• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

全单圈水平下两体部分衰变宽度的一般计算。

Generic calculation of two-body partial decay widths at the full one-loop level.

作者信息

Goodsell Mark D, Liebler Stefan, Staub Florian

机构信息

1Sorbonne Universités, UPMC Univ Paris 06, UMR 7589, LPTHE, 75005 Paris, France.

2CNRS, UMR 7589, LPTHE, 75005 Paris, France.

出版信息

Eur Phys J C Part Fields. 2017;77(11):758. doi: 10.1140/epjc/s10052-017-5259-x. Epub 2017 Nov 11.

DOI:10.1140/epjc/s10052-017-5259-x
PMID:31997930
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6956948/
Abstract

We describe a fully generic implementation of two-body partial decay widths at the full one-loop level in the SARAH and SPheno framework compatible with most supported models. It incorporates fermionic decays to a fermion and a scalar or a gauge boson as well as scalar decays into two fermions, two gauge bosons, two scalars or a scalar and a gauge boson. We present the relevant generic expressions for virtual and real corrections. Whereas wave-function corrections are determined from on-shell conditions, the parameters of the underlying model are by default renormalised in a (or ) scheme. However, the user can also define model-specific counter-terms. As an example we discuss the renormalisation of the electric charge in the Thomson limit for top-quark decays in the standard model. One-loop-induced decays are also supported. The framework additionally allows the addition of mass and mixing corrections induced at higher orders for the involved external states. We explain our procedure to cancel infrared divergences for such cases, which is achieved through an infrared counter-term taking into account corrected Goldstone boson vertices. We compare our results for sfermion, gluino and Higgs decays in the minimal supersymmetric standard model (MSSM) against the public codes SFOLD, FVSFOLD and HFOLD and explain observed differences. Radiatively induced gluino and neutralino decays are compared against the original implementation in SPheno in the MSSM. We exactly reproduce the results of the code CNNDecays for decays of neutralinos and charginos in -parity violating models. The new version SARAH 4.11.0 by default includes the calculation of two-body decay widths at the full one-loop level. Current limitations for certain model classes are described.

摘要

我们描述了在SARAH和SPheno框架中全一圈水平下两体部分衰变宽度的完全通用实现,该实现与大多数支持的模型兼容。它包括费米子衰变为一个费米子和一个标量或一个规范玻色子,以及标量衰变为两个费米子、两个规范玻色子、两个标量或一个标量和一个规范玻色子。我们给出了虚拟修正和实修正的相关通用表达式。波函数修正是根据壳上条件确定的,而基础模型的参数默认在一个(或)方案中进行重整化。然而,用户也可以定义特定于模型的抵消项。作为一个例子,我们讨论了标准模型中顶夸克衰变在汤姆逊极限下电荷的重整化。还支持一圈诱导衰变。该框架还允许添加对所涉及的外部态在高阶诱导的质量和混合修正。我们解释了在这种情况下消除红外发散的过程,这是通过考虑修正的戈德斯通玻色子顶点的红外抵消项来实现的。我们将最小超对称标准模型(MSSM)中sfermion、胶微子和希格斯衰变的结果与公共代码SFOLD、FVSFOLD和HFOLD进行比较,并解释观察到的差异。将辐射诱导的胶微子和中性子衰变与MSSM中SPheno的原始实现进行比较。我们精确地重现了代码CNNDecays在宇称破缺模型中中性子和带电粒子衰变的结果。新版本的SARAH 4.11.0默认包括全一圈水平下两体衰变宽度的计算。描述了某些模型类别的当前限制。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/1f025a653983/10052_2017_5259_Fig23_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/901825a0c5d0/10052_2017_5259_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/9a1e3e1964d8/10052_2017_5259_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/bcb20e81d330/10052_2017_5259_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/b2f6237149c3/10052_2017_5259_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/c9063286b9b9/10052_2017_5259_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/baa9862cb181/10052_2017_5259_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/075865d36da6/10052_2017_5259_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/eaf5978c7737/10052_2017_5259_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/3e0a36620558/10052_2017_5259_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/d4ec5770591a/10052_2017_5259_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/bc8138ea9a0b/10052_2017_5259_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/4c25525ae17c/10052_2017_5259_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/a64669b37346/10052_2017_5259_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/166453b00abe/10052_2017_5259_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/37e1df93c283/10052_2017_5259_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/37cc7159a84b/10052_2017_5259_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/45c558996ed4/10052_2017_5259_Fig17_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/58e08abeaa79/10052_2017_5259_Fig18_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/1f24fe32f252/10052_2017_5259_Fig19_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/eea79c0587c7/10052_2017_5259_Fig20_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/d44ecc27f09e/10052_2017_5259_Fig21_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/4f6809603a94/10052_2017_5259_Fig22_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/1f025a653983/10052_2017_5259_Fig23_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/901825a0c5d0/10052_2017_5259_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/9a1e3e1964d8/10052_2017_5259_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/bcb20e81d330/10052_2017_5259_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/b2f6237149c3/10052_2017_5259_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/c9063286b9b9/10052_2017_5259_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/baa9862cb181/10052_2017_5259_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/075865d36da6/10052_2017_5259_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/eaf5978c7737/10052_2017_5259_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/3e0a36620558/10052_2017_5259_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/d4ec5770591a/10052_2017_5259_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/bc8138ea9a0b/10052_2017_5259_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/4c25525ae17c/10052_2017_5259_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/a64669b37346/10052_2017_5259_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/166453b00abe/10052_2017_5259_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/37e1df93c283/10052_2017_5259_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/37cc7159a84b/10052_2017_5259_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/45c558996ed4/10052_2017_5259_Fig17_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/58e08abeaa79/10052_2017_5259_Fig18_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/1f24fe32f252/10052_2017_5259_Fig19_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/eea79c0587c7/10052_2017_5259_Fig20_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/d44ecc27f09e/10052_2017_5259_Fig21_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/4f6809603a94/10052_2017_5259_Fig22_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c44/6956948/1f025a653983/10052_2017_5259_Fig23_HTML.jpg

