import{_ as e}from"./chunks/PageInfo.vue_vue_type_script_setup_true_lang.250b3e56.js";import{_ as m,C as i,o as p,c as r,H as l,k as s,a,Q as c}from"./chunks/framework.b7580407.js";import"./chunks/commonjsHelpers.725317a4.js";const ss=JSON.parse('{"title":"Formulas for IPhO 日本語版: Section 7","description":"","frontmatter":{},"headers":[],"relativePath":"academic/physics/ipho-formulas-jpn/7.md","filePath":"academic/physics/ipho-formulas-jpn/7.md","lastUpdated":1706850107000}'),h={name:"academic/physics/ipho-formulas-jpn/7.md"},o=s("h1",{id:"formulas-for-ipho-日本語版-section-7",tabindex:"-1"},[a("Formulas for IPhO 日本語版: Section 7 "),s("a",{class:"header-anchor",href:"#formulas-for-ipho-日本語版-section-7","aria-label":'Permalink to "Formulas for IPhO 日本語版: Section 7"'},"")],-1),g=c('7: 波動光学
7.1: Huygens の原理に基づいた回折
- Huygens の原理に基づいた回折 : 障害物が波面を切断 すると波面は小さな断片に分割され，それが仮想的な 点波源となり，観測点での波の振幅はこれらの波源か らの寄与の重ね合わせとなる.
7.2: 二重スリット
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