International
Tables for
Crystallography
Volume C
Mathematical, physical and chemical tables
Edited by E. Prince

International Tables for Crystallography (2006). Vol. C. ch. 4.4, pp. 454-461

Section 4.4.5. Magnetic form factors

P. J. Browna

4.4.5. Magnetic form factors

| top | pdf |

The form factors used in the calculations of the cross sections for magnetic scattering of neutrons are defined in Subsection 6.1.2.3[link] as [\langle\, j_l(k)\rangle =\textstyle \int\limits^\infty_0\,U^2(r)\, j_l(kr)4\pi r^2\,{\rm d} r, \eqno (4.4.5.1)]in which U(r) is the radial wavefunction for the unpaired electrons in the atom, k is the length of the scattering vector, and [j_l(kr)] is the lth-order spherical Bessel function.

Tables 4.4.5.1[link][link][link][link][link][link][link]–4.4.5.8[link] give the coefficients in an analytical approximation to the [\langle \,j_0\rangle] magnetic form factors for the 3d and 4d transition series, the 4f electrons of rare-earth ions, and the 5f electrons of some actinide ions. The approximation has the form used by Forsyth & Wells (1959[link]) but allowing three instead of two exponential terms: [\eqalignno{ \langle\, j_0(s)\rangle &=A\exp(-as^2)+B\exp(-bs^2) \cr &\quad +C\exp(-cs^2)+D, &(4.4.5.2)}]where s is the value of [(\sin\theta)/\lambda] in Å−1.

Table 4.4.5.1| top | pdf |
j0〉 form factors for 3d transition elements and their ions

Atom or ionAaBbCcDe
Sc0.251290.0300.329039.4020.423514.322−0.00430.2029
Sc+0.488951.1600.520314.076−0.02860.1790.01850.1217
Sc2+0.504831.4030.518610.990−0.02411.1830.00000.0578
Ti0.465733.5900.54909.879−0.02910.3230.01230.1088
Ti+0.509336.7030.503210.371−0.02630.3110.01160.1125
Ti2+0.509124.9760.51628.757−0.02810.9160.00150.0589
Ti3+0.357122.8410.66888.931−0.03540.4830.00990.0575
V0.408628.8110.60778.544−0.02950.2770.01230.0970
V+0.444432.6480.56839.097−0.22850.0220.21500.1111
V2+0.408523.8530.60918.246−0.16760.0410.14960.0593
V3+0.359819.3360.66327.617−0.30640.0300.28350.0515
V4+0.310616.8160.71987.049−0.05210.3020.02210.0433
Cr0.113545.1990.348119.4930.54777.354−0.00920.1975
Cr+−0.09770.0470.454426.0050.55797.4890.08310.1114
Cr2+1.2024−0.0050.415820.5480.60326.956−1.22180.0572
Cr3+−0.30940.0270.368017.0350.65596.5240.28560.0436
Cr4+−0.23200.0430.310114.9520.71826.1730.20420.0419
Mn0.243824.9630.147215.6730.61896.540−0.01050.1748
Mn+−0.01380.4210.423124.6680.59056.655−0.00100.1242
Mn2+0.422017.6840.59486.00500.0043−0.609−0.02190.0589
Mn3+0.419814.2830.60545.4690.9241−0.009−0.94980.0392
Mn4+0.376012.5660.66025.133−0.03720.5630.00110.0393
Fe0.070635.0080.358915.3580.58195.561−0.01140.1398
Fe+0.125134.9630.362915.5140.52235.591−0.01050.1301
Fe2+0.026334.9600.366815.9430.61885.594−0.01190.1437
Fe3+0.397213.2440.62954.903−0.03140.3500.00440.0441
Fe4+0.378211.3800.65564.592−0.03460.4830.00050.0362
Co0.413916.1620.60134.780−0.15180.0210.13450.1033
Co+0.099033.1250.364515.1770.54705.008−0.01090.0983
Co2+0.433214.3550.58574.608−0.03820.1340.01790.0711
Co3+0.390212.5080.63244.457−0.15000.0340.12720.0515
Co4+0.351510.7780.67784.234−0.03890.2410.00980.0390
Ni−0.017235.7390.317414.2690.71364.566−0.01430.1072
Ni+0.070535.8560.398413.8040.54274.397−0.01180.0738
Ni2+0.016335.8830.391613.2230.60524.339−0.01330.0817
Ni3+0.001235.0000.346811.9870.66674.252−0.01480.0883
Ni4+−0.009035.8610.277611.7900.74744.201−0.01630.0966
Cu0.090934.9840.408811.4430.51283.825−0.01240.0513
Cu+0.074934.9660.414711.7640.52383.850−0.01270.0591
Cu2+0.023234.9690.402311.5640.58823.843−0.01370.0532
Cu3+0.003134.9070.358210.9140.65313.828−0.01470.0665
Cu4+−0.013230.6820.280111.1630.74903.817−0.01650.0767

