Towards an effective field theory on the light-shell
... Previously, [1] we expressed the hope of constructing an effective field theory on the 2-dimensional light-shell emerging from a high-energy collision. The idea was motivated by a classical picture of a very high energy hadronic collision in which colored particles are produced from an initially col ...
... Previously, [1] we expressed the hope of constructing an effective field theory on the 2-dimensional light-shell emerging from a high-energy collision. The idea was motivated by a classical picture of a very high energy hadronic collision in which colored particles are produced from an initially col ...
Chiral kinetic theory
... Forces (ṗ) should not be too strong ( B ≪ |p|2 ). However, we cannot neglect the diagonal components – Berry phases! Although non-abelian âp is pure gauge, abelian component [âp ]11 ≡ ap is non-trivial: the field of a “monopole” at |p| = 0 (as in ’t Hooft, Polyakov): b ≡ ∇ p × ap = ...
... Forces (ṗ) should not be too strong ( B ≪ |p|2 ). However, we cannot neglect the diagonal components – Berry phases! Although non-abelian âp is pure gauge, abelian component [âp ]11 ≡ ap is non-trivial: the field of a “monopole” at |p| = 0 (as in ’t Hooft, Polyakov): b ≡ ∇ p × ap = ...
Vacuum Energy and Effective Potentials
... This finite difference — called the Casimir effect — has observable consequences such as attractive force between two parallel plates at small distances from each other, Fc = − ...
... This finite difference — called the Casimir effect — has observable consequences such as attractive force between two parallel plates at small distances from each other, Fc = − ...
Identical Particles
... Hence the wave function of a system of two identical particles must be either symmetric or antisymmetric under the exchange of the two particles. The Spin-Statistics Theorem Systems of identical particles with integer spin (s = 0, 1, 2, . . .), known as bosons, have wave functions which are symmetri ...
... Hence the wave function of a system of two identical particles must be either symmetric or antisymmetric under the exchange of the two particles. The Spin-Statistics Theorem Systems of identical particles with integer spin (s = 0, 1, 2, . . .), known as bosons, have wave functions which are symmetri ...
Elementary Particle Physics
... L12 angular momentum of 1 and 2 in "subsystem" L3 angular momentum of 3 about c.m of 1 and 2 in the overall c.m. frame: Ltot L12 L3 We only consider ground state baryons: angular momentum comes only from spin: L12 L3 0 ...
... L12 angular momentum of 1 and 2 in "subsystem" L3 angular momentum of 3 about c.m of 1 and 2 in the overall c.m. frame: Ltot L12 L3 We only consider ground state baryons: angular momentum comes only from spin: L12 L3 0 ...
The Neutron - Miles Mathis
... The mainstream has mainly ignored it, focusing decades of attention on the electron. But of course the mainstream has mainly ignored all mechanics, being more interested in playing with their fancy maths. After more than forty years of toying with quarks, the mainstream still has not linked quark co ...
... The mainstream has mainly ignored it, focusing decades of attention on the electron. But of course the mainstream has mainly ignored all mechanics, being more interested in playing with their fancy maths. After more than forty years of toying with quarks, the mainstream still has not linked quark co ...
The Beh-MechaNiSM, iNTeracTioNS wiTh ShorT
... particles were discovered. Most of them decaying by the strong interaction were extremely short-lived with a lifetime of the order of 10-23 s. Others, like the charged pions, have a lifetime of typically 10-6 to 10-10 s. They decay by the weak nuclear force. The proliferation of new elementary parti ...
... particles were discovered. Most of them decaying by the strong interaction were extremely short-lived with a lifetime of the order of 10-23 s. Others, like the charged pions, have a lifetime of typically 10-6 to 10-10 s. They decay by the weak nuclear force. The proliferation of new elementary parti ...
Effective Field Theory Description of the Higher Dimensional
... arrive at a 4 + 1 dimensional continuum field theory by treating S 2 as a “fuzzy sphere,” with discrete matrix model degrees of freedom. By this procedure, we arrive at the equivalent SU (2) non-abelian CS gauge field theory in 4 + 1 dimensions, where particles with SU (2) internal isospin degrees o ...
... arrive at a 4 + 1 dimensional continuum field theory by treating S 2 as a “fuzzy sphere,” with discrete matrix model degrees of freedom. By this procedure, we arrive at the equivalent SU (2) non-abelian CS gauge field theory in 4 + 1 dimensions, where particles with SU (2) internal isospin degrees o ...
Structural( biology( at( the( single( particle( level:( imaging( tobacco
... improvement in precision by 1-2 orders of magnitude. This allows to probe these questions in a complementary way to LHC-based experiments or even constitutes a unique way. The research program focuses on four priority areas, which are directly related to specific physics/astrophysics issues: • Prior ...
... improvement in precision by 1-2 orders of magnitude. This allows to probe these questions in a complementary way to LHC-based experiments or even constitutes a unique way. The research program focuses on four priority areas, which are directly related to specific physics/astrophysics issues: • Prior ...
