We study possible exotic J~(PC)=0~+- states using tetraquark interpolating currents with the QCD sum rule approach. The extracted masses are around 4.85GeV for the charmonium-like states and 11.25 GeV for the bottomonium-like states. There is no working region for the light tetraquark currents, which implies that the light 0~+- state may not exist below 2GeV.中国科技核心期刊(ISTIC)0325-3
We study the mass of the state Y(2175) of J(PC)=1(--) in the QCD sum rule. We construct both the diq...
Stimulated by the renewed observation of Ds0⁎(2317) signal and its updated mass value 2318.3±1.2±1.2...
We study the tetraquark states with I(G)J(PC) = 1(-)1(-+) in the QCD sum rule. After exhausting all ...
We study possible exotic J(PC) = 0(+-) states using tetraquark interpolating currents with the QCD s...
We study the possible charmoniumlike states with J(PC) 0(--), 0(-+) using the tetraquark interpolati...
Some hadrons have the exotic quantum numbers that the traditional $$\bar{q} q$$ mesons and qqq baryo...
We study the tetraquark state with I(G)J(PC) = 0(+)1(-+) in the QCD sum rule. We exhaust all possibl...
We apply the method of QCD sum rules to study the $$s s {\bar{s}} {\bar{s}}$$ tetraquark states of $...
We study a QCD sum rule analysis for an exotic tetraquark ud (s) over bar (s) over bar of J(P)=0(+) ...
Lots of charmonium-like structures have been observed. Most of them share the same quantum numbers w...
We study the possible spin-1 charmonium-like states by using QCD sum rule approach. We calculate the...
We use QCD sum rules to test the nature of the recently observed mesons Y(4260), Y(4350) and Y(4660)...
We develop a moment QCD sum rule method augmented by fundamental inequalities to study the existence...
By using QCD Sum Rules, we found that the charged hidden charm tetraquark [cu][c¯d¯] states with JP=...
We test the validity of the QCD sum rules applied to the meson Z(+)(4430). by considering a diquark-...
We study the mass of the state Y(2175) of J(PC)=1(--) in the QCD sum rule. We construct both the diq...
Stimulated by the renewed observation of Ds0⁎(2317) signal and its updated mass value 2318.3±1.2±1.2...
We study the tetraquark states with I(G)J(PC) = 1(-)1(-+) in the QCD sum rule. After exhausting all ...
We study possible exotic J(PC) = 0(+-) states using tetraquark interpolating currents with the QCD s...
We study the possible charmoniumlike states with J(PC) 0(--), 0(-+) using the tetraquark interpolati...
Some hadrons have the exotic quantum numbers that the traditional $$\bar{q} q$$ mesons and qqq baryo...
We study the tetraquark state with I(G)J(PC) = 0(+)1(-+) in the QCD sum rule. We exhaust all possibl...
We apply the method of QCD sum rules to study the $$s s {\bar{s}} {\bar{s}}$$ tetraquark states of $...
We study a QCD sum rule analysis for an exotic tetraquark ud (s) over bar (s) over bar of J(P)=0(+) ...
Lots of charmonium-like structures have been observed. Most of them share the same quantum numbers w...
We study the possible spin-1 charmonium-like states by using QCD sum rule approach. We calculate the...
We use QCD sum rules to test the nature of the recently observed mesons Y(4260), Y(4350) and Y(4660)...
We develop a moment QCD sum rule method augmented by fundamental inequalities to study the existence...
By using QCD Sum Rules, we found that the charged hidden charm tetraquark [cu][c¯d¯] states with JP=...
We test the validity of the QCD sum rules applied to the meson Z(+)(4430). by considering a diquark-...
We study the mass of the state Y(2175) of J(PC)=1(--) in the QCD sum rule. We construct both the diq...
Stimulated by the renewed observation of Ds0⁎(2317) signal and its updated mass value 2318.3±1.2±1.2...
We study the tetraquark states with I(G)J(PC) = 1(-)1(-+) in the QCD sum rule. After exhausting all ...