From 979719066f570aff96306ccf9e3cc7e269b5326e Mon Sep 17 00:00:00 2001 From: Felix Hekhorn Date: Mon, 13 Jan 2025 14:40:00 +0200 Subject: [PATCH] rust: Add missing ref for polarized ad --- crates/ekore/refs.bib | 12 ++++++++++++ crates/ekore/src/bib.rs | 14 +++++++++++++- crates/ekore/src/constants.rs | 16 ++++++++-------- 3 files changed, 33 insertions(+), 9 deletions(-) diff --git a/crates/ekore/refs.bib b/crates/ekore/refs.bib index 0035b7a39..8d155ed48 100644 --- a/crates/ekore/refs.bib +++ b/crates/ekore/refs.bib @@ -107,3 +107,15 @@ @article{Bierenbaum2009zt pages = "401--406", year = "2009" } +@article{Gluck1995yr, + author = "Gluck, M. and Reya, E. and Stratmann, M. and Vogelsang, W.", + title = "{Next-to-leading order radiative parton model analysis of polarized deep inelastic lepton - nucleon scattering}", + eprint = "hep-ph/9508347", + archivePrefix = "arXiv", + reportNumber = "DO-TH-95-13, RAL-TR-95-042", + doi = "10.1103/PhysRevD.53.4775", + journal = "Phys. Rev. D", + volume = "53", + pages = "4775--4786", + year = "1996" +} diff --git a/crates/ekore/src/bib.rs b/crates/ekore/src/bib.rs index 3e8a1eb8f..175efe194 100644 --- a/crates/ekore/src/bib.rs +++ b/crates/ekore/src/bib.rs @@ -1,4 +1,4 @@ -//! List of References (autogenerated on 2024-09-10T11:22:16.645053). +//! List of References (autogenerated on 2025-01-13T14:38:04.013494). #[allow(non_snake_case)] /// The Three loop splitting functions in QCD: The Nonsinglet case @@ -107,3 +107,15 @@ pub fn Buza1996wv() {} /// /// DOI: [10.1016/j.physletb.2009.01.057](https:dx.doi.org/10.1016/j.physletb.2009.01.057) pub fn Bierenbaum2009zt() {} + +#[allow(non_snake_case)] +/// Next-to-leading order radiative parton model analysis of polarized deep inelastic lepton - nucleon scattering +/// +/// Gluck, M. and Reya, E. and Stratmann, M. and Vogelsang, W. +/// +/// Published in: Phys. Rev. D 53 (1996), 4775--4786 +/// +/// e-Print: [hep-ph/9508347](https://arxiv.org/abs/hep-ph/9508347) +/// +/// DOI: [10.1103/PhysRevD.53.4775](https:dx.doi.org/10.1103/PhysRevD.53.4775) +pub fn Gluck1995yr() {} diff --git a/crates/ekore/src/constants.rs b/crates/ekore/src/constants.rs index 43da87af8..10c8cc2d6 100644 --- a/crates/ekore/src/constants.rs +++ b/crates/ekore/src/constants.rs @@ -20,14 +20,14 @@ pub const CA: f64 = NC as f64; /// Defaults to $C_F = \frac{N_C^2-1}{2N_C} = 4/3$. pub const CF: f64 = ((NC * NC - 1) as f64) / ((2 * NC) as f64); -/// Up quark charge square. +/// Up quark electric charge square. /// -/// Defaults to $e_u^2 = 4./9$ +/// Defaults to $e_u^2 = 4./9$. pub const EU2: f64 = 4. / 9.; -/// Down quark charge square. +/// Down quark electric charge square. /// -/// Defaults to $e_d^2 = 1./9$ +/// Defaults to $e_d^2 = 1./9$. pub const ED2: f64 = 1. / 9.; /// Riemann zeta function at z = 2. @@ -52,16 +52,16 @@ pub const PID_NSM: u16 = 10201; /// non-singlet all-valence |PID|. pub const PID_NSV: u16 = 10200; -/// singlet-like non-singlet up-sector |PID| +/// singlet-like non-singlet up-sector |PID|. pub const PID_NSP_EU2: u16 = 10102; -/// singlet-like non-singlet down-sector |PID| +/// singlet-like non-singlet down-sector |PID|. pub const PID_NSP_ED2: u16 = 10103; -/// valence-like non-singlet up-sector |PID| +/// valence-like non-singlet up-sector |PID|. pub const PID_NSM_EU2: u16 = 10202; -/// valence-like non-singlet down-sector |PID| +/// valence-like non-singlet down-sector |PID|. pub const PID_NSM_ED2: u16 = 10203; /// |QED| electric charge combinations.