scholarly journals Anomaly constraint on massless QCD and the role of Skyrmions in chiral symmetry breaking

2018 ◽  
Vol 2018 (8) ◽  
Author(s):  
Yuya Tanizaki
Chirality ◽  
2003 ◽  
Vol 15 (3) ◽  
pp. 238-241 ◽  
Author(s):  
Kouichi Asakura ◽  
Masato Hayashi ◽  
Shuichi Osanai

2000 ◽  
Vol 84 (19) ◽  
pp. 4405-4408 ◽  
Author(s):  
T. Buhse ◽  
D. Durand ◽  
D. Kondepudi ◽  
J. Laudadio ◽  
S. Spilker

2022 ◽  
Vol 2022 (01) ◽  
pp. 005
Author(s):  
Mayumi Aoki ◽  
Jisuke Kubo ◽  
Jinbo Yang

Abstract Dynamical chiral symmetry breaking in a QCD-like hidden sector is used to generate the Planck mass and the electroweak scale including the heavy right-handed neutrino mass. A real scalar field transmits the energy scale of the hidden sector to the visible sectors, playing besides a role of inflaton in the early Universe while realizing a Higgs-inflation-like model. Our dark matter candidates are hidden pions that raise due to dynamical chiral symmetry breaking. They are produced from the decay of inflaton. Unfortunately, it will be impossible to directly detect them, because they are super heavy (109 ∼ 12 GeV), and moreover the interaction with the visible sector is extremely suppressed.


2011 ◽  
Vol 26 (04) ◽  
pp. 279-288 ◽  
Author(s):  
HARLEEN DAHIYA ◽  
NEETIKA SHARMA

The implications of chiral symmetry breaking and SU(3) symmetry breaking have been studied in the chiral constituent quark model (χCQM). The role of hidden strangeness component has been investigated for the scalar matrix elements of the nucleon with an emphasis on the meson–nucleon sigma terms. The χCQM is able to give a qualitative and quantitative description of the "quark sea" generation through chiral symmetry breaking. The significant contribution of the strangeness is consistent with the recent available experimental observations.


2011 ◽  
Vol 84 (3) ◽  
Author(s):  
Patrick O. Bowman ◽  
Kurt Langfeld ◽  
Derek B. Leinweber ◽  
André Sternbeck ◽  
Lorenz von Smekal ◽  
...  

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