Neoclassical Transport
... • In a pure hydrogen plasma DCL is the same for electrons and ions. • For impurities, collisions with electrons maeme can be neglected compared to collisions with ions. • The diffusion coefficient decreases with 1/B2 due to the quadratic dependence on the Larmor radius Our expression for the drift ...
... • In a pure hydrogen plasma DCL is the same for electrons and ions. • For impurities, collisions with electrons maeme can be neglected compared to collisions with ions. • The diffusion coefficient decreases with 1/B2 due to the quadratic dependence on the Larmor radius Our expression for the drift ...
![[235] JPhysConfSer_702(2016)012001](http://s1.studyres.com/store/data/003582913_1-c4e71fc2970976a1f51404875d70626d-300x300.png)
[235] JPhysConfSer_702(2016)012001
... crystalline (VBC) phases, in which specific combinations of the lattice spins combine into spin singlets, have zero magnetic order and break neither of the SU(2) spin-rotation and time-reversal symmetries, although they still break some lattice symmetries. Yet other states exist in which, for exampl ...
... crystalline (VBC) phases, in which specific combinations of the lattice spins combine into spin singlets, have zero magnetic order and break neither of the SU(2) spin-rotation and time-reversal symmetries, although they still break some lattice symmetries. Yet other states exist in which, for exampl ...
Statistical Mechanics to Disordered Quantum Optimization
... Thus, in Chapter 2, we review the classical complexity theory necessary to understand the important statement that P 6= NP and its more recent quantum generalization BQP 6= QMA. These complexity theoretic conjectures essentially assert that there exist natural classes of problems (called NP-complet ...
... Thus, in Chapter 2, we review the classical complexity theory necessary to understand the important statement that P 6= NP and its more recent quantum generalization BQP 6= QMA. These complexity theoretic conjectures essentially assert that there exist natural classes of problems (called NP-complet ...
Hydrodynamic theory of thermoelectric transport
... mechanism is between quasiparticles and impurities or phonons. In most simple crystals – including Weyl semimetals – it is likely that this description is reasonable. However, there are exotic metals in which the quasiparticle-quasiparticle scattering time is much smaller than the quasiparticle-impu ...
... mechanism is between quasiparticles and impurities or phonons. In most simple crystals – including Weyl semimetals – it is likely that this description is reasonable. However, there are exotic metals in which the quasiparticle-quasiparticle scattering time is much smaller than the quasiparticle-impu ...
Vlasov-code simulation J. B¨uchner
... plasma and waves have to be described, i.e., the propagation of kinetic Alfén waves in inhomogeneous media, collisionless shocks, warm beam instabilities, collisionless (“anomalous”) transport and magnetic reconnection. The physics of collisionless plasmas is well described by a self-consistent sol ...
... plasma and waves have to be described, i.e., the propagation of kinetic Alfén waves in inhomogeneous media, collisionless shocks, warm beam instabilities, collisionless (“anomalous”) transport and magnetic reconnection. The physics of collisionless plasmas is well described by a self-consistent sol ...
The evolution of free wave packets
... out without limit. How different this behavior is from that of a free classical particle. The reconciliation of the classical and quantum descriptions is part of the bigger question of the interpretation of quantum mechanics; here we will consider only the dynamics of free wave packets as given by S ...
... out without limit. How different this behavior is from that of a free classical particle. The reconciliation of the classical and quantum descriptions is part of the bigger question of the interpretation of quantum mechanics; here we will consider only the dynamics of free wave packets as given by S ...
Closed Timelike Curves Make Quantum and
... computational power of CTCs. We argue that if CTCs containing polynomially many bits could be created and maintained, then both classical and quantum computers would have exactly the power of the complexity class PSPACE, which consists of all problems solvable on a classical computer with a polynomi ...
... computational power of CTCs. We argue that if CTCs containing polynomially many bits could be created and maintained, then both classical and quantum computers would have exactly the power of the complexity class PSPACE, which consists of all problems solvable on a classical computer with a polynomi ...
M1.4 Dynamics
... same horizontal track, collide. The mass of A is 800 kg and the mass of B is m kg. Immediately before the collision the speed of A is 5 ms–1 and the speed of B is 4 ms–1. Immediately after the collision the trucks are joined together and move with the same speed, 1 ms–1. The direction of motion of A ...
... same horizontal track, collide. The mass of A is 800 kg and the mass of B is m kg. Immediately before the collision the speed of A is 5 ms–1 and the speed of B is 4 ms–1. Immediately after the collision the trucks are joined together and move with the same speed, 1 ms–1. The direction of motion of A ...
Parton model from bi-local solitonic picture of the baryon in two-dimensions
... model with the simpler relativistic parton picture of the baryon, in 2 dimensions. The main advantage of this new point of view is that the semi-classical approximation of hadron dynamics corresponds to the large Nc limit of 2d QCD, and so is capable of describing non-perturbative phenomena such as ...
... model with the simpler relativistic parton picture of the baryon, in 2 dimensions. The main advantage of this new point of view is that the semi-classical approximation of hadron dynamics corresponds to the large Nc limit of 2d QCD, and so is capable of describing non-perturbative phenomena such as ...
The Status of our Ordinary Three Dimensions in a Quantum Universe 1
... governing quantum systems is the Schrödinger equation. As noted above, this is a completely deterministic law describing the evolution of states of the quantum wavefunction over time. There is no collapse law on this version of quantum mechanics, and thus no need to distinguish (using for example, ...
... governing quantum systems is the Schrödinger equation. As noted above, this is a completely deterministic law describing the evolution of states of the quantum wavefunction over time. There is no collapse law on this version of quantum mechanics, and thus no need to distinguish (using for example, ...
