|
| 1 | +{ |
| 2 | + "data":[{ |
| 3 | + "x": [0, 1], |
| 4 | + "y": [0, 1.414], |
| 5 | + "text": ["Hx+yH", "H\\sqrt{2}H"], |
| 6 | + "mode": "text+markers", |
| 7 | + "name": "HE^2=m^2c^4+p^2c^2H" |
| 8 | + }, { |
| 9 | + "x": [0, 1], |
| 10 | + "y": [1.4, 0.1], |
| 11 | + "text": ["H1.400 \\pm 0.023H", "H0.100 \\pm 0.002H"], |
| 12 | + "textposition": "auto", |
| 13 | + "type": "bar", |
| 14 | + "name": "Hx=\\frac{-b \\pm \\sqrt{b^2-4ac}}{2a}H" |
| 15 | + }, { |
| 16 | + "type": "pie", |
| 17 | + "values": [1, 9], |
| 18 | + "labels": ["H\\frac{1}{10}=10\\%H", "H\\frac{9}{10}=90\\%H"], |
| 19 | + "textinfo": "label", |
| 20 | + "domain": {"x": [0.3, 0.75], "y": [0.55, 1]} |
| 21 | + }, { |
| 22 | + "type": "heatmap", |
| 23 | + "z": [[1,2],[3,4]], |
| 24 | + "xaxis": "x2", |
| 25 | + "yaxis": "y2", |
| 26 | + "colorbar": {"title": "He^{i\\pi}=-1H", "y": 0.225, "len": 0.45} |
| 27 | + }], |
| 28 | + "layout": { |
| 29 | + "yaxis":{"domain": [0, 0.45], "title": "$y=\\sin{2 \\theta}$"}, |
| 30 | + "xaxis":{ |
| 31 | + "domain": [0, 0.45], |
| 32 | + "title": "$x=\\int_0^a a^2+1$", |
| 33 | + "tickvals": [0, 1], |
| 34 | + "ticktext": ["$\\frac{0}{100}$", "$\\frac{100}{100}$"] |
| 35 | + }, |
| 36 | + "xaxis2": {"domain": [0.85, 1], "anchor": "y2"}, |
| 37 | + "yaxis2": { |
| 38 | + "domain": [0, 0.45], |
| 39 | + "anchor": "x2", |
| 40 | + "tickvals": [0, 1], |
| 41 | + "ticktext": ["Ha+b+c+dH", "He+f+g+hH"], |
| 42 | + "title": "$(||01\\rangle+|10\\rangle)/\\sqrt2$" |
| 43 | + }, |
| 44 | + "height":500, |
| 45 | + "width":800, |
| 46 | + "title": "$i\\hbar\\frac{d\\Psi}{dt}=-[V-\\frac{-\\hbar^2}{2m}\\nabla^2]\\Psi$", |
| 47 | + "annotations":[ |
| 48 | + { |
| 49 | + "text": "H is substituted for $<br>where we would like<br>math but do not yet<br>fully support it", |
| 50 | + "xref": "paper", "yref": "paper", |
| 51 | + "x": 1.2, "xanchor": "left", "y": 0, "yanchor": "bottom", |
| 52 | + "showarrow": false |
| 53 | + }, |
| 54 | + { |
| 55 | + "text":"$(top,left)$","showarrow":false,"xref":"paper","yref":"paper", |
| 56 | + "xanchor":"left","yanchor":"top","x":0,"y":1,"textangle":10, |
| 57 | + "bordercolor":"#0c0","borderpad":3,"bgcolor":"#dfd" |
| 58 | + }, |
| 59 | + { |
| 60 | + "text":"$(right,bottom)$","xref":"paper","yref":"paper", |
| 61 | + "xanchor":"right","yanchor":"bottom","x":0.2,"y":0.7,"ax":-20,"ay":-20, |
| 62 | + "textangle":-30,"bordercolor":"#0c0","borderpad":3,"bgcolor":"#dfd", |
| 63 | + "opacity":0.5 |
| 64 | + }, |
| 65 | + {"text":"$not-visible$", "visible": false}, |
| 66 | + { |
| 67 | + "text":"$^{29}Si$","x":0.7,"y":0.7,"showarrow":false, |
| 68 | + "xanchor":"right","yanchor":"top" |
| 69 | + }, |
| 70 | + { |
| 71 | + "text":"$^{17}O$","x":0.7,"y":0.7,"ax":15,"ay":-15, |
| 72 | + "xanchor":"left","yanchor":"bottom" |
| 73 | + } |
| 74 | + ] |
| 75 | + } |
| 76 | +} |
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