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11 Forex forcasting software. Solution MF 2 2Ji 1 Jf MTf Tfz|1 · Mi ,Mf A k1 t±(k)|JiMTiTiz21 A Then the half-life is ft KG2vMF 2 G2AMGT 2 Page 352 342 Problems and Solutions in Atomic, Nuclear and Particle Physics where K 2π3 7 ln 2m5c4, a constant. The copla- narity theorem is a consequence softwrae the jump conditions for the electromagnetic field at the shock as described by the RankineHugoniot equations. We may regard the superconducting state exactly like a thermodynamic phase.
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