228 lines
13 KiB
Typst
228 lines
13 KiB
Typst
#import "@preview/starter-journal-article:0.4.0": article, author-meta
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#import "@preview/tablem:0.2.0": tablem
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#set par.line(numbering: "1")
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#show: article.with(
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title: "Article Title",
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authors: (
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"Haonan Chen": author-meta(
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"xmu",
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// email: "chn@chn.moe",
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),
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"Junyong Kang": author-meta(
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"xmu",
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email: "jykang@xmu.edu.cn"
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)
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),
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affiliations: (
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"xmu": "Xiamen University",
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),
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abstract: [#lorem(100)],
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keywords: ("Typst", "Template", "Journal Article"),
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// template: (body: (body) => {
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// show heading.where(level: 1): it => block(above: 1.5em, below: 1.5em)[
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// #set pad(bottom: 2em, top: 1em)
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// #it.body
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// ]
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// set par(first-line-indent: (amount: 2em, all: true))
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// set footnote(numbering: "1")
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// body
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// })
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)
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= Introduction
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// SiC 是很好的材料。
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// 其中，4H-SiC 是SiC的一种多型，它的性质更好，近年来随着外延工艺的成熟而获得了更多的关注。
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SiC is a promising wide-bandgap semiconductor material
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with high critical electric field strength and high thermal conductivity.
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It has been widely used in power electronic devices and has long attracted a lot of research
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@casady_status_1996 @okumura_present_2006.
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The 4H-SiC has a wider bandgap, higher critical electric field strength,
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higher thermal conductivity, and higher electron mobility along the c-axis than other polytypes.
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Currently, the 4H-SiC has gradually received more attention than other polytypes,
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thanks to the development of epitaxy technology and the increasing application in the new energy industry
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@tsuchida_recent_2018 @harada_suppression_2022 @sun_selection_2022. // TODO: 多引用一些近年来的文献，有很多
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// 声子（量子化的原子振动）在理解晶体的原子结构以及热电性质方面起着重要作用。
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// 声子可以通过多种实验技术来探测，包括 EELS、IR 吸收谱等。
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// 拉曼光谱是最常用的方法，它提供了一种无损、非接触、快速和局部的声子测量方法，已被广泛用于确定晶体的原子结构（包括区分 SiC 的多型）。
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Phonons (quantized atomic vibrations) play a fundamental role
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in understanding the atomic structure
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as well as the thermal and electrical properties
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of crystals (including 4H-SiC).
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They could be probed by various experimental techniques,
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such as electron energy loss spectroscopy and infrared absorption spectroscopy.
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Among these techniques,
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Raman spectroscopy is the most commonly used method,
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as it provides non-destructive, non-contact, rapid and spatially localized measurement of phonons
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that near the $Gamma$ point in reciprocal space.
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Studies in Raman scattering of 4H-SiC have been conducted since as early as 1983
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and have been widely employed to identification of different SiC polytypes.
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// 近年来，更多信息被从拉曼光谱中挖掘出来。
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// LOPC 已经被用于快速估计 n 型 SiC 的掺杂浓度。
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// 层错的拉曼光谱也已经被研究，可以被用于检测特定结构层错的存在和位置。
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// 掺杂对拉曼光谱的潜在影响也已经被研究。
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// 然而，拉曼光谱上仍有一些不知来源的峰；同时，一些也缺少一些理论上预测应该存在的峰。
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// 此外，预测掺杂导致的新峰也没有说明原因。
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Increasingly rich information has been extracted from Raman spectra of 4H-SiC.
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Longitudinal optical phonon–plasmon coupling (LOPC) peek
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has been utilized to rapidly estimate the doping concentration in n-type SiC.
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Peeks associated with some stacking faults have also been investigated
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and used to detect the presence and location of specific structural faults.
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Moreover, the potential effects of doping on Raman spectra have been explored.
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However, some unidentified peaks still appear in the Raman spectra,
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while certain phonon modes predicted by theory remain unobserved.
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In addition, the origins of newly emerged peaks induced by doping are often unclear or unexplained.
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In this paper, we do some things. We do something for the first time.
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= Method
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= Results and Discussion
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// 拉曼活性的声子模式对应于 Gamma 点附近的声子模式。
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// 根据这些声子模式在拉曼实验中的表现，我们将这些声子分成三个部分。
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Raman scattering peeks correspond to phonons located near $Gamma$ point in reciprocal space.
