Ca2YO(BO3)3晶体的热物理性质研究

测量了新型非线性激光晶体Ca2YO(BO3)3（YCOB）的比热及其沿a,b,c三个方向的热膨胀系数，热扩散系数，导热系数，声子平均自由程和等效声速等热物理性质；讨论了属于单斜晶系的YCOB晶体的热物性的各向异性行为；实验结果表明YCOB晶体具有较大的比热和导热系数，其热膨胀系数各向异性相对较小，具有良好的热物理和力学性能。     

Ca2YO(BO3)3晶体的热物理性质研究

测量了新型非线性激光晶体Ca2YO(BO3)3(YCOB)的比热及其沿a、b、c三个方向的热膨胀系数、热扩散系数、导热系数、声子平均自由程和等效声速等热物理性质;讨论了属于单斜晶系的YCOB晶体的热物性的各向异性行为;实验结果表明YCOB晶体具有较大的比热和导热系数,其热膨胀系数各向异性相对较小,具有良好的热物理和力学性能.     

空间和地面生长LiIO3晶体比热的对比研究

用差示扫描量热计（DSC）测定了空间和地面生长的碘酸锂晶体在-100～350℃温度范围内的比热，据此分别给出了相应的计算比热的经验方程．经验方程计算值和实验值之间的最大百分偏差＜±1％.结果显示，空间和地面生长LiIO3晶体的比热在测量温度范围内无明显差别．     

高质量自调Q激光晶体Cr4+,Nd3+:Gd3Ga5O12的生长

用固相合成、共沉淀等方法合成了Cr4+,Nd3+GGG晶体的单相多晶材料.讨论了共沉淀法和固相合成法合成GGG单相的技术参数.用合成的单相多晶原料生长了高质量的Cr4+,Nd3+GGG单晶.通过测晶体的光谱性质发现Cr4+,Nd3+GGG晶体在400nm和520nm附近存在Cr3+离子的强的吸收峰.在808nm附近存在Nd3+离子宽的吸收带,能与InGa二极管激光有效的耦合;在1100附近有Cr4+的较强的吸收带,可实现对Nd3+的自调Q输出.Cr4+,Nd3+GGG晶体的荧光光谱与NdGGG晶体的一样,发光中心也位于1062nm,但其强度约为NdGGG的1/5～1/6.Cr4+,Nd3+GGG晶体是一种非常有潜力的自调Q激光晶体,可以实现大功率激光器的小型化和全固化.     

基于激光闪射法测量某内燃机铝合金活塞的热物性参数

基于激光闪射法,采用闪射法导热仪测量了不同温度下某内燃机铝合金活塞的比热容、热扩散系数及导热系数。结果表明：随着温度的升高,该内燃机铝合金活塞的热扩散系数逐渐减小,比热容逐渐升高,导热系数在一定温度范围内呈逐渐增大的趋势。     

掺钕氟磷酸锶单晶研究

为探索和评价新型激光晶体掺钛氟磷酸银Nd：Sr5（PO4）3F（Nd：SFAP）在制作激光器方面的应用，对其生长、结构、光谱与激光特性及一些物理性能进行了系统研究．采用Czochralski法成功地生长出单晶；用先进的设备对所生长之晶体进行了有关测量，并进行了以激光二极管为泵浦源、该晶体为工作物质的激光实验．结果表明：晶体生长中Nd的有效分凝系数为0.52；理想的泵浦光应是806um的π偏振光，荧光寿命为175μs；泵浦阈值15mW，斜效率为31．8％研究结论为：Nd：SFAP晶体是制作小型LD泵浦激光器的理想材料，但用它制作较大功率激光器是不合适的     

热障涂层用Nd2O3-CeO2-ZrO2陶瓷粉末制备及其性能研究

采用化学沉淀法制备了热障涂层用Nd2Zr2O7(NZ)以及CeO2-Nd2O3-ZrO2(NCZ)陶瓷粉末.通过电感耦合等离子体原子发射光谱(ICP-AES),X射线衍射、DSC及霍尔流速计对粉末化学组成、相组成,高温相稳定性和流动性能进行了研究.通过高温膨胀仪、DSC和激光热导仪分别测定其热膨胀系数和导热系数.结果表明,掺杂的NCZ粉末保持了NZ的烧绿石相结构, 120℃时粉末为无定形的混合氧化物,900℃时转化为复合氧化物,1200℃时转变为单一的锆酸钕烧绿石相;高温下NCZ无明显相变;在高于1400℃的温度下煅烧后,NCZ的流动性得到显著改善;添加CeO2可提高锆酸钕的热膨胀系数,而对其导热系数和比热系数的影响不大.     

