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Unformatted text preview: Phys 253a 1 Problem Set 9 Solutions December 2, 2010 1. (a) There are lots of diagrams. Most of them are just vertex and propagator cor rections. The other diagram well deal with is the one thats the same, but with the photon lines crossed in the middle. (b) As in problem set 6, well write the loop integral as R d 4 kd 4 q (2 ) 4 ( p 1 + p 2 k q ), or R for short. Ignoring factors of i and coupling constants, the diagrams are I = Z [ v 2 1 6 p 16 q m u 1 ][ u 3 1 6 p 36 k m v 4 ] ( k ) ( q ) II = Z [ v 2 1 6 p 16 q m u 1 ][ u 3 1 6 p 36 q m v 4 ] ( q ) ( k ) Where ( k ) = i k 2 ( +(1 ) k k k 2 ) is the photon propagator. As before, lets define V L = v 2 1 6 p 16 q m u 1 + v 2 1 6 p 16 k m u 1 V R = u 3 1 6 p 36 k m v 4 + u 3 1 6 p 36 q m v 4 Because of the symmetry q k under R , its easy to check that Z V L V R ( k ) ( q ) = 2(I + II) But k V L = v 2 6 k 1 6 k6 p 2 m u 1 + v 2 1 6 p 16 k m 6 ku 1 = v 2 ( 6 k6 p 2 m ) 1 6 k6 p 2 m u 1 + v 2 1 6 p 16 k m ( 6 k + m6 p 1 ) u 1 = v 2 u 1 v 2 u 1 = 0 where in getting to the second line, weve used the Dirac equations v 2 ( 6 p 2 + m ) = 0 and ( m6 p 1 ) u 1 = 0. Similarly, we can show q V L = 0 k V R = 0 q V R = 0 Thus, the gaugedependent terms in V L V R ( k ) ( q ) manifestly vanish. Phys 253a 2 2. (a) We proved in problem set 6 that the propagator for a vector boson is i  k k m 2 Z k 2 m 2 Z So the amplitude for e e is i M = [ v 2 i ( g V + g A 5 ) u 1 ][ u 3 i ( g V + g A 5 ) v 4 ] i (  k k m 2 Z ) k 2 m 2 Z With k = p 1 + p 2 . Now the Dirac equations 6 p 1 u 1 = 0 and v 2 6 p 2 = 0 imply k ( v 2 i ( g V + g A 5 ) u 1 ) = v 2 ( 6 p 1 + 6 p 2 ) i ( g V + g A 5 ) u 1 = v 2 6 p 2 i ( g V + g A 5 ) u 1 + v 2 i ( g V g A 5 ) 6 p 1 u 1 = 0 This is just a statement of current conservation: The current that Z couples to, J = ( g V + g A 5 ) , is conserved (by Noethers theorem), so k ( v 2 i ( g V + g A 5 ) u 1 ) = k h  J ( k )  e ,p 1 ; e + ,p 2 i = 0 Similarly, the other current u 3 i ( g V + g A 5 ) v 4 = h e ,p 3 ; e + ,p 4  J ( k )  i is conserved, so the k k m 2 Z part of the Z propagator doesnt contribute. Thus, i M = [ v 2 i ( g V + g A 5 ) u 1 ][ u 3 i ( g V + g A 5 ) v 4 ] i k 2 m 2 Z Since the neutrinos are massless (so there are no other mass scales besides m Z and k ), dimensional analysis tells us that M k 2 k 2 m 2 Z Then the cross section is 1 s M 2 = s ( s m 2 Z ) 2 which is increasing with energy when s is below m 2 Z . (Dont worry, by the way, about infinities in...
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This note was uploaded on 02/04/2012 for the course PHYS 253A at Harvard.
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 SCHWARTZ
 Photon

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