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In particle physics, Yukawa's interaction or Yukawa coupling, named after Hideki Yukawa, is an interaction between particles according to the Yukawa potential. Specifically, it is between a scalar field (or pseudoscalar field) ϕ and a Dirac field ψ of the type
A coupling plays an important role in dynamics. For example, one often sets up hierarchies of approximation based on the importance of various coupling constants. In the motion of a large lump of magnetized iron, the magnetic forces may be more important than the gravitational forces because of the relative magnitudes of the coupling constants.
For quantum chromodynamics, the constant changes with respect to the distance between the particles. This phenomenon is known as asymptotic freedom. Forces which have a coupling constant greater than 1 are said to be "strongly coupled" while those with constants less than 1 are said to be "weakly coupled." [7]
Coupled mode theory (CMT) is a perturbational approach for analyzing the coupling of vibrational systems (mechanical, optical, electrical, etc.) in space or in time. Coupled mode theory allows a wide range of devices and systems to be modeled as one or more coupled resonators.
Weinberg angle θ W, and relation between coupling constants g, g′, and e. Adapted from T D Lee's book Particle Physics and Introduction to Field Theory (1981). Due to the Higgs mechanism , the electroweak boson fields W 1 {\displaystyle W_{1}} , W 2 {\displaystyle W_{2}} , W 3 {\displaystyle W_{3}} , and B {\displaystyle B} "mix" to create ...
Weinberg angle θ W, and relation between couplings g, g ′, and e = g sin θ W. Adapted from Lee (1981). [1] The pattern of weak isospin, T 3, and weak hypercharge, Y W, of the known elementary particles, showing electric charge, Q, [a] along the Weinberg angle. The neutral Higgs field (upper left, circled) breaks the electroweak symmetry and ...
Thus, an electron may just "split" into an electron plus a photon, with a certain probability (which is roughly the coupling constant). This is described in string theory as one string splitting into two. This process is an integral part of the theory. The mode on the original string also "splits" between its two parts, resulting in two strings ...
The model belongs to the Griffiths-Simon class, [1] meaning that it can be represented also as the weak limit of an Ising model on a certain type of graph. The triviality of both the ϕ 4 {\displaystyle \phi ^{4}} model and the Ising model in d ≥ 4 {\displaystyle d\geq 4} can be shown via a graphical representation known as the random current ...