石墨烯/聚丙烯复合材料导热性能测量分析研究

针对现有文献报道的石墨烯/PP复合材料导热系数测量结果差异较大,该文对相应测量方法、仪器、样品尺寸和测量结果等进行分析和评价。制备质量分数为5%至30%的石墨烯/PP复合材料块状和薄片状等样品,分别通过QTM500型、TC3000型和DRE-Ⅲ型3种瞬态导热系数测试仪对块状样品导热系数进行直接测量,并通过LFA467型激光闪光法导热仪、DSC3+型差示扫描量热仪和ZB603C型电子天平和密度组件分别对各质量分数石墨烯/PP复合材料样品的热扩散系数、比热容和密度进行测量后计算获得导热系数。结果表明：3种瞬态导热系数测试仪测量纯PP、5%和10%质量分数石墨烯/PP复合样块导热系数偏差在2.6%～8.7%范围内,大于各仪器声称测量偏差;直接测量法与间接测量法获得的导热系数偏差大于36%,且随石墨烯质量分数的增加而变大。因此,在测量复合材料导热系数时应选择适用尺寸和量程的直接测量法,导热系数等热物性参数的量值传递体系仍需进一步建立和完善来提高直接测量法的准确性和间接测量法的可靠性。     

Nd:GdxY1-xCa4O(BO3)3晶体的生长及其光谱性能研究

利用熔体提拉法生长了大尺寸,高质量的新型激光自倍频晶体Nd:GdxY1-x(Ca4O(BO3)3(简称Nd:GdYCOB),对Nd:GdYCOB晶体的XRD衍射图进行指标化,得到它的晶胞参数为a=8.080A;b=16.016A;c=3.538A,β＝101．18,μ＝491．1A3,对取自不同部位的晶体粉末进行ICP原子发射光 分析表明晶体整体组份均匀一致,根据熔体和晶体粉末的ICP数据计算,Nd:GdYCOB晶体中Nd3 的分凝系数为0．63,首次报道了Nd:GdYCOB晶体200－3000nm室温透过光谱和室温荧光光谱及荧光寿命,室温透过光谱表明Nd:GdYCOB晶体的紫外吸收边在－220nm,具有很宽的透光波段（－220－2700nm);Nd:GdYCOB晶体在800nm附近存在很强的吸收,适合于LD泵汪,为光光谱表明Nd:GdYCOB晶体是一种很有潜力的RGB（red,green,blue)激光自倍频晶体,掺杂4％,5％ Nd:GdYCOB晶体的荧光寿命分别为105us和100us。     

Yb0.03Y0.19Gd0.78VO4晶体的生长和性能

液相合成了Yb∶YGdVO4多晶料,采用中频感应加热Czochralski法生长了Yb0.03Y0.19Gd0.78VO4晶体.用浮力法测定其密度为5.29g/cm3,X射线粉末衍射分析表明它的结构与YVO4和GdVO4的晶体结构相同,并计算出了它的晶胞参数为a0=b0=0.7191nm,c0=0.6329nm.用激光脉冲法测量了晶体的热扩散系数,比较了晶体a轴和c轴的热扩散系数随温度的变化关系.实验表明Yb0.03Y0.19Gd0.78VO4晶体有希望适合作为LD泵浦的激光晶体材料.     

Studies on the growth and physical properties of nonlinear optical crystal: 2-Amino-5-nitropyridinium-toluenesulfonate

Single crystals of 2-amino-5-nitropyridinium-toluenesulfonate (2A5NPT) were grown by the slow cooling method. The unit cell dimensions were determined from single crystal X-ray diffraction studies. The thermal parameters - thermal diffusivity (α), thermal effusivity (e), thermal conductivity (K) and heat capacity (C_p) of 2A5NPT were measured by an improved photopyroelectric technique at room temperature. Single and multiple shot experiments performed on the grown crystals for the second harmonic of pulsed Nd:YAG laser (532 nm) show that it exhibits a high laser damage threshold which is a favorable property for nonlinear optical applications. Dielectric constant and dielectric loss of the grown crystal were evaluated for the frequency range 1 kHz-1 MHz in the temperature region 40-130 °C. Hardness values were measured using Vickers hardness measurement.     

Li2B4O7晶体的比热,导温和导热性能

用ＤＳＣ和激光热导人义分别测定了Ｌｉ２Ｂ４Ｏ７（ＬＢＯ）晶体３５０－９７０Ｋ范围内的比热和６３０－９７０Ｋ范围内不同主晶轴方向的导温系数，并由此了导热系数和声子平均自由程。     

Nd3+:Y0.5Gd0.5VO4晶体生长和基本特性

Nd^3 :Y0.5Gd0.5VO4晶体作为一种新的激光材料，可以用中频感应加热提拉法生长。X射线粉末衍射分析表明它的结构与Nd^3 :YVO4晶体结构相同，它的晶格常数介于YVO4和NdVO4晶格常数之间。用ICP光谱法测定晶体中Nd^3 含量为0．8at％，分凝系数为0．8，与Nd^3 :GdVO4晶体中Nd^3 的分凝系数0．78相当；用称重法测定其密度为5．00g／cm^3；用稳态纵向热流法测出其室温热导率为12．5W／mK。实验表明Nd^3 :Y0.5Gd0.5VO4晶体有希望作为高功率ID泵浦激光晶体材料。     

