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Spin-orbit-coupled Bose
Spin-orbit-coupled Bose

... ^; are density operators for j"æ and j#æ, and normal ^: and r where r ordering is implied. In the 87Rb F 5 1 manifold, the spin-independent interaction is c0 5 7.79 3 10212 Hz cm3, the spin-dependent interaction22 is c2 5 23.61 3 10214 Hz cm3, and c’:; ~0. Because jc0 j?jc2 j, the interaction is alm ...
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Janiszewski_washington_0250E_13369
Janiszewski_washington_0250E_13369

LECTURE 3 PARTICLE INTERACTIONS & FEYNMAN DIAGRAMS PHY492 Nuclear and Elementary Particle Physics
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Effective field theory methods applied to the 2-body

... The existence of gravitational waves (GW) is an unavoidable prediction of General Relativity (GR): any change to a gravitating source must be communicated to distant observers no faster than the speed of light, c, leading to the existence of gravitational radiation, or GWs. The more precise evidence ...
Classical Field Theory
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... The inverse Λ−1 appears in the argument because we are dealing with an active transformation in which the field is truly shifted, while the coordinates are still (see Figure 1). To see why this means that the inverse appears, it will suffice to consider a non-relativistic example such as a temperatu ...
The Structure of Scientific Theory Change
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... the structure of scientific theories, it is crucial to attend to the role that theories play in the construction of their own replacements. Precisely here is where we find the crucial importance of the distinction between a purely model-theoretic account of theories and an account that takes due not ...
Visions of Revolutions: Microphysics and Cosmophysics in the 1930s
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... looked back on the stormy development of quantum physics. He expressed the view, at the same time optimistic and reductionistic, that apart from relativistic effects quantum theory was essentially complete. In an oft-quoted passage he wrote: “The general theory of quantum mechanics is now almost com ...
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... Murray Gell-Mann and Francis E. Low in 1954 restricted the idea to scale transformations in QED,[2] which are the most physically significant, and focused on asymptotic forms of the photon propagator at high energies. They determined the variation of the electromagnetic coupling in QED, by apprecia ...
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Geometric topology and connections with quantum field theory.

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Accuracy of microwave cavity perturbation measurements

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... i.e., E0 ­ DFyfR lns1 1 LyRdg. In the absence of any deformation (lr ­ 0) F ­ 2pa. The above functional is not bound from below if we allow for deformations of either sign. However, in practice the dislocation line forms close to the inner electrode, which acts as a hard circular wall. Thus, we mini ...
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... possible because anomalous (i.e. gauge-variant) terms in the effective action have topological nature and are therefore scale independent. As a result, they are not suppressed even at energies much smaller than the masses of the particles producing these terms via loop effects. This gives hope to s ...
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... strength of a dipole transition in the atom. Let us note that we do not use a rotating wave approximation in the coupling Hamiltonian (2b). As was shown previously in [28], the complete interaction term is necessary to obtain a correct expression for the polarizability of a two-level atom. 2.2. Two- ...
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... Over the last two decades powerful molecular modelling tools have been developed which are capable of accurately predicting structures, energetics, reactivities and other properties of molecules. These developments have come about largely due to: The dramatic increase in computer speed. The design o ...
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Edge theory of ferromagnetic quantum Hall states

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Yang–Mills theory

Yang–Mills theory is a gauge theory based on the SU(N) group, or more generally any compact, semi-simple Lie group. Yang–Mills theory seeks to describe the behavior of elementary particles using these non-Abelian Lie groups and is at the core of the unification of the electromagnetic and weak forces (i.e. U(1) × SU(2)) as well as quantum chromodynamics, the theory of the strong force (based on SU(3)). Thus it forms the basis of our understanding of particle physics, the Standard Model.
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