By Umezawa H.
This paintings starts through distinguishing the adaptation among quantum mechanics and quantum box thought. It then makes an attempt to increase box concept by means of including a thermal measure of freedom to phenomena happening inside a vacuum. The ensuing quantum box concept is termed Thermo box Dynamics (TFD).
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73) , that (p’JT lp) is not, Lorentz invariant 0 po (p’( T lp) is. 75) 41 Examples if there are T- fermions and s bosons such that m and n being the number of initial and final particles respectively. 79) Here ma, mb, m, and md are the masses of four particles a , b, c and d involved in a scattering or a decay process. g. g. nucleons. 82) We calculate the scattering cross section in the c. m. frame. 8313) = P c d = PI Ed. 84) Now from Eq. 86) The integration over d 3 p d in Eq. ( 8 5 ) can be removed by t,he threedimensional &function.
82) We calculate the scattering cross section in the c. m. frame. 8313) = P c d = PI Ed. 84) Now from Eq. 86) The integration over d 3 p d in Eq. ( 8 5 ) can be removed by t,he threedimensional &function. 87) d3p, = Ip1I2d (p’ldR’, we have from Eq. 89) we have from Eqs. 2 Three-body decay Three-body phase space. -lp’l [MI2 (PI 4T2 Consider a three-body decay m ml+m2+m3 K = Pl+P2+P3. The decay rate [cf. Eq. 93) Scattering and Particle Interaction 44 where for definiteness, we have taken all the particles to be fermions.
A is proton 1 GcVl. mass m= - which gives 011 using a: z rp - and mx M 1015 GeV (or less) 1031 years (or less). This prediction is not yet borne out by experiment,. In fact the world's largest (IBM) detector sensitive to the decay mode years. rro) > 5 x GUTS have some attract,ive fcatmes: Grand Unification 23 1 1 qlmeson r -J 4 4 proton R, Y Figure 4 I Decay of a proton via lepto-quarks. quark-lepton unification (ii) relationships between quark and lepton masses (iii) quantization of electric charge, for a simple group it, is a consequence of the charge operator being a generator of the group and traceless.