Diverging equilibration times in long
... of classical long-range systems [9]. Virtually all finitesystem results in the field have been obtained by numerical techniques, supplemented by analytical calculations in the N → ∞ Vlasov continuum limit [6]. In this Letter, analytic results on equilibration in longrange quantum spin models are rep ...
... of classical long-range systems [9]. Virtually all finitesystem results in the field have been obtained by numerical techniques, supplemented by analytical calculations in the N → ∞ Vlasov continuum limit [6]. In this Letter, analytic results on equilibration in longrange quantum spin models are rep ...
Probability in the Many-Worlds Interpretation of Quantum Mechanics
... a completely symmetrical situation there cannot be different names. So, the symmetry is not complete. We only assume that all relevant aspects of the three stations are completely identical, but we accept a possibility, and in fact a necessity, that there are other properties of the stations, like p ...
... a completely symmetrical situation there cannot be different names. So, the symmetry is not complete. We only assume that all relevant aspects of the three stations are completely identical, but we accept a possibility, and in fact a necessity, that there are other properties of the stations, like p ...
Quantum orders in an exact soluble model
... In 1989, it was realized that FQH states, having a robust topological degeneracy, contain a completely new kind of order - topological order.[5] A whole new theory was developed to describe the topological orders in FQH liquids. (For a review, see Ref. [6].) The Landau’s theory was developed for cla ...
... In 1989, it was realized that FQH states, having a robust topological degeneracy, contain a completely new kind of order - topological order.[5] A whole new theory was developed to describe the topological orders in FQH liquids. (For a review, see Ref. [6].) The Landau’s theory was developed for cla ...
Artificial Intelligence and Nature’s Fundamental Process Peter Marcer and Peter Rowlands
... iterative but the immediate zeroing gives us recursivity as well. A single fermion can only be ‘created’ if we simultaneously create the rest of the universe as a kind of reverse image, whose structure is completely defined. We don’t have to know how to construct the universe, only that it must have ...
... iterative but the immediate zeroing gives us recursivity as well. A single fermion can only be ‘created’ if we simultaneously create the rest of the universe as a kind of reverse image, whose structure is completely defined. We don’t have to know how to construct the universe, only that it must have ...
Quantum Leaps in Philosophy of Mind
... evolving quantum state to produce the actual sequence of psychophysical Process 1 events that constitute the cornerstone of von Neumann’s formulation of quantum theory. This ontological proposal goes well beyond what the pragmatic Copenhagen philosophy encompasses, but is in general alignment with t ...
... evolving quantum state to produce the actual sequence of psychophysical Process 1 events that constitute the cornerstone of von Neumann’s formulation of quantum theory. This ontological proposal goes well beyond what the pragmatic Copenhagen philosophy encompasses, but is in general alignment with t ...
PHYSICS VS. SEMANTICS: A PUZZLING CASE
... A case for the project of excising of confusion and obfuscation in the contemporary quantum theory initiated and promoted by David Deutsch has been made. It has been argued that at least some theoretical entities which are convenionally labelled as ”interpretations” of quantum mechanics are in fact ...
... A case for the project of excising of confusion and obfuscation in the contemporary quantum theory initiated and promoted by David Deutsch has been made. It has been argued that at least some theoretical entities which are convenionally labelled as ”interpretations” of quantum mechanics are in fact ...
Non Ideal Measurements by David Albert (Philosophy, Columbia) and Barry Loewer
... states like (3) in which, according to Healey's interpretation, pointers fail to have positions, or even approximately have positions. The question for the modal interpretation then is whether interactions like (2) actually occur. We argued previously that they do occur and that, in fact, non_ideal ...
... states like (3) in which, according to Healey's interpretation, pointers fail to have positions, or even approximately have positions. The question for the modal interpretation then is whether interactions like (2) actually occur. We argued previously that they do occur and that, in fact, non_ideal ...
Barad_On Touching--The Inhuman That Therefore I Am (v1.1)
... field theory, frames the difficulty in explicitly moral terms: “Instead of going directly from one point to another, the electron goes along for a while and suddenly emits a photon; then (horrors!) it absorbs its own photon. Perhaps there’s something ‘immoral’ about that, but the electron does it!” ...
... field theory, frames the difficulty in explicitly moral terms: “Instead of going directly from one point to another, the electron goes along for a while and suddenly emits a photon; then (horrors!) it absorbs its own photon. Perhaps there’s something ‘immoral’ about that, but the electron does it!” ...
Realization of the Quantum Toffoli Gate with Trapped Ions
... values of both the ideal and realized -matrices are depicted in Fig. 2. The ‘‘fingerprint’’ of the ideal -matrix is clearly visible in the experimental data. A quantitative measure for the performance of the gate operation is the mean gate fidelity Fmean ¼ mean c i ½h c i jUTy Eðj c i i h c i jÞ ...
... values of both the ideal and realized -matrices are depicted in Fig. 2. The ‘‘fingerprint’’ of the ideal -matrix is clearly visible in the experimental data. A quantitative measure for the performance of the gate operation is the mean gate fidelity Fmean ¼ mean c i ½h c i jUTy Eðj c i i h c i jÞ ...
Chapter_9 - Experimental Elementary Particle Physics Group
... If the meanings assigned to our labels are arbitrary, then these are simply two different manifolds with their own topologies, but for a physical theory we may wish to decide whether the true objects of our study - the objects with ontological status in our theory are formal fractions or the values ...
... If the meanings assigned to our labels are arbitrary, then these are simply two different manifolds with their own topologies, but for a physical theory we may wish to decide whether the true objects of our study - the objects with ontological status in our theory are formal fractions or the values ...
