- Page 2 and 3: INTRODUCTION TO THE WEAK INTERACTIO
- Page 6 and 7: Chapter One : Quantum Mechanics . 1
- Page 8 and 9: CHAPTER ONE : QUANTUM MEaiANICS . 1
- Page 10 and 11: observed were very similar to those
- Page 12 and 13: 'wave functio n at ( 1.3 .9 ) P —
- Page 14 and 15: of that measurement . Hence we may
- Page 16 and 17: 2 (x) n =. M e -~ ~2 n H (~' ) r. (
- Page 18 and 19: E2 = p 2 -~- m 2 By substituting th
- Page 20 and 21: The letters on the right-hand side
- Page 22 and 23: Similarly, from (1 .8.8), setting u
- Page 24 and 25: in two parts (1) : t ) = 2t (2 .1 .
- Page 26 and 27: In order to discover more about the
- Page 28 and 29: particles, a and b, is that the sig
- Page 30 and 31: g. Similarly we see that b (r) (g)
- Page 32 and 33: `,{ r (a/axr ) J(x) = ( Y i ('a /a
- Page 34 and 35: 'Heisenberg picture' may be used in
- Page 36 and 37: 2 .7 The CPT Theorem . (15 ) The CP
- Page 38 and 39: CHAPTER THREE : vCLEAR BETA DECAY .
- Page 40 and 41: and did not appear to decay, it was
- Page 42 and 43: traces of K-electron capture radiat
- Page 44 and 45: where rl 1 1 1 1 ; 4 -2 0 2 -4 I )
- Page 46 and 47: so that the condition for CPT invar
- Page 48 and 49: with momentum pv >pv + dpv . The nu
- Page 50 and 51: which has the limiting form s h(Q)
- Page 52 and 53: implying tha t C F 1.37 x 10- 65 3
- Page 54 and 55:
and then applying the matrix elemen
- Page 56 and 57:
final state coulomb interaction bet
- Page 58 and 59:
measuring the value of the coeffici
- Page 60 and 61:
The only two gonna-matrix products
- Page 62 and 63:
3 .7 The Nonconservation of Parity
- Page 64 and 65:
after which time the nuclei had bec
- Page 66 and 67:
implying that the constants GV and
- Page 68 and 69:
to be aligned in a direction opposi
- Page 70 and 71:
where B is the total electron energ
- Page 72 and 73:
splitting between the triplet (J =
- Page 74 and 75:
of iron whose direction of magnetiz
- Page 76 and 77:
For cases in which the neutrino has
- Page 78 and 79:
We find (76) that the matrix elemen
- Page 80 and 81:
See also e .g . L . Wolfendale : Es
- Page 82 and 83:
57 . A . De Shalit, S . Kuperman, H
- Page 84 and 85:
the simplest possible muon decay sc
- Page 86 and 87:
x = (2Ee )/mt „ (4 .2 .10 ) Thus
- Page 88 and 89:
4 .3 The Two Neutrinos . If the two
- Page 90 and 91:
much longer tracks than any of the
- Page 92 and 93:
interactions. The currents (4 .4 .1
- Page 94 and 95:
where 'CC = 2 g2 m2 /vc 8 .3 x 10
- Page 96 and 97:
4 .5 The Conservation of Leptons .
- Page 98 and 99:
helicities, it is unnecessary to di
- Page 100 and 101:
CHAPTER FIVE : THE HADRONIC STRUCTU
- Page 102 and 103:
interaction, and, in fact, we find
- Page 104 and 105:
- Jr(x) — g 't1p(x) Ir 7rn(x) . (
- Page 106 and 107:
y J r , and the weak leptonic curre
- Page 108 and 109:
3r = a o J + a, Jr . (5 .3 .20 ) Th
- Page 110 and 111:
5 .4 Form Factors . Before we may c
- Page 112 and 113:
form factors : an isoscalar fora fa
- Page 114 and 115:
and where q is the four-momentum of
- Page 116 and 117:
muon absorption : p ___ vt, + n . (
- Page 118 and 119:
Experiments give (26 ) 1/Tc = 480
- Page 120 and 121:
so that the total weak Hamiltonian
- Page 122 and 123:
and (5 .6 .26) might still be absen