Measurement of the branching fractions of $bar{B}to D^{(*)} K^- K^{(*)0}_{(S)}$ and $bar{B}to D^{(*)}D_s^{-}$ decays at Belle II

Kavli Affiliate: T. Higuchi | First 5 Authors: Belle II Collaboration, I. Adachi, L. Aggarwal, H. Aihara, N. Akopov | Summary: We present measurements of the branching fractions of eight $overline B{}^0to D^{(*)+} K^- K^{(*)0}_{(S)}$, $B^{-}to D^{(*)0} K^- K^{(*)0}_{(S)}$ decay channels. The results are based on data from SuperKEKB electron-positron collisions at the $Upsilon(4S)$ resonance […]


Continue.. Measurement of the branching fractions of $bar{B}to D^{(*)} K^- K^{(*)0}_{(S)}$ and $bar{B}to D^{(*)}D_s^{-}$ decays at Belle II

Measurement of the branching fractions of $bar{B}to D^{(*)} K^- K^{(*)0}_{(S)}$ and $bar{B}to D^{(*)}D_s^{-}$ decays at Belle II

Kavli Affiliate: T. Higuchi | First 5 Authors: Belle II Collaboration, I. Adachi, L. Aggarwal, H. Aihara, N. Akopov | Summary: We present measurements of the branching fractions of eight $overline B{}^0to D^{(*)+} K^- K^{(*)0}_{(S)}$, $B^{-}to D^{(*)0} K^- K^{(*)0}_{(S)}$ decay channels. The results are based on data from SuperKEKB electron-positron collisions at the $Upsilon(4S)$ resonance […]


Continue.. Measurement of the branching fractions of $bar{B}to D^{(*)} K^- K^{(*)0}_{(S)}$ and $bar{B}to D^{(*)}D_s^{-}$ decays at Belle II

Measurement of the branching fractions of $bar{B}to D^{(*)} K^- K^{(*)0}_{(S)}$ and $bar{B}to D^{(*)}D_s^{-}$ decays at Belle II

Kavli Affiliate: T. Higuchi | First 5 Authors: Belle II Collaboration, I. Adachi, L. Aggarwal, H. Aihara, N. Akopov | Summary: We present measurements of the branching fractions of eight $overline B{}^0to D^{(*)+} K^- K^{(*)0}_{(S)}$, $B^{-}to D^{(*)0} K^- K^{(*)0}_{(S)}$ decay channels. The results are based on data from SuperKEKB electron-positron collisions at the $Upsilon(4S)$ resonance […]


Continue.. Measurement of the branching fractions of $bar{B}to D^{(*)} K^- K^{(*)0}_{(S)}$ and $bar{B}to D^{(*)}D_s^{-}$ decays at Belle II

Measurement of the branching fractions of $bar{B}to D^{(*)} K^- K^{(*)0}_{(S)}$ and $bar{B}to D^{(*)}D_s^{-}$ decays at Belle II

Kavli Affiliate: T. Higuchi | First 5 Authors: Belle II Collaboration, I. Adachi, L. Aggarwal, H. Aihara, N. Akopov | Summary: We present measurements of the branching fractions of eight $overline B{}^0to D^{(*)+} K^- K^{(*)0}_{(S)}$, $B^{-}to D^{(*)0} K^- K^{(*)0}_{(S)}$ decay channels. The results are based on data from SuperKEKB electron-positron collisions at the $Upsilon(4S)$ resonance […]


Continue.. Measurement of the branching fractions of $bar{B}to D^{(*)} K^- K^{(*)0}_{(S)}$ and $bar{B}to D^{(*)}D_s^{-}$ decays at Belle II

Hawking-Page and entanglement phase transition in 2d CFT on curved backgrounds

Kavli Affiliate: Masahiro Nozaki | First 5 Authors: Akihiro Miyata, Masahiro Nozaki, Kotaro Tamaoka, Masataka Watanabe, | Summary: The thermodynamics and the entanglement properties of two-dimensional conformal field theories ($2$d CFTs) on curved backgrounds are studied. By means of conformal mapping we study the equivalent system on flat space governed by the deformed Hamiltonian, which […]


Continue.. Hawking-Page and entanglement phase transition in 2d CFT on curved backgrounds

Hypothalamic CRH Neurons Modulate Sevoflurane Anesthesia and The Post-anesthesia Stress Responses

Kavli Affiliate: Wei Min | Authors: Shan Jiang, Lu Chen, Wei-Min Qu, Zhi-Li Huang and Chang-Rui Chen | Summary: General anesthesia is a fundamental process required to undertake safely and humanely a high fraction of surgeries and invasive diagnostic procedures. However, the undesired stress response associated with general anesthesia (GA) causes delayed recovery and even […]


Continue.. Hypothalamic CRH Neurons Modulate Sevoflurane Anesthesia and The Post-anesthesia Stress Responses

Possible mixing of a diquark-antidiquark with a $p bar p$ hadronic molecule

Kavli Affiliate: Jonathan L. Rosner | First 5 Authors: Marek Karliner, Jonathan L. Rosner, , , | Summary: We discuss the possibility that the two nearby resonances observed by BESIII partially below the ,$pbar p$, threshold might be due to mixing between two metastable states with the same $J^{PC}=0^{-+}$ quantum numbers, but rather different internal […]


Continue.. Possible mixing of a diquark-antidiquark with a $p bar p$ hadronic molecule

Possible mixing of a diquark-antidiquark with a $p bar p$ hadronic molecule

Kavli Affiliate: Jonathan L. Rosner | First 5 Authors: Marek Karliner, Jonathan L. Rosner, , , | Summary: We discuss the possibility that the two nearby resonances observed by BESIII partially below the ,$pbar p$, threshold might be due to mixing between two metastable states with the same $J^{PC}=0^{-+}$ quantum numbers, but rather different internal […]


Continue.. Possible mixing of a diquark-antidiquark with a $p bar p$ hadronic molecule

Possible mixing of a diquark-antidiquark with a $p bar p$ hadronic molecule

Kavli Affiliate: Jonathan L. Rosner | First 5 Authors: Marek Karliner, Jonathan L. Rosner, , , | Summary: We discuss the possibility that the two nearby resonances observed by BESIII partially below the ,$pbar p$, threshold might be due to mixing between two metastable states with the same $J^{PC}=0^{-+}$ quantum numbers, but rather different internal […]


Continue.. Possible mixing of a diquark-antidiquark with a $p bar p$ hadronic molecule

Long Range Azimuthal Correlation, Entanglement and Bell Inequality Violation by Spinning Gluons at the LHC

Kavli Affiliate: Feng Yuan | First 5 Authors: Yuxun Guo, Xiaohui Liu, Feng Yuan, Hua Xing Zhu, | Summary: We apply the recently developed concept of the nucleon energy-energy correlator (NEEC) for the gluon sector to investigate the long-range azimuthal angular correlations in proton-proton collisions at the LHC. The spinning gluon in these collisions will […]


Continue.. Long Range Azimuthal Correlation, Entanglement and Bell Inequality Violation by Spinning Gluons at the LHC