{"status":"ok","message-type":"work-list","message-version":"1.0.0","message":{"facets":{},"total-results":12064,"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":"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":[[2026,4,7]],"date-time":"2026-04-07T09:37:34Z","timestamp":1775554654852,"version":"3.50.1"},"reference-count":84,"publisher":"Stichting SciPost","issue":"1","license":[{"start":{"date-parts":[[2022,1,4]],"date-time":"2022-01-04T00:00:00Z","timestamp":1641254400000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/501100001659","name":"Deutsche Forschungsgemeinschaft","doi-asserted-by":"publisher","award":["EXC 2181\/1 - 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The reconstruction is applied to both the dynamical fluctuation graviton and the background graviton propagator. We prove that the spectral function of the latter necessarily has negative parts similar to, and for the same reasons, as the gluon spectral function. In turn, the spectral function of the dynamical graviton is positive. We argue that the latter enters cross sections and other observables in asymptotically safe quantum gravity. Hence, its positivity may hint at the unitarity of asymptotically safe quantum gravity.<\/jats:p>","DOI":"10.21468\/scipostphys.12.1.001","type":"journal-article","created":{"date-parts":[[2022,1,4]],"date-time":"2022-01-04T05:08:11Z","timestamp":1641272891000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":85,"title":["Reconstructing the graviton"],"prefix":"10.21468","volume":"12","author":[{"given":"Alfio","family":"Bonanno","sequence":"first","affiliation":[{"name":"INFN Sezione di Catania"},{"name":"Osservatorio Astrofisico di Catania"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Tobias","family":"Denz","sequence":"additional","affiliation":[{"name":"Heidelberg University"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Jan M.","family":"Pawlowski","sequence":"additional","affiliation":[{"name":"ExtreMe Matter Institute"},{"name":"Heidelberg 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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 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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 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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":[[2026,4,3]],"date-time":"2026-04-03T05:29:19Z","timestamp":1775194159854,"version":"3.50.1"},"reference-count":34,"publisher":"Stichting 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Fund","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100008530","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100002809","name":"Generalitat de Catalunya","doi-asserted-by":"publisher","award":["2021 SGR 01519"],"award-info":[{"award-number":["2021 SGR 01519"]}],"id":[{"id":"10.13039\/501100002809","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["scipost.org"],"crossmark-restriction":false},"short-container-title":["SciPost Phys."],"accepted":{"date-parts":[[2025,4,2]]},"abstract":"\n We establish rigorous inequalities between different electronic properties linked to optical sum rules, and organize them into weak and strong bounds on three characteristic properties of insulators: electron localization length\n \n \n \\ell<\/jats:tex-math>\n \n \u2113<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n (the quantum fluctuations in polarization), electric susceptibility\n \n \n \\chi<\/jats:tex-math>\n \n \u03c7<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n , and optical gap\n \n \n E_{\\mathrm{G}}<\/jats:tex-math>\n \n \n E<\/mml:mi>\n \n G<\/mml:mi>\n <\/mml:mstyle>\n <\/mml:msub>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n . All-electron and valence-only versions of the bounds are given, and the latter are found to be more informative. The bounds on\n \n \n \\ell<\/jats:tex-math>\n \n \u2113<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n are particularly interesting, as they provide reasonably tight estimates for an ellusive ground-state property \u2013 the average localization length of valence electrons \u2013 from tabulated experimental data: electron density, high-frequency dielectric constant, and optical gap. The localization lengths estimated in this way for several materials follow simple chemical trends, especially for the alkali halides. We also illustrate our findings via analytically solvable harmonic oscillator models, which reveal an intriguing connection to the physics of long-ranged van der Waals forces.