guest ::
| Home > Publications database > Line defect correlators in fermionic CFTs > print |
| 001 | 639275 | ||
| 005 | 20251125210859.0 | ||
| 024 | 7 | _ | |a 10.1007/JHEP05(2025)146 |2 doi |
| 024 | 7 | _ | |a Barrat:2023ivo |2 INSPIRETeX |
| 024 | 7 | _ | |a inspire:2654489 |2 inspire |
| 024 | 7 | _ | |a 1126-6708 |2 ISSN |
| 024 | 7 | _ | |a 1029-8479 |2 ISSN |
| 024 | 7 | _ | |a 1127-2236 |2 ISSN |
| 024 | 7 | _ | |a arXiv:2304.13588 |2 arXiv |
| 024 | 7 | _ | |a 10.3204/PUBDB-2025-04376 |2 datacite_doi |
| 037 | _ | _ | |a PUBDB-2025-04376 |
| 041 | _ | _ | |a English |
| 082 | _ | _ | |a 530 |
| 088 | _ | _ | |a arXiv:2304.13588 |2 arXiv |
| 088 | _ | _ | |a HU-EP-23/10-RTG |2 Other |
| 088 | _ | _ | |a DESY-23-055 |2 DESY |
| 100 | 1 | _ | |a Barrat, Julien |0 P:(DE-H253)PIP1098469 |b 0 |u desy |
| 245 | _ | _ | |a Line defect correlators in fermionic CFTs |
| 260 | _ | _ | |a Heidelberg |c 2025 |b Springer |
| 336 | 7 | _ | |a article |2 DRIVER |
| 336 | 7 | _ | |a Output Types/Journal article |2 DataCite |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1764076356_3547116 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 500 | _ | _ | |a 44 pages, ancillary Mathematica notebook. V2 includes fixed typos, clarifications, additional references. Version accepted for publication in JHEP |
| 520 | _ | _ | |a Scalar-fermion models, such as the Gross-Neveu-Yukawa model, admit natural 1d defects given by the exponential of a scalar field integrated along a straight line. In 4 − ε dimensions the defect coupling is weakly relevant and the setup defines a non-trivial interacting defect CFT. In this work we study correlation functions on these defect CFTs to order ε. We focus on 1d correlators constrained to the line, which include canonical operators like the displacement and the one-dimensional analog of the spin field. These results give access to perturbative CFT data that can be used as input in the numerical bootstrap. We also consider local operators outside the line, in particular two-point functions of scalars whose dynamics are non-trivial due to the presence of the defect. |
| 536 | _ | _ | |a 611 - Fundamental Particles and Forces (POF4-611) |0 G:(DE-HGF)POF4-611 |c POF4-611 |f POF IV |x 0 |
| 536 | _ | _ | |a DFG project G:(GEPRIS)400570283 - Das Conformal Bootstrap Programm (400570283) |0 G:(GEPRIS)400570283 |c 400570283 |x 1 |
| 536 | _ | _ | |a GRK 2575 - GRK 2575: Überdenken der Quantenfeldtheorie (417533893) |0 G:(GEPRIS)417533893 |c 417533893 |x 2 |
| 536 | _ | _ | |a DFG project G:(GEPRIS)471314740 - Holographie und das Swampland: Konsistenzbedingungen an fundamentale Physik aus der Quantengravitation (471314740) |0 G:(GEPRIS)471314740 |c 471314740 |x 3 |
| 588 | _ | _ | |a Dataset connected to CrossRef, INSPIRE, Journals: bib-pubdb1.desy.de |
| 650 | _ | 7 | |a field theory: conformal |2 INSPIRE |
| 650 | _ | 7 | |a operator: local |2 INSPIRE |
| 650 | _ | 7 | |a two-point function: scalar |2 INSPIRE |
| 650 | _ | 7 | |a dimension: 1 |2 INSPIRE |
| 650 | _ | 7 | |a field theory: scalar |2 INSPIRE |
| 650 | _ | 7 | |a defect |2 INSPIRE |
| 650 | _ | 7 | |a correlation function |2 INSPIRE |
| 650 | _ | 7 | |a bootstrap |2 INSPIRE |
| 650 | _ | 7 | |a spin |2 INSPIRE |
| 650 | _ | 7 | |a Renormalization Group |2 autogen |
| 650 | _ | 7 | |a Scale and Conformal Symmetries |2 autogen |
| 650 | _ | 7 | |a Field Theories in Higher Dimensions |2 autogen |
| 650 | _ | 7 | |a Field Theories in Lower Dimensions |2 autogen |
| 693 | _ | _ | |0 EXP:(DE-MLZ)NOSPEC-20140101 |5 EXP:(DE-MLZ)NOSPEC-20140101 |e No specific instrument |x 0 |