Simultaneous measurements of thermal conductivity and thermal diffusivity of Se90?xTe5Sn5Inx (x?=?0, 3, 6, and 9) multi-component chalcogenide glasses

Measurements of thermal conductivity and thermal diffusivity of twin pellets of Se_90−x Te₅Sn₅In _x (x = 0, 3, 6, and 9) chalcogenide glasses were carried out at room temperature using transient plane source technique. The measured values of thermal conductivity and thermal diffusivity were used to determine the specific heat per unit volume of these glasses in the composition range of investigation. Results indicated that both values of thermal conductivity and thermal diffusivity were increased with addition of indium concentration at the cost of selenium, whereas the specific heat per unit volume was slightly decreases with increase of indium content. This compositional dependence behavior of the thermal conductivity and diffusivity can be explained in terms of the iono-covalent type of bonds, which In (indium) makes with Se as it is incorporated in the Se–Te–Sn glass.     

Thermal-Diffusivity Dependence on Temperature of Gadolinium Calcium Oxoborate Single Crystals

Thermal diffusivities of pure and doped gadolinium calcium oxoborate (GdCOB) single crystals were measured as a function of the temperature along optical indicatrix axes X, Y, and Z. Three GdCOB samples were investigated, chemically pure single crystal, the one doped with 4 at% of Nd and the next one doped with 7 at% of Yb. Measurements were carried out for temperature range 40 °C to 300 °C. Determination of the thermal diffusivity based on an analysis of thermal wave propagation in the sample. For a detection of temperature disturbance propagating in the sample the mirage effect was used. Obtained results show that the thermal diffusivity decreases with the increase of sample temperature for all investigated crystals. The GdCOB single crystals reveal a strong anisotropy. The thermal diffusivity along Y direction has the highest value while values obtained in X and Z axes are much lower. Dopants cause decrease in the thermal diffusivity for all investigated directions.     

Photoacoustic investigations on thermal anisotropy in urea l-malic acid single crystals

Laser-induced photoacoustic technique in the closed cell configuration has been employed to study the anisotropy in thermal parameters of urea l-malic acid, a nonlinear optical crystal. Thermal diffusivity values of the specimen along different crystallographic axes are evaluated from the measured amplitude and phase spectra of photoacoustic signal using one-dimensional model of Rosencwaig and Gersho. Thermal conductivity of the crystal along different axes is calculated using the measured thermal diffusivity and specific heat values. The measured thermal parameters are correlated with mechanical hardness as well as the bonding scheme of the crystal. Analyses of the results show that there is considerable anisotropy in heat diffusion parameters along different crystal orientations. Results are explained on the basis of crystallographic structure and the phonon-assisted heat diffusion mechanism in crystals.     

锗酸铋（Bi4Ge3O12）单晶热物理性质的研究

本文用不同的测试技术和方法测定了锗酸铋(BGO)单晶的比热(300～800K)热膨胀系数(100～1100K)和导温系数(140～700K),进而导出了 BGO 单晶不同温度下的导热系数、定容比热、德拜温度和格虑内森数。本文还对 BGO 单晶热物理性质的变化规律作了理论解释。     

Study of the Thermal Properties of a Ni<Subscript>3</Subscript>Ta Shape Memory Alloy

Dilatation characteristics, thermal diffusivity, and thermal conductivity of a Ni₃Ta shape memory alloy were studied over the temperature range from room temperature up to 950 °C. The Ni₃Ta alloy was investigated in both polycrystalline and single crystal forms. The shape memory effect was positive for the polycrystalline samples and negative for the single crystal. While the transformation temperature of the M (martensite) → A (austenite) phase transformation was the same for both types of alloys and all measurements, the transformation temperature for the reverse phase transformation A → M was dependent on the maximum cycle temperature. Higher maximum temperatures of the thermal cycle yielded lower transformation temperatures for the A → M transformation. The thermal diffusivity and thermal conductivity of the austenite were higher than those of the martensite. No latent heat was found for the phase transformations.     

Thermal conductivity and diffusivity measurements at cryogenic temperatures by double specimen technique

A double specimen technique is used in measuring the thermal conductivity and diffusivity of low thermal conductivity materials. In this technique good thermal contact is maintained between the heat source and sink and two geometrically similar specimens. A thin-copper heater plate is compressed between the two specimens and the temperature difference is measured between the heat source and the temperature controlled heat sink. Thermal conductivity is determined at steady state conditions by the differential method while the diffusivity is determined from transient measurements combined with an analytical solution to the one dimensional solution of the diffusion equation.