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Dispersive lensing and shadows in RN-AdS spacetimes with dark energy and plasma: theory and observational constraints. [PDF]
Pradhan A, Ghaderi K, Zeyauddin M.
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Renormalization group for Anderson localization on high-dimensional lattices. [PDF]
Altshuler BL +4 more
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Positronium Atoms Solvated in Liquid Alcohols: A Multicomponent Quantum Mechanics/Molecular Mechanics Approach. [PDF]
Martins L +5 more
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Quantum mechanics and path integrals
2015Abstract This chapter discusses the Feymann path-integral approach to quantum mechanics. First, it derives a path integral expression for the evolution operator. Next, it shows that the classical equations of motion, that is, those obtained from the principle of least action, are obtained from this path integral formulation in the limit ...
Efstratios Manousakis
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By expanding Feynman path integrals in a Fourier series a practical Monte Carlo method is developed to calculate the thermodynamic properties of interacting systems obeymg quantum Boltzmann statistical mechanics.
David L Freeman, Freeman David L
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Path Integrals in Relativistic Quantum Mechanics
1994This paper is a review of path integral representations for semigroups {exp(-t H_r/ħ)}{t≥0} where H_r's are relativistic quantum Hamiltonians. We consider three different cases: in the first one Hr is a relativistic Schrödinger operator, in the second is the Hamiltonian associated to Klein-Gordon equation and in the third is that coming from the Dirac
De Angelis G. F, SERVA, Maurizio
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Path integrals in quantum mechanics
2011Path integrals provide in many instances an elegant complementary description of quantum mechanics and also for the quantization of fields, which we will study from a canonical point of view in Chapter ?? and following chapters. Path integrals are particularly popular in scattering theory, because the techniques of path integration were originally ...
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Quantum Mechanical Path Integrals
2010The fundamental equation of quantum mechanics for a single particle is generally taken to be a Schrodinger equation of the form $$i\hbar\frac{\partial}{\partial t}\psi(x, t) =\left[-\frac{{\hbar}^{2}}{2m} \frac{{\partial}^{2}}{{\partial}{x}^{2}}+{V (x, t)}\right] \psi(x, t),$$ subject to some initial condition such as $$\lim_{t \rightarrow t^
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