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揭示了低温流体~3He的热导率在液态区随温度和压力两个状态参数变化的反常规律。综合该反常规律以及热导率在临界点附近的突变特性,首次提出了~3He在0.003 K至临界温度3.3157 K温区内完整的饱和线热导率方程以及压力高至20 MPa的压缩液相区热导率方程。方程计算值与实验数据相对偏差小于±1.5%,与高精度实验数据偏差小于±0.4%,并且在极低温条件下光滑过渡为由量子理论预测的理论极限. 相似文献
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《工程热物理学报》2021,42(6):1378-1383
针对离子液体[BMP] [Tf_2N]的物性数据缺乏的问题,本文在101.325 KPa下对[BMP] [Tf_2N]在温度范围为278.15~338.15 K的黏度和温度范围为298.15~338.15 K的密度、电导率进行了实验测定,结果表明:黏度、密度和电导率均受温度的影响较大,当压力一定时,[BMP] [Tf_2N]的黏度、密度随温度的升高而减小;而电导率随温度的升高而增大;通过选择分别用Arrhenius方程、自然对数方程和VFT方程关联[BMP] [Tf_2N]的黏度、密度和电导率;结果表明:模型值与实验值的最大相对误差和平均相对误差分别是2.25%和0.94%;5.74%和5.399;4.41%和4.24%。 相似文献
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气体压力光学非接触测量是目前激光技术重要应用领域之一,其中气压测量过程中温度耦合问题是现在面临的研究难点。故而提出一种光谱测量技术与激光干涉技术组合测量方法,通过积分吸光度和折射率融合的方式实现气体压力、温度解耦的目的。分析可调谐半导体激光光谱技术(TDLAS)的直接吸收法测量原理和基于折射率的激光干涉测量原理,建立基于吸收光谱的气压测量模型和基于折射率的激光干涉气压测量模型,通过利用三次多项式拟合吸收谱线强度函数的方式,建立了基于积分吸光度和折射率的气体压力、温度解耦的数学模型。实验搭建了基于TDLAS技术和激光干涉技术的气体压力检测系统,采用中心波长为2 004 nm的可调谐半导体激光器和波长为632.8 nm的激光干涉仪,气室长度为24.8 cm,将CO2作为研究对象,并以高精度压力控制器和温度传感器的测量结果分别作为压力温度参考值,以真空为背景信号,在室温环境中测量并计算出气体压力变化后积分吸光度值和折射率值,进而解算得到气体压力和温度值。实验结果显示:压力测量结果最大相对误差为3.61%,最小相对误差为0.5%,测量平均相对误差为1.99%;在以开尔文温度为前提下,温度解算结果最大绝对误差为7.66 K,最小绝对误差为0.78 K,测量平均绝对误差为3.29 K,测量结果与参考结果具有较高的吻合度,该研究可为以后光学法测量气体压力温度影响分析提供参考。 相似文献
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《工程热物理学报》2016,(1)
本文采用汽液双循环法测量了新型环保制冷剂R134a+DME在(253.15~273.15)K时的汽液相平衡数据。所测实验数据采用PR+LCVM+Wilson模型进行了关联,汽相组分的平均绝对误差绝对值为0.0043,最大绝对误差绝对值为0.0222;体系压力的平均相对误差绝对值为0.65%,最大相对误差绝对值为1.05%。关联结果和实验数据一致性较好,说明此模型能很好地描述该体系在实验条件下的汽液相平衡数据。从实验结果发现,R134a+DME是一种共沸制冷剂,处于共沸点时R134a摩尔组分0.4左右,而且该混合物在整体组分变化范围内的温度滑移也非常小。 相似文献
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Bai JZ Ban Y Bian JG Cai X Chang JF Chen HF Chen HS Chen HX Chen J Chen JC Chen J Chen ML Chen YB Chi SP Chu YP Cui XZ Dai HL Dai YS Deng ZY Dong LY Du SX Du ZZ Fang J Fang SS Fu CD Fu HY Fu LP Gao CS Gao ML Gao YN Gong MY Gong WX Gu SD Guo YN Guo YQ Guo ZJ Han SW Harris FA He J He KL He M He X Heng YK Hu HM Hu T Huang GS Huang L Huang XP Ji XB Jia QY Jiang CH Jiang XS Jin DP Jin S Jin Y Lai YF Li F Li G Li HH Li J Li JC Li QJ Li RB Li RY Li SM Li W Li WG Li XL Li XQ Li XS Liang YF Liao HB 《Physical review letters》2004,92(5):052001
The decay psi(2S)-->K(0)(S)K(0)(L) is observed using psi(2S) data collected with the Beijing Spectrometer at the Beijing Electron-Positron Collider; the branching fraction is determined to be B(psi(2S)-->K(0)(S)K(0)(L))=(5.24+/-0.47+/-0.48)x10(-5). Compared with J/psi-->K(0)(S)K(0)(L), the psi(2S) branching fraction is enhanced relative to the prediction of the perturbative QCD "12%" rule. The result, together with the branching fractions of psi(2S) decays to other pseudoscalar meson pairs (pi(+)pi(-) and K+K-), is used to investigate the relative phase between the three-gluon and the one-photon annihilation amplitudes of psi(2S) decays. 相似文献
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C. D. Armeniades I. Kuriyama J. M. Roe Eric Baer 《Journal of Macromolecular Science: Physics》2013,52(4):777-791
The mechanical behavior of poly(ethylene terephthalate) (PET) was studied at temperatures from 4 to 300°K with a free oscillating torsion pendulum and an Instron tester. Torsion pendulum data show the presence of relaxation maxima below 80°K. Noncrystalline specimens show a small peak at 48°K (δ) and a shoulder at 8-12° K (?). A peak at 20° K is observed in crystalline samples, both oriented and unoriented. In addition drawn specimens show a pronounced peak at 48° K and the assymmetric maximum in the 100-240° K region is split into two peaks. The logarithmic decrement in the β-loss region decreases with increasing crystallinity and orientation, while the cryogenic loss peaks increase in intensity. Tensile tests with biaxially oriented and heat-set films show a twofold increase in elastic modulus and a tenfold increase in toughness at cryogenic temperatures when compared with “amorphous” PET. 相似文献
