Proposing a Classical Explanation of the EPR
... requires an entire matrix of completely novel ad hoc hypotheses (about an infinite array of heretofore unknown particles and their powers of interaction with known particles) for which there is no evidence. That gives far greater probability to the third and only other logically possible explanation ...
... requires an entire matrix of completely novel ad hoc hypotheses (about an infinite array of heretofore unknown particles and their powers of interaction with known particles) for which there is no evidence. That gives far greater probability to the third and only other logically possible explanation ...
Dynamic model of elementary particles and the nature of mass and
... Leonid G. Kreidik and George P. Shpenkov Institute of Mathematics & Physics, UTA ...
... Leonid G. Kreidik and George P. Shpenkov Institute of Mathematics & Physics, UTA ...
THE RENORMALIZATION GROUP AND CRITICAL PHENOMENA
... step for each length scale. In the case ofcritical phenomena, the problem, technically, is to carry out statistical averages over thermal fluctuations on all size scales. The renormalization group approach is to integrate out the fluctuations in sequence starting with fluctuations on an atomic scale ...
... step for each length scale. In the case ofcritical phenomena, the problem, technically, is to carry out statistical averages over thermal fluctuations on all size scales. The renormalization group approach is to integrate out the fluctuations in sequence starting with fluctuations on an atomic scale ...
2. The Integer Quantum Hall Effect
... you can’t have charged chiral particles moving along a wire; there has to be particles which can move in the opposite direction as well. In the language of field theory, this follows from what’s called the chiral anomaly. In the language of condensed matter physics, with particles moving on a lattic ...
... you can’t have charged chiral particles moving along a wire; there has to be particles which can move in the opposite direction as well. In the language of field theory, this follows from what’s called the chiral anomaly. In the language of condensed matter physics, with particles moving on a lattic ...
CHAP3
... Energy flux of the beam is S = N (hn) /At = n0 chn (in unit of joule per unit time per unit area). N is obtained by ‘counting’ the total number of photons in the beam volume, N = n0V = n0 x (A ct), where n0 is the photon number density of the radiation (in unit of ...
... Energy flux of the beam is S = N (hn) /At = n0 chn (in unit of joule per unit time per unit area). N is obtained by ‘counting’ the total number of photons in the beam volume, N = n0V = n0 x (A ct), where n0 is the photon number density of the radiation (in unit of ...
Renormalization
In quantum field theory, the statistical mechanics of fields, and the theory of self-similar geometric structures, renormalization is any of a collection of techniques used to treat infinities arising in calculated quantities.Renormalization specifies relationships between parameters in the theory when the parameters describing large distance scales differ from the parameters describing small distances. Physically, the pileup of contributions from an infinity of scales involved in a problem may then result in infinities. When describing space and time as a continuum, certain statistical and quantum mechanical constructions are ill defined. To define them, this continuum limit, the removal of the ""construction scaffolding"" of lattices at various scales, has to be taken carefully, as detailed below.Renormalization was first developed in quantum electrodynamics (QED) to make sense of infinite integrals in perturbation theory. Initially viewed as a suspect provisional procedure even by some of its originators, renormalization eventually was embraced as an important and self-consistent actual mechanism of scale physics in several fields of physics and mathematics. Today, the point of view has shifted: on the basis of the breakthrough renormalization group insights of Kenneth Wilson, the focus is on variation of physical quantities across contiguous scales, while distant scales are related to each other through ""effective"" descriptions. All scales are linked in a broadly systematic way, and the actual physics pertinent to each is extracted with the suitable specific computational techniques appropriate for each.