相似文献

1
Generic calculation of two-body partial decay widths at the full one-loop level.全单圈水平下两体部分衰变宽度的一般计算。
Eur Phys J C Part Fields. 2017;77(11):758. doi: 10.1140/epjc/s10052-017-5259-x. Epub 2017 Nov 11.
2
Two-body decays of gluino at full one-loop level in the quark-flavour violating MSSM.在违反夸克味的最小超对称标准模型中,胶微子在完整一圈水平下的两体衰变
Eur Phys J C Part Fields. 2017;77(3):189. doi: 10.1140/epjc/s10052-017-4754-4. Epub 2017 Mar 25.
3
Supersymmetric and non-supersymmetric models without catastrophic Goldstone bosons.无灾难性戈德斯通玻色子的超对称和非超对称模型。
Eur Phys J C Part Fields. 2017;77(11):757. doi: 10.1140/epjc/s10052-017-5303-x. Epub 2017 Nov 10.
4
Six-quark decays of the Higgs boson in supersymmetry with R-parity violation.超对称中违反R宇称时希格斯玻色子的六夸克衰变
Phys Rev Lett. 2007 Nov 23;99(21):211801. doi: 10.1103/PhysRevLett.99.211801. Epub 2007 Nov 20.
5
HFOLD - A program package for calculating two-body MSSM Higgs decays at full one-loop level.HFOLD——一个用于在完整的单圈水平计算两体MSSM希格斯玻色子衰变的程序包。
Comput Phys Commun. 2011 Oct;182(10):2219-2226. doi: 10.1016/j.cpc.2011.05.007.
6
Supersymmetric exotic decays of the 125 GeV Higgs boson.125GeV 希格斯玻色子的超对称奇特衰变。
Phys Rev Lett. 2014 Jun 6;112(22):221803. doi: 10.1103/PhysRevLett.112.221803. Epub 2014 Jun 4.
7
Two-loop QCD corrections to the MSSM Higgs masses beyond the effective-potential approximation.超对称标准模型希格斯玻色子质量超出有效势近似的两圈量子色动力学修正
Eur Phys J C Part Fields. 2015;75(2):61. doi: 10.1140/epjc/s10052-015-3280-5. Epub 2015 Feb 10.
8
High-precision predictions for the light CP-even Higgs boson mass of the minimal supersymmetric standard model.高精度预测最小超对称标准模型中轻 CP 相等希格斯玻色子质量。
Phys Rev Lett. 2014 Apr 11;112(14):141801. doi: 10.1103/PhysRevLett.112.141801.
9
Search for scalar bottom quarks from gluino decays in collisions at.在对撞中从胶微子衰变中寻找标量底夸克。
Phys Rev Lett. 2006 May 5;96(17):171802. doi: 10.1103/PhysRevLett.96.171802. Epub 2006 May 4.
10
Complete two-loop QCD contributions to the lightest Higgs-boson mass in the MSSM with complex parameters.在具有复参数的最小超对称标准模型(MSSM)中,对最轻希格斯玻色子质量的完整两圈量子色动力学(QCD)贡献。
Eur Phys J C Part Fields. 2018;78(7):576. doi: 10.1140/epjc/s10052-018-6055-y. Epub 2018 Jul 14.