\n <\/jats:p>","DOI":"10.21468\/scipostphys.18.4.127","type":"journal-article","created":{"date-parts":[[2025,4,15]],"date-time":"2025-04-15T06:17:46Z","timestamp":1744697866000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":10,"title":["Optical bounds on many-electron localization"],"prefix":"10.21468","volume":"18","author":[{"ORCID":"https:\/\/orcid.org\/0000-0001-9901-5058","authenticated-orcid":true,"given":"Ivo","family":"Souza","sequence":"first","affiliation":[{"id":[{"id":"https:\/\/ror.org\/02hpa6m94","id-type":"ROR","asserted-by":"publisher"}],"name":"Center for Materials 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Avan\u00e7ats"},{"id":[{"id":"https:\/\/ror.org\/03hasqf61","id-type":"ROR","asserted-by":"publisher"}],"name":"Institut de Ci\u00e8ncia de Materials de Barcelona"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2025,4,15]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRev.133.A171"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.47.1651"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1017\/9781316662205"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.62.1666"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1007\/BF02193559"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.82.370"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.77.054438"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.56.12847"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.64.115202"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.66.235113"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.48550\/arXiv.cond-mat\/9902361"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.96.137601"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.86.468"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1017\/CBO9780511805769"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.48550\/arXiv.2403.07052"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.48550\/arXiv.2406.06783"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.1038\/s41467-024-48808-x"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1016\/C2013-0-07656-6"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.40.441"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.1201\/9780429493645"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.1088\/0143-0807\/17\/1\/006"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.12.5864"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRev.128.2093"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.1007\/978-3-642-00710-1"},{"key":"ref25","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.110.155107"},{"key":"ref26","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.74.235111"},{"key":"ref27","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.102.107603"},{"key":"ref28","doi-asserted-by":"publisher","DOI":"10.1016\/C2013-0-02793-4"},{"key":"ref29","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRev.155.896"},{"key":"ref30","doi-asserted-by":"publisher","DOI":"10.1016\/0022-3697(67)90280-6"},{"key":"ref31","doi-asserted-by":"publisher","DOI":"10.1016\/0375-9601(69)91018-4"},{"key":"ref32","doi-asserted-by":"publisher","DOI":"10.1007\/978-3-642-18865-7"},{"key":"ref33","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.49.14202"},{"key":"ref34","doi-asserted-by":"publisher","DOI":"10.1098\/rspa.1925.0047"}],"container-title":["SciPost 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Energy","doi-asserted-by":"publisher","award":["DE-SC0011632"],"award-info":[{"award-number":["DE-SC0011632"]}],"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":"\n We discuss symmetry fractionalization of the Lorentz group in\n(2+1)\n \n \n d<\/jats:tex-math>\n \n d<\/mml:mi>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n non-spin quantum field theory (QFT), and its implications for dualities.\nWe prove that two inequivalent non-spin QFTs are dual as spin QFTs if\nand only if they are related by a Lorentz symmetry fractionalization\nwith respect to an anomalous\n \n \n \\mathbb{Z}_2<\/jats:tex-math>\n \n \n \n \u2124<\/mml:mi>\n <\/mml:mstyle>\n 2<\/mml:mn>\n <\/mml:msub>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n one-form symmetry. Moreover, if the framing anomalies of two non-spin\nQFTs differ by a multiple of 8, then they are dual as spin QFTs if and\nonly if they are also dual as non-spin QFTs. Applications to summing\nover the spin structures, time-reversal symmetry, and level\/rank\ndualities are explored. The Lorentz symmetry fractionalization naturally\narises in Chern-Simons matter dualities that obey certain spin\/charge\nrelations, and is instrumental for the dualities to hold when viewed as\nnon-spin theories.