Classical Mechanics - UC Riverside (Math)
... Classical mechanics is a very peculiar branch of physics. It used to be considered the sum total of our theoretical knowledge of the physical universe (Laplace’s daemon, the Newtonian clockwork), but now it is known as an idealization, a toy model if you will. The astounding thing is that probably a ...
... Classical mechanics is a very peculiar branch of physics. It used to be considered the sum total of our theoretical knowledge of the physical universe (Laplace’s daemon, the Newtonian clockwork), but now it is known as an idealization, a toy model if you will. The astounding thing is that probably a ...
Fractals as macroscopic manifestation of squeezed
... Cantor set, etc.) is expressed in analytical form by Eqs. (6) and (7): “cutting a piece of a fractal and magnifying it isotropically to the size of the original, both the original and the magnification look the same” [18]. In this sense fractals are “scale free”, namely viewing a picture of part of ...
... Cantor set, etc.) is expressed in analytical form by Eqs. (6) and (7): “cutting a piece of a fractal and magnifying it isotropically to the size of the original, both the original and the magnification look the same” [18]. In this sense fractals are “scale free”, namely viewing a picture of part of ...
Solitons of the resonant nonlinear Schrödinger equation with
... conditions hence vanish for the dissipaton. At the critical value, the solution is a kink steady state in the moving frame e± = ±ke±kξ0 (1 ∓ tanh kξ) with the constant asymptotic behavior e± → ±2ke±kξ0 for x → ∓∞ and e± → ±0 for x → ±∞. In the supercritical case v > vcrit , e± → ±∞ for x → ∓∞ and e± ...
... conditions hence vanish for the dissipaton. At the critical value, the solution is a kink steady state in the moving frame e± = ±ke±kξ0 (1 ∓ tanh kξ) with the constant asymptotic behavior e± → ±2ke±kξ0 for x → ∓∞ and e± → ±0 for x → ±∞. In the supercritical case v > vcrit , e± → ±∞ for x → ∓∞ and e± ...
presentation pdf - EMERGENT QUANTUM MECHANICS
... These are the LOCAL expressions for the energy-momentum of the particle. Conservation of energy is maintained through the quantum Hamilton-Jacobi equation. Similar relations hold for the Pauli and Dirac particles. ...
... These are the LOCAL expressions for the energy-momentum of the particle. Conservation of energy is maintained through the quantum Hamilton-Jacobi equation. Similar relations hold for the Pauli and Dirac particles. ...
On Quantum Nonseparability - Philsci
... application of the conservation laws to the parts and the whole of a classical system and the requirement of additivity of the conserved mechanical quantities. Furthermore, derived quantities, such as the gravitational potential energy, that are not additive in the same simple way as the aforementio ...
... application of the conservation laws to the parts and the whole of a classical system and the requirement of additivity of the conserved mechanical quantities. Furthermore, derived quantities, such as the gravitational potential energy, that are not additive in the same simple way as the aforementio ...
On the Stability of Classical Orbits of the Hydrogen Ground State in
... The task is then to show that SED explains all quantum behaviour of matter at the statistical level. This has been argued to occur on general grounds [1,2]. SED is not ruled out by Bell’s theorem, since that has an irreparable fatality, the contextually loophole [3]. Testing the working of SED in sp ...
... The task is then to show that SED explains all quantum behaviour of matter at the statistical level. This has been argued to occur on general grounds [1,2]. SED is not ruled out by Bell’s theorem, since that has an irreparable fatality, the contextually loophole [3]. Testing the working of SED in sp ...
Quantum anomalous Hall effect with cold atoms trapped in a square
... pseudospin-1/2 subspace. We shall focus on the hybridized bands between ψa and ψb intermediated by the intersite hopping but neglect the hybridization between ψa,b and the lowest s orbital in the B sites since its onsite energy is far separated from those of ψa,b in the case of large trapping freque ...
... pseudospin-1/2 subspace. We shall focus on the hybridized bands between ψa and ψb intermediated by the intersite hopping but neglect the hybridization between ψa,b and the lowest s orbital in the B sites since its onsite energy is far separated from those of ψa,b in the case of large trapping freque ...
- Philsci
... principle and even suggest that it serves to show the incompleteness or inadequacy of the quantum formalism (Ford et al. 1990), (Ford and Mantica 1992). To counter such pessimistic conclusions, it is useful to begin with two alleged explanations for the failure. Both seem to indicate that chaotic q ...
... principle and even suggest that it serves to show the incompleteness or inadequacy of the quantum formalism (Ford et al. 1990), (Ford and Mantica 1992). To counter such pessimistic conclusions, it is useful to begin with two alleged explanations for the failure. Both seem to indicate that chaotic q ...
Lecture 12
... Partial trace (I) Two quantum registers (e.g. two qubits) in states and (respectively) are independent if then the combined system is in state = ...
... Partial trace (I) Two quantum registers (e.g. two qubits) in states and (respectively) are independent if then the combined system is in state = ...
Quantum Reflection at Strong Magnetic Fields
... plays the role of the attractive potential created by the condensed matter surface. However, probe photons unaffected by the vacuum fluctuations simply pass the entire region of inhomogeneity. This is in contrast to quantum reflection in the atomic case, where the repulsive potential of the condense ...
... plays the role of the attractive potential created by the condensed matter surface. However, probe photons unaffected by the vacuum fluctuations simply pass the entire region of inhomogeneity. This is in contrast to quantum reflection in the atomic case, where the repulsive potential of the condense ...
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... road to becoming scientific problems. Failing this, we might at least learn how to ignore them. From physics we hope to find analogues to psychological phenomena so the unlawful might be rendered lawful. From mathematics we seek ways to make illposed problems well-posed, to find connections among va ...
... road to becoming scientific problems. Failing this, we might at least learn how to ignore them. From physics we hope to find analogues to psychological phenomena so the unlawful might be rendered lawful. From mathematics we seek ways to make illposed problems well-posed, to find connections among va ...
Computational advantage from quantum
... first proposed in [2] that such a constraint can be relaxed: one can consider situations where the wires, and thus the order between gates, can be controlled by some extra variable. This is natural if one thinks of the circuit’s wires as quantum systems that can be in superposition. Such “superposit ...
... first proposed in [2] that such a constraint can be relaxed: one can consider situations where the wires, and thus the order between gates, can be controlled by some extra variable. This is natural if one thinks of the circuit’s wires as quantum systems that can be in superposition. Such “superposit ...