Erratum: Covariant light-front approach forB→K*γ,K1γ,K2γdecays [Phys. Rev. D69, 094007 (2004)]

Light - Front - Quantized Qcd in Covariant Gauge ∗

The light-front (LF) canonical quantization of quantum chromodynamics in covariant gauge is discussed. The Dirac procedure is used to eliminate the constraints in the gaugefixed front form theory quantum action and to construct the LF Hamiltonian formulation. The physical degrees of freedom emerge naturally. The propagator of the dynamical ψ+ part of the free fermionic propagator in the LF quan...

A Covariant Light-Front Model of Heavy Mesons within HQET

In this paper we construct a covariant light-front model of heavy mesons within the framework of heavy quark effective theory (HQET). The covariant model consists of the light-front heavy meson bound states constructed in the heavy quark limit with heavy quark symmetry and heavy quark effective theory as its basis. Within this model, the Isgur-Wise function and decay constants in the infinite q...

Erratum: "Uniqueness theorems in bioluminescence tomography" [Med. Phys. 31, 2289-2299 (2004)].

Erratum: Role of Tensorial Electronic Friction in Energy Transfer at Metal Surfaces [Phys. Rev. Lett. 116, 217601 (2016)].

This corrects the article DOI: 10.1103/PhysRevLett.116.217601.

Erratum: Growth of stochastic resonance in neuronal ensembles with the input signal intensity [Phys. Rev. E 86, 011922 (2012)].

The effective noise intensity D that is used to evaluate theoretical value of 〈C1〉 throughout the original paper is inaccurate. In Sec. III A, we derived the piecewise-linear FitzHugh-Nagumo (plFHN) neuron model, and we introduced the noise scaling ξ (t) → 7τξ (t̃) in correspondence with the time scaling t → 7τ t̃ . However, the noise should be scaled as ξ (t) → √7τξ (t̃). Therefore, the plFHN neu...