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研究了温度对聚合物poly(9,9-dioctylfluorene-co-benzothiadiazole)(F8BT)和poly(3-hexylthiophene)(P3HT)共混薄膜的放大自发辐射(ASE)的影响。在80~320 K温度范围测试了不同P3HT质量比的共混聚合物薄膜和纯F8BT薄膜的ASE特性。在室温条件下,共混聚合物的阈值随着P3HT所占比例的增加先降低后升高。当P3HT比例约为20%时,阈值最低约为2.59×10~3W/cm~2。当温度从320 K下降到80 K时,纯F8BT薄膜的ASE阈值光功率由5.36×10~3W/cm~2下降到4.15×10~3W/cm~2,P3HT质量比为20%的共混薄膜的ASE阈值光功率由2.84×10~3W/cm~2下降到2.03×10~3W/cm~2。在一特定泵浦光功率(5.29×10~3W/cm~2)下,当温度由320 K下降至80 K时,ASE强度约提高4倍。随着温度的降低,混合物薄膜的ASE峰位红移,移动达12 nm。 相似文献
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Choi KY Wang Z Ozarowski A van Tol J Zhou HD Wiebe CR Skourski Y Dalal NS 《J Phys Condens Matter》2012,24(24):246001
We report pulse-field magnetization, ac susceptibility, and 100 GHz electron spin resonance (ESR) measurements on the S = 5/2 two-dimensional triangular compound Ba3NbFe3Si2O14 with the Néel temperature T(N) = 26 K. The magnetization curve shows an almost linear increase up to 60 T with no indication of a one-third magnetization plateau. An unusually large frequency dependence of the ac susceptibility in the temperature range of T = 20-100 K reveals a spin-glass behavior or superparamagnetism, signaling the presence of frustration-related slow magnetic fluctuations. The temperature dependence of the ESR linewidth exhibits two distinct critical regimes; (i) ΔH(pp)(T) is proportional to (T-T(N))(-p) with the exponent p = 0.2(1)-0.2(3) for temperatures above 27 K, and (ii) ΔH(pp)(T) is proportional to (T-T*)(-p) with T* = 12 K and p = 0.8(1)-0.8(4) for temperatures between 12 and 27 K. This is interpreted as indicating a dimensional crossover of magnetic interactions and the persistence of short-range correlations with a helically ordered state. 相似文献
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H. Metzner G. Sulzer W. Seelinger B. Ittermann H. -P. Erank B. Fischer K. -H. Ergezinger R. Dippel E. Diehl H. -J. Stöckmann H. Ackermann 《Hyperfine Interactions》1990,60(1-4):769-772
Using β-NMR with12B as nuclear probes the temperature dependence of the lattice-site occupation of boron implanted into heavily doped silicon
is studied. In p-type material the unperturbed substitutional fraction of12B increases from 10% at 300 K to ≃40 % at 950 K. In n-type material this fraction starting from 20% at 300 K approaches the
saturation value of ≃80 % at 600 K already. This behaviour suggests that the site of implanted boron in silicon is controlled
by the Fermi level. 相似文献
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Zhou Y Bowler BE Eaton GR Eaton SS 《Journal of magnetic resonance (San Diego, Calif. : 1997)》2000,144(1):115-122
The temperature dependence of spin-lattice relaxation rates was analyzed for four high-spin nonheme iron proteins between 5 and 20 K, for three high-spin iron porphyrins between 5 and 118 K, and for four high-spin heme proteins between 5 and 150 to 298 K. For the nonheme proteins the zero-field splittings, D, are less than 0.7 cm(-1), and the relaxation is dominated by the Orbach and Raman processes. For the iron porphyrins and heme proteins D is between 4 and 12 cm(-1) and the relaxation is dominated by the Orbach process between about 5 and 100 K and by a local mode at higher temperatures. The relaxation rates for the heme proteins in glassy matrices extrapolated to values at room temperature that are similar to values obtained by NMR relaxivity in fluid solution. This similarity suggests that for high-spin Fe(III) heme proteins with effective intramolecular spin-lattice relaxation processes, the additional motional freedom gained when a relatively large protein goes from glassy solid to liquid solution at room temperature has little impact on spin-lattice relaxation. 相似文献
