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Particle Physics
Particle Physics

... 5. This is a problem set about QED. a. Prove that an electron in isolation cannot emit one photon because of momentum conservation. That is, the process e   p1   e  ( p 2 )    p3  (the letters in the parentheses are the corresponding momenta) is prohibited. b. However, if electron gets a s ...
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... The problem in this case is that the wavefunction is not normalizable, so it’s not a true wavefunction . It can be used to make true wavefunctions by superposition. The probability of finding the particle = Independent of position so the particle is equally likely to be anywhere. In the case of the ...
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... get the same from qualitative behavior the uncertainty principle idea. The Breit Wigner probability density function (pdf): P = 1/((E2-M2) 2+M22) where  is known as the width and is the inversely related to the lifetime. Note that this is clearly a relativistic equation. We’ll find this comes from ...
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The 1/N expansion method in quantum field theory
The 1/N expansion method in quantum field theory

... A new parameter may emerge if the system under consideration satisfies symmetry properties with respect to a group of internal transformations. For example, constituents of the system (particles, nucleons, nuclei, energy excitations, etc.) belonging to different species, may have the same masses an ...
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Chapter 3 Basic quantum statistical mechanics of spin

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Relativistic quantum mechanics

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