
Law of Conservation of Muons
... This argument therefore leads directly to a multiplicative conservation law of "muon parity. If no particular model is assumed for the weak interactions, no stronger, additive, conservation law is implied. Of course, we cannot rule out the possibility that there is an additive quantum number, which ...
... This argument therefore leads directly to a multiplicative conservation law of "muon parity. If no particular model is assumed for the weak interactions, no stronger, additive, conservation law is implied. Of course, we cannot rule out the possibility that there is an additive quantum number, which ...
String Theory
... String theory • The extra dimensions are hidden a la Kaluza, Klein theory (1921) • Supersymmetry is there but broken (somehow) • The fact that these aren’t observed at current scales is in no sense a theoretical problem, the natural scale for such things would be the string scale ie. around the pla ...
... String theory • The extra dimensions are hidden a la Kaluza, Klein theory (1921) • Supersymmetry is there but broken (somehow) • The fact that these aren’t observed at current scales is in no sense a theoretical problem, the natural scale for such things would be the string scale ie. around the pla ...
PowerPoint
... the fundamental assumptions could break down in some cases. 2. evaluation of correlation functions are done within classical or high-temperature approximations. not valid with strong quantum fluctuations ...
... the fundamental assumptions could break down in some cases. 2. evaluation of correlation functions are done within classical or high-temperature approximations. not valid with strong quantum fluctuations ...
a ∇ µ
... SU(3) classical gauge field does not interact with ordinary matter because ordinary matter is colorless. Thus one can suppose that SU(3) gauge field can be invisible matter in galaxies. The problem for such consideration is why the gauge field do not fill all Universe ? The probable answer is that, ...
... SU(3) classical gauge field does not interact with ordinary matter because ordinary matter is colorless. Thus one can suppose that SU(3) gauge field can be invisible matter in galaxies. The problem for such consideration is why the gauge field do not fill all Universe ? The probable answer is that, ...
Vacuum Bubbles Nucleation and Dark Matter Production through
... no “transversality” in one spatial dimension, the concept of spin is undefined, and the notion of “ vector field”, massless or massive, is purely formal. Thus, there is no radiation field associated with the Maxwell tensor. There is, however, the same background vacuum energy and long range static i ...
... no “transversality” in one spatial dimension, the concept of spin is undefined, and the notion of “ vector field”, massless or massive, is purely formal. Thus, there is no radiation field associated with the Maxwell tensor. There is, however, the same background vacuum energy and long range static i ...
Flavor Beyond Standard Model
... of our current understanding of particle physics. These transitions are forbidden at tree level in the SM, as all electrically neutral particles have only diagonal couplings in the flavor space. FCNC processes are therefore only allowed through loop contributions and probe the underlying fundamental ...
... of our current understanding of particle physics. These transitions are forbidden at tree level in the SM, as all electrically neutral particles have only diagonal couplings in the flavor space. FCNC processes are therefore only allowed through loop contributions and probe the underlying fundamental ...
Many_1 - USU physics
... In either of these cases, if two of the fermion detector positions are the same, so that two positions and two spins have the same indices (detectors measure spatial and spin quantum numbers), the wavefunction also vanishes: in other words, two identical fermions cannot occupy the same position in s ...
... In either of these cases, if two of the fermion detector positions are the same, so that two positions and two spins have the same indices (detectors measure spatial and spin quantum numbers), the wavefunction also vanishes: in other words, two identical fermions cannot occupy the same position in s ...