},{"key":"ref27","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.89.245405"},{"key":"ref28","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.90.115429"},{"key":"ref29","doi-asserted-by":"publisher","DOI":"10.1088\/1361-6528\/abc70f"},{"key":"ref30","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.87.075438"},{"key":"ref31","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevResearch.1.033207"},{"key":"ref32","doi-asserted-by":"publisher","DOI":"10.5281\/zenodo.5091744"},{"key":"ref33","doi-asserted-by":"publisher","DOI":"10.1070\/1063-7869\/44\/10s\/s29"},{"key":"ref34","doi-asserted-by":"publisher","DOI":"10.1038\/nmat4360"},{"key":"ref35","doi-asserted-by":"publisher","DOI":"10.1088\/0268-1242\/27\/12\/124003"},{"key":"ref36","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.99.245408"},{"key":"ref37","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.98.035428"},{"key":"ref38","doi-asserted-by":"publisher","DOI":"10.1038\/nphys1915"},{"key":"ref39","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.99.035307"}],"container-title":["SciPost Physics"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.11.5.090\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.11.5.090\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2021,11,12]],"date-time":"2021-11-12T10:58:10Z","timestamp":1636714690000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.11.5.090"}},"issued":{"date-parts":[[2021,11,12]]},"references-count":39,"journal-issue":{"issue":"5","published-online":{"date-parts":[[2021]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphys.11.5.090","archive":["CLOCKSS"],"relation":{"has-review":[{"id-type":"doi","id":"10.21468\/SciPost.Report.2930","asserted-by":"object"},{"id-type":"doi","id":"10.21468\/SciPost.Report.3316","asserted-by":"object"},{"id-type":"doi","id":"10.21468\/SciPost.Report.2936","asserted-by":"object"}]},"ISSN":["2542-4653"],"issn-type":[{"value":"2542-4653","type":"electronic"}],"published":{"date-parts":[[2021,11,12]]},"article-number":"090"},{"indexed":{"date-parts":[[2026,3,6]],"date-time":"2026-03-06T00:44:03Z","timestamp":1772757843838,"version":"3.50.1"},"reference-count":57,"publisher":"Stichting SciPost","issue":"6","license":[{"start":{"date-parts":[[2023,6,12]],"date-time":"2023-06-12T00:00:00Z","timestamp":1686528000000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/501100001665","name":"Agence Nationale de la Recherche","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100001665","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100020314","name":"QuantERA","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100020314","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys."],"abstract":"\n The study of non-equilibrium dynamics is one of the most important challenges of modern quantum many-body physics, in relationship with fundamental questions in quantum statistical mechanics, as well as with the fields of quantum simulation and computing. In this work we propose a Gaussian Ansatz for the study of the nonequilibrium dynamics of quantum spin systems. Within our approach, the quantum spins are mapped onto Holstein-Primakoff bosons, such that a coherent spin state - chosen as the initial state of the dynamics - represents the bosonic vacuum. The state of the system is then postulated to remain a bosonic Gaussian state at all times, an assumption which is exact when the bosonic Hamiltonian is quadratic; and which is justified in the case of a nonlinear Hamiltonian if the boson density remains moderate. We test the accuracy of such an Ansatz in the paradigmatic case of the\n \n \n S=1\/2<\/jats:tex-math>\n \n \n S<\/mml:mi>\n =<\/mml:mo>\n 1<\/mml:mn>\n \/<\/mml:mi>\n 2<\/mml:mn>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n transverse-field Ising model, in one and two dimensions, initialized in a state aligned with the applied field. We show that the Gaussian Ansatz, when applied to the bosonic Hamiltonian with nonlinearities truncated to quartic order, is able to reproduce faithfully the evolution of the state, including its relaxation to the equilibrium regime, for fields larger than the critical field for the paramagnetic-ferromagnetic transition in the ground state. In particular the spatio-temporal pattern of correlations reconstructed via the Gaussian Ansatz reveals the dispersion relation of quasiparticle excitations, exhibiting the softening of the excitation gap upon approaching the critical field. Our results suggest that the Gaussian Ansatz correctly captures the essential effects of nonlinearities in quantum spin dynamics; and that it can be applied to the study of fundamental phenomena such as quantum thermalization and its breakdown.