Table 4.4.5.2| top | pdf |
j0〉 form factors for 4d atoms and their ions

Atom or ionAaBbCcDe
Y0.591567.6081.512317.900−1.113014.1360.00800.3272
Zr0.410659.9961.054318.648−0.475110.5400.01060.3667
Zr+0.453259.5950.783421.436−0.24519.0360.00980.3639
Nb0.394649.2301.319714.822−0.72699.6160.01290.3659
Nb+0.457249.9181.027415.726−0.49629.1570.01180.3403
Mo0.180649.0571.230614.786−0.42686.9870.01710.4135
Mo+0.350048.0351.030515.060−0.39297.4790.01390.3510
Tc0.129849.6611.165614.131−0.31345.5130.01950.3869
Tc+0.267448.9570.956915.141−0.23875.4580.01600.3412
Ru0.106949.4241.191212.742−0.31764.9120.02130.3597
Ru+0.441033.3091.47759.553−0.93616.7220.01760.2608
Rh0.097649.8821.160111.831−0.27894.1270.02340.3263
Rh+0.334229.7561.22099.438−0.57555.3320.02100.2574
Pd0.200329.3631.14469.599−0.36894.0420.02510.2453
Pd+0.503324.5041.99826.908−1.52405.5130.02130.1909

Table 4.4.5.3| top | pdf |
j0〉 form factors for rare-earth ions

IonAaBbCcDe
Ce2+0.295317.6850.29236.7330.43135.383−0.01940.0845
Nd2+0.164525.0450.252211.9780.60124.946−0.01800.0668
Nd3+0.054025.0290.310112.1020.65754.722−0.02160.0478
Sm2+0.090925.2030.303711.8560.62504.237−0.02000.0408
Sm3+0.028825.2070.297311.8310.69544.212−0.02130.0510
Eu2+0.075525.2960.300111.5990.64384.025−0.01960.0488
Eu3+0.020425.3080.301011.4740.70053.942−0.02200.0356
Gd2+0.063625.3820.303311.2120.65283.788−0.01990.0486
Gd3+0.018625.3870.289511.1420.71353.752−0.02170.0489
Tb2+0.054725.5090.317110.5910.64903.517−0.02120.0342
Tb3+0.017725.5100.292110.5770.71333.512−0.02310.0512
Dy2+0.130818.3160.31187.6650.57953.147−0.02260.0315
Dy3+0.115715.0730.32706.7990.58213.020−0.02490.0146
Ho2+0.099518.1760.33057.8560.59212.980−0.02300.1240
Ho3+0.056618.3180.33657.6880.63172.943−0.02480.0068
Er2+0.112218.1220.34626.9110.56492.761−0.02350.0207
Er3+0.058617.9800.35407.0960.61262.748−0.02510.0171
Tm2+0.098318.3240.33806.9180.58752.662−0.02410.0404
Tm3+0.058115.0920.27877.8010.68542.793−0.02240.0351
Yb2+0.085518.5120.29437.3730.64122.678−0.02130.0421
Yb3+0.041616.0950.28497.8340.69612.672−0.02290.0344

Table 4.4.5.4| top | pdf |
j0〉 form factors for actinide ions

IonAaBbCcDe
U3+0.505823.2881.34647.003−0.87244.8680.01920.1507
U4+0.329123.5481.08368.454−0.43404.1200.02140.1757
U5+0.365019.8043.21996.282−2.60775.3010.02330.1750
Np3+0.515720.8652.27845.893−1.81634.8460.02110.1378
Np4+0.420619.8052.80045.978−2.24364.9850.02280.1408
Np5+0.369218.1903.15105.850−2.54464.9160.02480.1515
Np6+0.292917.5613.48665.785−2.80664.8710.02670.1698
Pu3+0.384016.6793.10495.421−2.51484.5510.02630.1280
Pu4+0.493416.8361.63945.638−1.15814.1400.02480.1242
Pu5+0.388816.5592.03625.657−1.45154.2550.02670.1287
Pu6+0.317216.0513.46545.351−2.81024.5130.02810.1382
Am2+0.474321.7761.58005.690−1.07794.1450.02180.1253
Am3+0.423919.5741.45735.872−0.90523.9680.02380.1054
Am4+0.373717.8621.35216.043−0.75143.7200.02580.1113
Am5+0.295617.3721.45256.073−0.77553.6620.02770.1202
Am6+0.230216.9531.48646.116−0.74573.5430.02940.1323
Am7+0.360112.7301.96405.120−1.35603.7140.03160.1232

