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Revisiting the chiral interactions with the local momentum-space regularization up to the third order and the nature of
We revisit the DD* interactions in chiral effective field theory up to the third order for the first
time. We deal with the pion-exchanged interactions via local momentum-space …
time. We deal with the pion-exchanged interactions via local momentum-space …
Doubly heavy tetraquark states in the constituent quark model using diffusion Monte Carlo method
We use the diffusion Monte Carlo (DMC) method to calculate the doubly heavy tetraquark T
cc system in two kinds of constituent quark models, the pure constituent quark model …
cc system in two kinds of constituent quark models, the pure constituent quark model …
Higher-order exceptional point in a pseudo-Hermitian cavity optomechanical system
Higher-order exceptional points (EPs), resulting from non-Hermitian degeneracies, have
shown greater advantages in sensitive enhancement than second-order EPs (EP2s) …
shown greater advantages in sensitive enhancement than second-order EPs (EP2s) …
Spectrum of the molecular tetraquarks: Unraveling the and
We relate the interactions of the D¯(*) K* and D (*) K* systems to those of D (*) D (*) and D
(*) D¯(*) respectively, considering the residual strong interactions at the near-threshold …
(*) D¯(*) respectively, considering the residual strong interactions at the near-threshold …
Higher-order exceptional point in a blue-detuned non-Hermitian cavity optomechanical system
Higher-order exceptional points (EPs) in non-Hermitian systems have attracted great interest
due to their advantages in sensitive enhancement and distinct topological features …
due to their advantages in sensitive enhancement and distinct topological features …
Doubly heavy tetraquark bound and resonant states
We calculate the energy spectrum of the S-wave doubly heavy tetraquark systems, including
the QQ (′) q¯ q¯, QQ (′) s¯ q¯, and QQ (′) s¯ s¯(Q (′)= b, c and q= u, d) systems within …
the QQ (′) q¯ q¯, QQ (′) s¯ q¯, and QQ (′) s¯ s¯(Q (′)= b, c and q= u, d) systems within …
Isospin violation effect and three-body decays of the state
In this work, we make a study of the T cc+ state observed by the LHCb collaboration in 2021.
In obtaining the effective potentials using the one-boson-exchange potential model we use …
In obtaining the effective potentials using the one-boson-exchange potential model we use …
Entanglement dynamics in anti--symmetric systems
YL Fang, JL Zhao, DX Chen, YH Zhou, Y Zhang… - Physical Review …, 2022 - APS
In the past years, many efforts have been made to study various noteworthy phenomena in
both parity-time (PT) and anti-parity-time (APT) symmetric systems. However, entanglement …
both parity-time (PT) and anti-parity-time (APT) symmetric systems. However, entanglement …
Controllable optical-sideband generation and synchronization in a mechanical gain-loss optomechanical system
The interaction between light and mechanical vibrations in a cavity is often exploited to
produce higher-order sidebands (HOSs) or combs, which are used in optical communication …
produce higher-order sidebands (HOSs) or combs, which are used in optical communication …
Extension of Noether's theorem in -symmetry systems and its experimental demonstration in an optical setup
QC Wu, JL Zhao, YL Fang, Y Zhang, DX Chen… - Science China Physics …, 2023 - Springer
Noether's theorem is one of the fundamental laws in physics, relating the symmetry of a
physical system to its constant of motion and conservation law. On the other hand, there …
physical system to its constant of motion and conservation law. On the other hand, there …