Landau`s Fermi Liquid Theory
... The concept of a Fermi Liquid describes (strongly) interacting fermions using concepts that naively would only be applicable to a very weakly interacting gas. That this is at all possible makes Fermi Liquid theory a very versatile, but at the same time its very success is puzzling. Fermi Liquid theo ...
... The concept of a Fermi Liquid describes (strongly) interacting fermions using concepts that naively would only be applicable to a very weakly interacting gas. That this is at all possible makes Fermi Liquid theory a very versatile, but at the same time its very success is puzzling. Fermi Liquid theo ...
here.
... 10.11Magnetic moments from quark model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 196 10.12QCD . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 198 10.13Spontaneous global symmetry breaking . . . . . . . . . . . . . . . . . . . ...
... 10.11Magnetic moments from quark model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 196 10.12QCD . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 198 10.13Spontaneous global symmetry breaking . . . . . . . . . . . . . . . . . . . ...
Weakly collisional Landau damping and three-dimensional
... observations that cannot be explained by 1D BGK wave theory18-20. There are also results from numerical simulations suggesting the possibility of higher-dimensional BGK solutions21-23. 3D BGK solutions have been constructed under the assumption of a strong magnetic field so that one can use some for ...
... observations that cannot be explained by 1D BGK wave theory18-20. There are also results from numerical simulations suggesting the possibility of higher-dimensional BGK solutions21-23. 3D BGK solutions have been constructed under the assumption of a strong magnetic field so that one can use some for ...
Number Archetypes and “Background” Control Theory Concerning
... which is such an essential quality of all atomic sources of electric fields actually occurring in nature.” [30] As also mentioned above, after 1910 the demand has arisen, beside the definitive calculations and spectroscopic measurements, to determine the “true value” of the fine structure constant o ...
... which is such an essential quality of all atomic sources of electric fields actually occurring in nature.” [30] As also mentioned above, after 1910 the demand has arisen, beside the definitive calculations and spectroscopic measurements, to determine the “true value” of the fine structure constant o ...
Hypergroups and Quantum Bessel Processes of Non
... The dimension of the Bessel process with index µ is δ = 2(µ + 1) and a common notation for the Bessel process with the dimension δ is BES(δ). It is well known that the notion of the Bessel process makes sense for any real number δ and that the Bessel processes of integer dimension δ ≥ 2 are the radi ...
... The dimension of the Bessel process with index µ is δ = 2(µ + 1) and a common notation for the Bessel process with the dimension δ is BES(δ). It is well known that the notion of the Bessel process makes sense for any real number δ and that the Bessel processes of integer dimension δ ≥ 2 are the radi ...
Notes for course on Physics of Particles and Fields, CMI, Autumn
... of quarks and gluons. • Roughly, an elementary particle is one that may be treated as a point particle (or at least one with fixed shape) with fixed properties and with no sub-structure for the purposes under consideration. Any system (like an atom, nucleus or perhaps even a black hole) in its groun ...
... of quarks and gluons. • Roughly, an elementary particle is one that may be treated as a point particle (or at least one with fixed shape) with fixed properties and with no sub-structure for the purposes under consideration. Any system (like an atom, nucleus or perhaps even a black hole) in its groun ...
Many-electron transport in strongly correlated nondegenerate two-dimensional electron systems *
... the rate at which electrons exchange momenta with each other is large or small compared to the momentum relaxation rate due to coupling with scatterers. In Sec. V we analyze the expression for the conductivity in classically weak and classically strong magnetic fields, and show when and how magnetor ...
... the rate at which electrons exchange momenta with each other is large or small compared to the momentum relaxation rate due to coupling with scatterers. In Sec. V we analyze the expression for the conductivity in classically weak and classically strong magnetic fields, and show when and how magnetor ...
Introduction to the Bethe Ansatz I
... array of electrons with uniform exchange interaction between nearest neighbors. Bethe’s parametrization of the eigenvectors, the Bethe ansatz, has become influential to an extent not imagined at the time. Today, many other quantum many body systems are known to be solvable by some variant of the Bet ...
... array of electrons with uniform exchange interaction between nearest neighbors. Bethe’s parametrization of the eigenvectors, the Bethe ansatz, has become influential to an extent not imagined at the time. Today, many other quantum many body systems are known to be solvable by some variant of the Bet ...
Generating entangled spin states for quantum metrology by single-photon detection
... angle β 2 = Sφ 2 /2 and is given by p = qSφ 2 /2 1, where q 1 is the photon detection efficiency. The probability of the incident photon being scattered into free space by the atomic ensemble is psc = 2Sη(/2)2 = 2Sφ 2 /η [35]. Therefore the success probability is simply related to the free- ...
... angle β 2 = Sφ 2 /2 and is given by p = qSφ 2 /2 1, where q 1 is the photon detection efficiency. The probability of the incident photon being scattered into free space by the atomic ensemble is psc = 2Sη(/2)2 = 2Sφ 2 /η [35]. Therefore the success probability is simply related to the free- ...
Many-electron transport in strongly correlated nondegenerate 2D
... the rate at which electrons exchange momenta with each other is large or small compared to the momentum relaxation rate due to coupling with scatterers. In Sec. V we analyze the expression for the conductivity in classically weak and classically strong magnetic fields, and show when and how magnetor ...
