In quark model, the strange axial vector mesons K1(1270) and K1(1400) are defined as the mixtures of orbital angular momentum states K1A and K1B. In this work, by using the orthogonality of the mass eigenstates, we have estimated the K1(1270, 1400) mixing angle θK1, where we have found that θK1 sime −(39 ± 4)°
AbstractWe calculate the mixing angles between the spin-1/2, Ξbc–Ξbc′ and Ωbc–Ωbc′ states of doubly ...
AbstractWe propose a new parametrization for the quark and lepton mixing matrices: the two 12-mixing...
We summarize and combine the known information on the decay rates of the strangeness-one axial vecto...
Due to copyright restrictions, the access to the full text of this article is only available via sub...
The masses of K 1(3 P 1) and K 1(1 P 1) are considered in a nonrelativistic constituent quark model,...
The implications of the $f_1(1285)-f_1(1420)$ mixing for the $K_1(^3P_1)-K_1(^1P_1)$ mixing angle is...
We study properties of the strange axial mesons in the relativized quark model. We calculate the K1 ...
The mixing angle of ρ-ω vector mesons is calculated using the QCD sum rule method.We find the value ...
In the presence of the ...
We consider the axial-vector mesons $$K_1(1270)$$ and $$K_1(1400)$$ as a mixture of two $$|^3P_1\ran...
In the Standard Model with SU(2) × U(1) as the gauge group of electroweak interactions, both the qu...
It is shown that if, from the starting point of a universal rank-one mass matrix long favoured by ph...
Recently LHCb predicted spin 1 and spin 3 states Ds1⁎(2860) and Ds3⁎(2860) which are studied through...
Using the pictures for $$X(3872)$$ as a mixture of charmonium and molecular $$D^{*0}D^0$$ states; $$...
In the Standard Model, CP violation in weak interactions involving quarks is parameterized by an irr...
AbstractWe calculate the mixing angles between the spin-1/2, Ξbc–Ξbc′ and Ωbc–Ωbc′ states of doubly ...
AbstractWe propose a new parametrization for the quark and lepton mixing matrices: the two 12-mixing...
We summarize and combine the known information on the decay rates of the strangeness-one axial vecto...
Due to copyright restrictions, the access to the full text of this article is only available via sub...
The masses of K 1(3 P 1) and K 1(1 P 1) are considered in a nonrelativistic constituent quark model,...
The implications of the $f_1(1285)-f_1(1420)$ mixing for the $K_1(^3P_1)-K_1(^1P_1)$ mixing angle is...
We study properties of the strange axial mesons in the relativized quark model. We calculate the K1 ...
The mixing angle of ρ-ω vector mesons is calculated using the QCD sum rule method.We find the value ...
In the presence of the ...
We consider the axial-vector mesons $$K_1(1270)$$ and $$K_1(1400)$$ as a mixture of two $$|^3P_1\ran...
In the Standard Model with SU(2) × U(1) as the gauge group of electroweak interactions, both the qu...
It is shown that if, from the starting point of a universal rank-one mass matrix long favoured by ph...
Recently LHCb predicted spin 1 and spin 3 states Ds1⁎(2860) and Ds3⁎(2860) which are studied through...
Using the pictures for $$X(3872)$$ as a mixture of charmonium and molecular $$D^{*0}D^0$$ states; $$...
In the Standard Model, CP violation in weak interactions involving quarks is parameterized by an irr...
AbstractWe calculate the mixing angles between the spin-1/2, Ξbc–Ξbc′ and Ωbc–Ωbc′ states of doubly ...
AbstractWe propose a new parametrization for the quark and lepton mixing matrices: the two 12-mixing...
We summarize and combine the known information on the decay rates of the strangeness-one axial vecto...
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