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Naumov- and Toshev-like relations in the renormalization-group evolution of quarks and Dirac neutrinos
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作者 邢志忠 周顺 《Chinese Physics C》 SCIE CAS CSCD 2018年第10期38-43,共6页
In an analytical way of studying matter effects on neutrino oscillations, the Naumov and Toshev relations have been derived to respectively link the Jarlskog invariant of CP violation and the Dirac phase in the standa... In an analytical way of studying matter effects on neutrino oscillations, the Naumov and Toshev relations have been derived to respectively link the Jarlskog invariant of CP violation and the Dirac phase in the standard parametrization of the 3×3 flavor mixing matrix to their matter-corrected counterparts. Here we show that there exist similar relations for Dirac neutrinos and charged leptons evolving with energy scales via the one-loop renormalizationgroup (RG) equations in the tau-dominance approximation, and for the running behaviors of up- and down-type quarks in the top-dominance approximation, provided a different parametrization is taken into account. 展开更多
关键词 fermion flavor mixing CP violation renormalization-group equations
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Entanglement and quantum phase transition in the Heisenberg-Ising model 被引量:1
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作者 谭小东 金柏琪 高微 《Chinese Physics B》 SCIE EI CAS CSCD 2013年第2期105-108,共4页
We use the quantum renormalization-group(QRG) method to study the entanglement and quantum phase transition(QPT) in the one-dimensional spin-1/2 Heisenberg-Ising model [Lieb E,Schultz T and Mattis D 1961 Ann.Phys.... We use the quantum renormalization-group(QRG) method to study the entanglement and quantum phase transition(QPT) in the one-dimensional spin-1/2 Heisenberg-Ising model [Lieb E,Schultz T and Mattis D 1961 Ann.Phys.(N.Y.) 16 407].We find the quantum phase boundary of this model by investigating the evolution of concurrence in terms of QRG iterations.We also investigate the scaling behavior of the system close to the quantum critical point,which shows that the minimum value of the first derivative of concurrence and the position of the minimum scale with an exponent of the system size.Also,the first derivative of concurrence between two blocks diverges at the quantum critical point,which is directly associated with the divergence of the correlation length. 展开更多
关键词 quantum renormalization-group quantum phase transition Heisenberg-Ising model
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Two-Dimensional Saddle Point Equation of Ginzburg-Landau Hamiltonian for the Diluted Ising Model
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作者 吴新天 《Chinese Physics Letters》 SCIE CAS CSCD 2006年第2期305-308,共4页
The saddle point equation of Ginzburg-Landau Hamiltonian for the diluted Ising model is developed. The ground state is solved numerically in two dimensions. The result is partly explained by the coarse-grained approxi... The saddle point equation of Ginzburg-Landau Hamiltonian for the diluted Ising model is developed. The ground state is solved numerically in two dimensions. The result is partly explained by the coarse-grained approximation. 展开更多
关键词 REPLICA-SYMMETRY-BREAKING CRITICAL-BEHAVIOR SUPERFLUID TRANSITION renormalization-group DISORDERED-SYSTEMS RANDOM TEMPERATURE FERROMAGNET PHASE LIQUID-HE-4 STABILITY
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Block Entanglement in the Single-Hole Hubbard Model
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作者 姚凯伦 孙效中 +3 位作者 刘祖黎 李彦超 喻莉 高国营 《Chinese Physics Letters》 SCIE CAS CSCD 2006年第9期2352-2355,共4页
We investigate the distribution of the entanglement of the one-dimensional single-hole Hubbard model (HM) and study the relationship between the entanglement and quantum phase transition in the model. The von Neuman... We investigate the distribution of the entanglement of the one-dimensional single-hole Hubbard model (HM) and study the relationship between the entanglement and quantum phase transition in the model. The von Neumann entropy of a block with neighbouring spins L for a single-hole HM is calculated using the densitymatrix renormalization group. The distributions of the entanglement entropy in the ground state, as a function of block length, show a dramatic effect, i.e. effectively decoupling with the centres, no matter how the Coulomb interaction u 〉0 or u 〈0. Contrarily, for the Coulomb interaction u = 0 or close to zero, the entanglement entropy in the single-hole model reaches a saturation value for a certain block size. For a fixed size L = 40, the ground state entanglement entropy measure, as a function of u1 shows a peak corresponding to the critical quantum phase transition. 展开更多
关键词 QUANTUM renormalization-groupS PHASE-TRANSITION ENTROPY
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Energy Spectrum of Turbulent Velocity Pulsations at Arbitrary Values of Fluid Viscosity
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作者 Edward V. Teodorovich 《Journal of Modern Physics》 2020年第10期1502-1513,共12页
The problem of calculating the energy spectrum of turbulent velocity pulsations in the case of homogeneous isotropic and stationary turbulence is considered. The domain of turbulent energy production is treated as “a... The problem of calculating the energy spectrum of turbulent velocity pulsations in the case of homogeneous isotropic and stationary turbulence is considered. The domain of turbulent energy production is treated as “a black box” on which boundary the spectral energy flux is given. It is assumed that the spectrum is formatted due to intermodal interactions being local in the wave-number space that leads to a cascade mechanism of energy transfer along the wave-number spectrum and the possibility of using the renormalization-group method related to the Markovian features of the process under consideration. The obtained formula for energy spectrum is valid in a wide wave-number range and at arbitrary values of fluid viscosity. It is shown that in functional formulation of the statistical theory of turbulence, the procedure of separating local intermodal interactions, which govern energy transfer (straining effect), and filtering out nonlocal interactions, which have no influence on energy transfer (sweeping effect), is directly described without providing additional arguments or conjectures commonly used in the renormalization-group analysis of turbulent spectra. 展开更多
关键词 Spectral Flux Spectral Energy Density Local and Nonlocal Interactions Inertial Term renormalization-group Invariance Epsilon-Expansion Procedure
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