... the rate at which electrons exchange momenta with each other is large or small compared to the momentum relaxation rate due to coupling with scatterers. In Sec. V we analyze the expression for the conductivity in classically weak and classically strong magnetic fields, and show when and how magnetor ...
![arXiv:1312.4758v2 [quant-ph] 10 Apr 2014](http://s1.studyres.com/store/data/021352507_1-d587dd4045ccae4ae6a47bb17173f358-300x300.png)
arXiv:1312.4758v2 [quant-ph] 10 Apr 2014
... QM A-completeness has been used to characterize the complexity of many computational problems in quantum physics. (A number of other QM A-complete problems are given in [6].) But some natural physical problems seem to have a complexity that is slightly above QM A. For example, one such problem is e ...
... QM A-completeness has been used to characterize the complexity of many computational problems in quantum physics. (A number of other QM A-complete problems are given in [6].) But some natural physical problems seem to have a complexity that is slightly above QM A. For example, one such problem is e ...
An experimental chemist`s guide to ab initio quantum chemistry
... After all, many chemists can ”guessn bond energies more accurately than even state-of-the-art ab initio computer codes can calculate them. The reasons include the following: A. Many-body problems with R 1 potentials are notoriously difficult. It is well-known that the Coulomb potential falls off so ...
... After all, many chemists can ”guessn bond energies more accurately than even state-of-the-art ab initio computer codes can calculate them. The reasons include the following: A. Many-body problems with R 1 potentials are notoriously difficult. It is well-known that the Coulomb potential falls off so ...
Advanced Quantum Mechanics
... Scattering theory The chapter begins with a phenomenological introduction to the concept of ’scattering’ in quantum theory. Specifically, we will define different paradigms of scattering techniques and introduce the concept of a scattering cross section. We then proceeds to develop the theory of ela ...
... Scattering theory The chapter begins with a phenomenological introduction to the concept of ’scattering’ in quantum theory. Specifically, we will define different paradigms of scattering techniques and introduce the concept of a scattering cross section. We then proceeds to develop the theory of ela ...
X-ray spectroscopies through damped linear response theory Thomas Fransson
... core excitations/de-excitations exhibit strong relaxation effects, making theoretical considerations of the processes particularly challenging. While the removal of a valence electron leaves the remaining electrons relatively unaffected, removing core electrons has a substantial effect on the other ...
... core excitations/de-excitations exhibit strong relaxation effects, making theoretical considerations of the processes particularly challenging. While the removal of a valence electron leaves the remaining electrons relatively unaffected, removing core electrons has a substantial effect on the other ...
Zahn, M., and S. Rhee. Electric Field Effects on the Equilibrium and Small Signal Stabilization of Electrofluidized Beds, IEEE Transactions on Industry Applications, IA-20, 137-147, January/February 1984
... on the dielectric particles. To eliminate space charge effects where u v are the respective fluid and particle interstitial in experiments, the gas is dried to minimize conduction, velocities. For simplicity we take the same simplifying assumpand an alternating high voltage is applied at a frequency ...
... on the dielectric particles. To eliminate space charge effects where u v are the respective fluid and particle interstitial in experiments, the gas is dried to minimize conduction, velocities. For simplicity we take the same simplifying assumpand an alternating high voltage is applied at a frequency ...
Programmable architecture for quantum computing Jialin Chen, Lingli Wang, Edoardo Charbon,
... for scalable chip-based quantum computer architectures as it allows the interaction between distant qubits without SWAP gates so as to offer individual addressability. For this reason, we will concentrate on the qubus system [14,15]—an important kind of ancilla-based model—which combines both matter ...
... for scalable chip-based quantum computer architectures as it allows the interaction between distant qubits without SWAP gates so as to offer individual addressability. For this reason, we will concentrate on the qubus system [14,15]—an important kind of ancilla-based model—which combines both matter ...
Creating fractional quantum Hall states with atomic clusters
... for investigating complex states of matter in a controlled environment, such as strongly interacting Fermi gases, lowdimensional states of matter, or lattice quantum systems [1]. The effect of a magnetic field on charged quantum many-body systems leads to a wealth of interesting states of matter, su ...
... for investigating complex states of matter in a controlled environment, such as strongly interacting Fermi gases, lowdimensional states of matter, or lattice quantum systems [1]. The effect of a magnetic field on charged quantum many-body systems leads to a wealth of interesting states of matter, su ...
Sharp Tunneling Peaks in a Parametric Oscillator: Quantum Resonances Missing
... It is not a sum of the kinetic and potential energy. For jj < 1, gðQ; PÞ has two symmetrically located minima, gmin ¼ ð1 þ Þ2 =4, and a saddle point, gS ¼ 0. In the presence of weak dissipation, the minima correspond to the period-2 vibrational states in the laboratory frame, which have equal amp ...
... It is not a sum of the kinetic and potential energy. For jj < 1, gðQ; PÞ has two symmetrically located minima, gmin ¼ ð1 þ Þ2 =4, and a saddle point, gS ¼ 0. In the presence of weak dissipation, the minima correspond to the period-2 vibrational states in the laboratory frame, which have equal amp ...
