The implications of the f 1(1285)-f 1(1420) mixing for the K 1(3 P 1)- K 1(1 P 1) mixing angle are investigated. Based on the f 1(1285)-f 1(1420) mixing angle ∼ 50° suggested from the analysis for a substantial body of data concerning the f 1(1420) and f 1(1285), the masses of the K 1(3 P 1) and K 1(1 P 1) are determined to be ∼ 1307.35±0.63 MeV and 1370.03±9.69 MeV, respectively, which therefore suggests that the K 1(3 P 1)- K 1(1 P 1) mixing angle is about ±(59.55±2.81)°. Also, it is found that the mass of the h ′ 1(1 P 1) (mostly of s¯) state is about 1495.18±8.82 MeV. Comparison of the predicted results and the available experimental information of the h 1(1380) shows that without further confirmation on the h 1(1380), the assignment of...
While the ground-state tensor ($J^{PC}=2^{++}$) mesons $a_{2}(1320)$, $K_{2}^{\ast}(1430)$, $f_{2}(1...
Abstract Estimating the contribution from axial-vector intermediate states to hadronic light-by-ligh...
We consider the axial-vector mesons $$K_1(1270)$$ and $$K_1(1400)$$ as a mixture of two $$|^3P_1\ran...
The implications of the $f_1(1285)-f_1(1420)$ mixing for the $K_1(^3P_1)-K_1(^1P_1)$ mixing angle is...
The masses of K 1(3 P 1) and K 1(1 P 1) are considered in a nonrelativistic constituent quark model,...
In quark model, the strange axial vector mesons K1(1270) and K1(1400) are defined as the mixtures of...
Due to copyright restrictions, the access to the full text of this article is only available via sub...
We summarize and combine the known information on the decay rates of the strangeness-one axial vecto...
The value of the η-η′ mixing angle θp is phenomenologically deduced from a rather exhaustive and up-...
We study properties of the strange axial mesons in the relativized quark model. We calculate the K1 ...
In the presence of the ...
Abstract The axial-vector mesons $$f_1(1285)$$ f 1 ( 1285 ) and $$f_1(1420)$$ f 1 ( 1420 ) are parti...
A new determination of the QA-QB mixing angle and of the antisymmetric coupling for the vector-pseud...
The mixing angle of ρ-ω vector mesons is calculated using the QCD sum rule method.We find the value ...
We perform a theoretical study of the χ→ϕKK¯→ϕKπK¯ reaction taking into account the KK¯ final state ...
While the ground-state tensor ($J^{PC}=2^{++}$) mesons $a_{2}(1320)$, $K_{2}^{\ast}(1430)$, $f_{2}(1...
Abstract Estimating the contribution from axial-vector intermediate states to hadronic light-by-ligh...
We consider the axial-vector mesons $$K_1(1270)$$ and $$K_1(1400)$$ as a mixture of two $$|^3P_1\ran...
The implications of the $f_1(1285)-f_1(1420)$ mixing for the $K_1(^3P_1)-K_1(^1P_1)$ mixing angle is...
The masses of K 1(3 P 1) and K 1(1 P 1) are considered in a nonrelativistic constituent quark model,...
In quark model, the strange axial vector mesons K1(1270) and K1(1400) are defined as the mixtures of...
Due to copyright restrictions, the access to the full text of this article is only available via sub...
We summarize and combine the known information on the decay rates of the strangeness-one axial vecto...
The value of the η-η′ mixing angle θp is phenomenologically deduced from a rather exhaustive and up-...
We study properties of the strange axial mesons in the relativized quark model. We calculate the K1 ...
In the presence of the ...
Abstract The axial-vector mesons $$f_1(1285)$$ f 1 ( 1285 ) and $$f_1(1420)$$ f 1 ( 1420 ) are parti...
A new determination of the QA-QB mixing angle and of the antisymmetric coupling for the vector-pseud...
The mixing angle of ρ-ω vector mesons is calculated using the QCD sum rule method.We find the value ...
We perform a theoretical study of the χ→ϕKK¯→ϕKπK¯ reaction taking into account the KK¯ final state ...
While the ground-state tensor ($J^{PC}=2^{++}$) mesons $a_{2}(1320)$, $K_{2}^{\ast}(1430)$, $f_{2}(1...
Abstract Estimating the contribution from axial-vector intermediate states to hadronic light-by-ligh...
We consider the axial-vector mesons $$K_1(1270)$$ and $$K_1(1400)$$ as a mixture of two $$|^3P_1\ran...