引用本文的文献

1
Unitarity constraints on general scalar couplings with SARAH.使用SARAH对一般标量耦合的幺正性约束。
Eur Phys J C Part Fields. 2018;78(8):649. doi: 10.1140/epjc/s10052-018-6127-z. Epub 2018 Aug 14.

本文引用的文献

1
Supersymmetric and non-supersymmetric models without catastrophic Goldstone bosons.无灾难性戈德斯通玻色子的超对称和非超对称模型。
Eur Phys J C Part Fields. 2017;77(11):757. doi: 10.1140/epjc/s10052-017-5303-x. Epub 2017 Nov 10.
2
Two-body decays of gluino at full one-loop level in the quark-flavour violating MSSM.在违反夸克味的最小超对称标准模型中,胶微子在完整一圈水平下的两体衰变
Eur Phys J C Part Fields. 2017;77(3):189. doi: 10.1140/epjc/s10052-017-4754-4. Epub 2017 Mar 25.
3
Interference effects in BSM processes with a generalised narrow-width approximation.
具有广义窄宽度近似的BSM过程中的干涉效应。
Eur Phys J C Part Fields. 2015;75(6):254. doi: 10.1140/epjc/s10052-015-3472-z. Epub 2015 Jun 9.
4
High-precision predictions for the light CP-even Higgs boson mass of the minimal supersymmetric standard model.高精度预测最小超对称标准模型中轻 CP 相等希格斯玻色子质量。
Phys Rev Lett. 2014 Apr 11;112(14):141801. doi: 10.1103/PhysRevLett.112.141801.
5
HFOLD - A program package for calculating two-body MSSM Higgs decays at full one-loop level.HFOLD——一个用于在完整的单圈水平计算两体MSSM希格斯玻色子衰变的程序包。
Comput Phys Commun. 2011 Oct;182(10):2219-2226. doi: 10.1016/j.cpc.2011.05.007.
6
Higgs boson couplings to bottom quarks: two-loop supersymmetry-QCD corrections.希格斯玻色子与底夸克的耦合:两圈超对称量子色动力学修正
Phys Rev Lett. 2008 Oct 31;101(18):181801. doi: 10.1103/PhysRevLett.101.181801. Epub 2008 Oct 27.
7
Squark production at the Fermilab Tevatron.费米实验室万亿电子伏特加速器上的S夸克产生。
Phys Rev Lett. 1995 Apr 10;74(15):2905-2908. doi: 10.1103/PhysRevLett.74.2905.
8
Erratum: Electroweak gauge boson self-energies: Complete QCD corrections.勘误:电弱规范玻色子自能:完整的量子色动力学修正。
Phys Rev D Part Fields. 1996 Apr 1;53(7):4111. doi: 10.1103/physrevd.53.4111.
9
Two-loop renormalization group equations for soft supersymmetry-breaking scalar interactions: Supergraph method.软超对称破缺标量相互作用的双圈重整化群方程:超图方法。
Phys Rev D Part Fields. 1994 Sep 1;50(5):3537-3545. doi: 10.1103/physrevd.50.3537.
10
Two-loop renormalization group equations for soft supersymmetry-breaking couplings.软超对称破缺耦合的双圈重整化群方程。
Phys Rev D Part Fields. 1994 Aug 1;50(3):2282-2292. doi: 10.1103/physrevd.50.2282.