122 resultados para SEGREGATION


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Floating zone crystal growth in microgravity environment is investigated numerically by a finite element method for semiconductor growth processing, which involves thermocapillary convection, phase change convection, thermal diffusion and solutal diffusion. The configurations of phase change interfaces and distributions of velocity, temperature and concentration fields are analyzed for typical conditions of pulling rates and segregation coefficients. The influence of phase change convection on the distribution of concentration is studied in detail. The results show that the thermocapillary convection plays an important role in mixing up the melt with dopant. The deformations of phase change interfaces by thermal convection-diffusion and pulling rods make larger variation of concentration field in comparison with the case of plane interfaces.

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The microgravity research, as a branch of the advanced sciences and a spe- cialized field of high technology, has been made in China since the late 1980's. The research group investigating microgravity fluid physics consisted of our col- leagues and the authors in the Institute of Mechanics of the Chinese Academy of Sciences (CAS), and we pay special attention to the floating zone convection as our first research priority. Now, the research group has expanded and is a part of the National Microgravity Laboratory of the CAS, and the research fields have been extended to include more subjects related to microgravity science. Howev- er, the floating zone convection is still an important topic that greatly holds our research interests.

目录

1. models of floating zone convection
1.1 floating-zone crystal growth
1.2 physical model
1.3 hydrodynamic model
1.4 mathematical model
references
2. basic features of floating zone convection
2.1 equations and boundary conditions
2.2 simple solutions of fz convection
2.3 solution for two-layers flow
2.4 numerical simulation
2.5 onset of oscillation
references
3. experimental method of fz convection
3.1 ground-based simulation experiments for pr≥1
3.2 temperature and velocity oscillations
3.3 optical diagnostics of free surface oscillation
3.4 critical parameters
3.5 microgravity experiments
3.6 ground-based simulation experiment for pr《1
.references
4. mechanism on the onset of oscillatory convection
4.1 order of magnitude analysis
4.2 mechanism of hydrothermal instability
4.3 linear stability analysis
4.4 energy instability of thermocapillary convection
4.5 unsteady numerical simulation of 2d and 3d
4.6 two bifurcation transitions in the case of small pr number fluid
4.7 two bifurcation transitions in the case of large pr number fluid
4.8 transition to turbulence
references
5. liquid bridge volume as a critical geometrical parameter
5.1 critical geometrical parameters
5.2 ground-based and mierogravity experiments
5.3 instability analyses of a large prandtl number (pr≥1)fluid
5.4 instability analyses of a small prandtl number (pr《1)fluid
5.5 numerical simulation on two bifurcation process
references
6. theoretical model of crystal growth by the floating zone method
6.1 concentration distribution in a pure diffusion process
6.2 solutal capillary convection and diffusion
6.3 coupling with phase change convection
6.4 engineering model of floating zone technique
references
7. influence of applied magnetic field on the fz convection
7.1 striation due to the time-dependent convection
7.2 applied steady magnetic field and rotational magnetic field
7.3 magnetic field design for floating half zone
7.4 influence of magnetic field on segregation
references
8. influence of residual acceleration and g-jitter
8.1 residual acceleration in microgravity experiments
8.2 order of magnitude analyses (oma)
8.3 rayleigh instability due to residual acceleration
8.4 ground-based experiment affected by a vibration field
8.5 numerical simulation of a low frequency g-jitter
8.6 numerical simulation of a high frequency g-jitter
references

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FSodium phosphate tellurite glasses in the system (NaPO3)(x)(TeO2)(1-x) were prepared and structurally characterized by thermal analysis, vibrational spectroscopy, X-ray photoelectron spectroscopy (XPS) and a variety of complementary solid-state nuclear magnetic resonance (NMR) techniques. Unlike the situation in other mixed-network-former glasses, the interaction between the two network formers tellurium oxide and phosphorus oxide produces no new structural units, and no sharing of the network modifier Na2O takes place. The glass structure can be regarded as a network of interlinked metaphosphate-type P(2) tetrahedral and TeO4/2 antiprismotic units. The combined interpretation of the O 1s XPS data and the P-31 solid-state NMR spectra presents clear quantitative evidence for a nonstatistical connectivity distribution. Rather the formation of homootomic P-O-P and Te-O-Te linkages is favored over mixed P-O-Te connectivities. As a consequence of this chemical segregation effect, the spatial sodium distribution is not random, as also indicated by a detailed analysis of P-31/No-23 rotational echo double-resonance (REDOR) experiments. ACHTUNGTRENUNG(TeO2)1 x were prepared and structurally characterized by thermal analysis,vibrat ional spectroscopy,X-ray photoelectron spectroscopy (XPS) and a variety of complementary solid-state nuclear magnetic resonance (NMR) techniques. Unlike the situation in other mixed-network-former glasses,the interaction between the two network formers tellurium oxide and phosphorus oxide produces no new structural units,and no sharing of the network modifier Na2O takes place. The glass structure can be regarded as a network of interlinked metaphosphate-type P(2) tetrahedral and TeO4/2 antiprismatic units. The combined interpretation of the O 1s XPS data and the 31P solid-state NMR spectra presents clear quantitative evidence for a nonstatistical connectivity distribution. Rather,the formation of homoatomic P O P and Te O Te linkages is favored over mixed P O Te connectivities. As a consequence of this chemical segregation effect,the spatial sodium distribution is not random,as also indicated by a detailed analysis of 31P/23Na rotational echo double-resonance (REDOR) experiments.

