deploy: 3a21ce3

cn/gallery/GRIN-slab.html

@@ -43,7 +43,7 @@
 <center>
 <h1><b><span>渐变折射率平板</span></b></h1>
 <p>
-贡献者：Stas Fainer
+贡献者：Stas Fainer, Yi-Ting Tu
 </p>
 <div class="description">
 <p>模拟折射率 \(n(\rho) = n_0 \sqrt{1-(\alpha \rho)^2}\)的介电材料，其中 \(n_0\) 是其中央轴的折射率，\(\rho \) 是从其中央轴的径向距离，使得 \(\alpha=\frac{\sqrt{3}}{2R} \)，其中 \(R=100 \) 是其半径。上方的介电材料为一系列的薄矩形，每个矩形具有恒定的折射率（根据前述 \(n(\rho)\) 的式子）。下方的介电材料是折射率为\(n(\rho)\)的渐变折射率材料。 </p>

cn/gallery/GRIN-slab.json

@@ -194,6 +194,5 @@
     "y": 483.9899180908078
   },
   "scale": 1,
-  "name": "{{GRIN-slab}}",
-  "title": "渐变折射率平板"
+  "name": "渐变折射率平板"
 }

cn/gallery/NL-simulation.json

@@ -430,6 +430,5 @@
     "y": 877.8549990900746
   },
   "scale": 1,
-  "name": "{{NL-simulation}}",
-  "title": "NL 双筒望远镜"
+  "name": "NL 双筒望远镜"
 }

cn/gallery/aplanatic-points.json

@@ -299,6 +299,5 @@
     "y": 1523.6425564126162
   },
   "scale": 1,
-  "name": "{{aplanatic-points}}",
-  "title": "等光程点"
+  "name": "等光程点"
 }

cn/gallery/apparent-depth.json

@@ -87,6 +87,5 @@
     "y": 71.9
   },
   "scale": 1,
-  "name": "{{apparent-depth}}",
-  "title": "视深度"
+  "name": "视深度"
 }

cn/gallery/beam-directors.json

@@ -160,6 +160,5 @@
     "y": 215.4517791218074
   },
   "scale": 1,
-  "name": "{{beam-directors}}",
-  "title": "光束导向器"
+  "name": "光束导向器"
 }

cn/gallery/beam-expanders.json

@@ -1,6 +1,6 @@
 {
   "version": 5,
-  "name": "{{beam-expanders}}",
+  "name": "扩束镜",
   "objs": [
     {
       "type": "IdealLens",
@@ -144,6 +144,5 @@
     "x": -94.58646616541341,
     "y": -99.65563909774437
   },
-  "scale": 1,
-  "title": "扩束镜"
+  "scale": 1
 }

cn/gallery/bended-pencil.json

@@ -149,7 +149,6 @@
     "y": 405.97089028460323
   },
   "scale": 1,
-  "name": "{{bended-pencil}}",
-  "backgroundImage": "bended-pencil-background.png",
-  "title": "弯曲的铅笔"
+  "name": "弯曲的铅笔",
+  "backgroundImage": "bended-pencil-background.png"
 }

cn/gallery/black-cat-becomes-white.json

@@ -705,7 +705,6 @@
     "y": 1210.1784161490682
   },
   "scale": 1,
-  "name": "{{black-cat-becomes-white}}",
-  "backgroundImage": "black-cat-becomes-white-background.png",
-  "title": "「黑猫变白猫」演示"
+  "name": "「黑猫变白猫」演示",
+  "backgroundImage": "black-cat-becomes-white-background.png"
 }

cn/gallery/branched-flow.json

@@ -71,6 +71,5 @@
     "y": -103.60224591966603
   },
   "scale": 1,
-  "name": "{{branched-flow}}",
-  "title": "分支流"
+  "name": "分支流"
 }

cn/gallery/broken-pencil.json

@@ -165,7 +165,6 @@
     "y": 387.6012114382306
   },
   "scale": 1,
-  "name": "{{broken-pencil}}",
-  "backgroundImage": "broken-pencil-background.png",
-  "title": "断裂的铅笔"
+  "name": "断裂的铅笔",
+  "backgroundImage": "broken-pencil-background.png"
 }

cn/gallery/camera-obscura.json

@@ -167,6 +167,5 @@
     "y": -8.005754960553588
   },
   "scale": 1,
-  "name": "{{camera-obscura}}",
-  "title": "暗箱"
+  "name": "暗箱"
 }

cn/gallery/caustics-from-a-reflective-sphere.json

@@ -94,6 +94,5 @@
   },
   "scale": 1,
   "simulateColors": true,
-  "name": "{{caustics-from-a-reflective-sphere}}",
-  "title": "反射性球体的焦散"
+  "name": "反射性球体的焦散"
 }

cn/gallery/chaff-countermeasure.html

@@ -43,7 +43,7 @@
 <center>
 <h1><b><span>干扰箔</span></b></h1>
 <p>
-贡献者：Stas Fainer
+贡献者：Stas Fainer, Yi-Ting Tu
 </p>
 <div class="description">
 <p>这是一个箔片反射对雷达效应的定性模拟（忽略衍射效应）。</p>