Table 4.4.5.5| top | pdf |
j2〉 form factors for 3d transition elements and their ions

Atom or ionAaBbCcDe
Sc10.817254.3274.735314.8470.60714.2180.00110.1212
Sc+8.502134.2853.211610.9940.42443.6050.00090.1037
Sc2+4.368328.6543.723110.8230.60743.6680.00140.0681
Ti4.358336.0563.823011.1330.68553.4690.00200.0967
Ti+6.156727.2752.68338.9830.40703.0520.00110.0902
Ti2+4.310718.3482.09606.7970.29842.5480.00070.0640
Ti3+3.371714.4441.82585.7130.24702.2650.00050.0491
V3.760021.8312.40267.5460.44642.6630.00170.0556
V+4.747423.3232.36097.8080.41052.7060.00140.0800
V2+3.438616.5301.96386.1410.29972.2670.00090.0565
V3+2.300514.6822.03646.1300.40992.3820.00140.0252
V4+1.837712.2671.82475.4580.39792.2480.00120.0399
Cr3.408520.1272.10066.8020.42662.3940.00190.0662
Cr+3.776820.3462.10286.8930.40102.4110.00170.0686
Cr2+2.642216.0601.91986.2530.44462.3720.00200.0480
Cr3+1.626215.0662.06186.2840.52812.3680.00230.0263
Cr4+1.029313.9501.99336.0590.59742.3460.00270.0366
Mn2.668116.0601.75615.6400.36752.0490.00170.0595
Mn+3.295318.6951.87926.2400.39272.2010.00220.0659
Mn2+2.051515.5561.88416.0630.47872.2320.00270.0306
Mn3+1.242714.9971.95676.1180.57322.2580.00310.0336
Mn4+0.787913.8861.87175.7430.59812.1820.00340.0434
Fe1.940518.4731.95666.3230.51662.1610.00360.0394
Fe+2.629018.6601.87046.3310.46902.1630.00310.0491
Fe2+1.649016.5591.90646.1330.52062.1370.00350.0335
Fe3+1.360211.9981.51885.0030.47051.9910.00380.0374
Fe4+1.55828.2751.18633.2790.13661.107−0.00220.0327
Co1.967814.1701.49114.9480.38441.7970.00270.0452
Co+2.409716.1611.57805.4600.40951.9140.00310.0581
Co2+1.904911.6441.31594.3570.31461.6450.00170.0459
Co3+1.70588.8591.14093.3090.14741.090−0.00250.0462
Co4+1.31108.0251.15513.1790.16081.130−0.00110.0374
Ni1.030212.2521.46694.7450.45211.7440.00360.0338
Ni+2.104014.8661.43025.0710.40311.7780.00340.0561
Ni2+1.708011.0161.21474.1030.31501.5330.00180.0446
Ni3+1.46838.6710.17941.1061.10683.257−0.00230.0373
Ni4+1.16127.7001.00273.2630.27191.3780.00250.0326
Cu1.918214.4901.33294.7300.38421.6390.00350.0617
Cu+1.881413.4331.28094.5450.36461.6020.00330.0590
Cu2+1.518910.4781.15123.8130.29181.3980.00170.0429
Cu3+1.27978.4501.03153.2800.24011.2500.00150.0389
Cu4+0.95687.4480.90993.3960.37291.4940.00490.0330

Table 4.4.5.6| top | pdf |
j2〉 form factors for 4d atoms and their ions

Atom or ionAaBbCcDe
Y14.408444.6585.104514.904−0.05353.3190.00280.1093
Zr10.137835.3374.773412.545−0.04892.6720.00360.0912
Zr+11.872234.9204.050212.127−0.06322.8280.00340.0737
Nb7.479633.1795.088411.571−0.02811.5640.00470.0944
Nb+8.773533.2854.655611.605−0.02681.5390.00440.0855
Mo5.118023.4224.18099.208−0.05051.7430.00530.0655
Mo+7.236728.1284.07059.923−0.03171.4550.00490.0798
Tc4.244121.3973.94398.375−0.03711.1870.00660.0645
Tc+6.405624.8243.54008.611−0.03661.4850.00440.0806
Ru3.744518.6133.47497.420−0.03631.0070.00730.0533
Ru+5.282623.6833.58138.152−0.02570.4260.01310.0830
Rh3.365117.3443.21216.804−0.03500.5030.01460.0545
Rh+4.026018.9503.16637.000−0.02960.4860.01270.0629
Pd3.310514.7262.63325.862−0.04371.1300.00530.0492
Pd+4.274917.9002.70216.354−0.02580.7000.00710.0768

