The Quantum Puzzle: Critique of Quantum Theory and
... A knowledge of these things [whether or not a current is material] would amount to at least the beginnings of a complete dynamical theory of electricity, not, as in this treatise, as a phenomenon due to an unknown cause, subject only to the general laws of dynamics, but as a result of known motions ...
... A knowledge of these things [whether or not a current is material] would amount to at least the beginnings of a complete dynamical theory of electricity, not, as in this treatise, as a phenomenon due to an unknown cause, subject only to the general laws of dynamics, but as a result of known motions ...
Influence of boundary conditions on quantum
... interacting with the wall. This occurs when 3σ 1 − τ 2 ≈ q, and so tw ≈ qσ/3 for σ ≪ 1. For times t > tw , oscillations appear due to reflection off the wall and interference occurs. The wall interaction, however, is different in each case due to the different BCs prescribed by η. It is clear from the f ...
... interacting with the wall. This occurs when 3σ 1 − τ 2 ≈ q, and so tw ≈ qσ/3 for σ ≪ 1. For times t > tw , oscillations appear due to reflection off the wall and interference occurs. The wall interaction, however, is different in each case due to the different BCs prescribed by η. It is clear from the f ...
A Signed Particle Formulation of Non
... to replicate the results of more conventional quantum theories. In particular we show that our suggested approach is a natural generalization of the Wigner Monte Carlo method which reconstructs the time-dependent Wigner quasidistribution function and, thus, the corresponding Schrödinger wave-functi ...
... to replicate the results of more conventional quantum theories. In particular we show that our suggested approach is a natural generalization of the Wigner Monte Carlo method which reconstructs the time-dependent Wigner quasidistribution function and, thus, the corresponding Schrödinger wave-functi ...
Quantum connection and Poincare19 e--Cartan form
... The second term in the above formula is the obstruction for the mapˆ: f 7→ fˆ to be a morphism of Lie algebras. There is any substantial physical reason by which the mapˆ should be a morphism of Lie algebras? On the other hand, the restriction of the mapˆ to the subalgebra of affine functions yields ...
... The second term in the above formula is the obstruction for the mapˆ: f 7→ fˆ to be a morphism of Lie algebras. There is any substantial physical reason by which the mapˆ should be a morphism of Lie algebras? On the other hand, the restriction of the mapˆ to the subalgebra of affine functions yields ...
PDF Version - Physics (APS)
... of this alloy are similar to the two-dimensional states in graphene. Near the Fermi level, electrons and holes in graphene are described by energy states that are linear in momentum. Electrons with a constant velocity are conveniently described by the relativistic Dirac equation for massless fermion ...
... of this alloy are similar to the two-dimensional states in graphene. Near the Fermi level, electrons and holes in graphene are described by energy states that are linear in momentum. Electrons with a constant velocity are conveniently described by the relativistic Dirac equation for massless fermion ...
Kondo effect of an antidot in the integer quantum Hall regime: a
... A quantum antidot is a potential hill in two dimensional electron gas (2DEG) systems [1–8]. It can be formed in GaAs/AlGaAs heterostructures by applying a gate potential or making an etched pit. In zero magnetic 2eld, it is a simple repulsive potential and acts as a scattering center for electrons. ...
... A quantum antidot is a potential hill in two dimensional electron gas (2DEG) systems [1–8]. It can be formed in GaAs/AlGaAs heterostructures by applying a gate potential or making an etched pit. In zero magnetic 2eld, it is a simple repulsive potential and acts as a scattering center for electrons. ...
Proton tomography with Wigner distributions
... The classical interpretation of GPDs as Wigner quasiprobabilities is valid in deep DGLAP domain! ...
... The classical interpretation of GPDs as Wigner quasiprobabilities is valid in deep DGLAP domain! ...
From Physics to Information Theory and Back - Philsci
... A (or B), there is an automorphism of the algebra A taking ρ into σ. This condition would entail that either all pure states are dispersion-free (in which case the algebra is abelian, and the state space is a classical simplex), or that none are (as in the quantum case). The virtues of the C ∗ -alg ...
... A (or B), there is an automorphism of the algebra A taking ρ into σ. This condition would entail that either all pure states are dispersion-free (in which case the algebra is abelian, and the state space is a classical simplex), or that none are (as in the quantum case). The virtues of the C ∗ -alg ...
Quantum Computer Compilers
... The Importance of Computational Thinking Computational thinking is a fundamental skill for everyone, not just for computer scientists. To reading, writing, and arithmetic, we should add computational thinking to every child’s analytical ability. Just as the printing press facilitated the spread of ...
... The Importance of Computational Thinking Computational thinking is a fundamental skill for everyone, not just for computer scientists. To reading, writing, and arithmetic, we should add computational thinking to every child’s analytical ability. Just as the printing press facilitated the spread of ...
Comparison of 3D classical and quantum mechanical He scattering
... numerical solution are presented in Section 3. The interaction potential of He±Rh(3 1 1) system is constructed in Section 4. Classical and quantum mechanical calculations are shown in Sections 5 and 6, respectively. At last the conclusions can be read in Section 7. 2. Model of classical atom surface ...
... numerical solution are presented in Section 3. The interaction potential of He±Rh(3 1 1) system is constructed in Section 4. Classical and quantum mechanical calculations are shown in Sections 5 and 6, respectively. At last the conclusions can be read in Section 7. 2. Model of classical atom surface ...