{"title":"晶格上的超对称 QCD:四元耦合的微调与反项","authors":"Marios Costa, Herodotos Herodotou, Haralambos Panagopoulos","doi":"arxiv-2409.09089","DOIUrl":null,"url":null,"abstract":"In this work we calculate the renormalization of counterterms which arise in\nthe lattice action of $N = 1$ Supersymmetric QCD (SQCD). In particular, the\nfine-tunings for quartic couplings are studied in detail through both continuum\nand lattice perturbation theory at one-loop level. For the lattice version of\nSQCD we make use of the Wilson gauge action for gluon fields and the Wilson\nfermion action for fermion fields (quarks, gluinos); for squark fields we use\nna\\\"ive discretization. On the lattice, different components of squark fields\nmix among themselves and a total of ten quartic terms arise at the quantum\nlevel. Consequently, the renormalization conditions must take into account\nthese effects in order to appropriately fine-tune all quartic couplings. All\nour results for Green's functions and renormalization factors exhibit an\nexplicit analytic dependence on the number of colors, $N_c$, the number of\nflavors, $N_f$, and the gauge parameter, $\\alpha$, which are left unspecified.\nResults for the specific case $N_f=1$ are also presented, where the symmetries\nallow only five linearly independent quartic terms. For the calculation of the\nGreen's functions, we consider both one-particle reducible and one-particle\nirreducible Feynman diagrams. Knowledge of these renormalization factors is\nnecessary in order to relate numerical results, coming from nonperturbative\nstudies, to ``physical'' observables.","PeriodicalId":501191,"journal":{"name":"arXiv - PHYS - High Energy Physics - Lattice","volume":"15 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Supersymmetric QCD on the lattice: Fine-tuning and counterterms for the quartic couplings\",\"authors\":\"Marios Costa, Herodotos Herodotou, Haralambos Panagopoulos\",\"doi\":\"arxiv-2409.09089\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this work we calculate the renormalization of counterterms which arise in\\nthe lattice action of $N = 1$ Supersymmetric QCD (SQCD). In particular, the\\nfine-tunings for quartic couplings are studied in detail through both continuum\\nand lattice perturbation theory at one-loop level. For the lattice version of\\nSQCD we make use of the Wilson gauge action for gluon fields and the Wilson\\nfermion action for fermion fields (quarks, gluinos); for squark fields we use\\nna\\\\\\\"ive discretization. On the lattice, different components of squark fields\\nmix among themselves and a total of ten quartic terms arise at the quantum\\nlevel. Consequently, the renormalization conditions must take into account\\nthese effects in order to appropriately fine-tune all quartic couplings. All\\nour results for Green's functions and renormalization factors exhibit an\\nexplicit analytic dependence on the number of colors, $N_c$, the number of\\nflavors, $N_f$, and the gauge parameter, $\\\\alpha$, which are left unspecified.\\nResults for the specific case $N_f=1$ are also presented, where the symmetries\\nallow only five linearly independent quartic terms. For the calculation of the\\nGreen's functions, we consider both one-particle reducible and one-particle\\nirreducible Feynman diagrams. Knowledge of these renormalization factors is\\nnecessary in order to relate numerical results, coming from nonperturbative\\nstudies, to ``physical'' observables.\",\"PeriodicalId\":501191,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Physics - Lattice\",\"volume\":\"15 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Physics - Lattice\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.09089\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Lattice","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.09089","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Supersymmetric QCD on the lattice: Fine-tuning and counterterms for the quartic couplings
In this work we calculate the renormalization of counterterms which arise in
the lattice action of $N = 1$ Supersymmetric QCD (SQCD). In particular, the
fine-tunings for quartic couplings are studied in detail through both continuum
and lattice perturbation theory at one-loop level. For the lattice version of
SQCD we make use of the Wilson gauge action for gluon fields and the Wilson
fermion action for fermion fields (quarks, gluinos); for squark fields we use
na\"ive discretization. On the lattice, different components of squark fields
mix among themselves and a total of ten quartic terms arise at the quantum
level. Consequently, the renormalization conditions must take into account
these effects in order to appropriately fine-tune all quartic couplings. All
our results for Green's functions and renormalization factors exhibit an
explicit analytic dependence on the number of colors, $N_c$, the number of
flavors, $N_f$, and the gauge parameter, $\alpha$, which are left unspecified.
Results for the specific case $N_f=1$ are also presented, where the symmetries
allow only five linearly independent quartic terms. For the calculation of the
Green's functions, we consider both one-particle reducible and one-particle
irreducible Feynman diagrams. Knowledge of these renormalization factors is
necessary in order to relate numerical results, coming from nonperturbative
studies, to ``physical'' observables.