Thermal effects on sudden changes and freezing
... based on the generalization to large number of excitations in the system. To the best of our knowledge, this approach of many excitations in similar systems [17–20] is not common, and may be one of few existing studies. To describe the evolution of an open quantum-optical system usually the approach ...
... based on the generalization to large number of excitations in the system. To the best of our knowledge, this approach of many excitations in similar systems [17–20] is not common, and may be one of few existing studies. To describe the evolution of an open quantum-optical system usually the approach ...
- RZ User
... pressure of a gas by the mean kinetic energy of small particles, but without recognizing its relation to the phenomenon of heat. If one regarded these particles themselves as small elastic spheres, though, the question for their internal structure might in principle arise anew. The picture of elemen ...
... pressure of a gas by the mean kinetic energy of small particles, but without recognizing its relation to the phenomenon of heat. If one regarded these particles themselves as small elastic spheres, though, the question for their internal structure might in principle arise anew. The picture of elemen ...
Different faces of integrability in the gauge theories or in the jungles
... In this “forced” quasiclassical regime the comparison can be made between perturbative YM calculations and stringy answers. Complete agreement where possible. First predictions from integrability for the all-loop answers for the simplest object – anomalous dimension of the operators with the lar ...
... In this “forced” quasiclassical regime the comparison can be made between perturbative YM calculations and stringy answers. Complete agreement where possible. First predictions from integrability for the all-loop answers for the simplest object – anomalous dimension of the operators with the lar ...
8 - ijssst
... of these. Qubits implementation for Q.C is represented by particles having two spin states i.e. “up” written as | 0> and “down” written as |1 >:). They can also be entwined with other qubits which results the astonishing computational power of a quantum computer. Entanglement is an exclusive quantum ...
... of these. Qubits implementation for Q.C is represented by particles having two spin states i.e. “up” written as | 0> and “down” written as |1 >:). They can also be entwined with other qubits which results the astonishing computational power of a quantum computer. Entanglement is an exclusive quantum ...
Glashow-Weinberg-Salam Model: An Example of Electroweak
... During the late 1950s, studies of the helicity dependence of weak interaction cross section and decay rates has shown that the weak interaction involves the coupling between vector current built of quark and lepton fields. It was thus natural to assume that the weak interaction is due to exchange of ...
... During the late 1950s, studies of the helicity dependence of weak interaction cross section and decay rates has shown that the weak interaction involves the coupling between vector current built of quark and lepton fields. It was thus natural to assume that the weak interaction is due to exchange of ...
213-236, 2015 Centro de Filosofia das Ciências da
... imagery of a planetary system, will work over the entire domain of atomic physics, whereas at its height it had only been shown to work for a nucleus surrounded by one electron. To be sure, the results were excellent and so expectations were running high. This confidence was based on an analogy with ...
... imagery of a planetary system, will work over the entire domain of atomic physics, whereas at its height it had only been shown to work for a nucleus surrounded by one electron. To be sure, the results were excellent and so expectations were running high. This confidence was based on an analogy with ...
Standard Model at the LHC (Lecture 1: Theoretical Recap) M. Schott
... Only the left-handed components of particles and right-handed components of antiparticles participate in weak interactions in the Standard Model Need to modify the Fermi theory only a little bit M = (n̄γ µ (1 − γ 5 )p)GF (v̄e γ µ (1 − γ 5 )e) This operator only involves eL− , νL or (eR+ , νR ) ...
... Only the left-handed components of particles and right-handed components of antiparticles participate in weak interactions in the Standard Model Need to modify the Fermi theory only a little bit M = (n̄γ µ (1 − γ 5 )p)GF (v̄e γ µ (1 − γ 5 )e) This operator only involves eL− , νL or (eR+ , νR ) ...
