Recent content by nadia8999

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    Why there is 2[itex]\pi[/itex] in every dirac delta function

    in QF, every dirac delta function is accompanied by 2\pi,i.e.(2\pi)\delta(p-p_0) or (2\pi)^3\delta(\vec{p}-\vec{p_0}) the intergral element in QF is \int\frac{d^3p}{(2\pi)^3}\frac{1}{2E_P}, it comes from the integral element \int\frac{d^4p}{(2\pi)^4}(2\pi)\delta(p^2-m^2),I want to know why...
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    In <Cosmology> written by Weinberg, in page 109

    the press should be reflected in the equation, the question is what does press include. Of course it includes press from radiation and anything else? In my opinion, baryons or dusts, whatever, should have press, as far as they constitutes the gas, baryon gas or dust gas. However, the press of...
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    In <Cosmology> written by Weinberg, in page 109

    What is the criterion to determine whether they can express press or not?
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    In <Cosmology> written by Weinberg, in page 109

    The particles in the air, as we all know, are non-relativistic, but they can express press. However, I still wonder what is the criterion to determine whether they can press or not, the press of dust is 0 and why. You can refer to #8.
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    In <Cosmology> written by Weinberg, in page 109

    I agree with you, but why after recombination, the baryons do not experience pressure.
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    In <Cosmology> written by Weinberg, in page 109

    I referred to the Statistical books and found that for non-relativistic gas the press is\frac{2}{3}n \bar{\epsilon}, n is the number density and \bar{\epsilon}is the energy density. I think the baryons should be treated as gas rather than as dust.
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    In <Cosmology> written by Weinberg, in page 109

    \alpha_Bcomes from \int_0^{\infty} h \nu n(\nu)d\nu=\alpha_B T^4 so it means the average energy density of radiation. n_Bmeans the number density of bayons. Nmeans the non-relativistic particles per baryon.
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    In <Cosmology> written by Weinberg, in page 109

    In <Cosmology> written by Weinberg, in page 109, it says that \epsilon=\alpha_{B}T^4+\frac{3}{2}n_{B}Nk_{B}T p=\frac{1}{3}\alpha_{B}T^4+n_{B}Nk_{B}T \alpha_{B}T^4is the average energy density of black-body radition, then what does \frac{3}{2}n_{B}Nk_{B}Tmeans? the energy density of...
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