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@@ -98,8 +98,16 @@ Thus, it was not typically observed in normal incidence Raman experiments (cite)
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but could be clearly detected in edge incidence configurations in our experiments.
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// TODO: 这里缺两个引用
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不同方向的入射配置会导致微小但可观测的峰位差异。
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非零长度的波矢(i.e. 参与散射的声子不在 Gamma 点)导致不同入射配置的峰位具有微小但可观测的差异,如色散图所示。
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相比于正入射,肩入射时,E2-1与E2-2的间距会减小、E2-2会展宽;E2-3会展宽,同时略微蓝移动。我们的计算结果为xxx,实验结果为xxx。
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相比于正入射,肩入射时,E2-1与E2-2的间距会减小、E2-2会展宽;E2-3会展宽,同时略微蓝移动。
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我们的计算结果为xxx,实验结果为xxx。
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// 198.43184855558061
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// 199.03816532139587
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// 257.87910853505343
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// 258.4149982771832
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// 其它峰在其它章节中解释。
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@@ -7,6 +7,7 @@
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- [x] 排版:如何让图片固定在原位置?10分钟。
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- [x] 排版:旋转内容而不是旋转页面。10分钟。
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- [ ] 实验:缺少肩入射的稳定的结果。
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剩余工作量估计:
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画图/声子不连续/freq_at_edge.csv
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画图/声子不连续/freq_at_edge.csv
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@@ -0,0 +1,24 @@
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11.438612167488849
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13.096182193217222
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21.22517926580885
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191.0992491263573
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191.77252066290447
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198.43184855558061
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199.03816532139587
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257.87910853505343
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258.4149982771832
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390.18078902973957
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397.67948042840044
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591.7690959178592
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747.3859960437837
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747.5398010710838
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756.7096254154966
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756.899914473123
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762.2773404925831
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764.8175584985144
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764.9562101805996
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777.0955580229571
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813.824669608532
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886.2276940301315
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894.6683750829986
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941.8414103176491
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画图/声子不连续/freq_at_normal.csv
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画图/声子不连续/freq_at_normal.csv
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@@ -0,0 +1,24 @@
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11.996875783054959
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11.996875783206022
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22.026249438233176
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186.3883538786764
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186.38835388124227
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201.84270995619016
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201.84270995851526
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257.37090939813936
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257.3709094013408
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376.2654896588351
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411.24309895859597
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591.5953989013976
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747.4649008869136
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747.4649008984917
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756.6326123405026
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756.6326123522597
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765.0225143366765
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765.0225143484857
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777.0536945057479
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777.0536945177406
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813.827140178508
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884.3098126911134
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896.5564951887419
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934.3358423539902
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画图/弱极性不同方向偏移/fwhm_E22.csv
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画图/弱极性不同方向偏移/fwhm_E22.csv
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@@ -0,0 +1,4 @@
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1.7608270175274945 1.7095382677800082 1.6908206133855936 1.641072964651852 1.6077984597054702
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1.8521285781470913 1.8070926863375696 1.8063564129426537 1.7796436816826098 1.7863596199454495
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1.8550653942136455 1.8454179607235797 1.8355798460139852 1.8640304200694087 2.1953176226936186
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1.8046549945528232 1.702570082702504 1.790691823550824 1.805662743000825 2.1233278447896313
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画图/弱极性不同方向偏移/plot.ipynb
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画图/弱极性不同方向偏移/shift_A11.csv
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画图/弱极性不同方向偏移/shift_A11.csv
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610.1213008890824 610.1330681678368 610.1588530411506 610.1811021981093 610.1986449965905
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609.7440349023198 609.9115498133125 609.956740868125 609.9158791976113 610.0334707759941
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609.6677307789029 609.6669096041305 609.7130323351229 609.7274691263951 609.4912325733311
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609.7087116252412 609.5493648779523 609.632471522247 609.7291873589254 609.4961232284547
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画图/弱极性不同方向偏移/shift_E21.csv
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画图/弱极性不同方向偏移/shift_E21.csv
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195.73602107894294 195.74080631709137 195.77557988756905 195.76148803134245 195.76983155098773
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195.96055989744724 195.85259578794742 195.7927026486199 195.83645434579918 195.76794597230077
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196.19825656128967 196.20368948678166 196.19343990422314 196.16722948184966 196.0690751103817
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195.97757968839247 196.74028227696692 196.3986248349401 196.26794625826986 195.98019647684944
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画图/弱极性不同方向偏移/shift_E22.csv
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画图/弱极性不同方向偏移/shift_E22.csv
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@@ -0,0 +1,4 @@
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203.6801432038987 203.68814481324 203.68505961884634 203.69299952913238 203.6904003764694
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203.91071868059444 203.765195365188 203.73916579371567 203.8009438952096 203.70415932586553
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203.73665069017437 203.74307378471798 203.7412374475013 203.7355035381401 203.68224371967472
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203.68505533371479 203.83431521382425 203.71910427658776 203.79953992752039 203.66963877731052
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画图/拉曼结果拟合/250910/3/fitting.ipynb
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