Spin or, Actually: Spin and Quantum Statistics
... understand how crystalline or quasi-crystalline order can be derived as a consequence of equilibrium quantum statistical mechanics. All this shows how little we understand about ‘emergent behavior’ of many-particle systems on the basis of fundamental theory. We are not trying to make an argument aga ...
... understand how crystalline or quasi-crystalline order can be derived as a consequence of equilibrium quantum statistical mechanics. All this shows how little we understand about ‘emergent behavior’ of many-particle systems on the basis of fundamental theory. We are not trying to make an argument aga ...
Document
... Coherent state is an eigen state of the annihilation operator: Removing one boson does NOT change a coherent state! ...
... Coherent state is an eigen state of the annihilation operator: Removing one boson does NOT change a coherent state! ...
Neural Network Algorithms-Quantum-Glia
... If left alone – a linear ‘combination’ of basis states (in coherence) ...
... If left alone – a linear ‘combination’ of basis states (in coherence) ...
Aalborg Universitet Cornean, Decebal Horia
... • [BCS 1] Briet, P., Cornean, H.D., Savoie, B.: Diamagnetism of quantum gases with singular potentials. J. Phys. A: Math. Theor. 43, 474008 (2010) • [CN 1] Cornean, H.D., Nenciu, G.: The Faraday effect revisited: Thermodynamic limit. J. Funct. Anal. 257 (7), 2024-2066 (2009) • [BCS 2] Briet, P., Cor ...
... • [BCS 1] Briet, P., Cornean, H.D., Savoie, B.: Diamagnetism of quantum gases with singular potentials. J. Phys. A: Math. Theor. 43, 474008 (2010) • [CN 1] Cornean, H.D., Nenciu, G.: The Faraday effect revisited: Thermodynamic limit. J. Funct. Anal. 257 (7), 2024-2066 (2009) • [BCS 2] Briet, P., Cor ...
What is CPH_Theory - VBN
... sub-quantum scale such as in the structure of a photon? In interaction between gravity and photon (blueshift), when gravity acts on photon and gravitons enter the structure of photon, gravitons do change the intensity of electric and magnetic fields which belong to photon. So, gravitons behave so th ...
... sub-quantum scale such as in the structure of a photon? In interaction between gravity and photon (blueshift), when gravity acts on photon and gravitons enter the structure of photon, gravitons do change the intensity of electric and magnetic fields which belong to photon. So, gravitons behave so th ...
Zitterbewegung and the Electron - Scientific Research Publishing
... the photon when it follows a straight axis and has momentum ( p = mc ) in direction of that axis, represents the particle of mass (m) when its axis forms a circle around a fixed point in space and is thus completely localized. Its possible positions then lie on a torus around the fixed point, with t ...
... the photon when it follows a straight axis and has momentum ( p = mc ) in direction of that axis, represents the particle of mass (m) when its axis forms a circle around a fixed point in space and is thus completely localized. Its possible positions then lie on a torus around the fixed point, with t ...
Vacuum-Entanglement
... (II) Are Bells' inequalities violated? Yes, for arbitrary separation. (Filtration, “hidden” non-locality). (III) Where does it “come from”? Localization, shielding. (Harmonic Chain). ...
... (II) Are Bells' inequalities violated? Yes, for arbitrary separation. (Filtration, “hidden” non-locality). (III) Where does it “come from”? Localization, shielding. (Harmonic Chain). ...
Macroscopic Distinguishability Between Quantum States
... F (|gihg|, |g̃ihg̃|) = |hg|g̃i|, and for U < Uc (and δU sufficiently small, i.e. δU < Uc − U ) we see that the fidelity is identical to 1. This is a simple consequence of our mean-field approximation based on a simplified description in terms of single particle energy states. On the magnetic side of ...
... F (|gihg|, |g̃ihg̃|) = |hg|g̃i|, and for U < Uc (and δU sufficiently small, i.e. δU < Uc − U ) we see that the fidelity is identical to 1. This is a simple consequence of our mean-field approximation based on a simplified description in terms of single particle energy states. On the magnetic side of ...
POISSON BOUNDARIES OVER LOCALLY COMPACT
... It is known that there exists a probability measure space (Π, ν), the Poisson boundary of (G, µ), such that L∞ (Π, ν) can be identified with the weak* closed subspace Hµ of L∞ (G) which consists of all µ-harmonic functions, i.e., functions h on G satisfying Φµ (h) = h. The noncommutative version of ...
... It is known that there exists a probability measure space (Π, ν), the Poisson boundary of (G, µ), such that L∞ (Π, ν) can be identified with the weak* closed subspace Hµ of L∞ (G) which consists of all µ-harmonic functions, i.e., functions h on G satisfying Φµ (h) = h. The noncommutative version of ...
Quantum mechanical modeling of the CNOT (XOR) gate
... However, in Section 4 we have considered the two-qubit system as an isolated system, but we have obtained that Ĥint does not have any global symmetry - which, also, directly follows from eq. (5). This produces a contradiction. 5.2 The contradiction It is worth emphasizing the above distinguished co ...
... However, in Section 4 we have considered the two-qubit system as an isolated system, but we have obtained that Ĥint does not have any global symmetry - which, also, directly follows from eq. (5). This produces a contradiction. 5.2 The contradiction It is worth emphasizing the above distinguished co ...
A Suggested Interpretation of the Quantum Theory in Terms of
... the particle position, but can say only that the particle must be somewhere in the region in which ~f~ is appreciable. Similarly, the momentum of a particle that happens to be at the point, x, is given by p= Vs(x), so that since x is not known, the precise value of p is also not, in general, inferra ...
... the particle position, but can say only that the particle must be somewhere in the region in which ~f~ is appreciable. Similarly, the momentum of a particle that happens to be at the point, x, is given by p= Vs(x), so that since x is not known, the precise value of p is also not, in general, inferra ...
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... a (semi)additive structure, the superpositions characteristic of quantum phenomena can be captured at this abstract level. Moreover, the biproduct structure interacts with the compact-closed structure in a non-trivial fashion. In particular, the distributivity of tensor product over biproduct allows ...
... a (semi)additive structure, the superpositions characteristic of quantum phenomena can be captured at this abstract level. Moreover, the biproduct structure interacts with the compact-closed structure in a non-trivial fashion. In particular, the distributivity of tensor product over biproduct allows ...
Aharonov-Bohm effect
... charged particle and electric and magnetic fields [1]. Electric and magnetic fields are uniquely described by Maxwell’s equations, which we will describe in detail in next section. As we will see, description of electromagnetic phenomena can be simplified by introduction of electromagnetic potential ...
... charged particle and electric and magnetic fields [1]. Electric and magnetic fields are uniquely described by Maxwell’s equations, which we will describe in detail in next section. As we will see, description of electromagnetic phenomena can be simplified by introduction of electromagnetic potential ...