Epstein Secrets

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§0,(x) where 122 = 1 + 2e4)t./All, (2) is the conformal factor and Alp is the reduced Planck mass. By doing so, one passes from the Jordan to the Einstein frame. The scalar potential in the new frame becomes V (h) Am 4 (1 + ) 2 (3) where we have written et = h2/ 2. At large field values, h > Mp/

d Fa; = 7',Ivj with Tal the sym- metry generators and vj the symmetry-breaking vacuum ex- pectation value. (See, e.g., [33]). A corresponding Fadeev- Popov ghost term is also added. Physical or "on-shell" quan- tities, such as cross sections and decay rates, may be calcu- lated perturbatively, and any de

li,„(s) where D2 = 1 + 2e(}141/4/1, (2) is the conformal factor and My is the reduced Planck mass. By doing so. one passes from the Jordan to the Einstein frame. The scalar potential in the new frame becomes V(h) 2 (3) 4 (1 + where we have written 4.147, = h2/ 2. At large field values. h > ii/p/V

and F° = riv, with 711 the sym- metry generators and vj the symmetry-breaking vacuum ex- pectation value. (See. e.g., [33]). A corresponding Fadeev- Popov ghost term is also added. Physical or "on-shell" quan- tities, such as cross sections and decay rates, may be calcu- lated penurbatively, and any dep