\u95f2\u7740\u86cb\u75bc\uff0c\u56de\u5fc6\u4e0bLatex\u91cc\u7684\u516c\u793a\u7f16\u8f91\uff0c\u968f\u4fbf\u627e\u4e86\u4e2a\u63a8\u5bfc\u8fdb\u884c\u6392\u7248\u3002<\/p>\n
\u5229\u7528\u4e00\u7ef4\u5e73\u9762\u7b80\u8c10\u6ce2\u7684\u6ce2\u52a8\u65b9\u7a0b\uff0c\u5bf9\u5176\u8fdb\u884c\u91cf\u5b50\u5316\uff0c\u5f97\u51fa\u4e00\u7ef4\u5b9a\u6001\u859b\u5b9a\u8c14\u65b9\u7a0b\u3002\u63a8\u5bfc\u7834\u7efd\u8f83\u591a\uff0c\u660e\u773c\u4eba\u4e00\u773c\u5c31\u80fd\u770b\u51fa\u5176\u4e2d\u7684\u95ee\u9898\uff0c\u53ea\u662f\u505a\u4e2a\u8fd1\u4f3c\u5904\u7406\uff0c\u66f4\u591a\u7684\u662f\u8054\u7cfblatex\u4e86\u3002<\/p>\n
\u7ecf\u5178\u7684\u6ce2\u52a8\u65b9\u7a0b\u5982\u4e0b\uff1a<\/p>\n
$$\\frac{\\partial^2 V(x)}{\\partial x^2}+\\left( \\frac{\\omega^2}{v^2_p}\\right) V(x)=0 $$<\/p>\n
\u4ee4$$\\psi(x)=V(x)$$\uff0c\u5f97\u5230\uff082\uff09\u5f0f\uff1a<\/p>\n
$$\\frac{\\partial^2 \\psi(x)}{\\partial x^2}+\\left( \\frac{\\omega^2}{v^2_p}\\right) \\psi(x)=0 $$<\/p>\n
\u53c8\uff1a<\/p>\n
$$ \\frac{\\omega^2}{v^2_p}=\\left( \\frac{2\\pi v}{v_p}\\right)^2=\\left( \\frac{2\\pi}{\\lambda}\\right) ^2$$<\/p>\n
\u7531\u6ce2\u7c92\u4e8c\u8c61\u6027$$\\lambda=\\frac{h}{p}$$\u5f97\uff1a<\/p>\n
$$\\left( \\frac{2\\pi}{\\lambda}\\right) ^2=\\left( \\frac{2\\pi}{h}\\cdot p\\right) ^2=\\left( \\frac{p}{\\hbar}\\right) ^2=\\frac{2m}{\\hbar^2}\\left( \\frac{p^2}{2m}\\right)$$<\/p>\n
\u4e14$$\\frac{p^2}{2m}=T=E-V$$\uff0c\u5219\uff1a<\/p>\n
$$\\frac{\\omega^2}{v^2_p}=\\frac{2m}{\\hbar^2}\\left( \\frac{p^2}{2m}\\right)=\\frac{2m}{\\hbar^2} \\left( E-V\\right)$$<\/p>\n
\u4e0a\u5f0f\u4ee3\u56de\uff082\uff09\u5f0f\uff1a<\/p>\n
$$\\frac{\\partial^2\\psi(x)}{\\partial x^2}+\\frac{2m}{\\hbar}\\left( E-V\\right) \\psi(x)=0$$<\/p>\n","protected":false},"excerpt":{"rendered":"
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