{"id":2370,"date":"2022-02-26T10:56:50","date_gmt":"2022-02-26T01:56:50","guid":{"rendered":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/?page_id=2370"},"modified":"2025-08-06T11:49:30","modified_gmt":"2025-08-06T02:49:30","slug":"%e3%83%95%e3%83%bc%e3%83%aa%e3%82%a8%e7%a9%8d%e5%88%86%e3%83%bb%e3%83%95%e3%83%bc%e3%83%aa%e3%82%a8%e5%a4%89%e6%8f%9b","status":"publish","type":"page","link":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/%e7%90%86%e5%b7%a5%e7%b3%bb%e3%81%ae%e6%95%b0%e5%ad%a6c\/%e3%83%95%e3%83%bc%e3%83%aa%e3%82%a8%e8%a7%a3%e6%9e%90\/%e3%83%95%e3%83%bc%e3%83%aa%e3%82%a8%e7%a9%8d%e5%88%86%e3%83%bb%e3%83%95%e3%83%bc%e3%83%aa%e3%82%a8%e5%a4%89%e6%8f%9b\/","title":{"rendered":"\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206\u30fb\u30d5\u30fc\u30ea\u30a8\u5909\u63db"},"content":{"rendered":"<p>\u4efb\u610f\u306e\u5468\u671f \\(2L\\) \u3092\u3082\u3064\u95a2\u6570\u306e\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u7d1a\u6570\u5c55\u958b\u3092\uff0c\u975e\u5468\u671f\u7684\u73fe\u8c61\u306b\u307e\u3067\u62e1\u5f35\u3057\u305f\u3082\u306e\u304c\u300c<span style=\"font-family: helvetica, arial, sans-serif;\"><strong>\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206<\/strong><\/span>\u300d\u3067\u3042\u308a\uff0c\u30d5\u30fc\u30ea\u30a8\u4fc2\u6570\u306e\u62e1\u5f35\u304c\u300c<span style=\"font-family: helvetica, arial, sans-serif;\"><strong>\u30d5\u30fc\u30ea\u30a8\u5909\u63db<\/strong><\/span>\u300d\u3002<br \/>\n<!--more--><\/p>\n<hr \/>\n<h3 id=\"yui_3_17_2_1_1645840462347_1395\">\u4efb\u610f\u306e\u5468\u671f \\(2L\\) \u3092\u6301\u3064\u95a2\u6570\u306e\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u5909\u63db\u306e\u307e\u3068\u3081<\/h3>\n<p>\u533a\u9593 \\( -L \\le x \\le L\\) \u3067\u5b9a\u7fa9\u3055\u308c\u305f\u95a2\u6570 \\(f(x)\\) \u304c\u533a\u9593\u5916\u3067\u306f\u5468\u671f \\(2 L\\) \u306e\u5468\u671f\u95a2\u6570\u3067\u3042\u308b\u5834\u5408\uff0c\u305d\u306e<span style=\"font-family: helvetica, arial, sans-serif;\"><b>\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u7d1a\u6570<\/b><\/span>\u306f<br \/>\n$$f(x) = \\sum_{n = -\\infty}^{\\infty} c_n \\,\\exp\\left({i \\frac{n\\pi x}{L}}\\right)$$ \u3067\u3042\u308a\uff0c\u305d\u306e<span style=\"font-family: helvetica, arial, sans-serif;\"><b>\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u4fc2\u6570<\/b><\/span>\u306f<br \/>\n$$<br \/>\nc_n =\u00a0 \\frac{1}{2L} \\int_{-L}^{L} f(x)\\,\\biggl(\\exp\\left(i\\frac{n\\pi x}{L}\\right)\\biggr)^* \\, dx<br \/>\n$$ \u3068\u66f8\u3051\u308b\u306e\u3067\u3042\u3063\u305f\u3002<\/p>\n<h3>\u5468\u671f\u6027\u3092\u6301\u305f\u306a\u3044\u95a2\u6570\u3078\u306e\u62e1\u5f35\u306e\u305f\u3081\u306e\u6e96\u5099<\/h3>\n<p>\\(c_n\\) \u3092\u3042\u3089\u305f\u3081\u3066\u5143\u306e \\(f(x)\\) \u306e\u5f0f\u306b\u4ee3\u5165\u3057\u3066<\/p>\n<p>\\begin{eqnarray}<br \/>\nf(x) &amp;=&amp; \\sum_{n = -\\infty}^{\\infty} \\left\\{ \\frac{1}{2L}<br \/>\n\\int_{-L}^{L} f(x&#8217;)\\, e^{-i\\frac{n\\pi}{L}x&#8217;} \\, dx&#8217; \\right\\} \\ e^{i \\frac{n\\pi}{L}x}\\\\<br \/>\n&amp;=&amp; \\frac{1}{2L} \\sum_{n = -\\infty}^{\\infty}\\int_{-L}^{L} f(x&#8217;) \\,e^{i \\frac{n\\pi}{L}(x-x&#8217;)}\\ dx&#8217; \\\\<br \/>\n&amp;=&amp; \\frac{1}{2\\pi} \\sum_{n = -\\infty}^{\\infty} \\frac{\\pi}{L} \\int_{-L}^{L} f(x&#8217;) \\,e^{i \\frac{n\\pi}{L}(x-x&#8217;)}\\ dx&#8217;<br \/>\n\\end{eqnarray}<\/p>\n<p>\u3053\u3053\u3067\uff0c<br \/>\n$$ k_n \\equiv \\frac{ n\\pi}{L}, \\quad \\Delta k \\equiv k_{n+1} -k_n = \\frac{\\pi}{L}$$<br \/>\n\u3068\u3059\u308b\u3068\uff0c<br \/>\n$$ f(x) = \\frac{1}{2\\pi} \\sum_{n = -\\infty}^{\\infty} \\Delta k \\int_{-L}^{L} f(x&#8217;) \\,e^{i k_n \\,(x-x&#8217;)}\\ dx&#8217;$$<\/p>\n<h3>\\( L \\rightarrow \\infty\\) \u3068\u3057\u3066\u5468\u671f\u6027\u306e\u306a\u3044\u95a2\u6570\u3078&#8230;<\/h3>\n<p>\\(L \\rightarrow \\infty \\) \u3068\u3059\u308c\u3070\uff0c\u5468\u671f\u304c\u7121\u9650\u5927\uff0c\u3064\u307e\u308a\u5468\u671f\u6027\u306e\u306a\u3044\u95a2\u6570\u3082\u30d5\u30fc\u30ea\u30a8\u7d1a\u6570\u306e\u62e1\u5f35\u3068\u3057\u3066\u3042\u3089\u308f\u3059\u3053\u3068\u304c\u3067\u304d\u308b\u306f\u305a\u3002\u3053\u306e\u6975\u9650\u3067\u96e2\u6563\u7684\u306a \\(k_n\\) \u306f\u9023\u7d9a\u5909\u6570 \\(k\\) \u306b\u306a\u308a\uff0c<br \/>\n$$ {\\color{red}{L \\rightarrow \\infty}} \\ \\ \\Rightarrow \\ \\ {\\color{green}{k_n \\rightarrow k}}, \\ {\\color{blue}{\\Delta k \\rightarrow dk}}, \\ {\\color{blue}{\\sum_{n = -\\infty}^{\\infty} \\Delta k \\rightarrow \\int_{-\\infty}^{\\infty} dk}} $$ \u3068\u3059\u308c\u3070\uff0c\\(L \\rightarrow \\infty \\) \u306e\u6975\u9650\u3067 \\(f(x)\\) \u306f\u4ee5\u4e0b\u306e\u3088\u3046\u306b\u3042\u3089\u308f\u3059\u3053\u3068\u304c\u3067\u304d\u308b\u306f\u3059\u3067\u3042\u308b\u3002<\/p>\n<p>\\begin{eqnarray}<br \/>\nf(x) &amp;=&amp; \\frac{1}{2\\pi} {\\color{blue}{\\sum_{n = -\\infty}^{\\infty} \\Delta k}} \\int_{-{\\color{red}{L}}}^{{\\color{red}{L}}} f(x&#8217;) \\,e^{i {\\color{green}{k_n}} (x-x&#8217;)}\\ dx&#8217;\\\\<br \/>\n&amp;\\Rightarrow&amp; \\frac{1}{2\\pi} {\\color{blue}{\\int_{-\\infty}^{\\infty} dk}} \\int_{-\\color{red}{\\infty}}^{\\color{red}{\\infty}}f(x&#8217;) \\,e^{i {\\color{green}{k}} (x-x&#8217;)}\\ dx&#8217;\\\\<br \/>\n&amp;=&amp; \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} \\ \\int_{-\\infty}^{\\infty} \\ f(x&#8217;) \\ e^{i k \\,(x-x&#8217;)}\\,dx&#8217; \\, dk \\tag{1}<br \/>\n\\end{eqnarray}<\/p>\n<h4>\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206\uff0c\u30d5\u30fc\u30ea\u30a8\u5909\u63db\uff0c\u30d1\u30ef\u30fc\u30b9\u30da\u30af\u30c8\u30eb<\/h4>\n<p>\u4e0a\u3067\u5f97\u3089\u308c\u305f $(1)$ \u5f0f\u3092\u3042\u3089\u305f\u3081\u3066\u4ee5\u4e0b\u306e\u3088\u3046\u306b\u66f8\u304f\uff082\u91cd\u7a4d\u5206\u306f $x&#8217;$ \u3067\u5148\u306b\u7a4d\u5206\u3059\u308b\u3053\u3068\u306b\u3059\u308b\uff09\uff1a<\/p>\n<p>\\begin{eqnarray}<br \/>\nf(x) &amp;=&amp; \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} \\ \\int_{-\\infty}^{\\infty} \\ f(x&#8217;) \\ e^{i k \\,(x-x&#8217;)}\\,dx&#8217; \\, dk \\\\<br \/>\n&amp;=&amp; \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} \\left\\{ \\int_{-\\infty}^{\\infty} \\ f(x&#8217;) \\ e^{-i k x&#8217;}\\,dx&#8217;\\right\\} \\, e^{i k x}\\, dk\\\\<br \/>\n&amp;\\equiv&amp;\u00a0 \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} \\ F(k)\\ e^{i k x} dk<br \/>\n\\end{eqnarray}<\/p>\n<p>\u3053\u308c\u3092\uff08\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u7d1a\u6570\u306e\u5468\u671f\u7121\u9650\u5927\u6975\u9650\u3068\u3057\u3066\uff0c\u5468\u671f\u6027\u306e\u306a\u3044\uff09\u95a2\u6570 $f(x)$ \u306e<span style=\"font-family: helvetica, arial, sans-serif;\"><strong>\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206<\/strong><\/span>\u3068\u547c\u3076\u3002\u307e\u305f\uff0c<\/p>\n<p>$$ F(k) \\equiv \\int_{-\\infty}^{\\infty}\u00a0 \\ f(x&#8217;) \\ e^{-i k x&#8217;} \\,dx&#8217;$$ \u3067\u5b9a\u7fa9\u3055\u308c\u308b \\(F(k)\\) \u3092\uff08\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u4fc2\u6570\u306e\u5468\u671f\u7121\u9650\u5927\u6975\u9650\u3068\u3057\u3066\uff0c\u5468\u671f\u6027\u306e\u306a\u3044\uff09\u95a2\u6570 $f(x)$ \u306e<span style=\"font-family: helvetica, arial, sans-serif;\"><b>\u30d5\u30fc\u30ea\u30a8\u5909\u63db<\/b><\/span>\u3068\u547c\u3076\u3002<\/p>\n<p>\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206\u306e\u5f62\u3092\u3064\u3089\u3064\u3089\u3068\u773a\u3081\u308b\u3068\uff0c$f(x)$ \u306e\u4e2d\u306b\u3042\u308b\u300c\u6ce2\u300d\u306e\u6210\u5206 $e^{i k x}$ \u306e\u632f\u5e45\u3092\u8868\u3059\u306e\u304c $F(k)$ \u3067\u3042\u308b\u3053\u3068\u304c\u308f\u304b\u308b\u3002\u632f\u5e45\u306e\uff08\u7d76\u5bfe\u5024\u306e\uff09\u4e8c\u4e57\u306f\u300c\u6ce2\u300d\u306e\u5f37\u5ea6\u3092\u3042\u3089\u308f\u3059\u304b\u3089\uff0c<\/p>\n<p>$$ S(k) \\equiv |F(k)|^2 = F(k)\\,\\left\\{F(k)\\right\\}^{*}$$<\/p>\n<p>\u3068\u3057\u3066\uff0c$S(k)$ \u3092 $f(x)$ \u306e<span style=\"font-family: helvetica, arial, sans-serif;\"><strong>\u30d1\u30ef\u30fc\u30b9\u30da\u30af\u30c8\u30eb<\/strong><\/span>\u3068\u547c\u3093\u3067\u3044\u308b\u3002\uff08$\\left\\{F(k)\\right\\}^{*}$ \u306f $F(k)$ \u306e\u8907\u7d20\u5171\u5f79\u3002\uff09<\/p>\n<h3>\u30d5\u30fc\u30ea\u30a8\u7d1a\u6570\u3068\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206\u3092\u4e26\u3079\u3066\u6bd4\u8f03<\/h3>\n<p>\u6bd4\u8f03\u306e\u305f\u3081\u306b\uff0c\u4e26\u3079\u3066\u307f\u308b\u3002\u304b\u305f\u3084\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u4fc2\u6570\u306b $\\dfrac{1}{2L}$ \u304c\u3064\u304d\uff0c\u304b\u305f\u3084\u30d5\u30fc\u30ea\u30a8\u5909\u63db\u3067\u306f\u306a\u304f\u3066\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206\u306e\u307b\u3046\u306b $\\dfrac{1}{2\\pi}$ \u304c\u3064\u3044\u3066\u3044\u3066\uff0c\u5bfe\u5fdc\u304c\u30a4\u30de\u30a4\u30c1\u304b\u3082\u3057\u308c\u307e\u305b\u3093\u304c\uff0c\u3054\u5bb9\u8d66\u3002<\/p>\n<h4>\u5468\u671f \\(2L\\) \u306e\u5468\u671f\u95a2\u6570\u306b\u5bfe\u3059\u308b\uff08\u96e2\u6563\u7684\u306a\uff09\u30d5\u30fc\u30ea\u30a8\u7d1a\u6570\u5c55\u958b<\/h4>\n<p>\\( k_n \\equiv \\frac{n\\pi}{L} \\) \u3068\u3057\u3066<\/p>\n<p>$${\\color{blue}{ f(x) = \\sum_{n = -\\infty}^{\\infty} c_n \\ e^{i k_n x}}}, \\quad {\\color{red}{c_n = \\frac{1}{2L} \\int_{-L}^{L} f(x) \\ e^{- i k_n x}\\ dx }}$$<\/p>\n<h4>\u5468\u671f\u6027\u306e\u306a\u3044\u95a2\u6570\u306b\u5bfe\u3059\u308b\uff08\u9023\u7d9a\u6975\u9650\u3068\u3057\u3066\u306e\uff09\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206<\/h4>\n<p>$$ {\\color{blue}{f(x) = \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty}\\ F(k)\\ e^{i k x}\\ dk}}, \\quad\u00a0 {\\color{red}{F(k) \\equiv \\int_{-\\infty}^{\\infty} f(x) \\ e^{-i k x} \\ dx }}$$<\/p>\n<h3>\u95a2\u6570 \\(\\exp\\left(i\\frac{n\\pi x}{L}\\right) \\) \u306e\u76f4\u4ea4\u6027\u306e\u9023\u7d9a\u6975\u9650\uff1a\u30c7\u30a3\u30e9\u30c3\u30af\u306e\u30c7\u30eb\u30bf\u95a2\u6570<\/h3>\n<p>\u5468\u671f\u95a2\u6570\u306b\u5bfe\u3059\u308b\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u7d1a\u6570\u306b\u95a2\u3059\u308b\u96e2\u6563\u7684\u95a2\u6570\\(\\exp\\left(i\\dfrac{n\\pi x}{L}\\right) \\) \u306e\u76f4\u4ea4\u6027\u306f\uff0c<br \/>\n\\begin{eqnarray}<br \/>\n\\int_{-L}^L\\exp\\left(i\\frac{(n-n&#8217;)\\pi}{L}x\\right)\\,dx<br \/>\n&amp;=&amp; \\begin{cases}<br \/>\n2L &amp; (n = n&#8217;) \\\\<br \/>\n0\u00a0 &amp; (n \\neq n&#8217;)<br \/>\n\\end{cases} \\\\ &amp;=&amp; 2L \\,\\delta_{n n&#8217;}<br \/>\n\\end{eqnarray}<br \/>\n\u3067\u3042\u3063\u305f\u3002<br \/>\n$$ k_n \\equiv \\frac{n\\pi}{L}, \\ \\quad k_{n&#8217;} \\equiv \\frac{n&#8217; \\pi}{L}, \\quad \\Delta k = k_{n+1} -k_n = \\frac{\\pi}{L} $$ \u3068\u3057\u3066\u66f8\u304d\u76f4\u3059\u3068<br \/>\n\\begin{eqnarray}<br \/>\n\\int_{-L}^L e^{i(k_n -k_{n&#8217;}) x}\\ dx &amp;=&amp; 2L \\,\\delta_{n\u00a0 n&#8217;}\\\\<br \/>\n&amp;=&amp; 2\\pi \\frac{\\delta_{n\u00a0 n&#8217;}}{ \\frac{\\pi}{L} }<br \/>\n\\end{eqnarray}<\/p>\n<p>$$\\therefore\\ \\frac{1}{2\\pi} \\int_{-L}^L e^{i(k_n -k_{n&#8217;}) x}\\ dx = \\frac{\\delta_{n\u00a0 n&#8217;}}{ \\Delta k }$$<\/p>\n<p>\\(L \\rightarrow \\infty \\) \u306e\u3068\u304d\uff0c\u96e2\u6563\u7684\u306a \\(k_n\\) \u3082\u9023\u7d9a\u7684\u306a \\(k\\) \u306b\u306a\u308b\u306e\u3067 \\(k_n \\rightarrow k, \\ k_{n&#8217;} \\rightarrow k&#8217;\\) \u3068\u3057\uff0c\u3053\u306e\u7a4d\u5206\u3092\u4ee5\u4e0b\u306e\u3088\u3046\u306b<br \/>\n$$\\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} e^{i (k -k&#8217;) x}\\ dx \\equiv \\delta(k -k&#8217;) \\tag{2}$$ \u3068\u3057\u3066\uff0c<span style=\"font-family: helvetica, arial, sans-serif;\"><b>\u30c7\u30a3\u30e9\u30c3\u30af\u306e\u30c7\u30eb\u30bf\u95a2\u6570 \\(\\delta(k -k&#8217;)\\) <\/b><\/span>\u3092\u5b9a\u7fa9\u3059\u308b\u3002<\/p>\n<p id=\"yui_3_17_2_1_1645840462347_1404\">\u3053\u306e\u30c7\u30a3\u30e9\u30c3\u30af\u306e\u30c7\u30eb\u30bf\u95a2\u6570 \\(\\delta(k -k&#8217;)\\) \u306f\uff0c\u30af\u30ed\u30cd\u30c3\u30ab\u30fc\u306e\u30c7\u30eb\u30bf \\(\\delta_{n n&#8217;}\\) \u3092 \\(\\Delta k = \\frac{\\pi}{L}\\) \u3067\u5272\u3063\u305f\u91cf\u306e \\(L \\rightarrow \\infty\\) \u6975\u9650\u3067\u5b9a\u7fa9\u3055\u308c\u305f\u95a2\u6570<br \/>\n$$<br \/>\n\\delta(k -k&#8217;) \\equiv \\lim_{L \\rightarrow \\infty} \\frac{\\delta_{n\u00a0 n&#8217;}}{\\Delta k},\\\u00a0 \\quad k \\equiv \\frac{n\\pi}{L}, \\ \\ k&#8217; \\equiv \\frac{n&#8217; \\pi}{L}<br \/>\n$$\u3067\u3042\u308b\u305f\u3081\uff0c\\( k \\neq k&#8217;\\) \u306e\u3068\u304d\u306f \\(\\delta(k -k&#8217;) = 0\\) \u3067\u3042\u308b\u3053\u3068\u306f\u306a\u3093\u3068\u304b\u308f\u304b\u308b\u306b\u3057\u3066\u3082\uff0c\\( k = k&#8217;\\) \u306e\u3068\u304d\u306f\uff0c \\(L \\rightarrow 0\\) \u3067\u5206\u6bcd\u304c\\(\\Delta k \\rightarrow 0\\) \u3068\u306a\u3063\u3066\u3057\u307e\u3046\u305f\u3081\uff0c\\( \\delta(0) \\rightarrow \\infty !?\\) \u3068\u306a\u3063\u3066\u3057\u307e\u3046\u3088\u3046\u3067\u3042\u308a\uff0c\u3068\u3066\u3082\u666e\u901a\u306e\u95a2\u6570\u3068\u306f\u601d\u3048\u306a\u3044\u306e\u3067\uff0c\u300c\u8d85\u95a2\u6570\u300d\u3068\u547c\u3070\u308c\u308b\u3082\u306e\u306e1\u3064\u3067\u3042\u308b\u3002<\/p>\n<p>\u3053\u306e\u30c7\u30eb\u30bf\u95a2\u6570\u3092\u4f7f\u3063\u3066\u3042\u3089\u305f\u3081\u3066\u30d5\u30fc\u30ea\u30a8\u5909\u63db $F(k^{\\prime})$ \u3092\u66f8\u304f\u3068<\/p>\n<p>\\begin{eqnarray}<br \/>\nF(k^{\\prime}) &amp;=&amp; \\int_{-\\infty}^{\\infty} \\, f(x) \\,e^{-i k^{\\prime} x} \\,dx\\\\<br \/>\n&amp;=&amp; \\int_{-\\infty}^{\\infty} \\left\\{ \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} \\, F(k)\\, e^{i k x} \\,dk \\right\\} \\,e^{-i k^{\\prime} x}\\,dx\\\\<br \/>\n&amp;=&amp; \\frac{1}{2\\pi}\\int_{-\\infty}^{\\infty} \\int_{-\\infty}^{\\infty} \\, F(k)\\, e^{i (k-k^{\\prime}) x} \\,dx \\,dk\\\\<br \/>\n&amp;=&amp; \\int_{-\\infty}^{\\infty} \\, F(k) \\left\\{\\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} \\, e^{i (k-k^{\\prime}) x} \\,dx\\right\\}\\,dk \\\\<br \/>\n&amp;=&amp; \\int_{-\\infty}^{\\infty} \\, F(k)\\, \\delta(k -k^{\\prime}) \\,dk<br \/>\n\\end{eqnarray}<\/p>\n<p>\u3053\u306e\u6027\u8cea\u306f\uff0c\u96fb\u78c1\u6c17\u5b66\u3067\u3082\u51fa\u3066\u304d\u3066\u307e\u3057\u305f\u3002$k$\u00a0 \u3067\u306e\u7a4d\u5206\u306e\u969b\uff0c\u30c7\u30eb\u30bf\u95a2\u6570\u306e\u5f15\u6570 $k-k^{\\prime}$ \u304c\u30bc\u30ed\u306e\u6642\u306e\u5024\u3060\u3051\uff08\u3059\u306a\u308f\u3061 $k = k^{\\prime}$ \u306e\u3068\u304d\u306e $F(k^{\\prime})$ \u3060\u3051\uff09\u304c\u6b8b\u308a\u307e\u3059\u3002<\/p>\n<ul>\n<li>\u53c2\u8003\uff1a<a href=\"https:\/\/home.hirosaki-u.ac.jp\/relativity\/%e9%9b%bb%e7%a3%81%e6%b0%97%e5%ad%a6-i\/%e9%9d%99%e9%9b%bb%e5%a0%b4%ef%bc%9a%e7%82%b9%e9%9b%bb%e8%8d%b7%e3%81%ae%e9%9b%bb%e8%8d%b7%e5%af%86%e5%ba%a6%e3%81%a8%e3%83%87%e3%82%a3%e3%83%a9%e3%83%83%e3%82%af%e3%81%ae%e3%83%87%e3%83%ab%e3%82%bf\/#1\" target=\"_blank\" rel=\"noopener\">\u9759\u96fb\u5834\uff1a\u70b9\u96fb\u8377\u306e\u96fb\u8377\u5bc6\u5ea6\u3068\u30c7\u30a3\u30e9\u30c3\u30af\u306e\u30c7\u30eb\u30bf\u95a2\u6570<\/a><\/li>\n<\/ul>\n<p>\u307e\u305f\uff0c$(1)$ \u5f0f\u306e2\u91cd\u7a4d\u5206\u3092\u5148\u306b $k$ \u3067\u7a4d\u5206\u3059\u308b\u3053\u3068\u306b\u3059\u308c\u3070\uff0c<\/p>\n<p>\\begin{eqnarray}<br \/>\nf(x) &amp;=&amp; \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty}\u00a0 \\int_{-\\infty}^{\\infty} \\ f(x&#8217;) \\ e^{i k \\,(x-x&#8217;)}\\,dx&#8217; \\, dk \\\\<br \/>\n&amp;=&amp; \\int_{-\\infty}^{\\infty} \\, f(x&#8217;) \\left\\{\\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty}\u00a0 \\ \\ e^{i k \\,(x-x&#8217;)}\\,dk\\right\\} \\, dx&#8217;\\\\<br \/>\n&amp;=&amp; \\int_{-\\infty}^{\\infty} \\, f(x&#8217;)\\, \\delta(x -x&#8217;)\\, dx<br \/>\n\\end{eqnarray}<\/p>\n<p>\u3068\u306a\u308a\uff0c\u30c7\u30eb\u30bf\u95a2\u6570 $\\delta(x-x&#8217;)$ \u306e\u5f15\u6570 $x -x&#8217;$ \u304c\u30bc\u30ed\u306e\u3068\u304d\u306e\u5024\u3060\u3051\uff08\u3059\u306a\u308f\u3061 $x&#8217; = x$ \u306e\u3068\u304d\u306e $f(x)$ \u3060\u3051\uff09\u304c\u6b8b\u308a\u307e\u3059\u3002\u306a\u304a\uff0c\u8a00\u308f\u305a\u3082\u304c\u306a\u3067\u306f\u3042\u308a\u307e\u3059\u304c\uff0c$(2)$ \u5f0f\u3067\u5b9a\u7fa9\u3055\u308c\u305f\u30c7\u30eb\u30bf\u95a2\u6570<\/p>\n<p>$$\\delta(k -k&#8217;) \\equiv \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} e^{i (k -k&#8217;) x}\\ dx$$<\/p>\n<p>\u306f\uff0c\u5909\u6570\u3092 $(k -k&#8217;) \\rightarrow (x -x&#8217;), \\ x \\rightarrow k$ \u3068\u7f6e\u304d\u63db\u3048\u308c\u3070\u4ee5\u4e0b\u306e\u3088\u3046\u306b\u306a\u308b\u3053\u3068\u3092\u4f7f\u3063\u3066\u307e\u3059\u3088\u3002<\/p>\n<p>$$\\delta(x -x&#8217;) \\equiv \\frac{1}{2\\pi} \\int_{-\\infty}^{\\infty} e^{i (x -x&#8217;) k}\\ dk$$<\/p>\n<h4>\u30c7\u30eb\u30bf\u95a2\u6570\u306e\u4e00\u822c\u7684\u6027\u8cea<\/h4>\n<p>\u3042\u3089\u305f\u3081\u3066\u30c7\u30a3\u30e9\u30c3\u30af\u306e\u30c7\u30eb\u30bf\u95a2\u6570\u306e\u6027\u8cea\u3092\u307e\u3068\u3081\u3066\u304a\u304d\u307e\u3059\u3002\uff08$x$ \u306e\u95a2\u6570\u3068\u3057\u3066\u66f8\u304d\u76f4\u3059\u3002\uff09<\/p>\n<p>\u30c7\u30eb\u30bf\u95a2\u6570\u306f\u4ee5\u4e0b\u306e\u3088\u3046\u306b\u3057\u3066\u5b9a\u7fa9\u3059\u308b\u3002<\/p>\n<p>$$\\delta(x) = 0\\ \\\u00a0 \\mbox{for}\\ \\ x \\neq 0, \\quad \\int_{-\\infty}^{\\infty} f(x) \\delta(x-a) \\, dx = f(a) \\tag{3}$$<\/p>\n<p>\u7279\u306b $f(x) = 1, a = 0$ \u3068\u3059\u308c\u3070<\/p>\n<p>$$\\int_{-\\infty}^{\\infty}\u00a0 \\delta(x) \\, dx = 1$$<\/p>\n<p>\u3053\u306e\u5b9a\u7fa9\u304b\u3089\uff0c\u30c7\u30eb\u30bf\u95a2\u6570\u306b\u306f\u4ee5\u4e0b\u306e\u3088\u3046\u306a\u6027\u8cea\u304c\u3042\u308b\u3053\u3068\u304c\u308f\u304b\u308a\u307e\u3059\u3002\u3053\u308c\u3089\u306e\u6027\u8cea\u306f\u5168\u3066\u30c7\u30eb\u30bf\u95a2\u6570\u306e\u5b9a\u7fa9\u5f0f $(3)$ \u304b\u3089\u5c0e\u304f\u3053\u3068\u304c\u3067\u304d\u308b\u3002<\/p>\n<p>$\\quad\\displaystyle \\delta(-x) = \\delta(x)$ \u3059\u306a\u308f\u3061 $\\delta(x)$ \u306f\u5076\u95a2\u6570\u3002<\/p>\n<p>$\\quad\\displaystyle x \\delta(x) = 0$\u3002 \u3042\u308b\u3044\u306f\uff0c\u3088\u308a\u4e00\u822c\u7684\u306b $\\displaystyle f(x) \\delta(x-a) = f(a) \\delta(x-a)$<\/p>\n<p>$\\quad\\displaystyle \\delta(a x) = \\frac{1}{|a|} \\delta(x)$<\/p>\n<p>\u307e\u305f\uff0c\u95a2\u6570 $f(x)$ \u306e\u30d5\u30fc\u30ea\u30a8\u5909\u63db\u306e\u5f0f<\/p>\n<p>$$F(k) = \\int_{-\\infty}^{\\infty} \\ f(x) \\,e^{- i k x}\\, dx$$<\/p>\n<p>\u3092\u4f7f\u3063\u3066\uff0c\u30c7\u30eb\u30bf\u95a2\u6570 $\\delta(x)$ \u306e\u30d5\u30fc\u30ea\u30a8\u5909\u63db\u3092\u6c42\u3081\u308b\u3068\uff0c\uff08$f(x) \\rightarrow \\delta(x)$ \u306e\u7f6e\u304d\u63db\u3048\u3092\u3059\u308c\u3070\u3044\u3044\u3060\u3051\u3060\u304b\u3089\uff09<\/p>\n<p>\\begin{eqnarray}<br \/>\nF(k) &amp;=&amp; \\int_{-\\infty}^{\\infty} \\ \\delta(x) \\,e^{- i k x}\\, dx \\\\<br \/>\n&amp;=&amp; e^{- i k \\cdot 0} \\\\ &amp;=&amp; 1<br \/>\n\\end{eqnarray}<\/p>\n<p>\u3068\u3044\u3046\u3053\u3068\u306f\uff0c\u30c7\u30eb\u30bf\u95a2\u6570 $\\delta(x)$ \u306e\u30d5\u30fc\u30ea\u30a8\u5909\u63db\u306f $1$ \u3067\u3042\u308b\u3053\u3068\u3092\u793a\u3057\u3066\u3044\u308b\u3002\u3053\u306e\u3053\u3068\u306f\u307e\u305f\uff0c\u30d5\u30fc\u30ea\u30a8\u5909\u63db $F(k)$ \u3092\u4f7f\u3063\u3066\u66f8\u3044\u305f\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206\u306e\u5f0f<\/p>\n<p>$$f(x) = \\frac{1}{2 \\pi} \\int_{-\\infty}^{\\infty} \\ F(k) \\, e^{i k x} \\, dk$$<\/p>\n<p>\u306e\u5f0f\u3068\u30c7\u30eb\u30bf\u95a2\u6570 $\\delta(x)$ \u306e\u5b9a\u7fa9\u5f0f<\/p>\n<p>$$\\delta(x) = \\frac{1}{2 \\pi} \\int_{-\\infty}^{\\infty} \\ e^{i k x} \\, dk$$<\/p>\n<p>\u306e\u4e21\u8fba\u3092\u898b\u6bd4\u3079\u3066\u307f\u3066\u3082\uff0c\u30c7\u30eb\u30bf\u95a2\u6570 $\\delta(x)$ \u306e\u30d5\u30fc\u30ea\u30a8\u5909\u63db\u306f $F(k) = 1$ \u3068\u306a\u308b\u3053\u3068\u306f\u660e\u3089\u304b\u3067\u3042\u308d\u3046\u3002<\/p>\n<p>\u307e\u305f\uff0c\u6388\u696d\u3067\u306f\u4f7f\u3046\u6a5f\u4f1a\u304c\u306a\u3044\u304b\u3068\u601d\u3046\u304c\uff0c\u30c7\u30eb\u30bf\u95a2\u6570\u306e\u5fae\u5206\u306b\u3064\u3044\u3066\u3082\u4ee5\u4e0b\u306e\u5f0f\u304c\u6210\u308a\u7acb\u3064\u3053\u3068\u3092\u90e8\u5206\u7a4d\u5206\u3067\u793a\u3059\u3053\u3068\u304c\u3067\u304d\u308b\u3002<\/p>\n<p>$$f(x) \\left(\\frac{d}{dx} \\delta(x)\\right) = -\\left(\\frac{d}{dx} f(x)\\right) \\delta(x)$$ \u3042\u308b\u3044\u306f\u7c21\u5358\u306b<\/p>\n<p>$$ f(x) \\delta^{\\prime}(x) = -f^{\\prime}(x) \\delta(x)$$<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>\u4efb\u610f\u306e\u5468\u671f \\(2L\\) \u3092\u3082\u3064\u95a2\u6570\u306e\u8907\u7d20\u30d5\u30fc\u30ea\u30a8\u7d1a\u6570\u5c55\u958b\u3092\uff0c\u975e\u5468\u671f\u7684\u73fe\u8c61\u306b\u307e\u3067\u62e1\u5f35\u3057\u305f\u3082\u306e\u304c\u300c\u30d5\u30fc\u30ea\u30a8\u7a4d\u5206\u300d\u3067\u3042\u308a\uff0c\u30d5\u30fc\u30ea\u30a8\u4fc2\u6570\u306e\u62e1\u5f35\u304c\u300c\u30d5\u30fc\u30ea\u30a8\u5909\u63db\u300d\u3002<\/p><p><a class=\"more-link btn\" href=\"https:\/\/home.hirosaki-u.ac.jp\/relativity\/%e7%90%86%e5%b7%a5%e7%b3%bb%e3%81%ae%e6%95%b0%e5%ad%a6c\/%e3%83%95%e3%83%bc%e3%83%aa%e3%82%a8%e8%a7%a3%e6%9e%90\/%e3%83%95%e3%83%bc%e3%83%aa%e3%82%a8%e7%a9%8d%e5%88%86%e3%83%bb%e3%83%95%e3%83%bc%e3%83%aa%e3%82%a8%e5%a4%89%e6%8f%9b\/\">\u7d9a\u304d\u3092\u8aad\u3080<\/a><\/p>\n","protected":false},"author":33,"featured_media":0,"parent":2230,"menu_order":4,"comment_status":"closed","ping_status":"closed","template":"","meta":{"inline_featured_image":false,"footnotes":""},"class_list":["post-2370","page","type-page","status-publish","hentry","nodate","item-wrap"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages\/2370","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/users\/33"}],"replies":[{"embeddable":true,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/comments?post=2370"}],"version-history":[{"count":19,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages\/2370\/revisions"}],"predecessor-version":[{"id":10591,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages\/2370\/revisions\/10591"}],"up":[{"embeddable":true,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages\/2230"}],"wp:attachment":[{"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/media?parent=2370"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}