¡ ± Æ æ Ê ê £ ³ ñ Ñ ó Ó ¶ ¦ ¼ ¬ ¿ ¯ %$\lambda_{J}=\sqrt{\frac{\Pi k T}{G m \rho_{0}}}$% %$\int cdt=0$% To tylko próby %MATHMODE{\int cdt=0}% %MATHMODE{n + \ ^3He \rightarrow \cases{\quad T + p \cr ^4He + \gamma}% %$n + \ ^3He \rightarrow \cases{\quad T + p \cr ^4He + \gamma$% (28) %$D + D \rightarrow \cases{^3He + n \cr \quad T + p$% (22) %$\frac{n_n}{n_p} = \cases{(\frac{m_n}{m_p})^{\frac{3}{2}} = 1 \qquad ;\ E_K \gg 1MeV \cr 0 \qquad \qquad \qquad ;\ E_K \rightarrow O$% (16) c.d.n -- Main.RoWia - 01 Mar 2004
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