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In this paper, high optical quality cerium-doped lutetium pyrosilicate(LPS:Ce) crystal has been grown by Czochralski method with the seed oriented along cleavage plane (1 1 0). The structure, segregation coefficient of Ce3+ and optical characterization of LPS:Ce crystal have been compared with those of LSO:Ce crystal. The results show that LPS:Ce has the advantage over LSO:Ce by having a larger segregation coefficient of Ce3+, lower cost of starting material, lower melting point and only one luminescence mechanism. Thus, LPS:Ce crystal offers an attractive alternative to LSO:Ce for scintillator applications. (c) 2005 Elsevier B.V. All rights reserved.

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For the first time, a high optical quality 10 at.% Yb3+-doped gadolinium oxyorthosilicate laser crystal Gd2SiO5 (GSO) was grown by the Czochralski (Cz) method. The segregation coefficient of Yb3+ was studied by the inductively coupled plasma atomic emission spectrometer (ICP-AES) method. The crystal structure has monoclinic symmetry with space group P2(1)/c; this was determined by means of an x-ray diffraction analysis. The absorption spectra, fluorescence spectra and fluorescence decay curves of Yb3+ ions in a GSO crystal at room temperature were also studied. Then, the spectroscopic parameters of Yb:GSO were calculated. The advantages of the Yb:GSO crystal include high crystal quality, quasi-four-level laser operating scheme, high absorption cross-sections and particularly broad emission bandwidth (similar to 72 nm). The results indicated that the Yb:GSO crystal seemed to be a very promising laser gain medium in diode-pumped femtosecond laser and tunable solid state laser applications when LD pumped at 940 and 980 nm.

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Cerium-doped lutetium pyrosilicate crystal, Ce:Lu2Si2O7 (Ce:LPS), was grown by the Czochralski method. The segregation coefficient of Ce3+ ion was studied by the ICP-AES method. X-ray diffraction analysis showed that the structure of Ce:LPS crystal was monoclinic symmetry with space group of C2/m. Perfect cleavage planes (110) and imperfect cleavage planes (001) were observed by optical microscope. The reasons why it is difficult to grow crack-free crystals were studied. After optimized growth parameters, a Ce:LPS crystal with dimension of Phi 25 x 30 mm was grown, which is colorless, high optical quality, cracking-free and no inclusions. The transmittance of Ce:LPS crystal from 380 to 800 nm is over 82% and there is no observable absorption. (c) 2005 Elsevier B.V. All rights reserved.

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应用中频感应提拉法生长出不同掺杂浓度的Yb:FAP激光晶体,运用电感耦合等离子体原子发射光谱仪(ICP-AES)测定了Yb^3+离子存Yb:FAP晶体中的分凝系数约为0.03。随着晶体的生长,晶体中Yb^3+离子的轴向浓度逐渐增大。研究Yb:FAP晶体在77K和300K温度下的吸收光谱发现,振动谱的变化主要是由电子-声子近共振耦合作用引起的。系统地研究了不同Yb^3+离子掺杂浓度Yb:FAP晶体的吸收光谱和荧光光谱。通过吸收光谱的测量计算了晶体的吸收截面。Yb:FAP晶体在904nm和982nm处存在Yb

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A large and transparent Yb:FAP crystal with dimensions up to circle divide 30 mm x 85 mm has been grown by the Czochralski method. The preparation of the raw material has been investigated. X-ray power diffraction studies of Yb:FAP crystal confirm that the as-grown crystal is isostructural with the FAP crystal. The crystalline quality has been studied using X-ray rocking curve analysis. The segregation coefficient of Yb3+ in the Yb:FAP crystal has been also determined. Linear thermal expansion coefficients in [001] and [100] directions have been measured in the 30-800 degrees C temperature range. (c) 2005 Elsevier B.V. All rights reserved.

