006 18.04 3.712 3.731 3.721 3.725 3.724 3.727 008 25.43 3.762 3.730 3.735 3.731 3.729 0010 32.96 3.712 3.711 3.714
从以上计算可以证明我们的零点漂移计算方法是比较精确的,而且也证明了我们的误 差估计公式的正确性。经过零点校正,我们可以求得该Bi2201单晶的晶格常数:
hkl 004 006 008 0010 0012 0014 0016 0020
2q ( ) 14.46 21.76 29.15 36.68 44.36 52.27 60.45 77.99 d( ) 6.12073 4.08090 3.06090 2.44802 2.04039 1.74870 1.53017 1.22414 c( ) 24.4829 24.4854 24.4872 24.4802 24.4847 24.4818 24.4827 24.4828
从上表可以看出,经过零点漂移校正,尽管实验中衍射角测定范围较小(q<40度),但 晶格参数的相对误差已接近1×10-4。 经过长时间使用,发现我们的零点漂移校正公式非常实用。最近对电化学方法掺氧LaCu O4
+d的超导样品和郑东宁博士从英国带回的(Gd,Pb)Mo6S8样品的衍射数据都是经过零点 漂移校正以后才得出准确的晶格参数。
3.5.3未知晶体结构时零点漂移的校正
一个未知结构的Pr-Li-Ni-O体系的化合物,其衍射数据如下: 2Thetad(A)HeightAreaFWHMLine pair
14.286.19717112.22009.70.20001 17.085.18708429.06041.30.31032 18.524.78688372.010660.00.6195 25.243.5255715109.075974.70.1253 28.643.114297281.034662.70.12191 32.462.7559824664.0138512.00.1394 34.382.6063417423.0116272.00.15572 37.462.398812091.021900.00.2293 43.722.068755809.029656.00.1322 45.242.0027213188.065306.70.1207 49.321.846169258.046973.30.1215 56.121.637513232.019993.30.1484 56.441.628992025.012366.70.1371 57.241.608115062.025429.30.1157 59.061.562821342.07269.30.12411 60.201.535927466.044300.00.1356 67.901.379273203.019152.00.1325 70.061.341942043.010786.70.1243 72.241.306711986.014645.30.17062 77.801.22663642.05049.30.1604 78.781.213813255.020288.00.1393
......
使用原始数据用TREOR90程序未能指标化,经分析推测可能存在严重的零点漂移,使 用d值比例接近1:2:4的17.08 ,34.38 和72.24 的衍射线对,利用零点漂移校正公 式进行计算,得到零点漂移值为0.16 ,然后对衍射数据进行零点漂移校正,所得数据 用TREOR90成功地进行了指标化,得到品质因数M(20)=29,F(20)=19的结果,确定该化 合物为四方晶系,a=5.237,c=12.536,并进而解出了该化合物的晶体结构。
3.6指标化
利用3.5.1中经零点校正后的Si粉的衍射数据,可以编辑指标化输入控制文件如下:
Si粉的衍射数据指标化输入控制文件内容 si6
28.4371000 47.291493 56.107291 69.11559 76.35692 88.004103 94.92264 106.68033 114.05964 127.50844 136.85324
KH=4, KK=4, KL=4, KS=12, THS=0, OS1=0, MONO=0, SHORT=1, MERIT=10, NIX=1, IDIV=1,
WAVE=1.5405981, VOL=1000, CEM=25, D1=0.0002, SSQTL=0.05, CHOICE=3, TRIC=0, END*
利用以上指标化输入控制文件进行指标化得到的指标化结果如下:
VBVERSIONBYCHENGDONGBASEDONTREOR90 si6
28.4370001000 47.291000493 56.107000291 69.11500059 76.35600092 88.004000103 94.92200064 106.68000033 114.05900064 127.50800044 136.85300024
LINENUMBER=7SHOULDNOTBEINCLUDEDINTHETREOR BASELINESETS.SINESQUARETHETAFORTHISLINE=9 TIMESSINESQUARETHETAFORLINENUMBER=1
LINENUMBER=7WILLBESKIPPEDINTHETRIALPHASE. LINENUMBER=8SHOULDNOTBEINCLUDEDINTHETREOR BASELINESETS.SINESQUARETHETAFORTHISLINE=4 TIMESSINESQUARETHETAFORLINENUMBER=2
LINENUMBER=8WILLBESKIPPEDINTHETRIALPHASE. STOPLIMITS
FIGUREOFMERITREQUIRED=10
MAXNUMBEROFUNINDEXEDLINESINFIGUREOFMERITTEST=1 THE7FIRSTLINESADJUSTEDBYTHEIRHIGHERORDERS
CUBIC,TETRAGONAL,HEXAGONALANDORTHOROMBICSYMMETRY MAXCELLEDGE=25.0MAXCELLVOLUME=1000.0
D1=0.000200SSQTL=0.050000D2=0.000400WAVE=1.540598 NUMBEROFLINESWITHSQLESSTHAN0.327NOTEQUALTO9 NUMBEROFTESTLINES=4IQREQUIRED=1
**CUBICTEST*********************MAX.VOLUME=1000 SELECTEDBASELINES(1)(2)
BASELINEONE.(HKL)-MAX444MAXH+K+L=12 THISMAYBETHESOLUTION!!!
