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- Chiral condensate from renormalization group optimized perturbation doi link

Auteur(s): Kneur J.-L., Neveu A.

(Article) Publié: Physical Review D, vol. 92 p.074027 (2015)
Texte intégral en Openaccess : arxiv


Ref HAL: hal-01177136_v1
Ref Arxiv: 1506.07506
DOI: 10.1103/PhysRevD.92.074027
WoS: WOS:000363237400004
Ref. & Cit.: NASA ADS
Exporter : BibTex | endNote
18 Citations
Résumé:

Our recently developed variant of variationnally optimized perturbation (OPT), in particular consistently incorporating renormalization group properties (RGOPT), is adapted to the calculation of the QCD spectral density of the Dirac operator and the related chiral quark condensate $\langle \bar q q \rangle$ in the chiral limit, for $n_f=2$ and $n_f=3$ massless quarks. The results of successive sequences of approximations at two-, three-, and four-loop orders of this modified perturbation, exhibit a remarkable stability. We obtain $\langle \bar q q\rangle^{1/3}_{n_f=2}(2\, {\rm GeV}) = -(0.833-0.845) \bar\Lambda_2 $, and $ \langle\bar q q\rangle^{1/3}_{n_f=3}(2\, {\rm GeV}) = -(0.814-0.838) \bar\Lambda_3 $ where the range spanned by the first and second numbers (respectively four- and three-loop order results) defines our theoretical error, and $\bar\Lambda_{n_f}$ is the basic QCD scale in the $\overline{MS}$-scheme. We obtain a moderate suppression of the chiral condensate when going from $n_f=2$ to $n_f=3$. We compare these results with some other recent determinations from other nonperturbative methods (mainly lattice and spectral sum rules).



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