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采用中频感应提拉法生长了Yb:FAP晶体。对晶体生长中影响晶体质量的因素特别是原料的处理、CaF2的挥发等进行了研究和讨论。运用ICP-AES测定Yb^3+离子在Yb:FAP晶体中的分凝系数。对Yb:FAP晶体进行了高分辨X射线的四圆衍射实验,结果表明晶体具有比较高的晶格完整性。

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For the first time, a high optical quality Yb3+-doped lutetium pyrosilicate laser crystal Lu2Si2O7 (LPS) was grown by the Czochralski (Cz) method. The segregation coefficient of ytterbium ion in Yb:LPS crystal detected by the inductively coupled plasma atomic emission spectrometer (TCP-AES) method is equal to 0.847. X-ray powder diffraction result confirms the C2/m phase monoclinic space group of the grown crystal and the peaks corresponding to different phases were indexed. The absorption and fluorescence spectra, as well as fluorescence decay lifetime of Yb3+ ion in LPS have been investigated. The absorption and fluorescence cross-sections of the transitions F-2(7/2) <-> F-2(5/2) of Yb3+ ion in LPS crystal have been determined. The advantages of the Yb:LPS crystal including high crystal quality, quasi-four-level laser operating scheme, high absorption cross-sections (1.33 x 10(-2) cm(2)) and particularly broad emission bandwidth (similar to 62 nm) indicated that the Yb:LPS crystal seemed to be a promising candidate used as compact, efficient thin chip lasers when LD is pumped at 940 and 980 nm due to its low-symmetry monoclinic structure and single crystallographic site. (c) 2007 Elsevier B.V. All rights reserved.

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In this paper, single crystal of ytterbium (Yb) doped Ca-5(PO4)(3)F (FAP) has been grown along the c-axis by using the Czochralski method. The segregation coefficients of Yb3+ in the Yb:FAP crystal has been determined by ICP-AES method. The absorption spectrum, fluorescence spectrum and fluorescence lifetime of the Yb:FAP crystal has been also measured at room temperature. In the absorption spectra, there are two absorption bands at 904 and 982 nm, respectively, which are suitable for InGaAs diode laser pumping. The absorption cross-section (sigma(abs)) is 5.117 x 10(-20) cm(2) with an FWHM of 4 nm at 982 nm. The emission cross-section is (sigma(em)) 3.678 x 10(-20) cm(2) at 1042 nm. Favorable values of the absorption cross-section at about 982 nm are promising candidates for laser diode (LD) pumping. (c) 2005 Elsevier B.V. All rights reserved.

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The 2 at.% Sm:GdVO4 crystal was grown by the Czochralski method. The segregation coefficient of Sm3+ ion in this crystal is 0.98. The crystal structure of the Sm:GdVO4 crystal was determined by X-ray diffraction analysis. Judd-Ofelt theory was used to calculate the intensity parameters (Omega(i)), the spontaneous emission probability, the luminary branching ratio and the radiative lifetime of the state (4)G(5/2). The stimulated emission cross-sections at 567, 604 and 646 nm are calculated to be 5.92 x 10(-21), 7.62 x 10(-21) and 5.88 x 10(-21) cm(2), respectively. The emission cross-section at 604 nm is 4.4 times lager than that in Sm: YAP at 607 nm. (C) 2007 Elsevier B.V. All rights reserved.

