Logarithmic corrections to O(a) and O( $$a^2$$ a 2 ) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks
Abstract We derive the asymptotic lattice spacing dependence $$a^n[2b_0\bar{g}^2(1/a)]^{\hat{\Gamma }_i}$$ a n [ 2 b 0 g ¯ 2 ( 1 / a ) ] Γ ^ i relevant for spectral quantities of lattice QCD, when using Wilson, $$\textrm{O}(a)$$ O ( a ) improved Wilson or Ginsparg–Wilson quarks. We give some example...
| الحاوية / القاعدة: | European Physical Journal C: Particles and Fields |
|---|---|
| المؤلف الرئيسي: | |
| التنسيق: | مقال |
| اللغة: | الإنجليزية |
| منشور في: |
SpringerOpen
2023-02-01
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| الوصول للمادة أونلاين: | https://doi.org/10.1140/epjc/s10052-023-11258-8 |
| _version_ | 1851893579350278144 |
|---|---|
| author | Nikolai Husung |
| author_facet | Nikolai Husung |
| author_sort | Nikolai Husung |
| collection | DOAJ |
| container_title | European Physical Journal C: Particles and Fields |
| description | Abstract We derive the asymptotic lattice spacing dependence $$a^n[2b_0\bar{g}^2(1/a)]^{\hat{\Gamma }_i}$$ a n [ 2 b 0 g ¯ 2 ( 1 / a ) ] Γ ^ i relevant for spectral quantities of lattice QCD, when using Wilson, $$\textrm{O}(a)$$ O ( a ) improved Wilson or Ginsparg–Wilson quarks. We give some examples for the spectra encountered for $$\hat{\Gamma }_i$$ Γ ^ i including the partially quenched case, mixed actions and using two different discretisations for dynamical quarks. This also includes maximally twisted mass QCD relying on automatic $$\textrm{O}(a)$$ O ( a ) improvement. At $$\textrm{O}(a^2)$$ O ( a 2 ) , all cases considered have $$\min _i\hat{\Gamma }_i\gtrsim -0.3$$ min i Γ ^ i ≳ - 0.3 if $$N_{\textrm{f}}\le 4$$ N f ≤ 4 , which ensures that the leading order lattice artifacts are not severely logarithmically enhanced in contrast to the O(3) non-linear sigma model (Balog et al. in Nucl Phys B 824:563–615, 2010; Balog et al. in Phys Lett B 676:188–192, 2009). However, we find a very dense spectrum of these leading powers, which may result in major pile-ups and cancellations. We present in detail the computational strategy employed to obtain the 1-loop anomalous dimensions already used in Husung et al. (Phys Lett B 829:137069, 2022). |
| format | Article |
| id | doaj-art-d7bf65fc930a402ea9b2c35bda66889e |
| institution | Directory of Open Access Journals |
| issn | 1434-6052 |
| language | English |
| publishDate | 2023-02-01 |
| publisher | SpringerOpen |
| record_format | Article |
| spelling | doaj-art-d7bf65fc930a402ea9b2c35bda66889e2025-08-19T22:08:41ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60522023-02-0183212410.1140/epjc/s10052-023-11258-8Logarithmic corrections to O(a) and O( $$a^2$$ a 2 ) effects in lattice QCD with Wilson or Ginsparg–Wilson quarksNikolai Husung0Physics and Astronomy, University of SouthamptonAbstract We derive the asymptotic lattice spacing dependence $$a^n[2b_0\bar{g}^2(1/a)]^{\hat{\Gamma }_i}$$ a n [ 2 b 0 g ¯ 2 ( 1 / a ) ] Γ ^ i relevant for spectral quantities of lattice QCD, when using Wilson, $$\textrm{O}(a)$$ O ( a ) improved Wilson or Ginsparg–Wilson quarks. We give some examples for the spectra encountered for $$\hat{\Gamma }_i$$ Γ ^ i including the partially quenched case, mixed actions and using two different discretisations for dynamical quarks. This also includes maximally twisted mass QCD relying on automatic $$\textrm{O}(a)$$ O ( a ) improvement. At $$\textrm{O}(a^2)$$ O ( a 2 ) , all cases considered have $$\min _i\hat{\Gamma }_i\gtrsim -0.3$$ min i Γ ^ i ≳ - 0.3 if $$N_{\textrm{f}}\le 4$$ N f ≤ 4 , which ensures that the leading order lattice artifacts are not severely logarithmically enhanced in contrast to the O(3) non-linear sigma model (Balog et al. in Nucl Phys B 824:563–615, 2010; Balog et al. in Phys Lett B 676:188–192, 2009). However, we find a very dense spectrum of these leading powers, which may result in major pile-ups and cancellations. We present in detail the computational strategy employed to obtain the 1-loop anomalous dimensions already used in Husung et al. (Phys Lett B 829:137069, 2022).https://doi.org/10.1140/epjc/s10052-023-11258-8 |
| spellingShingle | Nikolai Husung Logarithmic corrections to O(a) and O( $$a^2$$ a 2 ) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks |
| title | Logarithmic corrections to O(a) and O( $$a^2$$ a 2 ) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks |
| title_full | Logarithmic corrections to O(a) and O( $$a^2$$ a 2 ) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks |
| title_fullStr | Logarithmic corrections to O(a) and O( $$a^2$$ a 2 ) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks |
| title_full_unstemmed | Logarithmic corrections to O(a) and O( $$a^2$$ a 2 ) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks |
| title_short | Logarithmic corrections to O(a) and O( $$a^2$$ a 2 ) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks |
| title_sort | logarithmic corrections to o a and o a 2 a 2 effects in lattice qcd with wilson or ginsparg wilson quarks |
| url | https://doi.org/10.1140/epjc/s10052-023-11258-8 |
| work_keys_str_mv | AT nikolaihusung logarithmiccorrectionstooaandoa2a2effectsinlatticeqcdwithwilsonorginspargwilsonquarks |