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We classified these phonons into three categories according to their behavior in Raman scattering:
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(1) phonons could not be observed in Raman scattering spectrum,
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either because they are Raman inactive or their scattering intensity is too weak;
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(2) phonons could be observed in Raman scattering spectrum and with weak or no polarities,
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their frequencies were independent of the direction of the incident light;
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(3) strong polar phonons,
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which were visible in Raman scattering spectrum,
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and their frequencies depend on the direction of the incident light.
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// 我们计算了 4H-SiC 在 A-Gamma 和 Gamma-M 上的声子频率，如图和附录1所示。
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// 在拉曼散射中，起作用的模式都是那些非常接近于 Gamma 的模式
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// （如图中的点所示，分为位于 1/50 和 1/100 处，这两条线分别对应于拉曼散射在 z 方向入射/散射和 y 方向入射/散射）。
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// 大多数声子模式在 Gamma 附近都是连续的，这使得它们的频率对入射光的方向不敏感；
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// 然而，少数声子具有较强的极性，这使得声子之间存在长程的库伦相互作用（引用文献），并导致 gamma 附近的频率不同，如图中的某两条线所示。
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// 据此，我们将无缺陷的 4H-SiC 的声子分成三类：
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// 无拉曼活性或拉曼散射强度太弱的模式，它们在拉曼散射谱上不可见；
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// 拉曼散射强度足够大且极性不强的模式，它们在拉曼散射谱上可以看到，且频率与拉曼入射光方向无关；
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// 极性声子，它们在拉曼散射谱上可以看到，不仅频率与入射光方向有关，而且可与载流子发生一些相互作用。
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Phonons in defect-free 4H-SiC are calculated at A-$Gamma$ and $Gamma$-M,
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as shown in Figure \ref{fig:phonon} and Table \ref{tab:phonon}.
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Raman active phonons are very close to $Gamma$,
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as indicated by the points in the figure.
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Because of the consistency of the most phonon modes near $Gamma$,
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most of the phonon frequencies are insensitive to the direction of the incident light.
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However, some phonons have strong polarities,
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which leads to long-range Coulomb interactions between phonons,
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and results in different frequencies near $Gamma$,
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as shown by the two lines in the figure.
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Thus, we divide the phonons of defect-free 4H-SiC into three categories:
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(1) Raman inactive or too weak Raman intensity,
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which are invisible in the Raman scattering spectrum;
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(2) Raman active phonons with strong polarities,
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which are visible in the Raman scattering spectrum,
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and their frequencies are independent of the direction of the incident light;
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(3) Polar phonons,
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which are visible in the Raman scattering spectrum,
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and their frequencies depend on the direction of the incident light,
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and can interact with carriers.
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#page(flipped: true)[
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#let m(n, content) = table.cell(colspan: n, content);
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#let mCell(n, content) = m(n, content);
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#let A1 = [A#sub[1]];
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#let A2 = [A#sub[2]];
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#let B1 = [B#sub[1]];
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#let B2 = [B#sub[2]];
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#let E1 = [E#sub[1]];
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#let E2 = [E#sub[2]];
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#figure(
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table(columns: 27, align: center + horizon, inset: (x: 3pt, y: 5pt),
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[*Direction of Incident & Scattered Light*],
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m(26)[Any direction (not depend on direction of incident & scattered light)],
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[*Number of Phonon*],
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// E2 E2 E1 2B1 A1
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[1], m(2)[2], [3], m(2)[4], [5], [6], [7], [8], m(3)[9],
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// E1 E2 E2 A1 2B1
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[10], [11], [12], m(2)[13], [14], m(2)[15], m(3)[16], [17], [18],
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[*Vibration Direction*],
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// E2 E2 E1 2B1 A1
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[x], m(2)[y], [x], m(2)[y], [x], [y], [z], [z], m(3)[z],
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// E1 E2 E2 A1 2B1
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[x], [y], [x], m(2)[y], [x], m(2)[y], m(3)[z], [z], [z],
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[*Representation in Group C#sub[6v]*],
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m(3, E2), m(3, E2), m(2, E1), B1, B1, m(3, A1), m(2, E1), m(3, E2), m(3, E2), m(3, A1), B1, B1,
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[*Representation in Group C#sub[2v]*],
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// E2 E2 E1 2B1 A1 E1 E2 E2 A1 2B1
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A2, m(2, A1), A2, m(2, A1), B2, B1, B1, B1, m(3, A1), B2, B1, A2, m(2, A1), A2, m(2, A1), m(3, A1), B1, B1,
