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        "quote": "其中符号适用于费米子，而符号适用于玻色子。参数$\\lambda$常写作$\\lambda = \\operatorname { e } ^ { \\beta \\mu }$，其中$\\mu$称为<u class=\"concept-term\" data-concept-identity=\"urn:uuid:01ff489c-58d1-4d75-87b2-d1cd999d36bd\" data-concept-route=\"/concept-identities#concept-01ff489c-58d1-4d75-87b2-d1cd999d36bd\" id=\"first-f00a4551bf40bd071302-zh\">化学势(chemical potential)</u>。可以证明，使用最速下降法（见[10]），公式<a href=\"#equation-14-53\" class=\"cross-reference\" id=\"xref-04-quantum-statistical-mechanics-6\" data-reference=\"equation-14-53\">式 (14.53)</a>对于正则系综也成立。在这种情况下，总粒子数固定，因此化学势可由下式求得",
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        "quote": "where the sign applies to Fermi particles, and the to Bose. The parameter $\\lambda$ is often written $\\lambda = \\operatorname { e } ^ { \\beta \\mu }$ , where $\\mu$ is known as the <u class=\"concept-term\" data-concept-identity=\"urn:uuid:01ff489c-58d1-4d75-87b2-d1cd999d36bd\" data-concept-route=\"/concept-identities#concept-01ff489c-58d1-4d75-87b2-d1cd999d36bd\" id=\"first-f00a4551bf40bd071302-en\">chemical potential</u>. It can be shown, using the method of steepest descent (see [10]) that the formulae <a href=\"#equation-14-53\" class=\"cross-reference\" id=\"xref-04-quantum-statistical-mechanics-11\" data-reference=\"equation-14-53\">Eq. (14.53)</a> are also valid for the canonical ensemble. In this case the total particle number is fixed so that the chemica potential may be found from",
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