Table 4.4.5.7| top | pdf |
j2〉 form factors for rare-earth ions

IonAaBbCcDe
Ce2+0.980918.0631.84137.7690.99052.8450.01200.0448
Nd2+1.453018.3401.61967.2850.87522.6220.01260.0461
Nd3+0.675118.3421.62727.2600.96442.6020.01500.0450
Sm2+1.036018.4251.47697.0320.88102.4370.01520.0345
Sm3+0.470718.4301.42617.0340.95742.4390.01820.0510
Eu2+0.897018.4431.37697.0050.90602.4210.01900.0511
Eu3+0.398518.4511.33076.9560.96032.3780.01970.0447
Gd2+0.775618.4691.31246.8990.89562.3380.01990.0441
Gd3+0.334718.4761.24656.8770.95372.3180.02170.0484
Tb2+0.668818.4911.24876.8220.88882.2750.02150.0439
Tb3+0.289218.4971.16786.7970.94372.2570.02320.0458
Dy2+0.591718.5111.18286.7470.88012.2140.02290.0439
Dy3+0.252318.5171.09146.7360.93452.2080.02500.0476
Ho2+0.509418.5151.12346.7060.87272.1590.02420.0560
Ho3+0.218818.5161.02406.7070.92512.1610.02680.0503
Er2+0.469318.5281.05456.6490.86792.1200.02610.0413
Er3+0.171018.5340.98796.6250.90442.1000.02780.0489
Tm2+0.419818.5420.99596.6000.85932.0820.02840.0457
Tm3+0.176018.5420.91056.5790.89702.0620.02940.0468
Yb2+0.385218.5500.94156.5510.84922.0430.03010.0478
Yb3+0.157018.5550.84846.5400.88802.0370.03180.0498

Table 4.4.5.8| top | pdf |
j2〉 form factors for actinide ions

IonAaBbCcDe
U3+4.158216.5342.46755.952−0.02520.7650.00570.0822
U4+3.744913.8942.64534.863−0.52183.1920.00090.0928
U5+3.072412.5462.30765.231−0.06441.4740.00350.0477
Np3+3.717015.1332.32165.503−0.02750.8000.00520.0948
Np4+2.920314.6462.59795.559−0.03010.3670.01410.0532
Np5+2.330813.6542.72195.494−0.13570.0490.12240.0553
Np6+1.824513.1802.85085.407−0.15790.0440.14380.0585
Pu3+2.088512.8712.59615.190−0.14650.0390.13430.0866
Pu4+2.724412.9262.33875.163−0.13000.0460.11770.0490
Pu5+2.140912.8322.56645.152−0.13380.0460.12100.0491
Pu6+1.726212.3242.66525.066−0.16950.0410.15500.0502
Am2+3.523715.9552.28555.195−0.01420.5850.00330.1120
Am3+2.862214.7332.40995.144−0.13260.0310.12330.0727
Am4+2.414112.9482.36874.945−0.24900.0220.23710.0502
Am5+2.010912.0532.41554.836−0.22640.0270.21280.0414
Am6+1.677811.3372.45314.725−0.20430.0340.18920.0387
Am7+1.88459.1612.07464.042−0.13181.7230.00200.0379

Tables 4.4.5.9[link][link][link][link][link]–4.4.5.14[link] give coefficients in the approximation used by Lisher & Forsyth (1971[link]) to the [\langle \,j_2\rangle], [\langle\,j_4\rangle], and [\langle\,j_6\rangle] form factors for the same series of atoms and ions, again using three rather than two exponential terms, viz for [l\neq0]: [\eqalignno{ \langle \,j_l(s)\rangle &=As^2\exp(-as^2)+B s^2\exp(-bs^2) \cr &\quad+Cs^2\exp(-cs^2)+Ds^2. & (4.4.5.3)}]