\n <\/jats:p>","DOI":"10.21468\/scipostphys.8.2.018","type":"journal-article","created":{"date-parts":[[2020,2,4]],"date-time":"2020-02-04T05:26:08Z","timestamp":1580793968000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":30,"title":["Lorentz symmetry fractionalization and dualities in (2+1)d"],"prefix":"10.21468","volume":"8","author":[{"given":"Po-Shen","family":"Hsin","sequence":"first","affiliation":[{"name":"Walter Burke Institute for Theoretical Physics"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Shu-Heng","family":"Shao","sequence":"additional","affiliation":[{"name":"Institute for Advanced Study, Princeton University"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2020,2,4]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.62.82"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevX.6.011034"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.97.195126"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP02(2015)172"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.89.195124"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.91.239902"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.92.085024"},{"key":"ref8","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP02(2015)152"},{"key":"ref9","doi-asserted-by":"publisher","DOI":"10.1063\/1.5082852"},{"key":"ref10","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP03(2019)118"},{"key":"ref11","doi-asserted-by":"publisher","DOI":"10.1016\/j.aop.2020.168074"},{"key":"ref12","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.100.085012"},{"key":"ref13","doi-asserted-by":"publisher","DOI":"10.1007\/BF01238857"},{"key":"ref14","doi-asserted-by":"publisher","DOI":"10.1016\/j.aop.2005.10.005"},{"key":"ref15","doi-asserted-by":"publisher","DOI":"10.1007\/s00220-009-0908-z"},{"key":"ref16","doi-asserted-by":"publisher","DOI":"10.1093\/nsr\/nwv077"},{"key":"ref17","doi-asserted-by":"publisher","DOI":"10.4171\/QT\/6"},{"key":"ref18","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.87.104406"},{"key":"ref19","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.100.115147"},{"key":"ref20","doi-asserted-by":"publisher","DOI":"10.1016\/j.aop.2015.05.012"},{"key":"ref21","doi-asserted-by":"publisher","DOI":"10.1088\/1367-2630\/18\/3\/035006"},{"key":"ref22","doi-asserted-by":"publisher","DOI":"10.1007\/BF02096988"},{"key":"ref23","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhys.6.3.039"},{"key":"ref24","doi-asserted-by":"publisher","DOI":"10.1007\/BF02568048"},{"key":"ref25","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP08(2013)115"},{"key":"ref26","doi-asserted-by":"publisher","DOI":"10.4310\/ATMP.2014.v18.n5.a4"},{"key":"ref27","doi-asserted-by":"publisher","DOI":"10.2307\/1993484"},{"key":"ref28","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhys.4.4.021"},{"key":"ref29","doi-asserted-by":"publisher","DOI":"10.1007\/BF01217730"},{"key":"ref30","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(89)90310-6"},{"key":"ref31","doi-asserted-by":"publisher","DOI":"10.1142\/S0217751X90001367"},{"key":"ref32","doi-asserted-by":"publisher","DOI":"10.1016\/j.nuclphysb.2004.05.014"},{"key":"ref33","doi-asserted-by":"publisher","DOI":"10.1016\/0550-3213(89)90511-7"},{"key":"ref34","doi-asserted-by":"publisher","DOI":"10.1016\/0370-2693(89)90897-6"},{"key":"ref35","doi-asserted-by":"publisher","DOI":"10.1093\/ptep\/ptw083"},{"key":"ref36","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP10(2012)053"},{"key":"ref37","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP09(2012)091"},{"key":"ref38","doi-asserted-by":"publisher","DOI":"10.1142\/S0217751X16450445"},{"key":"ref39","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.85.245132"},{"key":"ref40","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.88.064507"},{"key":"ref41","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.89.201113"},{"key":"ref42","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP12(2015)052"},{"key":"ref43","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhys.5.1.007"},{"key":"ref44","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhys.5.1.006"},{"key":"ref45","doi-asserted-by":"publisher","DOI":"10.1142\/9789812793850_0013"},{"key":"ref46","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP09(2016)095"},{"key":"ref47","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP02(2017)072"},{"key":"ref48","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhys.7.4.056"},{"key":"ref49","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.98.115129"},{"key":"ref50","doi-asserted-by":"publisher","DOI":"10.1016\/j.aop.2016.08.007"},{"key":"ref51","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevX.6.031043"},{"key":"ref52","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP01(2018)109"},{"key":"ref53","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP01(2020)004"},{"key":"ref54","doi-asserted-by":"publisher","DOI":"10.1088\/1126-6708\/2001\/10\/005"},{"key":"ref55","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.83.084019"},{"key":"ref56","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP04(2014)001"},{"key":"ref57","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP04(2017)096"},{"key":"ref58","doi-asserted-by":"publisher","DOI":"10.1007\/JHEP10(2017)080"},{"key":"ref59","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhys.7.1.007"}],"container-title":["SciPost Physics"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.8.2.018\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.8.2.018\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2020,2,4]],"date-time":"2020-02-04T05:26:11Z","timestamp":1580793971000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhys.8.2.018"}},"issued":{"date-parts":[[2020,2,4]]},"references-count":59,"journal-issue":{"issue":"2","published-online":{"date-parts":[[2020]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphys.8.2.018","archive":["CLOCKSS"],"relation":{"has-review":[{"id-type":"doi","id":"10.21468\/SciPost.Report.1428","asserted-by":"object"}]},"ISSN":["2542-4653"],"issn-type":[{"value":"2542-4653","type":"electronic"}],"published":{"date-parts":[[2020,2,4]]},"article-number":"018"},{"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":[[2026,3,27]],"date-time":"2026-03-27T12:28:01Z","timestamp":1774614481827,"version":"3.50.1"},"reference-count":7,"publisher":"Stichting SciPost","issue":"5","license":[{"start":{"date-parts":[[2021,9,6]],"date-time":"2021-09-06T00:00:00Z","timestamp":1630886400000},"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":"Two target stations in the 590 MeV proton beamline of the High Intensity Proton Accelerator (HIPA) at the Paul Scherrer Institut (PSI) produce pions and muons for seven secondary beamlines, leading to several experimental stations. The two target stations are 18 m apart. Target M is a graphite target with an effective thickness of 5 mm, Target E is a graphite wheel with a thickness of 40 mm or 60 mm. Due to the spreading of the beam in the thick target, a high power collimator system is needed to shape the beam for further transport. The beam is then transported to either the SINQ target, a neutron spallation source, or stopped in the beam dump, where about 450 kW beam power is dissipated. Targets, collimators and beam dumps are described.<\/jats:p>","DOI":"10.21468\/scipostphysproc.5.003","type":"journal-article","created":{"date-parts":[[2021,9,6]],"date-time":"2021-09-06T12:57:00Z","timestamp":1630933020000},"update-policy":"https:\/\/doi.org\/10.21468\/scipost.crossmarkpolicy","source":"Crossref","is-referenced-by-count":9,"title":["The Meson Production Targets in the high energy beamline of HIPA at PSI"],"prefix":"10.21468","author":[{"given":"Daniela","family":"Kiselev","sequence":"first","affiliation":[{"name":"Paul Scherrer Institute"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Pierre-Andr\u00e9","family":"Duperrex","sequence":"additional","affiliation":[{"name":"Paul Scherrer Institute"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Sven","family":"Jollet","sequence":"additional","affiliation":[{"name":"Paul Scherrer Institute"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Stefan","family":"Joray","sequence":"additional","affiliation":[{"name":"Paul Scherrer Institute"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Daniel","family":"Laube","sequence":"additional","affiliation":[{"name":"Paul Scherrer