27,931 research outputs found

    Theoretical investigation of the molecular nature of Ds0βˆ—(2317)D_{s0}^*(2317) and Ds1(2460)D_{s1}(2460) and the possibility of observing the DDΛ‰KD\bar{D}K bound state KccΛ‰(4180)K_{c\bar{c}}(4180) in inclusive e+eβˆ’β†’ccΛ‰e^+e^-\to c\bar{c} collisions

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    Searching for exotic multiquark states and elucidating their nature remains a central topic in understanding quantum chromodynamics--the underlying theory of the strong interaction. Two of the most studied such states are the charm-strange states Ds0βˆ—(2317)D_{s0}^*(2317) and Ds1(2460)D_{s1}(2460). In this letter, we show for the first time that their prompt production yields in inclusive e+eβˆ’β†’ccΛ‰e^+e^-\to c\bar{c} collisions near s=10.6\sqrt{s}=10.6 GeV measured by the BABAR Collaboration, Y(Ds0βˆ—(2317))Y(D_{s0}^*(2317)) and Y(Ds1(2460))Y(D_{s1}(2460)), in particular the ratio R=Y(Ds0βˆ—(2317))/Y(Ds1(2460))R=Y(D_{s0}^*(2317))/Y(D_{s1}(2460)), can be well explained in the molecular picture, which provide a highly nontrivial verification of their nature being DK/Dβˆ—KDK/D^*K molecules. On the contrary, treating them as pure csΛ‰c\bar{s} Pβˆ’P-wave states, the statistical model predicts a ratio RR smaller than unity, in contrast with the experimental central value, though in agreement with it considering its relatively large uncertainty. In addition, we predict the production yield of the DDΛ‰KD\bar{D}K three-body bound state, KccΛ‰(4180)K_{c\bar{c}}(4180), in e+eβˆ’β†’ccΛ‰e^+e^-\to c\bar{c} collisions and find that it is within the reach of the ongoing Belle II experiment. The present study demonstrates the feasibility of a novel method to unravel the nature of exotic hadrons and the potential of electron-positron collisions in this regard.Comment: 8 pages, 3 figures; more discussions and comparison with the statistical model adde

    A Comparative Study on Spin-Orbit Torque Efficiencies from W/ferromagnetic and W/ferrimagnetic Heterostructures

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    It has been shown that W in its resistive form possesses the largest spin-Hall ratio among all heavy transition metals, which makes it a good candidate for generating efficient dampinglike spin-orbit torque (DL-SOT) acting upon adjacent ferromagnetic or ferrimagnetic (FM) layer. Here we provide a systematic study on the spin transport properties of W/FM magnetic heterostructures with the FM layer being ferromagnetic Co20_{20}Fe60_{60}B20_{20} or ferrimagnetic Co63_{63}Tb37_{37} with perpendicular magnetic anisotropy. The DL-SOT efficiency ∣ξDL∣|\xi_{DL}|, which is characterized by a current-induced hysteresis loop shift method, is found to be correlated to the microstructure of W buffer layer in both W/Co20_{20}Fe60_{60}B20_{20} and W/Co63_{63}Tb37_{37} systems. Maximum values of ∣ξDLβˆ£β‰ˆ0.144|\xi_{DL}|\approx 0.144 and ∣ξDLβˆ£β‰ˆ0.116|\xi_{DL}|\approx 0.116 are achieved when the W layer is partially amorphous in the W/Co20_{20}Fe60_{60}B20_{20} and W/Co63_{63}Tb37_{37} heterostructures, respectively. Our results suggest that the spin Hall effect from resistive phase of W can be utilized to effectively control both ferromagnetic and ferrimagnetic layers through a DL-SOT mechanism
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