cn/gallery/chaff-countermeasure.json

@@ -302,6 +302,5 @@
     "y": 599.352086802087
   },
   "scale": 1,
-  "name": "{{chaff-countermeasure}}",
-  "title": "干扰箔"
+  "name": "干扰箔"
 }

cn/gallery/chromatic-aberration.json

@@ -554,6 +554,5 @@
   },
   "scale": 1,
   "simulateColors": true,
-  "name": "{{chromatic-aberration}}",
-  "title": "色像差"
+  "name": "色像差"
 }

cn/gallery/chromatic-dispersion.json

@@ -360,6 +360,5 @@
   },
   "scale": 1,
   "simulateColors": true,
-  "name": "{{chromatic-dispersion}}",
-  "title": "色散"
+  "name": "色散"
 }

cn/gallery/compound-microscope.json

@@ -93,6 +93,5 @@
     "y": 79.87890987581412
   },
   "scale": 1,
-  "name": "{{compound-microscope}}",
-  "title": "复式显微镜"
+  "name": "复式显微镜"
 }

cn/gallery/concave-lens.json

@@ -80,6 +80,5 @@
     "y": 658.5192683356722
   },
   "scale": 1,
-  "name": "{{concave-lens}}",
-  "title": "凹透镜"
+  "name": "凹透镜"
 }

cn/gallery/concave-mirror-wearable-display.json

@@ -270,6 +270,5 @@
   },
   "scale": 1,
   "simulateColors": true,
-  "name": "{{concave-mirror-wearable-display}}",
-  "title": "凹面镜可穿戴显示器"
+  "name": "凹面镜可穿戴显示器"
 }

cn/gallery/convex-lens.json

@@ -1,6 +1,6 @@
 {
   "version": 5,
-  "name": "{{convex-lens}}",
+  "name": "凸透镜",
   "objs": [
     {
       "type": "SphericalLens",
@@ -79,6 +79,5 @@
     "x": 1234.3602113369022,
     "y": 587.2073615756722
   },
-  "scale": 1,
-  "title": "凸透镜"
+  "scale": 1
 }

cn/gallery/data.json

@@ -97,7 +97,8 @@
       {
         "id": "chaff-countermeasure",
         "contributors": [
-          "Stas Fainer"
+          "Stas Fainer",
+          "Yi-Ting Tu"
         ],
         "title": "干扰箔",
         "description": "<p>这是一个箔片反射对雷达效应的定性模拟（忽略衍射效应）。</p>"
@@ -363,7 +364,8 @@
       {
         "id": "GRIN-slab",
         "contributors": [
-          "Stas Fainer"
+          "Stas Fainer",
+          "Yi-Ting Tu"
         ],
         "title": "渐变折射率平板",
         "description": "<p>模拟折射率 \\(n(\\rho) = n_0 \\sqrt{1-(\\alpha \\rho)^2}\\)的介电材料，其中 \\(n_0\\) 是其中央轴的折射率，\\(\\rho \\) 是从其中央轴的径向距离，使得 \\(\\alpha=\\frac{\\sqrt{3}}{2R} \\)，其中 \\(R=100 \\) 是其半径。上方的介电材料为一系列的薄矩形，每个矩形具有恒定的折射率（根据前述 \\(n(\\rho)\\) 的式子）。下方的介电材料是折射率为\\(n(\\rho)\\)的渐变折射率材料。 </p>"
@@ -395,7 +397,8 @@
       {
         "id": "luneburg-lens",
         "contributors": [
-          "Stas Fainer"
+          "Stas Fainer",
+          "Yi-Ting Tu"
         ],
         "title": "龙勃透镜",
         "description": "<p>龙勃透镜（Luneburg lens）是一个球形介电材料，折射率为 \\(n(\\rho) = \\sqrt{n_0-(\\frac{\\rho}{R})^2} \\)，其中 \\(n_0=2\\) 是其球心的折射率，\\(R=100\\) 是球的半径，\\(\\rho\\) 是与球心的距离。 </p><p>上方的介电材料为由 \\(N=20\\) 个同心球组成的龙勃透镜，半径 \\(R_i=5(N+1-i)\\)，折射率 \\(n_i = \\sqrt{n_0-(\\frac{R_i}{R})^2} \\)，其中 \\(i=1,...,N\\)。然而，由于此模拟器会将互相重叠的光学元件的折射率相乘，所以第 \\(i\\) 个同心球形镜的数值折射率为 \\(n_{i}^\\text{numerical}=\\frac{n_i}{n_{i-1}}\\)。 </p><p>下方的介电材料是折射率为\\(n(r)\\)的渐变折射率材料。 </p>"

cn/gallery/dichroic-rbg-splitter-and-combiner.json

@@ -202,6 +202,5 @@
   },
   "scale": 1,
   "simulateColors": true,
-  "name": "{{dichroic-rbg-splitter-and-combiner}}",
-  "title": "二色性RGB分光器与合光器"
+  "name": "二色性RGB分光器与合光器"
 }

