9,923 research outputs found

    Raman fingerprint of semi-metal WTe2 from bulk to monolayer

    Get PDF
    Tungsten ditelluride (WTe2), a layered transition-metal dichalcogenide (TMD), has recently demonstrated an extremely large magnetoresistance effect, which is unique among TMDs. This fascinating feature seems to be correlated with its special electronic structure. Here, we report the observation of 6 Raman peaks corresponding to the A_2^4, A_1^9, A_1^8, A_1^6, A_1^5 and A_1^2 phonons, from the 33 Raman-active modes predicted for WTe2. This provides direct evidence to distinguish the space group of WTe2 from that of other TMDs. Moreover, the Raman evolution of WTe2 from bulk to monolayer is clearly revealed. It is interesting to find that the A_2^4 mode, centered at ~109.8 cm-1, is forbidden in a monolayer, which may be attributable to the transition of the point group from C2v (bulk) to C2h (monolayer). Our work characterizes all observed Raman peaks in the bulk and few-layer samples and provides a route to study the physical properties of two-dimensional WTe2.Comment: 19 pages, 4 figures and 2 table

    Holographic R\'enyi entropy for CFT with WW symmetry

    Get PDF
    In this paper we investigate the holographic R\'enyi entropy of two disjoint intervals on complex plane with small cross ratio xx for conformal field theory with WW symmetry in the ground state, which could be dual to a higher spin AdS3_3 gravity. We focus on the cases of W3W_3 and W4W_4 symmetries. In order to see the nontrivial contributions from the WW fields, we calculate the R\'enyi entropy in the expansion of xx to order x8x^8 in both the gravity and the CFT sides. In the gravity side the classical contributions to the entanglement entropy is still given by the Ryu-Takayanagi area formula under the reasonable assumption, while the 1-loop quantum corrections have to take into account of the contributions not only from massless gravitons, but also from massless higher spin fields. In the CFT side we still use the operator product expansion of twist operators in the small interval limit, but now we need to consider the quasiprimary fields constructed from WW fields, besides the ones from Virasoro Verma module. In the large central charge limit, we obtain the classical, 1-loop, 2-loop, and 3-loop parts of the R\'enyi entropy. The classical and 1-loop results in the gravity and the CFT sides are in exact match. This confirms the higher spin gravity/CFT correspondence, and also supports the holographic computation of R\'enyi entanglement entropy, including the quantum correction, in both the AdS3_3 gravity and the higher spin AdS3_3 gravity.Comment: 32 pages, published versio

    Hidden Conformal Symmetry of Extremal Black Holes

    Full text link
    We study the hidden conformal symmetry of the extremal black holes. We introduce a new set of conformal coordinates to write the SL(2,R)SL(2,R) generators. We find that the Laplacian of the scalar field in many extremal black holes could be written in terms of the SL(2,R)SL(2,R) quadratic Casimir. This suggests that there exist dual CFT descriptions of these black holes. From the conformal coordinates, the temperatures of the dual CFTs could be read directly. For the extremal black hole, the Hawking temperature is vanishing. Correspondingly, only the left (right) temperature of the dual CFT is non-vanishing and the excitations of the other sector are suppressed. In the probe limit, we compute the scattering amplitudes of the scalar off the extremal black holes and find perfect agreement with the CFT prediction.Comment: 16 pages; Published versio

    The Electromagnetic Decays of BcΒ±(2S)B^{\pm}_c(2S)

    Full text link
    We calculate the electromagnetic (EM) decay widths of the BcΒ±(2S)B^{\pm}_c(2S) meson, which is observed recently by the ATLAS Collaboration. The main EM decay channels of this particle are 13S1Ξ³1{^3S_1}\gamma and 1PΞ³1{P}\gamma, which, in literature, are estimated to have the branching ratio of about 1/101/10. In this work, we get the partial decay widths: Ξ“(21S0β†’13S1Ξ³)=0.192\Gamma(2{^1S_0}\rightarrow 1{^3S_1}\gamma)=0.192 keV, Ξ“(21S0β†’1P1Ξ³)=2.24\Gamma(2{^1S_0}\rightarrow 1{P_1}\gamma) = 2.24 keV and Ξ“(21S0β†’1P1β€²Ξ³)=11.4\Gamma(2{^1S_0}\rightarrow 1{P_1^\prime}\gamma) = 11.4 keV. In the calculation, the instantaneous approximated Bethe-Salpeter method is used. For the PP-wave BcB_c mesons, the wave functions are given by mixing the 3P1^3P_1 and 1P1^1P_1 states. Within the Mandelstam formalism, the decay amplitude is given, which includes the relativistic corrections.Comment: 9 pages, 3 figures, 3 table
    • …
    corecore