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物种形成一直以来是进化生物学的一个中心议题。因为杂交能够快速创造出新的遗传变异和提高基因组重组率,加速物种形成和适应性进化,所以杂交物种形成是其重要的组成部分。但是直到最近几年,人们才逐渐意识到同倍体杂种形成的重要性和普遍性。此外,人工杂交种群结果证实了杂种的适应性起源于亲本基因的超亲分离现象,这些基因之间通过加和效应或上位效应相互连锁,并在杂种后代中逐渐固定,因此,探讨维持这种适应机制的杂种的连锁不平衡模式就显得尤为重要。到目前为止,关于自然杂种的核苷酸多态性和连锁不平衡结构的报道非常稀见,对杂种的进化历史知之更少。高山松能生长于亲本种不能正常繁殖生长的青藏高原上,这种极端环境为杂种的适应性进化和与亲本的生态隔离造就了绝佳的条件,其生态和生殖的稳定性极大地方便了我们研究植物物种形成和适应性进化的遗传机理,对高山松开展的生态学、遗传学的系列分析已使高山松成为同倍体杂种形成的经典范例。 该论文通过随机挑选7个核基因位点对5个高山松群体、3个油松群体和3个云南松群体的164个大配子体单倍体基因组进行了核苷酸多态性分析。研究发现:所有基因座位的单倍型组成和基因谱系的拓扑结构都支持高山松的多次杂交起源。高山松的平均核苷酸多态性与油松相当,θW达到0.0107;比云南松高出一倍;高于已报道的裸子植物类群遗传变异水平。高山松如此高的遗传多态性与其杂交特性和有效群体大有关。我们运用分子钟和共祖模拟分析,推测出高山松的有效群体为7.32 x 105。等位基因共祖时间模拟分析发现,杂交过程早于青藏高原的隆升,也即是说,在杂种稳定成种以前,两个亲本种之间存在广泛的渐渗杂交。此外,高山松杂种的群体间分化严重,并且在不同的群体中,我们找到了多个偏离中性的基因座位。由此说明,高山松复杂的进化历史和适应的策略区域化。 在显著偏离中性的基因座位上,选取群体历史清晰的高山松群体,对其全基因序列多态性和连锁不平衡结构进行了深入调查,以期找到选择作用位点或区域。Ara-like和Dhn1两个基因在高山松与亲本之间都没有发现固定变异。在高山松中,Ara-like基因和Dhn1基因核苷酸多态性式样和连锁不平衡结构存在明显差异,这说明在两个基因上选择作用的程度和方向不尽相同。 我们对Dhn1基因的多态性分布、LD结构和中性偏离水平进行了分析,结果表明,该基因可能在PdNX和PdLZ群体中受到平衡选择的作用。从Dhn1基因谱系结构可以看出有两种来源的等位基因造成这种平衡多态性,一种属于祖先类型,另一种是从云南松继承衍生而来。这两种等位基因之间的分化很大,极有可能造成编码蛋白的亚功能化。事实上,Dhn1编码的脱水蛋白在植物对环境的抗逆过程中发挥着重要作用。由此我们推测高山松在高海拔极端环境中的适应性进化与Dhn1基因的平衡作用有关。 对Ara-like和Dhn1基因进行HKA检测,结果表明,与Dhn1基因相比,在Ara-like基因上,双维管束亚属与单维管束亚属之间存在显著分化,沉默突变位点的分化Ksil达到了0.1392,远远高于平均水平0.0508;在双维管束亚属共发现了43个固定突变位点,其中有6个能导致氨基酸突变,它们有可能导致了Ara-like基因功能的分化。结合裸子植物近缘物种间共享多态性的普遍性,我们推测Ara-like基因可能在单维管束亚属中的进化速率加快,暗示其在单维管束亚属中的适应性进化。 最后,基因内连锁不平衡分析结果显示,随机筛选的基因座位之间不存在连锁不平衡。高山松平均的基因内LD程度非常低,仅有18%的信息位点之间显著连锁。平均基因内LD在油松和高山松中的衰减速率很快,尤其在杂种中下降最快,在不到200bp以内就降到0.1以下。 LD的结果印证了高山松的有效群体大和多次起源特性。另外,我们也怀疑杂交物种形成过程中染色体组的重组和重排频繁发生,也是造成自然杂种现有群体的LD水平低的一个主要原因。 通过LD衰减曲线估计高山松的平均单位重组率,比亲本油松高17倍,比云南松高45倍。这个结果表明,杂种共适应的基因间要维持超亲分离,需要强烈的自然选择压力,才能保持它们之间的连锁不平衡。

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在榕树与其传粉小蜂组成的互利阿共生系统中,理解传粉小蜂与各种非传粉小蜂如何共存是解决这一系统稳定性维持机制问题的关键之一.生态位分化被普遍认为是传粉小蜂与各种非传粉小蜂共存的最主要动力.而作为生态位分化中最基础的食性分化在这一系统中如何具体实现尚小清楚.2006年12月至2007年6月.我们以聚果榕(Ficus racemosa)为材料,通过对果内6种榕小蜂进行独立放蜂及两两组合定最放蜂,并对传粉小蜂分别进行不携带花粉和不能产卵的技术处理,研究了寄生在聚果榕果内的5种非传粉小蜂的食性及相互关系,分析了在不同季节下寄生蜂与寄主间的相关系数.研究结果表明:在5种非传粉小蜂中,Platyneura testacea和P mayri是造瘿者,能独立刺激子房发育成瘿花,并使果实发育成熟;而 Apocrypta sp、A.westwoodi和P.agraensis只能寄生于某些已发育的虫瘿,为拟寄生者,它们各自分别与P.testacea,P.mayri和传粉小蜂Ceratosolen fusciceps存在着一对一的寄生关系.拟寄生者与寄主间的相关性在不同季节下会显示出不同的结果,这表明过去文献中用物种间的相关系数推理而确定的食性关系可能是不可靠的.对自然采集榕果内的小蜂群落分析表明,传粉小蜂处于优势地位,这说明在自然情况下非传粉小蜂的种群维持在一个较低水平,对榕树-传粉小蜂系统稳定性影响较小,故能与之长期共存.

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The centromere protein A (CENP-A), a histone H3-like protein, provides an essential role for chromosomal segregation during mitosis and meiosis. In this study we identified ten new CENP-A-like genes (excluding the original CENP-A gene) in cow by searching