\n <\/jats:p>","DOI":"10.21468\/scipostphys.14.6.151","type":"journal-article","created":{"date-parts":[[2023,6,12]],"date-time":"2023-06-12T10:29:53Z","timestamp":1686565793000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":8,"title":["Gaussian-state Ansatz for the non-equilibrium dynamics of quantum spin lattices"],"prefix":"10.21468","volume":"14","author":[{"given":"Rapha\u00ebl","family":"Menu","sequence":"first","affiliation":[{"name":"Saarland University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Tommaso","family":"Roscilde","sequence":"additional","affiliation":[{"name":"Laboratoire de Physique de l'ENS de Lyon"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2023,6,12]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1016\/j.physrep.2011.08.003"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.86.153"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.90.035005"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1038\/s42254-019-0090-y"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.83.863"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1038\/nphys3215"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1146\/annurev-conmatphys-031016-025451"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1080\/00018732.2016.1198134"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1088\/1742-5468\/2016\/06\/064007"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.91.021001"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1038\/s41567-018-0295-5"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1126\/science.1237557"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevA.98.043604"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.98.205145"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevA.100.063632"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevA.102.033337"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.1016\/j.aop.2010.09.012"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1016\/j.aop.2014.06.013"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.1126\/science.aag2302"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.1038\/srep38185"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevA.105.022625"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.129.150503"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.1088\/1367-2630\/10\/3\/033032"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevX.5.011022"},{"key":"ref25","doi-asserted-by":"publisher","DOI":"10.1038\/s41467-019-09699-5"},{"key":"ref26","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevA.96.033604"},{"key":"ref27","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.40.2494"},{"key":"ref28","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.111.207202"},{"key":"ref29","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.98.024302"},{"key":"ref30","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.99.045128"},{"key":"ref31","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.124.130604"},{"key":"ref32","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevResearch.3.L012022"},{"key":"ref33","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.125.100503"},{"key":"ref34","doi-asserted-by":"publisher","DOI":"10.1126\/science.1180085"},{"key":"ref35","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevX.4.031008"},{"key":"ref36","doi-asserted-by":"publisher","DOI":"10.3254\/978-1-61499-526-5-169"},{"key":"ref37","doi-asserted-by":"publisher","DOI":"10.1038\/s41567-019-0733-z"},{"key":"ref38","doi-asserted-by":"publisher","DOI":"10.1038\/s41586-021-03585-1"},{"key":"ref39","doi-asserted-by":"publisher","DOI":"10.1038\/s41586-021-03582-4"},{"key":"ref40","doi-asserted-by":"publisher","DOI":"10.1038\/s41567-022-01741-6"},{"key":"ref41","doi-asserted-by":"publisher","DOI":"10.1088\/1367-2630\/12\/5\/053036"},{"key":"ref42","doi-asserted-by":"publisher","DOI":"10.1016\/0003-4916(61)90115-4"},{"key":"ref43","doi-asserted-by":"publisher","DOI":"10.1016\/0003-4916(70)90270-8"},{"key":"ref44","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.96.136801"},{"key":"ref45","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.97.050401"},{"key":"ref46","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.120.050401"},{"key":"ref47","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevE.66.066110"},{"key":"ref48","doi-asserted-by":"publisher","DOI":"10.1017\/CBO9780511584398"},{"key":"ref49","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.81.865"},{"key":"ref50","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.92.115129"},{"key":"ref51","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevE.66.046701"},{"key":"ref52","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevResearch.2.043243"},{"key":"ref53","doi-asserted-by":"publisher","DOI":"10.1088\/1361-6633\/aaaf9a"},{"key":"ref54","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.115.260501"},{"key":"ref55","doi-asserted-by":"publisher","DOI":"10.1088\/1361-6633\/aa8b38"},{"key":"ref56","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevResearch.2.022037"},{"key":"ref57","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevA.102.063314"}],"container-title":["SciPost 