共查询到20条相似文献,搜索用时 328 毫秒
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本文研究了室温下1—40kbar流体静压力范围内三元化合物半磁半导体Cd1-xMnxTe光吸收边的压力效应。实验结果给出:x<0.5的样品,吸收边随压力增加向高能方向以α=6—8×10-3eV/kbar的速率漂移,并具有10-5/kbar2量级的二级非线性系数;x≥0.5的样品,表观吸收边随压力增加向低能方向漂移,压力系数为α-5×10-3eV/kbar。高压下所研究的样品均有一从闪锌矿结构到NaCl结构的相变发生。这一相变可以是不可逆的,相变压力与样品组分有关,大致在25—40kbar范围内。根据半导体能带畸变势效应和晶体场理论模型估计了压力系数的理论值,讨论了不同压力系数的物理原因。
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在流体静压力为0.5—11.6kbar,温度-80—80℃范围内,测量了Rb_4Cu_(16)I_7Cl_(13)多晶粉末“松散”样品和“致密”样品的离子电导。“松散”样品电导与压力的关系表明,在4.0—5.0kbar附近,电导存在极大值;“致密”样品电导随压力单调下降。在一定压力下,“致密”样品电导率随温度变化的趋势与常压结果相同,压力对Rb_4Cu_(16)I_7Cl(13)α→β相转变温度没有明显影响。α和β相的激活体积分别为0.90cm~3/mol和1.55cm~3/mol。 相似文献
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用X射线衍射法研究了(Fe0.1Co0.55Ni0.35)78Si8B14金属玻璃在常压下及20kbar高压下晶化过程中的析出相及析出过程。结果表明在上述压力下晶化过程都分成两个阶段,分别对应于初级晶化和共晶晶化。在常压下,初级晶化时析出fcc-Co晶体,而共晶晶化对应着Ni31Si12和(FeCoNi)3(SiB)相的析出。随着回火温度的增高或时间的延长,(FeCoNi)3(SiB)相逐渐转变为(FeCoNi)23B6相。20kbar高压下的晶化析出过程与常压下不同的是:提高了晶化温度,在共晶晶化阶段出现了Co2B相。此外,压力还阻止(FeCoNi)23B6相的形成。从热力学和动力学的角度讨论了压力对金属玻璃晶化过程的影响。
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本文研究了室温下1—40kbar流体静压力范围内三元化合物半磁半导体Cd_(1-x)Mn_xTe光吸收边的压力效应。实验结果给出:x<0.5的样品,吸收边随压力增加向高能方向以α=6—8×10~(-3)eV/kbar的速率漂移,并具有10~(-5)/kbar~2量级的二级非线性系数;x≥0.5的样品,表观吸收边随压力增加向低能方向漂移,压力系数为α-5×10~(-3)eV/kbar。高压下所研究的样品均有一从闪锌矿结构到NaCl结构的相变发生。这一相变可以是不可逆的,相变压力与样品组分有关,大致在25—40kbar范围内。根据半导体能带畸变势效应和晶体场理论模型估计了压力系数的理论值,讨论了不同压力系数的物理原因。 相似文献
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用金刚石对顶砧高压显微光谱系统在室温和1bar—66kbar的流体静压力范围内研究了(Zn0.85Cd0.15)S:Cu,Al磷光体的发光峰位置和相对发光强度随压力而变化的规律。随着压力的增加,发射峰值波长迅速移向短波方向,而发射峰值对应的光子能量随压力增加的速率为4.7meV/kbar(38cm-1/kbar)。这个值比该材料的吸收边随压力增加的速率要小。随着压力的增加,该磷光体的发光峰值相对强度急骤下降,当压力从常压升到66kbar时,发光峰值相对强度下降到原值的6%。这些结果可以用Al3+-Cu+的施主-受主对模型来解释。本文还估计施主(Al3+)和受主(Cu+)的激活能之和随压力增加的速率为3.7meV/kbar(30cm-1/kbar)。
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I. N. Derkach E. A. Kudryashov G. N. Kachalin N. A. Kirdyaev V. V. Ladeishchikova D. S. Timaev 《JETP Letters》2018,107(6):379-383
The structure and properties of high-pressure phases of iron nitrides Fe7N3 in the pressure range of 50–150 GPa have been studied with ab initio calculations within the electron density functional theory. A new phase Amm2-Fe7N3, which is the most energetically favorable in the pressure range of 43–128 GPa, has been found using the USPEX (Universal Structure Predictor: Evolutionary Xtallography) algorithms. It has been thermodynamically shown that another high-pressure phase β-Fe7N3 is isostructural to a similar phase of iron carbide. The elastic properties have been calculated for all modifications ε-, β-, and Amm2-Fe7N3 stable at high pressures. 相似文献
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Clarke G Homan 《Journal of Physics and Chemistry of Solids》1975,36(11):1249-1254
The phase diagram of Bi has been studied by resistometric techniques in the temperature range of 30 to 300°K up to pressures of 140 kbars. Using the original Bridgman phase notation, the phase transitions I–II, II–III, I–III, III–IV and V–VI were observed. Two new phases, designated VIII and IX were observed in this region. The triple points occurring between I–II–III near 29.5 kbars and 160°K, between IV–V–VIII near 55 kbars and 240°K, between V–VI–VIII near 72 kbars and 255°K and between VI–VIII–IX near 135 kbars and 250°K. Earlier measurements were adjusted to the 1970 Drickamer pressure scale and compared to the present results. A phase diagram is proposed for pressures to 140 kbars. Calculations of the volume changes and latent heats of transformation are made near the triple points I–II–III, IV–V–VIII and V–VI–VIII using the measured volume changes of Bridgman for the I–II, IV–V and V–VI transitions. The latent heat associated with the III–IV transition was calculated using the volume data of Bridgman to be less than ? 2 cal/mol. 相似文献
