{"published":"2018-06-23 00:28:51","url":"https://www.k-pmpstudy.com/entry/2018/06/23/002851","width":"100%","author_name":"OviskoutaR","version":"1.0","provider_url":"https://hatena.blog","image_url":"http://ecx.images-amazon.com/images/I/41uyD3UY2qL.jpg","title":"1\u6b21\u5143\u8abf\u548c\u632f\u52d5\u5b50\u306e\u4f4d\u7f6e\u3068\u904b\u52d5\u91cf\u306e\u884c\u5217\u8981\u7d20\u306e\u8a08\u7b97 [PDF\u3042\u308a] ","categories":["\u91cf\u5b50\u529b\u5b66","\u91cf\u5b50\u529b\u5b66-\u6f14\u7fd2","\u7269\u7406\u5b66"],"blog_title":"\u4e09\u6d66\u30ce\u30fc\u30c8","height":"190","provider_name":"Hatena Blog","author_url":"https://blog.hatena.ne.jp/OviskoutaR/","html":"<iframe src=\"https://hatenablog-parts.com/embed?url=https%3A%2F%2Fwww.k-pmpstudy.com%2Fentry%2F2018%2F06%2F23%2F002851\" title=\"1\u6b21\u5143\u8abf\u548c\u632f\u52d5\u5b50\u306e\u4f4d\u7f6e\u3068\u904b\u52d5\u91cf\u306e\u884c\u5217\u8981\u7d20\u306e\u8a08\u7b97 [PDF\u3042\u308a]  - \u4e09\u6d66\u30ce\u30fc\u30c8\" class=\"embed-card embed-blogcard\" scrolling=\"no\" frameborder=\"0\" style=\"display: block; width: 100%; height: 190px; max-width: 500px; margin: 10px 0px;\"></iframe>","description":"\u672c\u8a18\u4e8b\u306ePDF\u7248\u3092BOOTH\u306b\u3066\u7121\u6599\u3067\u516c\u958b\u3057\u3066\u304a\u308a\u307e\u3059\uff0e\u5370\u5237\u3057\u3066\u8aad\u307f\u305f\u3044\u65b9\u306a\u3069\u662f\u975e\u3054\u5229\u7528\u304f\u3060\u3055\u3044\uff0e \u4e09\u6d66\u3068\u7aae\u7406\u3068\u30d6\u30ed\u30b0--1 \u6b21\u5143\u8abf\u548c\u632f\u52d5\u5b50\u306e\u4f4d\u7f6e\u3068\u904b\u52d5\u91cf\u306e\u884c\u5217\u8981\u7d20\u306e\u8a08\u7b97 - k-pmpstudy - BOOTH\uff08\u540c\u4eba\u8a8c\u901a\u8ca9\u30fb\u30c0\u30a6\u30f3\u30ed\u30fc\u30c9\uff09 1\u6b21\u5143\u8abf\u548c\u632f\u52d5\u5b50\u306e\u6ce2\u52d5\u95a2\u6570\u306f\u30a8\u30eb\u30df\u30fc\u30c8\u591a\u9805\u5f0f\u3092\u7528\u3044\u3066 $ \\psi_n(\\xi) = A_n H_n (\\xi) e^{-\\xi^2/2} $ \u3068\u8868\u305b\u308b\uff0e\u3053\u3053\u3067\uff0c$ \\xi =\\sqrt{m\\omega/\\hbar} x $\uff0c$ A_n = \\frac{1}{\\sqrt{2^n n!}} \\left (\\frac{m\\omega}{\\pi\\hbar}\\ri\u2026","blog_url":"https://www.k-pmpstudy.com/","type":"rich"}