THEREFINEMENTOFTHECELLWILLNOWBEREPEATED THREECYCLESMORE.---GOODLUCK! CYCLERESULTS
0.0201100.0000000.0000000.0000000.0000000.000000 0.0201100.0000000.0000000.0000000.0000000.000000 0.0201100.0000000.0000000.0000000.0000000.000000 NUMBEROFSINGLEINDEXEDLINES=11
TOTALNUMBEROFLINES=11
A=5.4319280.000062AALFA=90.0000000.000000DEG. B=5.4319280.000062ABETA=90.0000000.000000DEG. C=5.4319280.000062AGAMMA=90.0000000.000000DEG. UNITCELLVOLUME=160.27
HKLSST-OBSSST-CALCDELTA2TH-OBS2TH-CALCD-OBSFREEPARAM. 1110.0603220.060330-0.00000828.43528.4373.13631000 2200.1608780.160879-0.00000147.29347.2941.9205493 3110.2211780.221209-0.00003156.10756.1111.6379291 4000.3217530.321759-0.00000669.11569.1161.358059 3310.3820560.382089-0.00003376.35676.3601.246292 4220.4825850.482638-0.00005388.00488.0101.1088103 5110.5429000.542968-0.00006994.92294.9301.045464 4400.6435130.643518-0.000005106.680106.6810.960233 5310.7038390.703848-0.000009114.059114.0600.918264 6200.8044360.8043970.000039127.508127.5020.858844 5330.8648010.8647270.000073136.853136.8410.828324 NUMBEROFOBS.LINES=11 NUMBEROFCALC.LINES=11 M(11)=297AV.EPS=0.0000297 F11=56.(0.004050,49)
MCF.J.APPL.CRYST.1(1968)108 FCF.J.APPL.CRYST.12(1979)60 0LINESAREUNINDEXED.
ANYCOMMONFACTORINTHEQUADRATICFORMS?? CHECKCONVERGENCEINTHEREFINEMENT (EV.USEPROGRAMPIRUMORPURUM) endsubOFINDEXINGCALCULATIONS SETKS=0TOCHECKTHESOLUTION..... ANDRUNTREORONCEMORE.
IFYOUWANTTOLOOKFORABETTERSOLUTIONYOU
MAYTRYTOINCREASETHEPARAMETERMERITABOVE297 ....ORPERHAPSTHISWASTHEBESTSOLUTION...
3.7由晶格参数计算衍射位置(dhkl)
以下给出利用PowderX程序中的dhkl功能计算得出的石英从10度到140度之间的衍射位
置和晶面间距(使用铜靶Ka1辐射):
SampleNameSiO2(Quartz)
Crystalsystem:HexagonalLatticeType:P Radiation:CuWaveLength:1.540598
LatticeParameter:a=4.9133b=4.9133c=5.4053 LatticeParameter:Alpha=90Beta=90Gama=120
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