Potential (vc<) = cx? - gre3 - fx4 : Partition function (2) = dn dp: d - BV(x) e e zm where; m→ mass of the ascillator; B: Ta temberature. To Jet finite Z; § hag to be negative af it if the leading term in e-BUCx) af x→ + d. Let; go g Ş be Sufficientiy Small S.t. = I + B( gx? x) 2. = I + Bgz + Bfz + Bgx
Potential (vc<) = cx? - gre3 - fx4 : Partition function (2) = dn dp: d - BV(x) e e zm where; m→ mass of the ascillator; B: Ta temberature. To Jet finite Z; § hag to be negative af it if the leading term in e-BUCx) af x→ + d. Let; go g Ş be Sufficientiy Small S.t. = I + B( gx? x) 2. = I + Bgz + Bfz + Bgx
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