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Quantum field theory for matter under extreme conditions
... Hadron Physics lies at the interface between nuclear and particle (high energy) physics. Its focus is an elucidation of the role played by quarks and gluons in the structure of, and interactions between, hadrons. This was once particle physics but that has since moved to higher energy in search of a ...
... Hadron Physics lies at the interface between nuclear and particle (high energy) physics. Its focus is an elucidation of the role played by quarks and gluons in the structure of, and interactions between, hadrons. This was once particle physics but that has since moved to higher energy in search of a ...
Chapter 20: Particle Kinetics of Plasma [version 1220.1.K]
... and ions to isotropize, and the rates for them to thermalize. Our calculations reveal that Coulomb scattering is so weak that, in most plasmas encountered in Nature, it is unlikely to produce isotropized or thermalized velocity distributions. In Sec. 20.5 we give a brief preview of the fact that in ...
... and ions to isotropize, and the rates for them to thermalize. Our calculations reveal that Coulomb scattering is so weak that, in most plasmas encountered in Nature, it is unlikely to produce isotropized or thermalized velocity distributions. In Sec. 20.5 we give a brief preview of the fact that in ...
Quantum one-time programs
... Can quantum one-time programs be constructed? If so, how? If not, why not, and under what additional assumptions can they be achieved? QOTPs, if they do exist, would be useful for a variety of secure quantum computation tasks, such as providing copy protection of software [4] and implementing verifi ...
... Can quantum one-time programs be constructed? If so, how? If not, why not, and under what additional assumptions can they be achieved? QOTPs, if they do exist, would be useful for a variety of secure quantum computation tasks, such as providing copy protection of software [4] and implementing verifi ...
Switching via quantum activation: A parametrically modulated oscillator 兲
... balance holds leads to a sharp change of the statistical distribution and the switching rate. This change occurs already for an infinitesimally small deviation from detailed balance, in the semiclassical limit. The fragility of the detailed balance solution is previewed in Fig. 2. This figure shows ...
... balance holds leads to a sharp change of the statistical distribution and the switching rate. This change occurs already for an infinitesimally small deviation from detailed balance, in the semiclassical limit. The fragility of the detailed balance solution is previewed in Fig. 2. This figure shows ...
Quantum supergroups and canonical bases Sean Clark University of Virginia Dissertation Defense
... No examples despite extensive study, experts don’t believe. Why should canonical bases exist? Because now we have I ...
... No examples despite extensive study, experts don’t believe. Why should canonical bases exist? Because now we have I ...
Jamming/flowing transition of non-Brownian particles suspended in
... size, the liquid flow rate and the particle morphology on the avalanche size. We define the dimensionless opening ratio R as the restriction width w divided by the particle diameter dP . It ranges between 1.83 and 4.2. The restriction cross-section area is labeled Σr ≡ w.H = R.dP .H. Three flowrates Q ...
... size, the liquid flow rate and the particle morphology on the avalanche size. We define the dimensionless opening ratio R as the restriction width w divided by the particle diameter dP . It ranges between 1.83 and 4.2. The restriction cross-section area is labeled Σr ≡ w.H = R.dP .H. Three flowrates Q ...
ON THE ELECTRODYNAMICS OF MOVING BODIES By A. Einstein June 30, 1905
... action of a magnet and a conductor. The observable phenomenon here depends only on the relative motion of the conductor and the magnet, whereas the customary view draws a sharp distinction between the two cases in which either the one or the other of these bodies is in motion. For if the magnet is i ...
... action of a magnet and a conductor. The observable phenomenon here depends only on the relative motion of the conductor and the magnet, whereas the customary view draws a sharp distinction between the two cases in which either the one or the other of these bodies is in motion. For if the magnet is i ...
Million-Atom Pseudopotential Calculation of GX Mixing in GaAs AlAs
... 140 quantum dot are shown in Figs. 2(b) and 2(c) (where the supercell contains 2 3 106 atoms). The calculation takes ,30 min on a IBM RSy6000 work station model 590 for one pressure value. We find that the G-X coupling in these QD’s is smaller than in the corresponding 20 3 20 superlattice [compare ...
... 140 quantum dot are shown in Figs. 2(b) and 2(c) (where the supercell contains 2 3 106 atoms). The calculation takes ,30 min on a IBM RSy6000 work station model 590 for one pressure value. We find that the G-X coupling in these QD’s is smaller than in the corresponding 20 3 20 superlattice [compare ...
Invitation to Local Quantum Physics
... The Bisognano-Wichmann Theorem The PCT theorem was used by J. Bisognano and E. Wichmann in 1976 to derive a structural result that is of fundamental importance for the application of Tomita-Takesaki modular theory in relativistic quantum field theory. Let W be a space-like wedge in space-time, i.e. ...
... The Bisognano-Wichmann Theorem The PCT theorem was used by J. Bisognano and E. Wichmann in 1976 to derive a structural result that is of fundamental importance for the application of Tomita-Takesaki modular theory in relativistic quantum field theory. Let W be a space-like wedge in space-time, i.e. ...
Dirac monopoles and gravitation
... is that a non-zeroed charge monopole implies in some physical consequences. In Singleton model it is the new massive photon according to our interpretation. Therefore according to these works [4, 5] some new physics is involved when the monopole charge is different from zero. The present work addres ...
... is that a non-zeroed charge monopole implies in some physical consequences. In Singleton model it is the new massive photon according to our interpretation. Therefore according to these works [4, 5] some new physics is involved when the monopole charge is different from zero. The present work addres ...
Deformation quantization for fermionic fields
... The deformation quantization is an alternative and independent formulation to the canonical quantization and the path integral quantization in quantum mechanics. In this formalism, the quantization is understood as a deformation of the structure of the algebra of classical observables instead of a r ...
... The deformation quantization is an alternative and independent formulation to the canonical quantization and the path integral quantization in quantum mechanics. In this formalism, the quantization is understood as a deformation of the structure of the algebra of classical observables instead of a r ...
Many Oscillators
... The unitary counterpart: a strong coupling can struggle the effects of a weaker one, realizing the partitioning of the Hilbert space: ...
... The unitary counterpart: a strong coupling can struggle the effects of a weaker one, realizing the partitioning of the Hilbert space: ...
Metal Insulator Transition
... Moreover, the second-order perturbation theory in terms of t/U leads to the t − J model[3]: ...
... Moreover, the second-order perturbation theory in terms of t/U leads to the t − J model[3]: ...
Quantum electrodynamics
![](https://commons.wikimedia.org/wiki/Special:FilePath/Dirac_3.jpg?width=300)
In particle physics, quantum electrodynamics (QED) is the relativistic quantum field theory of electrodynamics. In essence, it describes how light and matter interact and is the first theory where full agreement between quantum mechanics and special relativity is achieved. QED mathematically describes all phenomena involving electrically charged particles interacting by means of exchange of photons and represents the quantum counterpart of classical electromagnetism giving a complete account of matter and light interaction.In technical terms, QED can be described as a perturbation theory of the electromagnetic quantum vacuum. Richard Feynman called it ""the jewel of physics"" for its extremely accurate predictions of quantities like the anomalous magnetic moment of the electron and the Lamb shift of the energy levels of hydrogen.