6,429 research outputs found

    Coupled-channel analysis of the possible D(βˆ—)D(βˆ—)D^{(*)}D^{(*)}, BΛ‰(βˆ—)BΛ‰(βˆ—)\bar{B}^{(*)}\bar{B}^{(*)} and D(βˆ—)BΛ‰(βˆ—)D^{(*)}\bar{B}^{(*)} molecular states

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    We perform a coupled-channel study of the possible deuteron-like molecules with two heavy flavor quarks, including the systems of D(βˆ—)D(βˆ—)D^{(*)}D^{(*)} with double charm, BΛ‰(βˆ—)BΛ‰(βˆ—)\bar{B}^{(*)}\bar{B}^{(*)} with double bottom and D(βˆ—)BΛ‰(βˆ—)D^{(*)}\bar{B}^{(*)} with both charm and bottom, within the one-boson-exchange model. In our study, we take into account the S-D mixing which plays an important role in the formation of the loosely bound deuteron, and particularly, the coupled-channel effect in the flavor space. According to our calculation, the states D(βˆ—)D(βˆ—)[I(JP)=0(1+)]D^{(*)}D^{(*)}[I(J^P)=0(1^+)] and (D(βˆ—)D(βˆ—))s[JP=1+](D^{(*)}D^{(*)})_s[J^P=1^+] with double charm, the states BΛ‰(βˆ—)BΛ‰(βˆ—)[I(JP)=0(1+),0(2+),1(0+),1(1+),1(2+)]\bar{B}^{(*)}\bar{B}^{(*)}[I(J^P)=0(1^+),0(2^+),1(0^+),1(1^+),1(2^+)], (BΛ‰(βˆ—)BΛ‰(βˆ—))s[JP=0+,1+,2+](\bar{B}^{(*)}\bar{B}^{(*)})_s[J^P=0^+,1^+,2^+] and (BΛ‰(βˆ—)BΛ‰(βˆ—))ss[JP=0+,1+,2+](\bar{B}^{(*)}\bar{B}^{(*)})_{ss}[J^P=0^+,1^+,2^+] with double bottom, and the states D(βˆ—)BΛ‰(βˆ—)[I(JP)=0(0+),0(1+)]D^{(*)}\bar{B}^{(*)}[I(J^P)=0(0^+),0(1^+)] and (D(βˆ—)BΛ‰(βˆ—))s[JP=0+,1+](D^{(*)}\bar{B}^{(*)})_s[J^P=0^+,1^+] with both charm and bottom are good molecule candidates. However, the existence of the states D(βˆ—)D(βˆ—)[I(JP)=0(2+)]D^{(*)}D^{(*)}[I(J^P)=0(2^+)] with double charm and D(βˆ—)BΛ‰(βˆ—)[I(JP)=1(1+)]D^{(*)}\bar{B}^{(*)}[I(J^P)=1(1^+)] with both charm and bottom is ruled out.Comment: 1 figure added, published in Physical Review

    CW-pumped telecom band polarization entangled photon pair generation in a Sagnac interferometer

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    A polarization entangled photon pair source is widely used in many quantum information processing applications such as teleportation, quantum swapping, quantum computation and high precision quantum metrology. Here, we report on the generation of a continuous-wave pumped degenerated 1550 nm polarization entangled photon pair source at telecom wavelength using a type-II phase-matched periodically poled KTiOPO4 crystal in a Sagnac interferometer. Hong-Ou-Mandel-type interference measurement shows the photon bandwidth of 2.4 nm. High quality of entanglement is verified by various kinds of measurements, for example two-photon interference fringes, Bell inequality and quantum states tomography. The wavelength of photons can be tuned over a broad range by changing the temperature of crystal or pump power without losing the quality of entanglement. This source will be useful for building up long-distance quantum networks

    BKP hierarchy and Pfaffian point process

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    Inspired by Okounkov's work [\emph{Selecta Mathematica}, 7(1):57--81, 2001] which relates KP hierarchy to determinant point process, we establish a relationship between BKP hierarchy and Pfaffian point process. We prove that the correlation function of the shifted Schur measures on strict partitions can be expressed as a Pfaffian of skew symmetric matrix kernel, whose elememts are certain vacuum expectations of neutral fermions. We further show that the matrix integrals solution of BKP hierarchy can also induce a certain Pfaffian point process.Comment: 17 page

    Enhanced spectral sensitivity of a chip-scale photonic-crystal slow-light interferometer

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    We experimentally demonstrate that the spectral sensitivity of a Mach-Zehnder (MZ) interferometer can be enhanced through structural slow light. We observe a 20 times enhancement by placing a dispersion-engineered-slow-light photonic-crystal waveguide in one arm of a fibre-based MZ interferometer. The spectral sensitivity of the interferometer increases roughly linearly with the group index, and we have quantified the resolution in terms of the spectral density of interference fringes. These results show promise for the use of slow-light methods for developing novel tools for optical metrology and, specifically, for compact high-resolution spectrometers
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