cn/gallery/einstein-ring-refocused-to-single-image-via-eyepiece.json

@@ -282,6 +282,5 @@
   },
   "scale": 1,
   "simulateColors": true,
-  "name": "{{einstein-ring-refocused-to-single-image-via-eyepiece}}",
-  "title": "经由目镜将爱因斯坦环重新聚焦为单一影像"
+  "name": "经由目镜将爱因斯坦环重新聚焦为单一影像"
 }

cn/gallery/fresnel-lens.json

@@ -1,6 +1,6 @@
 {
   "version": 5,
-  "name": "{{fresnel-lens}}",
+  "name": "菲涅耳透镜",
   "modules": {
     "FresnelLens": {
       "numPoints": 2,
@@ -136,6 +136,5 @@
     "x": -592.6404282550802,
     "y": -201.1562930131771
   },
-  "scale": 1,
-  "title": "菲涅耳透镜"
+  "scale": 1
 }

cn/gallery/gan-based-lcd-pixel.json

@@ -284,6 +284,5 @@
   },
   "scale": 1,
   "simulateColors": true,
-  "name": "{{gan-based-lcd-pixel}}",
-  "title": "液晶显示器像素"
+  "name": "液晶显示器像素"
 }

cn/gallery/hyperbolic-lens.json

@@ -182,6 +182,5 @@
     "y": 1524.3702610244623
   },
   "scale": 1,
-  "name": "{{hyperbolic-lens}}",
-  "title": "双曲透镜"
+  "name": "双曲透镜"
 }

cn/gallery/hyperbolic-mirror.json

@@ -99,6 +99,5 @@
     "y": 68.27868584504733
   },
   "scale": 1,
-  "name": "{{hyperbolic-mirror}}",
-  "title": "双曲面镜"
+  "name": "双曲面镜"
 }

cn/gallery/images-formed-by-two-mirrors.json

@@ -85,6 +85,5 @@
     "y": 100.47857142857148
   },
   "scale": 1,
-  "name": "{{images-formed-by-two-mirrors}}",
-  "title": "两面镜子成像"
+  "name": "两面镜子成像"
 }

cn/gallery/index.html

@@ -249,7 +249,7 @@ <h2>光的反射</h2>
   <img src="chaff-countermeasure-thumbnail.png" alt="Thumbnail" class="img-rounded example-image" loading="lazy">
   <div class="caption">
     <p class="example-title">干扰箔</p>
-    <p class="example-contributor">Stas Fainer</p>
+    <p class="example-contributor">Stas Fainer, Yi-Ting Tu</p>
   </div>
 </a>
 <a href="caustics-from-a-reflective-sphere" class="thumbnail example-container">
@@ -475,7 +475,7 @@ <h2>渐变折射率光学</h2>
   <img src="GRIN-slab-thumbnail.png" alt="Thumbnail" class="img-rounded example-image" loading="lazy">
   <div class="caption">
     <p class="example-title">渐变折射率平板</p>
-    <p class="example-contributor">Stas Fainer</p>
+    <p class="example-contributor">Stas Fainer, Yi-Ting Tu</p>
   </div>
 </a>
 <a href="inferior-mirage" class="thumbnail example-container">
@@ -503,7 +503,7 @@ <h2>渐变折射率光学</h2>
   <img src="luneburg-lens-thumbnail.png" alt="Thumbnail" class="img-rounded example-image" loading="lazy">
   <div class="caption">
     <p class="example-title">龙勃透镜</p>
-    <p class="example-contributor">Stas Fainer</p>
+    <p class="example-contributor">Stas Fainer, Yi-Ting Tu</p>
   </div>
 </a>
 <a href="maxwell-fisheye-lens" class="thumbnail example-container">

cn/gallery/inferior-mirage.json

@@ -1,6 +1,6 @@
 {
   "version": 5,
-  "name": "{{inferior-mirage}}",
+  "name": "下蜃景",
   "objs": [
     {
       "type": "Ruler",
@@ -295,6 +295,5 @@
     "x": 336.04494830125213,
     "y": 138.31747905060888
   },
-  "scale": 1,
-  "title": "下蜃景"
+  "scale": 1
 }

cn/gallery/internal-reflection.json

@@ -60,6 +60,5 @@
     "y": -226.4779819320001
   },
   "scale": 1,
-  "name": "{{internal-reflection}}",
-  "title": "全反射"
+  "name": "全反射"
 }

cn/gallery/interrogation-room.json

@@ -271,6 +271,5 @@
     "y": -17.26591738399503
   },
   "scale": 1,
-  "name": "{{interrogation-room}}",
-  "title": "审讯室"
+  "name": "审讯室"
 }

cn/gallery/keplerian-telescope.json

@@ -271,6 +271,5 @@
     "y": 568.7345616434184
   },
   "scale": 1,
-  "name": "{{keplerian-telescope}}",
-  "title": "开普勒望远镜"
+  "name": "开普勒望远镜"
 }

cn/gallery/lens-images.json

@@ -92,6 +92,5 @@
     "y": 113.28387096774179
   },
   "scale": 1,
-  "name": "{{lens-images}}",
-  "title": "透镜成像"
+  "name": "透镜成像"
 }