| 700 | 1 | _ | |a Liendo, Pedro |0 P:(DE-H253)PIP1031480 |b 1 |
| 700 | 1 | _ | |a Vliet, Philine Julia van |0 P:(DE-H253)PIP1090382 |b 2 |e Corresponding author |
| 773 | _ | _ | |a 10.1007/JHEP05(2025)146 |g Vol. 05, no. 5, p. 146 |0 PERI:(DE-600)2027350-2 |n 5 |p 146 |t Journal of high energy physics |v 05 |y 2025 |x 1126-6708 |
| 787 | 0 | _ | |a Barrat, Julien et.al. |d 2023 |i IsParent |0 PUBDB-2023-01928 |r DESY-23-055 ; arXiv:2304.13588 ; HU-EP-23/10-RTG |t Line defect correlators in fermionic CFTs |
| 856 | 4 | _ | |y OpenAccess |u https://bib-pubdb1.desy.de/record/639275/files/JHEP05%282025%29146.pdf |
| 856 | 4 | _ | |y OpenAccess |x pdfa |u https://bib-pubdb1.desy.de/record/639275/files/JHEP05%282025%29146.pdf?subformat=pdfa |
| 909 | C | O | |o oai:bib-pubdb1.desy.de:639275 |p openaire |p open_access |p VDB |p driver |p dnbdelivery |
| 910 | 1 | _ | |a Deutsches Elektronen-Synchrotron |0 I:(DE-588b)2008985-5 |k DESY |b 0 |6 P:(DE-H253)PIP1098469 |
| 910 | 1 | _ | |a Deutsches Elektronen-Synchrotron |0 I:(DE-588b)2008985-5 |k DESY |b 1 |6 P:(DE-H253)PIP1031480 |
| 910 | 1 | _ | |a External Institute |0 I:(DE-HGF)0 |k Extern |b 2 |6 P:(DE-H253)PIP1090382 |
| 913 | 1 | _ | |a DE-HGF |b Forschungsbereich Materie |l Matter and the Universe |1 G:(DE-HGF)POF4-610 |0 G:(DE-HGF)POF4-611 |3 G:(DE-HGF)POF4 |2 G:(DE-HGF)POF4-600 |4 G:(DE-HGF)POF |v Fundamental Particles and Forces |x 0 |
| 914 | 1 | _ | |y 2025 |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0200 |2 StatID |b SCOPUS |d 2024-12-16 |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0160 |2 StatID |b Essential Science Indicators |d 2024-12-16 |
| 915 | _ | _ | |a Creative Commons Attribution CC BY 4.0 |0 LIC:(DE-HGF)CCBY4 |2 HGFVOC |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0600 |2 StatID |b Ebsco Academic Search |d 2024-12-16 |
| 915 | _ | _ | |a OpenAccess |0 StatID:(DE-HGF)0510 |2 StatID |
| 915 | _ | _ | |a JCR |0 StatID:(DE-HGF)0100 |2 StatID |b J HIGH ENERGY PHYS : 2022 |d 2024-12-16 |
| 915 | _ | _ | |a IF >= 5 |0 StatID:(DE-HGF)9905 |2 StatID |b J HIGH ENERGY PHYS : 2022 |d 2024-12-16 |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0501 |2 StatID |b DOAJ Seal |d 2023-05-02T09:05:11Z |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0500 |2 StatID |b DOAJ |d 2023-05-02T09:05:11Z |
| 915 | _ | _ | |a WoS |0 StatID:(DE-HGF)0113 |2 StatID |b Science Citation Index Expanded |d 2024-12-16 |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0199 |2 StatID |b Clarivate Analytics Master Journal List |d 2024-12-16 |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0150 |2 StatID |b Web of Science Core Collection |d 2024-12-16 |
| 915 | _ | _ | |a SCOAP3 |0 StatID:(DE-HGF)0570 |2 StatID |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0571 |2 StatID |b SCOAP3 sponsored Journal |d 2024-12-16 |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)1150 |2 StatID |b Current Contents - Physical, Chemical and Earth Sciences |d 2024-12-16 |
| 915 | _ | _ | |a National-Konsortium |0 StatID:(DE-HGF)0430 |2 StatID |d 2024-12-16 |w ger |
| 915 | _ | _ | |a DBCoverage |0 StatID:(DE-HGF)0300 |2 StatID |b Medline |d 2024-12-16 |
| 915 | _ | _ | |a Peer Review |0 StatID:(DE-HGF)0030 |2 StatID |b DOAJ : Anonymous peer review |d 2023-05-02T09:05:11Z |
| 920 | 1 | _ | |0 I:(DE-H253)T-20120731 |k T |l Theorie-Gruppe |x 0 |
| 980 | _ | _ | |a journal |
| 980 | _ | _ | |a VDB |
| 980 | _ | _ | |a UNRESTRICTED |
| 980 | _ | _ | |a I:(DE-H253)T-20120731 |
| 980 | 1 | _ | |a FullTexts |
| Library | Collection | CLSMajor | CLSMinor | Language | Author |
|---|