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[*Scattering in Polarization*],
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// E2 E2 E1 2B1 A1
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[xy], [xx], [yy], [xy], [xx], [yy], [xz], [yz], [-], [-], [xx], [yy], [zz],
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// E1 E2 E2 A1 2B1
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[xz], [yz], [xy], [xx], [yy], [xy], [xx], [yy], [xx], [yy], [zz], [-], [-],
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[*Raman Intensity (a.u.)*],
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// E2 E2 E1 2B1 A1
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m(3)[0.17], m(3)[1.13], m(2)[2.43], [0], [0], m(2)[2.83], [1.79],
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// E1 E2 E2 A1 2B1
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m(2)[0.09], m(3)[88.54], m(3)[0.50], m(2)[0.01], [1.78], [0], [0],
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[*Visible in Common Raman Experiment*],
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// E2 E2 E1 2B1 A1
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m(3)[Yes], m(3)[Yes], m(2)[Yes], [No], [No], m(3)[Yes],
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// E1 E2 E2 A1 2B1
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m(2)[No], m(3)[Yes], m(3)[No], m(2)[No], [Yes], [No], [No],
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[*Wavenumber (Simulation) (cm#super[-1])*],
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// E2 E2 E1 2B1 A1
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m(3)[190.51], m(3)[197.84], m(2)[257.35], [389.96], [397.49], m(3)[591.90],
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// E1 E2 E2 A1 2B1
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m(2)[746.91], m(3)[756.25], m(3)[764.33], m(3)[812.87], [885.68], [894.13],
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[*Wavenumber (Experiment) (cm#super[-1])*],
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// E2 E2 E1 2B1 A1
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m(3)[195.5], m(3)[203.3], m(2)[269.7], [-], [-], m(3)[609.5],
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// E1 E2 E2 A1 2B1
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m(2)[-], m(3)[776], m(3)[-], m(2)[-], [839], [-], [-],
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[*Electrical Polarity*],
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// E2 E2 E1 2B1 A1
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m(3)[None], m(3)[None], m(2)[Weak], [None], [None], m(3)[Weak],
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// E1 E2 E2 A1 2B1
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m(2)[Weak], m(3)[None], m(3)[None], m(3)[Weak], [None], [None],
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),
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caption: [Weak- and None-polarized phonons near $Gamma$ point],
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)
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#figure({
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let NA = [Not Applicable];
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let yzmix = [y-z mixed#linebreak() (LO-TO mixed)];
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let lopc = [Yes#linebreak() (LOPC)];
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let overf = [Yes#linebreak() (overfocused)];
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table(columns: 20, align: center + horizon, inset: (x: 3pt, y: 5pt),
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[*Direction of Incident & Scattered Light*], m(5)[z], m(5)[y], m(9)[between z and y, 10#sym.degree to z],
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// z y 45 y&z
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[*Number of Phonon*], [1], [2], m(3)[3], m(3)[1], [2], [3], m(4)[1], [2], m(4)[3],
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[*Vibration Direction*],
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[x#linebreak() (TO)], [y#linebreak() (TO)], m(3)[z (LO)], // z
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m(3)[z (TO)], [x#linebreak() (TO)], [y (LO)], // y
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m(4, yzmix), [x#linebreak() (TO)], m(4, yzmix), // 45 y&z
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[*Representation in Group C#sub[6v]*], m(2, E1), m(3, A1), m(14, NA),
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// z y 45 y&z
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[*Representation in Group C#sub[2v]*], B2, B1, m(3, A1), m(3, A1), B2, B1, m(4, NA), B2, m(4, NA),
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[*Scattering in Polarization*],
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[xz], [yz], [xx], [yy], [zz], // z
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[xx], [yy], [zz], [xz], [yz], // y
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[xx], [yy], [yz], [zz], [xz], [xx], [yy], [yz], [zz], // 45 y&z
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[*Raman Intensity (a.u.)*],
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m(2)[53.52], m(2)[58.26], [464.69], // z
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m(2)[58.26], [454.09], [53.52], [53.55], // y
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m(2)[53.71], [3.20], [425.98], [53.56], m(2)[3.60], [50.36], [27.99], // 45 y&z
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[*Visible in Common Raman Experiment*],
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m(2)[Yes], m(2, lopc), [No], // z
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overf, [No], overf, [Yes], lopc, // y
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m(4)[???], [???], m(4)[???], // 45 y&z
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[*Wavenumber (Simulation) (cm#super[-1])*],
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// z y 45 y&z
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m(2)[776.57], m(3)[933.80], m(3)[761.80], [776.57], [941.33], m(4)[762.76], [776.57], m(4)[940.86],
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[*Electrical Polarity*], m(19)[Strong]
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)},
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caption: [Strong-polarized phonons near $Gamma$ point],
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)
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]
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#bibliography("./ref.bib", title: "Reference", style: "american-physics-society")
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