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Revisiting \(K_1(1270)- K_1(1400)\) mixing in QCD sum rules
We investigate the \(K_1(1270)-K_1(1400)\) mixing caused by the flavor \(SU(3)\) symmetry breaking. The mixing angle is expressed by a \(K_{1A}\to K_{1B}\) matrix element induced by the operators that breaks flavor \(SU(3)\) symmetry. The QCD contribution to this matrix element is assumed to be domi...
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description | We investigate the \(K_1(1270)-K_1(1400)\) mixing caused by the flavor \(SU(3)\) symmetry breaking. The mixing angle is expressed by a \(K_{1A}\to K_{1B}\) matrix element induced by the operators that breaks flavor \(SU(3)\) symmetry. The QCD contribution to this matrix element is assumed to be dominated and calculated by QCD sum rules. A three-point correlation function is defined and handled both at the hadron and quark-gluon levels. The quark-gluon level calculation is based on operator product expansion up to dimension-5 condensates. A detailed numerical analysis is performed to determine the Borel parameters, and the obtained mixing angle is \(\theta_{K_1}=22^{\circ}\pm 7^{\circ}\) or \(\theta_{K_1}=68^{\circ}\pm 7^{\circ}\). |
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The mixing angle is expressed by a \(K_{1A}\to K_{1B}\) matrix element induced by the operators that breaks flavor \(SU(3)\) symmetry. The QCD contribution to this matrix element is assumed to be dominated and calculated by QCD sum rules. A three-point correlation function is defined and handled both at the hadron and quark-gluon levels. The quark-gluon level calculation is based on operator product expansion up to dimension-5 condensates. 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subjects | Broken symmetry Correlation Flavor (particle physics) Gluons Numerical analysis Operators (mathematics) Quantum chromodynamics Quarks Sum rules |
title | Revisiting \(K_1(1270)- K_1(1400)\) mixing in QCD sum rules |
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