fermi dirac statistics in solids
... must be much larger, this is because the electrons are not classical particles, but wavicals, don’t scatter like particles, in addition, the vrms from Boltzmann-Maxwell is one order of magnitude smaller than the vfermi following from Fermi-Dirac statistics ...
... must be much larger, this is because the electrons are not classical particles, but wavicals, don’t scatter like particles, in addition, the vrms from Boltzmann-Maxwell is one order of magnitude smaller than the vfermi following from Fermi-Dirac statistics ...
The variational principle and simple properties of the ground
... restrict ourselves to this case, because velocity-dependent potentials can give rise to spontaneous symmetry breaking, as pointed out in Ref. 4. Spontaneous symmetry breaking could lead to degeneracy in the ground-state wave function and the proof given here does not hold. If the Hamiltonian is rota ...
... restrict ourselves to this case, because velocity-dependent potentials can give rise to spontaneous symmetry breaking, as pointed out in Ref. 4. Spontaneous symmetry breaking could lead to degeneracy in the ground-state wave function and the proof given here does not hold. If the Hamiltonian is rota ...
How to use the Cosmological Schwinger principle for Energy
... the frequency [TΔS / dist ] = h ⋅ [[ω Final − ω initial ] / dist ] to obey, in the limits that k Æ 0 as is in Eq. (3) above. If , as an example, Donnelly_ and Jacobson’s dispersion relationship[21] as of his Eq. (30) can be reconciled with the limits of k Æ 0 as is in our Eq. (3) , and [TΔS / dist ] ...
... the frequency [TΔS / dist ] = h ⋅ [[ω Final − ω initial ] / dist ] to obey, in the limits that k Æ 0 as is in Eq. (3) above. If , as an example, Donnelly_ and Jacobson’s dispersion relationship[21] as of his Eq. (30) can be reconciled with the limits of k Æ 0 as is in our Eq. (3) , and [TΔS / dist ] ...
Chaotic field theory: a sketch
... Armed with a computer and a great deal of skill, one can obtain a numerical solution to a nonlinear PDE. The real question is; once a solution is found, what is to be done with it? The periodic orbit theory is an answer to this question. Dynamics drives a given spatially extended system through a re ...
... Armed with a computer and a great deal of skill, one can obtain a numerical solution to a nonlinear PDE. The real question is; once a solution is found, what is to be done with it? The periodic orbit theory is an answer to this question. Dynamics drives a given spatially extended system through a re ...
Quantum Computing
... • An atom, not an electron, is the physical bit – An electron is 0 or 1 – Quantum mechanics: at atom is 0, 1, or both – “coherent superposition” ...
... • An atom, not an electron, is the physical bit – An electron is 0 or 1 – Quantum mechanics: at atom is 0, 1, or both – “coherent superposition” ...
Is the Final Piece of the Natural Law Puzzle Almost Solved
... establishing the mass of specific particles and subparticles using a Lagrangian – “a mathematical function which represents how the various particles interact” (Kane.1). Scientists understand that the Standard Model “requires only one Higgs field to generate all the elementary particle masses” but m ...
... establishing the mass of specific particles and subparticles using a Lagrangian – “a mathematical function which represents how the various particles interact” (Kane.1). Scientists understand that the Standard Model “requires only one Higgs field to generate all the elementary particle masses” but m ...
On the Motion of Solids in Modified Quantum Mechanics.
... proposing original formaIisms and/or mechanisms for the quantum localization of macroobjects. Most recently, Ghirardi, Rimini and Weber (GRW) proposed a theory that utilized some of the techniques of the continuous quantum measurement theory of Barchielli et al. [5] and they have suggested ungied dy ...
... proposing original formaIisms and/or mechanisms for the quantum localization of macroobjects. Most recently, Ghirardi, Rimini and Weber (GRW) proposed a theory that utilized some of the techniques of the continuous quantum measurement theory of Barchielli et al. [5] and they have suggested ungied dy ...
The Road to Loop Quantum Gravity - Theoretical High
... very well developed and supported by a large amount of experimental evidence. It is therefore only natural to try to unify these theories to obtain one theory that describes all four fundamental forces of nature. The most logical point to begin is to obtain a quantum theory of gravity by using a per ...
... very well developed and supported by a large amount of experimental evidence. It is therefore only natural to try to unify these theories to obtain one theory that describes all four fundamental forces of nature. The most logical point to begin is to obtain a quantum theory of gravity by using a per ...
Light-like -deformations and scalar field theory via Drinfeld twist
... for diffeomorphisms that leave the physical action invariant leads to deformation of Poincaré symmetry, with κ-Poincaré symmetry being among the most extensively studied [3, 4, 5]. κ-deformed Poincaré symmetry is algebraically described by the κ-Poincaré-Hopf algebra and is an example of deforme ...
... for diffeomorphisms that leave the physical action invariant leads to deformation of Poincaré symmetry, with κ-Poincaré symmetry being among the most extensively studied [3, 4, 5]. κ-deformed Poincaré symmetry is algebraically described by the κ-Poincaré-Hopf algebra and is an example of deforme ...
differential equation
... ( dP / dt ) = k P and any exponential function of the form P(t) = Ce k t. ( dP / dt ) k P if P is small ( dP / dt ) < 0 if P > K. Then we can conclude that ( dP / dt ) = k P ( 1 – ( P / K ). ...
... ( dP / dt ) = k P and any exponential function of the form P(t) = Ce k t. ( dP / dt ) k P if P is small ( dP / dt ) < 0 if P > K. Then we can conclude that ( dP / dt ) = k P ( 1 – ( P / K ). ...
The Learnability of Quantum States
... ~2n bits to specify. But that fact seems to be “more about the map than the territory” Holevo’s Theorem (1973): By sending an n-qubit quantum state, Alice can transmit no more than n classical bits to Bob This talk: New limitations on the information content of quantum states [A. 2004], [A. 2006], [ ...
... ~2n bits to specify. But that fact seems to be “more about the map than the territory” Holevo’s Theorem (1973): By sending an n-qubit quantum state, Alice can transmit no more than n classical bits to Bob This talk: New limitations on the information content of quantum states [A. 2004], [A. 2006], [ ...
Projects - Department of Computer Science and Engineering, CUHK
... We talked about a recent protocol [Z14] in Lecture 8. It’ll be great if the exponential dependence on the degree can be improved. Bait 1: It may not be that hard (actually I didn’t put too much time on this yet). Bait 2: If you can improve it, you’ll get a publication, likely in a top conference. [Z ...
... We talked about a recent protocol [Z14] in Lecture 8. It’ll be great if the exponential dependence on the degree can be improved. Bait 1: It may not be that hard (actually I didn’t put too much time on this yet). Bait 2: If you can improve it, you’ll get a publication, likely in a top conference. [Z ...
Document
... Hamiltonian (linear in the external forces). From the reversibility in time follow the Onsager reciprocity r e lations, from the second and third assumpti& follow the fluctuation-dissipation theorems, and from the combination of all three assumptions follow the multi-index relations of nonlinear flu ...
... Hamiltonian (linear in the external forces). From the reversibility in time follow the Onsager reciprocity r e lations, from the second and third assumpti& follow the fluctuation-dissipation theorems, and from the combination of all three assumptions follow the multi-index relations of nonlinear flu ...