Search results for "Reduced density matrix"

showing 10 items of 14 documents

Long-range interactions and the sign of natural amplitudes in two-electron systems

2013

In singlet two-electron systems the natural occupation numbers of the one-particle reduced density matrix are given as squares of the natural amplitudes which are defined as the expansion coefficients of the two-electron wave function in a natural orbital basis. In this work we relate the sign of the natural amplitudes to the nature of the two-body interaction. We show that long-range Coulomb-type interactions are responsible for the appearance of positive amplitudes and give both analytical and numerical examples that illustrate how the long-distance structure of the wave function affects these amplitudes. We further demonstrate that the amplitudes show an avoided crossing behavior as func…

Atomic Physics (physics.atom-ph)General Physics and AstronomyInteraction strengthFOS: Physical sciences02 engineering and technologyElectron01 natural sciencesPhysics - Atomic PhysicsCondensed Matter - Strongly Correlated Electronssymbols.namesakeQuantum mechanics0103 physical sciencesCoulombPhysical and Theoretical ChemistryWave functionPhysicsQuantum Physicsta114010304 chemical physicsStrongly Correlated Electrons (cond-mat.str-el)Avoided crossingComputational Physics (physics.comp-ph)021001 nanoscience & nanotechnologyAmplitudesymbolsReduced density matrix0210 nano-technologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Physics - Computational Physics
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Meaning and magnitude of the reduced density matrix cumulants

2012

Abstract Within the framework of a generalized normal ordering (GNO), invented by Mukherjee [1] , the reduced density matrix cumulants of the (multiconfigurational) reference wave function play a central role, as they arise directly from the contraction rules. The extended Wick theorem allows contractions of an arbitrary number of active annihilators and creators through a cumulant of corresponding rank. Because the cumulant rank truncates naturally only at the number of active spin orbitals, practical applications of the GNO concept seem to rely on a fast convergence of the cumulant series, allowing one to neglect cumulants with high rank. By computing cumulant norms for selected systems (…

Atomic orbitalExponential growthComputational chemistryChemistryGeneral Physics and AstronomySinglet stateReduced density matrixStatistical physicsElectronPhysical and Theoretical ChemistryEdgeworth seriesNotationCumulantChemical Physics
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Integral-geometrical consideration of density matrices

1995

The ensemble N-representability problem for the k-th order reduced density matrix (k-RDM) as well as the problem of reconstruction of the N-particle system density matrices (N-DM) from a given k-RDM are studied. The spatial parts of the k-RDM expansion in terms of spin tensorial operators {Theta}{sub {lambda}} are represented using particular values (at specially chosen {Xi} = {Xi}{sub o}) of the Radon transform D{sub N{lambda}} D{sub N{lambda}}({Xi}) of the N-DM spatial parts (or their sums) D{sub N{lambda}}({chi}{prime}{vert_bar}{chi}{double_prime}) (here, {Xi} is a d-plane in the n-space {Re}{double_prime} of {chi} = ({chi}{prime}, {chi}{double_prime}), with n = 6N, d = 3(N - k), {chi}{p…

Density matrixCombinatoricsOrder (ring theory)Reduced density matrixPhysical and Theoretical ChemistrySymmetry (geometry)Condensed Matter PhysicsLambdaAtomic and Molecular Physics and OpticsPrime (order theory)Spin-½International Journal of Quantum Chemistry
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Approximate energy functionals for one-body reduced density matrix functional theory from many-body perturbation theory

2018

We develop a systematic approach to construct energy functionals of the one-particle reduced density matrix (1RDM) for equilibrium systems at finite temperature. The starting point of our formulation is the grand potential $\Omega [\mathbf{G}]$ regarded as variational functional of the Green's function $G$ based on diagrammatic many-body perturbation theory and for which we consider either the Klein or Luttinger-Ward form. By restricting the input Green's function to be one-to-one related to a set on one-particle reduced density matrices (1RDM) this functional becomes a functional of the 1RDM. To establish the one-to-one mapping we use that, at any finite temperature and for a given 1RDM $\…

Grand potentialSolid-state physicsComplex systemFOS: Physical sciencesdensity matrix functional theory01 natural sciencesCondensed Matter - Strongly Correlated Electronssymbols.namesakePhysics - Chemical Physics0103 physical sciencesSDG 7 - Affordable and Clean Energy010306 general physicsMathematical physicsEnergy functionalChemical Physics (physics.chem-ph)PhysicsQuantum Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyStrongly Correlated Electrons (cond-mat.str-el)010304 chemical physicstiheysfunktionaaliteoriamany-body perturbation theory16. Peace & justiceCondensed Matter PhysicsStationary pointElectronic Optical and Magnetic MaterialsCondensed Matter - Other Condensed Matterapproximate energy functionalssymbolsReduced density matrixapproksimointiQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)Ground stateOther Condensed Matter (cond-mat.other)The European Physical Journal B
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E0 suppression in pion photoproduction on 13C

1990

Abstract Recently measured anomalously low cross sections for 13 C(γ, π − ) 13 N at low energy and θ π lab = 90° 0761 have been analyzed in a DWIA calculation. It has been found that the EO contribution alone is able to explain the data, so that the M1 cross section is expected to vanish. Using constraints from recent magnetic electron scattering, an explanation is possible by assuming a significantly lower reduced density matrix element for spin-flip isovector transitions with angular momentum L = 2 than predicted by Cohen and Kurath.

