Search results for "Runge–Gross theorem"

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Continuity equation and local gauge invariance for the N3LO nuclear energy density functionals

2011

Background: The next-to-next-to-next-to-leading order (N3LO) nuclear energy density functional extends the standard Skyrme functional with new terms depending on higher-order derivatives of densities, introduced to gain better precision in the nuclear many-body calculations. A thorough study of the transformation properties of the functional with respect to different symmetries is required, as a step preliminary to the adjustment of the coupling constants. Purpose: Determine to which extent the presence of higher-order derivatives in the functional can be compatible with the continuity equation. In particular, to study the relations between the validity of the continuity equation and invari…

PhysicsDensity matrixNuclear and High Energy PhysicsNuclear Theoryta114IsovectorOrbital-free density functional theoryRunge–Gross theoremFOS: Physical sciencesTime-dependent density functional theoryNuclear Theory (nucl-th)Continuity equationQuantum mechanicsDensity functional theoryGauge theoryMathematical physicsPhysical Review C
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Beyond the Runge–Gross Theorem

2012

The Runge–Gross theorem (Runge and Gross, Phys Rev Lett, 52:997–1000, 1984) states that for a given initial state the time-dependent density is a unique functional of the external potential. Let us elaborate a bit further on this point. Suppose we could solve the time-dependent Schrodinger equation for a given many-body system, i.e. we specify an initial state \(| \Uppsi_0 \rangle\) at \(t=t_0\) and evolve the wavefunction in time using the Hamiltonian \({\hat{H}} (t).\) Then, from the wave function, we can calculate the time-dependent density \(n (\user2{r},t).\) We can then ask the question whether exactly the same density \(n(\user2{r},t)\) can be reproduced by an external potential \(v^…

Physicssymbols.namesakeModuloQuantum mechanicsRunge–Gross theoremsymbolsLinear response functionWave functionHamiltonian (quantum mechanics)Schrödinger equationMathematical physics
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