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The compression curve (to 200 kbars) and the ambient resistivity versus temperature (1.5K <T < 300K) of CeS have been measured. The results are compared to the analogous experiments on the compound CeAl2. A high pressure valence instability and ambient pressure crystalline electric field, spin fluctuation and magnetic order effects are found to be common to both compounds. 相似文献
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用X射线衍射照相、X射线衍射仪及透射电子显微镜分析了用液相淬火技术制备的La80Al20合金样品,结果表明样品是非晶态结构。差热分析(DTA)结果表明,非晶态样品的晶化温度Tcr为280℃左右,玻璃温度Tg为242℃左右。非晶态样品低温高压(流体静压法)试验结果表明:压力从0至4.77kbar,Tc从3.87K提高到4.18K。高压下,超导前的剩余电阻与常压下相比较有明显下降。非晶态样品经高温高压
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本文用差热分析、恒温热处理、X射线衍射等方法,对LiIO3在常压的相变过程做了进一步的研究。对于LiIO3的常压相变机制有了较为详尽的了解。并发现LiIO3在高温可相对稳定存在三个相:β,η和δ,它们可分别自行熔化,其熔点相应为:432℃,421℃和416℃,从它们的热经历和存在的温度范围,表明其稳定性顺序为β>η>δ。在室温干燥空气中,与α相和β相共存的还有ζ相,ζ相升温放热转变为β相。在α相存在的温区里,ζ相经过长时间热处理并不转变为α相,同时,ζ相转变为β相的温度比α相高。与α→β的情况相同,β对ζ→β也有诱导作用。而且的ζ存在对α→β也有促进作用。θ相(θ1与θ2)与γ相一样,是相变过程的中间过渡相。
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A. N. Ivanov D. F. Litvin B. N. Savenko L. S. Smirnov V. I. Voronin A. E. Teplykh 《高压研究》2013,33(1-3):209-214
Abstract The design of a titanium-zirconium clamped cylinder-piston type pressure cell for neutron diffraction investigations under hydrostatic pressure up to 10 kbars without supports is described. It is the first time that Freon-11 has been used as a hydrostatic pressure transmitting medium. The following results carried out at the room temperature are presented: the discovery of the transition from I to 111 phase in a LiKSO4 single crystal and the results of the investigation on the influence of pressure upon the structure of the YBaCuO HTSC obtained by means of the powder diffraction method. 相似文献
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晶体学室相图与相变研究组 《物理学报》1977,26(5):199-207
本文用差热分析、恒温热处理、室温及高温X射线衍射等方法,对LiIO3晶体的相变问题进行了研究。弄清了升温过程中γ相的本质,它是并没有稳定存在的温度区间,只能在一定温度范围,一定时间内存在的,从α相转变为β相的过渡相。熔态LiIO3的冷凝过程不同于固态升温过程;这里存在着另一些新相——δ相。由于冷凝条件不同,因而结构也不尽相同,这些δ相在继续冷却时大部分转变为α相,但在未转变为α相之前,再度升温时,则转变为β相。从高温X射线衍射发现:差热分析曲线上所示的α←→γ和δ→α的相变温度是出现新相的温度,这时还伴随着大量的原有相的衍射线,随着时间的延长和温度的改变,原来的相才逐渐消失。同时也证实了γ→β的相变过程需要保温时间和β相的下种自催化作用。 相似文献
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S. G. Jabarov D. P. Kozlenko S. E. Kichanov A. V. Belushkin A. I. Mammadov B. N. Savenko R. Z. Mekhtieva C. Lathe 《Journal of Surface Investigation: X-ray, Synchrotron and Neutron Techniques》2012,6(3):546-551
The crystal structure of sodium niobate (NaNbO3) has been investigated by energy-dispersive X-ray diffraction at high pressures (up to 4.3 GPa) in the temperature range 300–1050 K. At normal conditions, NaNbO3 has an orthorhombic structure with Pbcm symmetry (antiferroelectric P phase). Upon heating, sodium niobate undergoes a series of consecutive transitions between structural modulated phases P-R-S-T(1)-T(2)-U; these transitions manifest themselves as anomalies in the temperature dependences of the positions and widths of diffraction peaks. Application of high pressure leads to a decrease in the temperatures of the structural transitions to the R, S, T(1), T(2), and U phases with different baric coefficients. A phase diagram for sodium niobate has been build in the pressure range 0–4.3 GPa and the temperature range 300–1050 K. The dependences of the unit-cell parameters and volume on pressure and temperature have been obtained. The bulk modulus and the volume coefficients of thermal expansion have been calculated for different structural modulated phases of sodium niobate. A phase transition (presumably, from the antiferroelectric orthorhombic P phase to the ferroelectric rhombohedral N phase) has been observed at high pressure (P = 1.6 GPa) and room temperature. 相似文献