Nuclear physicsPhysicsNuclear and High Energy PhysicsCross section (physics)Angular momentumPionLow energyIsovectorQuantum electrodynamicsReduced density matrixElectron scatteringPhysics Letters B
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Phononic heat transport in the transient regime: An analytic solution

2016

We investigate the time-resolved quantum transport properties of phonons in arbitrary harmonic systems connected to phonon baths at different temperatures. We obtain a closed analytic expression of the time-dependent one-particle reduced density matrix by explicitly solving the equations of motion for the nonequilibrium Green's function. This is achieved through a well-controlled approximation of the frequency-dependent bath self-energy. Our result allows for exploring transient oscillations and relaxation times of local heat currents, and correctly reduces to an earlier known result in the steady-state limit. We apply the formalism to atomic chains, and benchmark the validity of the approx…

PhononEnergy dispersionphononsFOS: Physical sciencesNon-equilibrium thermodynamics02 engineering and technology01 natural sciencesSettore FIS/03 - Fisica della MateriaQuantum transportMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesElectronicOptical and Magnetic Materials010306 general physicsquantum transportfononitElectronic Optical and Magnetic Materials; Condensed Matter PhysicsPhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsAnalytical expressionsta114Equations of motionCondensed Matter Physics021001 nanoscience & nanotechnologyClassical mechanicsReduced density matrix0210 nano-technologyAnalytic solutionheat transport
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A Wigner molecule at extremely low densities: a numerically exact study

2019

In this work we investigate Wigner localization at very low densities by means of the exact diagonalization of the Hamiltonian. This yields numerically exact results. In particular, we study a quasi-one-dimensional system of two electrons that are confined to a ring by three-dimensional gaussians placed along the ring perimeter. To characterize the Wigner localization we study several appropriate observables, namely the two-body reduced density matrix, the localization tensor and the particle-hole entropy. We show that the localization tensor is the most promising quantity to study Wigner localization since it accurately captures the transition from the delocalized to the localized state an…

Physics010304 chemical physicsStrongly Correlated Electrons (cond-mat.str-el)PhysicsQC1-999FOS: Physical sciencesObservableElectron01 natural sciences[CHIM.THEO]Chemical Sciences/Theoretical and/or physical chemistryDelocalized electronCondensed Matter - Strongly Correlated ElectronsExact resultsQuantum mechanics0103 physical sciencesMoleculeEntropy (information theory)Reduced density matrix[PHYS.COND]Physics [physics]/Condensed Matter [cond-mat]010306 general physics
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Number-parity effect for confined fermions in one dimension

2015

For $N$ spin-polarized fermions with harmonic pair interactions in a $1$-dimensional trap an odd-even effect is found. The spectrum of the $1$-particle reduced density matrix of the system's ground state differs qualitatively for $N$ odd and $N$ even. This effect does only occur for strong attractive and repulsive interactions. Since it does not exists for bosons, it must originate from the repulsive nature implied by the fermionic exchange statistics. In contrast to the spectrum, the $1$-particle density and correlation function for strong attractive interactions do not show any sensitivity on the number parity. This also suggests that reduced-density-matrix-functional theory has a more su…

PhysicsCondensed Matter::Quantum GasesQuantum PhysicsFOS: Physical sciencesParity (physics)Fermion01 natural sciences010305 fluids & plasmasQuantum Gases (cond-mat.quant-gas)Quantum mechanics0103 physical sciencesReduced density matrixCondensed Matter - Quantum GasesQuantum Physics (quant-ph)010306 general physicsGround stateParity effectBosonPhysical Review A
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Diverging exchange force and form of the exact density matrix functional

2019

For translationally invariant one-band lattice models, we exploit the ab initio knowledge of the natural orbitals to simplify reduced density matrix functional theory (RDMFT). Striking underlying features are discovered: First, within each symmetry sector, the interaction functional $\mathcal{F}$ depends only on the natural occupation numbers $\bf{n}$. The respective sets $\mathcal{P}^1_N$ and $\mathcal{E}^1_N$ of pure and ensemble $N$-representable one-matrices coincide. Second, and most importantly, the exact functional is strongly shaped by the geometry of the polytope $\mathcal{E}^1_N \equiv \mathcal{P}^1_N $, described by linear constraints $D^{(j)}(\bf{n})\geq 0$. For smaller systems,…

PhysicsDensity matrixChemical Physics (physics.chem-ph)Exchange forceQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)General Physics and AstronomyFOS: Physical sciences01 natural sciencesCombinatoricsCondensed Matter - Strongly Correlated ElectronsAtomic orbitalLattice (order)Physics - Chemical Physics0103 physical sciencesReduced density matrix010306 general physicsFunctional theoryQuantum Physics (quant-ph)
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Estimation of the Repeatedly-Projected Reduced Density Matrix under Decoherence

2007

Decoherence is believed to deteriorate the ability of a purification scheme that is based on the idea of driving a system to a pure state by repeatedly measuring another system in interaction with the former and hinder for a pure state to be extracted asymptotically. Nevertheless, we find a way out of this difficulty by deriving an analytic expression of the reduced density matrix for a two-qubit system immersed in a bath. It is shown that we can still extract a pure state if the environment brings about only dephasing effects. In addition, for a dissipative environment, there is a possibility of obtaining a dominant pure state when we perform a finite number of measurements.

PhysicsDensity matrixQuantum PhysicsQuantum decoherenceSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciAnalytical expressionsDephasingsteFoundations of quantum mechanicFOS: Physical sciencesState (functional analysis)DecoherenceAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della MateriaClassical mechanicsDissipative systemReduced density matrixopen systemQuantum Physics (quant-ph)Finite set
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