Table 4.4.5.9| top | pdf |
j4〉 form factors for 3d atoms and their ions

Atom or ionAaBbCcDe
Sc1.342010.2000.38373.0790.04680.118−0.03280.1343
Sc+7.116715.487−6.667118.2690.49002.9920.00470.1624
Sc2+−1.668415.6481.77429.0620.40752.4120.00420.1105
Ti−2.151511.2712.51498.8590.35552.1490.00450.1244
Ti+−1.038316.1901.46998.9240.36312.2830.00440.1270
Ti2+−1.324215.3101.20427.8990.39762.1560.00510.0820
Ti3+−1.111714.6350.76896.9270.43852.0890.00600.0572
V−0.963315.2730.92747.7320.38912.0530.00630.0840
V+−0.960615.5451.12788.1180.36532.0970.00560.1027
V2+−1.172914.9730.90927.6130.41052.0390.00670.0719
V3+−0.941714.2050.52846.6070.44111.9670.00760.0569
V4+−0.765413.0970.30715.6740.44761.8710.00810.0518
Cr−0.667019.6130.53426.4780.36411.9050.00730.0628
Cr+−0.830918.0430.72527.5310.38282.0030.00730.0781
Cr2+−0.893015.6640.55907.0330.40931.9240.00810.0631
Cr3+−0.732714.0730.32685.6740.41141.8100.00850.0505
Cr4+−0.674812.9460.18056.7530.45261.8000.00980.0644
Mn−0.545215.4710.44064.9020.28841.5430.00590.0488
Mn+−0.794717.8670.60787.7040.37981.9050.00870.0737
Mn2+−0.741615.2550.38316.4690.39351.8000.00930.0577
Mn3+−0.660313.6070.23226.2180.41041.7400.01010.0579
Mn4+−0.512713.4610.03137.7630.42821.7010.01130.0693
Fe−0.502919.6770.29993.7760.25761.4240.00710.0292
Fe+−0.510919.2500.38964.8910.28101.5260.00690.0375
Fe2+−0.540117.2270.28653.7420.26581.4240.00760.0278
Fe3+−0.550711.4930.21534.9060.34681.5230.00950.0314
Fe4+−0.53529.5070.17835.1750.35841.4690.00970.0360
Co−0.422114.1950.29003.9790.24691.2860.00630.0400
Co+−0.411514.5610.35804.7170.26441.4180.00740.0541
Co2+0.475914.0460.27473.7310.24581.2500.00570.0282
Co3+−0.446613.3910.14193.0110.27731.3350.00930.0341
Co4+−0.409113.194−0.01943.4170.35341.4210.01120.0622
Ni−0.442814.4850.08703.2340.29321.3310.00960.0554
Ni+−0.383613.4250.31164.4620.24711.3090.00790.0515
Ni2+−0.380310.4030.28383.3780.21081.1040.00500.0474
Ni3+−0.40149.0460.23143.0750.21921.0840.00600.0323
Ni4+−0.35098.1570.22202.1060.15670.9250.00650.0352
Cu−0.320415.1320.23354.0210.23121.1960.00680.0457
Cu+−0.357215.1250.23363.9660.23151.1970.00700.0397
Cu2+−0.391414.7400.12753.3840.25481.2550.01030.0394
Cu3+−0.367114.082−0.00783.3150.31541.3770.01320.0534
Cu4+−0.291514.124−0.10654.2010.32471.3520.01480.0579

Table 4.4.5.10| top | pdf |
j4〉 form factors for 4d atoms and their ions

Atom or ionAaBbCcDe
Y−8.076732.2017.919725.1561.40676.827−0.00010.1031
Zr−5.269732.8684.193024.1831.52026.048−0.00020.0855
Zr+−5.638433.6074.672922.3381.32585.924−0.00030.0674
Nb−3.137725.5952.341116.5691.23044.990−0.00050.0615
Nb+−3.359825.8202.829716.4271.12034.982−0.00050.0724
Mo−2.886020.5721.813014.6281.18994.264−0.00080.0410
Mo+−3.261825.4862.359616.4621.11644.491−0.00070.0592
Tc−2.797520.1591.652016.2611.17263.943−0.00080.0657
Tc+−2.047019.6831.630611.5920.86983.769−0.00100.0723
Ru−1.504217.9490.60279.9610.97003.393−0.00100.0338
Ru+1.627818.5061.182810.1890.81383.418−0.00090.0673
Rh−1.349217.5770.452710.5070.92853.155−0.00090.0483
Rh+−1.467317.9570.73819.9440.84853.126−0.00120.0487
Pd−1.195517.6280.318311.3090.86962.909−0.00060.0555
Pd+−1.409817.7650.79279.9990.77102.930−0.00060.0530

