Page 2 of 2

Re: Referat and Exam of Viktor Atroschenko

New postPosted: Sat 12 Jan 2013 17:49
by Maxim Khlopov
Dear Viktor,
Please, find answer to your question:
Energy density of inflaton is distributed between ordinary and mirror particles in proportion to K and K'.
It determines temperature of ordinary and mirror matter at heating after inflation.
In the same way, in which we treated ratio of primordial neutrinos and photons you can deduce the temperatures of ordinary and mirror matter at 1 s of expansion (with the account for the change of number of species)
Regards
M.Yu.Khlopov

Re: Referat and Exam of Viktor Atroschenko

New postPosted: Sat 12 Jan 2013 18:45
by Viktor_mephi_40
Стало еще непонятнее
Ведь E'/E=(K'/K)*(T'/T)^4
Если энергия инфлатона Einf разделяется на зеркальные и обычные частицы, т.е Einf=E + E',
а E~K' и E~K, то (T'/T)^4=1, т.е. T'=T сразу после нагрева

Re: Referat and Exam of Viktor Atroschenko

New postPosted: Sat 12 Jan 2013 19:07
by Maxim Khlopov
If Einf=E + E', E= K/(K+K')Einf and E'=K'/(K+K')Einf, isn't it?
Regards
M.Yu.Khlopov

Re: Referat and Exam of Viktor Atroschenko

New postPosted: Sat 12 Jan 2013 19:30
by Viktor_mephi_40
Да, я просто опустил подробности

E = K * Einf / (K+K') и E = K * s * T^4, аналогично для E' (s=\sigma)

T^4 = E/(K * s)=Einf/{s*(K+K')} так как К сократилось

для Т'^4 получается абсолютно то же самое

значит T=T'

Re: Referat and Exam of Viktor Atroschenko

New postPosted: Sun 13 Jan 2013 00:00
by Maxim Khlopov
Yes, if you distribute energy in proportionality to the number of species, you have the same temperatures and the temperatures at t=1s is determined by separate entropy conservation for ordinary and mirror matter.
Regards
M.Yu.Khlopov