Institute"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Davide","family":"Reggiani","sequence":"additional","affiliation":[{"name":"Paul Scherrer Institute"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Raffaello","family":"Sobbia","sequence":"additional","affiliation":[{"name":"Paul Scherrer Institute"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Vadim","family":"Talanov","sequence":"additional","affiliation":[{"name":"Paul Scherrer Institute"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"8907","published-online":{"date-parts":[[2021,9,6]]},"reference":[{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.7566\/JPSCP.33.011004"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.21468\/SciPostPhysProc.5.002"},{"key":"ref3","doi-asserted-by":"publisher","DOI":"10.7566\/JPSCP.33.011102"},{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevAccelBeams.19.024701"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1063\/1.1522602"},{"key":"ref6","doi-asserted-by":"publisher","DOI":"10.18429\/JACoW-Cyclotrons2019-TUP016"},{"key":"ref7","doi-asserted-by":"publisher","DOI":"10.1088\/1742-6596\/1046\/1\/012003"}],"container-title":["SciPost Physics Proceedings"],"link":[{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.5.003\/pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.5.003\/pdf","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2021,9,6]],"date-time":"2021-09-06T12:57:03Z","timestamp":1630933023000},"score":0.0,"resource":{"primary":{"URL":"https:\/\/scipost.org\/10.21468\/SciPostPhysProc.5.003"}},"issued":{"date-parts":[[2021,9,6]]},"references-count":7,"journal-issue":{"issue":"5","published-online":{"date-parts":[[2021]]}},"URL":"https:\/\/doi.org\/10.21468\/scipostphysproc.5.003","archive":["CLOCKSS"],"relation":{"has-review":[{"id-type":"doi","id":"10.21468\/SciPost.Report.3091","asserted-by":"object"},{"id-type":"doi","id":"10.21468\/SciPost.Report.3049","asserted-by":"object"},{"id-type":"doi","id":"10.21468\/SciPost.Report.3074","asserted-by":"object"},{"id-type":"doi","id":"10.21468\/SciPost.Report.3205","asserted-by":"object"}]},"ISSN":["2666-4003"],"issn-type":[{"value":"2666-4003","type":"electronic"}],"published":{"date-parts":[[2021,9,6]]},"article-number":"003"},{"indexed":{"date-parts":[[2026,3,26]],"date-time":"2026-03-26T01:51:59Z","timestamp":1774489919086,"version":"3.50.1"},"reference-count":40,"publisher":"Stichting SciPost","issue":"3","license":[{"start":{"date-parts":[[2024,9,11]],"date-time":"2024-09-11T00:00:00Z","timestamp":1726012800000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"funder":[{"DOI":"10.13039\/100005235","name":"Institute for Advanced Study","doi-asserted-by":"publisher","id":[{"id":"10.13039\/100005235","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/100000015","name":"United States Department of Energy","doi-asserted-by":"publisher","award":["DE-SC0009988"],"award-info":[{"award-number":["DE-SC0009988"]}],"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":"\n We engineer compact contours on the moduli spaces of genus-zero Riemann surfaces that achieve analytic continuation from Euclidean to Lorentzian worldsheets. These generalized Pochhammer contours are based on the combinatorics of associahedra and make the analytic properties of tree-level amplitudes entirely manifest for any number and type of external strings. We use them in practice to perform first numerical computations of open and closed string amplitudes directly in the physical kinematics for\n \n \n n=4,5,6,7,8,9<\/jats:tex-math>\n \n \n n<\/mml:mi>\n =<\/mml:mo>\n 4<\/mml:mn>\n ,<\/mml:mo>\n 5<\/mml:mn>\n ,<\/mml:mo>\n 6<\/mml:mn>\n ,<\/mml:mo>\n 7<\/mml:mn>\n ,<\/mml:mo>\n 8<\/mml:mn>\n ,<\/mml:mo>\n 9<\/mml:mn>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n . 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Namely, Kitaev-Yoshida and Gao-Jafferis-Wall protocols have a phase transition if we apply them at a large projection rate or at a large coupling rate respectively. It is well-known that at small rates they allow teleportation to happen only within a small time-window. We show that at large rates, the system goes into a new steady state, where the teleportation can be performed at any moment. In dual Jackiw-Teitelboim gravity these phase transitions correspond to the formation of an eternal traversable wormhole. 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