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采用激射波长为850 nm的AlGaInAs/AlGaAs梯度折射率波导分别限制增益量子阱结构的外延片,分别制备了具有锥形结构和条形结构的半导体激光器,并对比分析了两者的温度特性。结果显示,测试温度为20~70℃时,锥形结构器件的特征温度为164 K,远高于条形结构器件的96 K;占空比为0.5%(t=50μs,f=100 Hz),1 000 mA脉冲电流注入条件下,锥形激光器和条形激光器的波长漂移系数分别为0.25和0.28 nm/K;测试温度〈50℃时,锥形激光器和条形激光器的光谱半高宽分别约为1.12和1.24 nm。实验结果表明:相同外延层结构条件下,锥形激光器比条形激光器拥有更高的特征温度。 相似文献
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A. Benfredj D. Gamra S. Romdhane T. Barhoumi C. Guthmann J.L. Monge H. Bouchriha 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,19(3):385-391
The effect of a magnetic field (6 kG) on the delayed fluorescence in a 1,4-Dibromonaphtalene at 300 K and 20 K is analysed
using a new approach of calculation of the triplet-triplet annihilation rate constant. The agreement of the best fit between
experiment and theory allows reaching at 300 K and 20 K respectively the lifetimes and the interaction constant of the triplets
pairs.
Received 12 March 1999 and Received in final form 27 April 2000 相似文献
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P.M. Silvaggio D. Goorvitch R.W. Boese 《Journal of Quantitative Spectroscopy & Radiative Transfer》1981,26(2):103-106
A theoretical fit has been made to oue laboratory measurements of the 2-0 collisionally induced H2 absorption band for temperatures of 122 and 273.3 K and at a density of 20 amagats. A Lennard-Jones 6–12 intermolecular potential and a Birnbaum-Cohen line profile have been used. The fit resulted in a chi-square of 0.2%. Line widths have also been derived as a function of temperature. The lifetimes of the states have been calculated. 相似文献
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Rosner JL Alexander JP Cassel DG Duboscq JE Ehrlich R Fields L Gibbons L Gray R Gray SW Hartill DL Heltsley BK Hertz D Jones CD Kandaswamy J Kreinick DL Kuznetsov VE Mahlke-Krüger H Mohapatra D Onyisi PU Patterson JR Peterson D Riley D Ryd A Sadoff AJ Shi X Stroiney S Sun WM Wilksen T Athar SB Patel R Yelton J Rubin P Eisenstein BI Karliner I Mehrabyan S Lowrey N Selen M White EJ Wiss J Mitchell RE Shepherd MR Besson D Pedlar TK Cronin-Hennessy D Gao KY Hietala J Kubota Y Klein T Lang BW 《Physical review letters》2008,100(22):221801
We exploit the quantum coherence between pair-produced D0 and D[over]0 in psi(3770) decays to study charm mixing, which is characterized by the parameters x and y, and to make a first determination of the relative strong phase delta between D0-->K+pi- and D[over]0-->K+pi-. Using 281 pb(-1) of e+e- collision data collected with the CLEO-c detector at Ecm=3.77 GeV, as well as branching fraction input and time-integrated measurements of RM identical with (x2 + y2)/2 and RWS identical with Gamma(D0-->K+pi-)/Gamma(D[over]0-->K+pi-) from other experiments, we find cosdelta=1.03(-0.17)(+0.31)+/-0.06, where the uncertainties are statistical and systematic, respectively. By further including other mixing parameter measurements, we obtain an alternate measurement of cosdelta=1.10+/-0.35+/-0.07, as well as x sindelta=(4.4(-1.8)(+2.7)+/-2.9)x10(-3) and delta=(22(-12-11)(+11+9)) degrees . 相似文献