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E = - \\frac{1}{2} \\alpha E^2\n\\]\n<\/pre>\n<p>\u3053\u3053\u3067\u3001<\/p>\n<ul>\n<li>\\(\\Delta E\\) \u306f\u30a8\u30cd\u30eb\u30ae\u30fc\u6e96\u4f4d\u306e\u5909\u5316\u3002<\/li>\n<li>\\(\\alpha\\) \u306f\u5206\u6975\u7387\uff08Polarizability\uff09\u3068\u547c\u3070\u308c\u308b\u5b9a\u6570\u3002<\/li>\n<li>\\(E\\) 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