首页> 外文期刊>Physics and Chemistry of Minerals >The thermal expansion and crystal structure of mirabilite (Na2SO4·10D2O) from 4.2 to 300 K, determined by time-of-flight neutron powder diffraction
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The thermal expansion and crystal structure of mirabilite (Na2SO4·10D2O) from 4.2 to 300 K, determined by time-of-flight neutron powder diffraction

机译:钛铁矿(Na 2 SO 4 ·10D 2 O)的热膨胀和晶体结构从4.2 K到300 K,由时间确定飞行中子粉末衍射

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We have collected high resolution neutron powder diffraction patterns from Na2SO4·10D2O over the temperature range 4.2–300 K following rapid quenching in liquid nitrogen, and over a series of slow warming and cooling cycles. The crystal is monoclinic, space-group P21/c (Z = 4) with a = 11.44214(4) Å, b = 10.34276(4) Å, c = 12.75486(6) Å, β = 107.847(1)°, and V = 1436.794(8) Å3 at 4.2 K (slowly cooled), and a = 11.51472(6) Å, b = 10.36495(6) Å, c = 12.84651(7) Å, β = 107.7543(1)°, V = 1460.20(1) Å3 at 300 K. Structures were refined to R P (Rietveld powder residual, RP = å| Itextobs - Itextcalc | mathord/ vphantom å| Itextobs - Itextcalc | åItextobs åItextobs R_{P} = {{sum {left| {I_{text{obs}} - I_{text{calc}} } right|} } mathord{left/ {vphantom {{sum {left| {I_{text{obs}} - I_{text{calc}} } right|} } {sum {I_{text{obs}} } }}} right. kern-nulldelimiterspace} {sum {I_{text{obs}} } }} ) better than 2.5% at 4.2 K (quenched and slow cooled), 150 and 300 K. The sulfate disorder observed previously by Levy and Lisensky (Acta Cryst B34:3502–3510, 1978) was not present in our specimen, but we did observe changes with temperature in deuteron occupancies of the orientationally disordered water molecules coordinated to Na. The temperature dependence of the unit-cell volume from 4.2 to 300 K is well represented by a simple polynomial of the form V = − 4.143(1) × 10−7 T 3 + 0.00047(2) T2 − 0.027(2) T + 1437.0(1) Å3 (R 2 = 99.98%). The coefficient of volume thermal expansion, α V , is positive above 40 K, and displays a similar magnitude and temperature dependence to α V in deuterated epsomite and meridianiite. The relationship between the magnitude and orientation of the principal axes of the thermal expansion tensor and the main structural elements are discussed; freezing in of deuteron disorder in the quenched specimen affects the thermal expansion, manifested most obviously as a change in the behaviour of the unit-cell parameter β.
机译:快速淬火后,我们在4.2–300 K的温度范围内从Na 2 SO 4 ·10D 2 O收集了高分辨率中子粉末衍射图在液氮中,以及一系列缓慢的加热和冷却周期。晶体为单斜晶体,空间群P2 1 / c(Z = 4),a = 11.44214(4)Å,b = 10.34276(4)Å,c = 12.75486(6)Å,β = 107.847(1)°,V = 1436.794(8)Å 3 在4.2 K(缓慢冷却)下,a = 11.51472(6)Å,b = 10.36495(6)Å,c = 12.84651(7)Å,β= 107.7543(1)°,V = 1460.20(1)Å 3 在300 K.结构细化为R P (Rietveld粉末残留,R P =å| I textobs -I textcalc | mathord / vphantomå| I textobs -I < sub> textcalc |åI textobs åI textobs R_ {P} = {{sum {left | {I_ {text {obs}}-I_ {text { calc}}}右|}} mathord {left / {vphantom {{sum {left | {I_ {text {obs}}-I_ {text {calc}}}} right |}}} {sum {I_ {text {obs} }}}}}对。kern-nulldelimiterspace} {sum {I_ {text {obs}}}}}))在4.2 K(淬火和慢冷),150和300 K时优于2.5%。 Levy和Lisensky(Acta Cryst B34:3502–3510,1978)没有出现在我们的标本中,但我们我观察到与Na配位的定向无序水分子的氘核占据度随温度的变化。一个简单的多项式形式V = − 4.143(1)×10 −7 T 3 + 0.00047(2)T 2 -0.027(2)T + 1437.0(1)Å 3 (R 2 = 99.98%)。在40 K以上时,体积热膨胀系数α V 为正,并且在重晶石和美铁矿中显示出与α V 相似的量级和温度依赖性。讨论了热膨胀张量主轴的大小和方向与主要结构元素之间的关系;淬灭样品中氘核失稳的冻结影响热膨胀,最明显表现为晶胞参数β行为的变化。

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