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Proc."],"abstract":"Rapidly rotating Myers-Perry-AdS black holes are unstable against\nrotational superradiance. From the onset of the instability,\ncohomogeneity-1 black resonators are constructed in five-dimensional\nasymptotically AdS space. By using the cohomogeneity-1 metric,\nperturbations of the cohomogeneity-1 black resonators are also\nstudied.<\/jats:p>","DOI":"10.21468\/scipostphysproc.4.008","type":"journal-article","created":{"date-parts":[[2021,8,13]],"date-time":"2021-08-13T12:11:44Z","timestamp":1628856704000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":3,"title":["Superradiant instability and black resonators in AdS"],"prefix":"10.21468","author":[{"given":"Takaaki","family":"Ishii","sequence":"first","affiliation":[{"name":"Kyoto University"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2021,8,13]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.74.084021"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1143\/PTP.121.1099"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP12(2015)171"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1088\/1361-6382\/ab1d76"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1088\/1361-6382\/ab7418"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP07(2020)206"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP08(2020)136"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1088\/0264-9381\/33\/12\/125022"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.4.008\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.4.008\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2021,8,13]],"date-time":"2021-08-13T12:11:46Z","timestamp":1628856706000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.4.008"}},"issued":{"date-parts":[[2021,8,13]]},"references-count":8,"journal-issue":{"issue":"4","published-online":{"date-parts":[[2021]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.4.008","archive":["CLOCKSS"],"relation":{"has-review":[{"id-type":"doi","id":"10.21468\/SciPost.Report.2190","asserted-by":"object"}]},"ISSN":["2666-4003"],"issn-type":[{"value":"2666-4003","type":"electronic"}],"published":{"date-parts":[[2021,8,13]]},"article-number":"008"},{"indexed":{"date-parts":[[2026,4,22]],"date-time":"2026-04-22T01:22:18Z","timestamp":1776820938910,"version":"3.51.2"},"reference-count":63,"publisher":"Stichting SciPost","issue":"5","license":[{"start":{"date-parts":[[2025,5,6]],"date-time":"2025-05-06T00:00:00Z","timestamp":1746489600000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"},{"start":{"date-parts":[[2025,5,6]],"date-time":"2025-05-06T00:00:00Z","timestamp":1746489600000},"content-version":"am","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys."],"accepted":{"date-parts":[[2025,4,15]]},"abstract":"\n We derive constraints on dimension-six light-quark dipole operators within the Standard Model (SM) effective field theory, based on measurements of\n \n \n Z<\/jats:tex-math>\n \n Z<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n production at SLC and LEP, as well as\n \n \n Z<\/jats:tex-math>\n \n Z<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n +jet production at the LHC. Our new constraints exclude the parameter space that could potentially explain the observed discrepancy between theoretical predictions and experimental data for the Lam-Tung relation. With these updated limits, we model-independently determine the maximum possible influence that beyond-SM contributions could have on the angular coefficients\n \n \n A_0<\/jats:tex-math>\n \n \n A<\/mml:mi>\n 0<\/mml:mn>\n <\/mml:msub>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n and\n \n \n A_2<\/jats:tex-math>\n \n \n A<\/mml:mi>\n 2<\/mml:mn>\n <\/mml:msub>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n , which enter the Lam-Tung relation.\n <\/jats:p>","DOI":"10.21468\/scipostphys.18.5.148","type":"journal-article","created":{"date-parts":[[2025,5,6]],"date-time":"2025-05-06T06:10:41Z","timestamp":1746511841000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":4,"title":["A tale of $Z$+jet: SMEFT effects and the Lam-Tung 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