On the Formulation of Quant`um Mechanics associated with
... instant, and thus a connection between this formulation and that of Feyninan's is taken out. Hydrodynamical picture formally equivalent to the statistical picture in one-body problems is also considered, and from such analogy certain formal generalization of SchrOdinger equation is suggested. ...
... instant, and thus a connection between this formulation and that of Feyninan's is taken out. Hydrodynamical picture formally equivalent to the statistical picture in one-body problems is also considered, and from such analogy certain formal generalization of SchrOdinger equation is suggested. ...
Cosmic quantum measurement - Proceedings of the Royal Society A
... at the time t0 when both of them ®ash. The light from S0 is received simultaneously at A0 and B0 with respect to L0 , and this is clearly not simultaneous with respect to L. Hence relativity. There is an alternative proof (Percival 1998b) of Hardy’s theorem, which depends on two Bell experiments in ...
... at the time t0 when both of them ®ash. The light from S0 is received simultaneously at A0 and B0 with respect to L0 , and this is clearly not simultaneous with respect to L. Hence relativity. There is an alternative proof (Percival 1998b) of Hardy’s theorem, which depends on two Bell experiments in ...
`To Be, To Be, What Does it Mean to Be?` : On Quantum
... assumed to exist, “it can hardly be assumed to change causally” [4, p. 154]. In other words, while phenomena and events in question can be seen as “effects” brought about by certain processes, these processes cannot be seen in causal terms: these effects are effect without (classical) causes. I sha ...
... assumed to exist, “it can hardly be assumed to change causally” [4, p. 154]. In other words, while phenomena and events in question can be seen as “effects” brought about by certain processes, these processes cannot be seen in causal terms: these effects are effect without (classical) causes. I sha ...
SOLID-STATE PHYSICS 3, Winter 2008 O. Entin-Wohlman Conductivity and conductance
... (denoted “1”) to another (denoted “2”), by a diffusion process. The electron can take many paths between 1 and 2. In a classical calculation, we sum all over all the probabilities of the various paths; in quantum mechanics, we sum over the amplitudes of the various paths, and only then compute the t ...
... (denoted “1”) to another (denoted “2”), by a diffusion process. The electron can take many paths between 1 and 2. In a classical calculation, we sum all over all the probabilities of the various paths; in quantum mechanics, we sum over the amplitudes of the various paths, and only then compute the t ...
QMLeipzig_June02 - Buffalo Ontology Site
... ... and always up-to-date To be a book = to have a reference number in the Catalogue System Each of the ontologies produced by ontological engineers deals with objects which are constructed (Kantians would say ‚constituted‘) by the database itself ...
... ... and always up-to-date To be a book = to have a reference number in the Catalogue System Each of the ontologies produced by ontological engineers deals with objects which are constructed (Kantians would say ‚constituted‘) by the database itself ...
--Fundamental Problems and Application to Material Science-
... seek for a universal theory behind the quantum chaos. In §4, we derive a universal dynamical system from generic quantum systems whose Hamiltonians possess only a singl~ nonintegrability parameter. In § 5, a high-dimensional field theory is constructed, corresponding to adiabatic-ansatz induced eige ...
... seek for a universal theory behind the quantum chaos. In §4, we derive a universal dynamical system from generic quantum systems whose Hamiltonians possess only a singl~ nonintegrability parameter. In § 5, a high-dimensional field theory is constructed, corresponding to adiabatic-ansatz induced eige ...
Beating the Standard Quantum Limit
... associated to A and B.] In (B) we see a coherent state (depicted through its Wigner function): it has the same spreads in position and momentum ∆x = ∆p. In (C) and (D), squeezed states are shown: they have reduced fluctuations in one of the two incompatible observables [i.e. x for (C) and p for (D)] ...
... associated to A and B.] In (B) we see a coherent state (depicted through its Wigner function): it has the same spreads in position and momentum ∆x = ∆p. In (C) and (D), squeezed states are shown: they have reduced fluctuations in one of the two incompatible observables [i.e. x for (C) and p for (D)] ...
Matthew Hastings
... must be small since the entropy across the cut is large. So, by Lindblad-Uhlmann theorem, the relative entropy S(ρj−l+1,j+l ||ρj−l+1,j ⊗ ρj+1,j+l ) must be large. But this is bounded by S2l − 2Sl . Putting in the constants gives the desired result. ...
... must be small since the entropy across the cut is large. So, by Lindblad-Uhlmann theorem, the relative entropy S(ρj−l+1,j+l ||ρj−l+1,j ⊗ ρj+1,j+l ) must be large. But this is bounded by S2l − 2Sl . Putting in the constants gives the desired result. ...
Gauge-Gravity Duality and the Black Hole Interior
... point of view of an external observer. Here we apply this to examine recent claims [4] and counterclaims regarding the nature of the black hole interior. In Sec. II we present an argument that, without other significant departures from effective field theory (EFT), typical black holes must have fire ...
... point of view of an external observer. Here we apply this to examine recent claims [4] and counterclaims regarding the nature of the black hole interior. In Sec. II we present an argument that, without other significant departures from effective field theory (EFT), typical black holes must have fire ...
Parallel Universes
... 1.This type of parallel universes is sort of a catch-all for other mathematical structures which we can conceive of, but which we don't observe as physical realities in our universe. 2.The Level 4 parallel universes are ones which are governed by different equations from those that govern our univer ...
... 1.This type of parallel universes is sort of a catch-all for other mathematical structures which we can conceive of, but which we don't observe as physical realities in our universe. 2.The Level 4 parallel universes are ones which are governed by different equations from those that govern our univer ...