The Ontology of Bohmian Mechanics
... at rest, while particles ‘acted upon’ by a wave-function are moving—or anything of that kind. Rather, it tells us that certain wave-functions correspond to particles not moving at all, whereas other (generic) wave-functions correspond to particles moving in a particular way, as described by the guid ...
... at rest, while particles ‘acted upon’ by a wave-function are moving—or anything of that kind. Rather, it tells us that certain wave-functions correspond to particles not moving at all, whereas other (generic) wave-functions correspond to particles moving in a particular way, as described by the guid ...
Microscopic theory for quantum mirages in quantum corrals D. Porras, J. Ferna´ndez-Rossier,
... the presence of the corral is accounted for by replacing the plane waves, which diagonalize the free-surface electron Hamiltonian, by the corral states. Throughout the paper, we neglect the magnetic moment of the corral atoms. This is justified because the mirage appears also when the corral atoms a ...
... the presence of the corral is accounted for by replacing the plane waves, which diagonalize the free-surface electron Hamiltonian, by the corral states. Throughout the paper, we neglect the magnetic moment of the corral atoms. This is justified because the mirage appears also when the corral atoms a ...
Qubits with electrons on liquid helium * M. I. Dykman, P. M. Platzman,
... in helium. The relevant phonons propagate nearly normal to the surface. We find the mechanisms of electron-phonon coupling and analyze their contribution to the decay rate. Electron coupling to excitations in helium leads also to dephasing, i.e. to randomization of the phase difference between the e ...
... in helium. The relevant phonons propagate nearly normal to the surface. We find the mechanisms of electron-phonon coupling and analyze their contribution to the decay rate. Electron coupling to excitations in helium leads also to dephasing, i.e. to randomization of the phase difference between the e ...
two-loop large higgs mass contribution to vector boson anomalous
... the most important goals for the future experiments. Starting from the two-loop level radiative corrections exhibit power growth for mH ≫ MW . Leading m2H two-loop corrections to the ρ-parameter [3, 5] and to vector boson masses [4] were calculated more than ten years ago. These two-loop large Higgs ...
... the most important goals for the future experiments. Starting from the two-loop level radiative corrections exhibit power growth for mH ≫ MW . Leading m2H two-loop corrections to the ρ-parameter [3, 5] and to vector boson masses [4] were calculated more than ten years ago. These two-loop large Higgs ...
Quantification of Linear Entropy for Quantum Entanglement in He, H
... I4 (i, j, k, l, m, n, p, q, s, t, a, b, c, d) = r1i r2 r3k r4l r12 r13r14r23r24r34 e dr1 dr2 dr3 dr4 . (9) In the Appendix of this paper, we present the detailed results of Eq. (8) in terms of the I4 integrals. In [1,3,4], the authors solved this kind of four-electron integrals by carrying out the 1 ...
... I4 (i, j, k, l, m, n, p, q, s, t, a, b, c, d) = r1i r2 r3k r4l r12 r13r14r23r24r34 e dr1 dr2 dr3 dr4 . (9) In the Appendix of this paper, we present the detailed results of Eq. (8) in terms of the I4 integrals. In [1,3,4], the authors solved this kind of four-electron integrals by carrying out the 1 ...
PrntFile text - Electrogravity
... having the same units as Planck's constant but containing the required A-Vector coming from any proton. The double cross-product is then utilized as the necessary mechanics for reversing the action into a net reaction in the negative energy sense. The result is gravitational action. The acceleration ...
... having the same units as Planck's constant but containing the required A-Vector coming from any proton. The double cross-product is then utilized as the necessary mechanics for reversing the action into a net reaction in the negative energy sense. The result is gravitational action. The acceleration ...
God, Belief and Explanation
... Let us start with the assumption that we do, in some sense, see tables and chairs in a good light possessing normal eyesight and so on. Even if we don’t actually see them, ie, they are not actually being observed, nevertheless they are observable in the sense that it is possible to see them. Some ph ...
... Let us start with the assumption that we do, in some sense, see tables and chairs in a good light possessing normal eyesight and so on. Even if we don’t actually see them, ie, they are not actually being observed, nevertheless they are observable in the sense that it is possible to see them. Some ph ...
Line junctions in the quantum Hall effect - Penn Physics
... attractive interaction, a disorder-driven metal-insulator transition was predicted. This metal-insulator transition should be directly observable in such a fractional quantum Hall effect line contact. In this paper we describe in detail the experimental signature of a 1D metal-insulator transition f ...
... attractive interaction, a disorder-driven metal-insulator transition was predicted. This metal-insulator transition should be directly observable in such a fractional quantum Hall effect line contact. In this paper we describe in detail the experimental signature of a 1D metal-insulator transition f ...
Renormalization
In quantum field theory, the statistical mechanics of fields, and the theory of self-similar geometric structures, renormalization is any of a collection of techniques used to treat infinities arising in calculated quantities.Renormalization specifies relationships between parameters in the theory when the parameters describing large distance scales differ from the parameters describing small distances. Physically, the pileup of contributions from an infinity of scales involved in a problem may then result in infinities. When describing space and time as a continuum, certain statistical and quantum mechanical constructions are ill defined. To define them, this continuum limit, the removal of the ""construction scaffolding"" of lattices at various scales, has to be taken carefully, as detailed below.Renormalization was first developed in quantum electrodynamics (QED) to make sense of infinite integrals in perturbation theory. Initially viewed as a suspect provisional procedure even by some of its originators, renormalization eventually was embraced as an important and self-consistent actual mechanism of scale physics in several fields of physics and mathematics. Today, the point of view has shifted: on the basis of the breakthrough renormalization group insights of Kenneth Wilson, the focus is on variation of physical quantities across contiguous scales, while distant scales are related to each other through ""effective"" descriptions. All scales are linked in a broadly systematic way, and the actual physics pertinent to each is extracted with the suitable specific computational techniques appropriate for each.