Electronic structure and spectroscopy
... • Ĥ being the Hamilton operator of the system; • Ψ is the state function of the system; • E is the energy of the system. This is an eigenvalue equation, Ψ being the eigenfunction of Ĥ, E is the eigenvalue. This has to be solved in order to obtain the states of, e.g. molecules. According to Dirac ( ...
... • Ĥ being the Hamilton operator of the system; • Ψ is the state function of the system; • E is the energy of the system. This is an eigenvalue equation, Ψ being the eigenfunction of Ĥ, E is the eigenvalue. This has to be solved in order to obtain the states of, e.g. molecules. According to Dirac ( ...
Conductance-peak height correlations for a Coulomb
... a chaotic wave function and no correlations between different wave functions.4,5 It is known that nonuniversal correlations between different wave functions and, hence, correlations between conductance peak heights exist in both ballistic and diffusive dots.6 In ballistic quantum dots, such correlat ...
... a chaotic wave function and no correlations between different wave functions.4,5 It is known that nonuniversal correlations between different wave functions and, hence, correlations between conductance peak heights exist in both ballistic and diffusive dots.6 In ballistic quantum dots, such correlat ...
Continuous Matrix Product States for Quantum Fields
... [1] and the density matrix renormalization group (DMRG) of White [2] revolutionized the way strongly correlated quantum systems can be simulated and understood. The applicability of those approaches has been better understood during the last 5 years by rephrasing those methods in terms of matrix pro ...
... [1] and the density matrix renormalization group (DMRG) of White [2] revolutionized the way strongly correlated quantum systems can be simulated and understood. The applicability of those approaches has been better understood during the last 5 years by rephrasing those methods in terms of matrix pro ...
glvt-cnrs.fr
... 3 )2 linked by moderately strong hydrogen bonds (figure 1) [11, 12]. Decoherence is cancelled by the dynamical separation of protons from the rest of the lattice [13]. Neutron diffraction reveals, in addition to Bragg’s peaks, rods of diffuse scattering, suggesting the existence of macroscopic state ...
... 3 )2 linked by moderately strong hydrogen bonds (figure 1) [11, 12]. Decoherence is cancelled by the dynamical separation of protons from the rest of the lattice [13]. Neutron diffraction reveals, in addition to Bragg’s peaks, rods of diffuse scattering, suggesting the existence of macroscopic state ...