Table 4.4.5.11| top | pdf |
j4〉 form factors for rare-earth ions

IonAaBbCcDe
Ce2+−0.646810.5330.40525.6240.34121.5350.00800.0522
Nd2+−0.541612.2040.35716.1690.31541.4850.00980.0519
Nd3+−0.405314.0140.03297.0050.37591.7070.02090.0372
Sm2+−0.415014.0570.13687.0320.32721.5820.01920.0319
Sm3+−0.428810.0520.17825.0190.28331.2360.00880.0328
Eu2+−0.414510.1930.24475.1640.26611.2050.00650.0516
Eu3+−0.409510.2110.14855.1750.27201.2370.01310.0494
Gd2+−0.382410.3440.19555.3060.26221.2030.00970.0363
Gd3+−0.362110.3530.10165.3100.26491.2190.01470.0494
Tb2+−0.344310.4690.14815.4160.25751.1820.01040.0280
Tb3+−0.322810.4760.06385.4190.25661.1960.01590.0439
Dy2+−0.320612.0710.09048.0260.26161.2300.01430.0767
Dy3+−0.28299.5250.05654.4290.24371.0660.00920.0181
Ho2+−0.29769.7190.12244.6350.22791.0050.00630.0452
Ho3+−0.27179.7310.04744.6380.22921.0470.01240.0310
Er2+−0.29759.8290.11894.7410.21161.0040.01170.0524
Er3+−0.25689.8340.03564.7410.21721.0280.01480.0434
Tm2+−0.26779.8880.09254.7840.20560.9900.01240.0396
Tm3+−0.22929.8950.01244.7850.21081.0070.01510.0334
Yb2+−0.23939.9470.06634.8230.20090.9650.01220.0311
Yb3+−0.21218.1970.03253.1530.19750.8840.00930.0435

Table 4.4.5.12| top | pdf |
j4〉 form factors for actinide ions

IonAaBbCcDe
U3+−0.985916.6010.61166.5150.60202.597−0.00100.0599
U4+−1.054016.6050.43396.5120.67462.599−0.00110.0471
U5+−0.958816.4850.15766.4400.77852.640−0.00100.0493
Np3+0.902916.5860.40066.4700.65452.563−0.00040.0470
Np4+−0.988712.4410.59185.2940.53062.263−0.00210.0583
Np5+−0.814616.581−0.00556.4750.79562.562−0.00040.0600
Np6+0.673816.553−0.22976.5050.85132.553−0.00030.0623
Pu3+−0.701416.369−0.11626.6970.77782.4500.00000.0546
Pu4+−0.916012.2030.48915.1270.52902.149−0.00220.0520
Pu5+−0.703516.360−0.09796.7060.77262.4470.00000.0610
Pu6+−0.556016.322−0.30466.7680.81462.4260.00010.0596
Am2+−0.743316.4160.34816.7880.60142.3460.00000.0566
Am3+0.809212.8540.41615.4590.54762.172−0.00110.0530
Am4+−0.854812.2260.30375.9090.61732.188−0.00160.0456
Am5+−0.653815.462−0.09485.9970.72952.2970.00000.0594
Am6+−0.539015.449−0.26896.0170.77112.2970.00020.0729
Am7+−0.468812.019−0.26927.0420.72972.164−0.00110.0262

Table 4.4.5.13| top | pdf |
j6〉 form factors for rare-earth ions

IonAaBbCcDe
Ce2+−0.12127.994−0.06394.0240.15191.0960.00780.0388
Nd2+−0.16008.0090.02724.0280.11041.0680.01390.0363
Nd3+0.04168.014−0.12614.0400.14001.0870.01020.0367
Sm2+0.14286.0410.07232.0330.05500.5130.00810.0450
Sm3+−0.09446.030−0.04982.0740.13720.645−0.01320.0387
Eu2+−0.12526.0490.05072.0850.05720.6460.01320.0403
Eu3+−0.08176.039−0.05962.1200.12430.764−0.00010.0206
Gd2+−0.13515.0300.08282.0250.03150.5030.01870.0453
Gd3+−0.06626.031−0.08502.1540.13230.8910.00480.0371
Th2+−0.07586.032−0.05402.1580.11990.8900.00510.0488
Tb3+−0.05596.031−0.10202.2370.12641.1070.01670.0170
Dy2+−0.05686.032−0.10032.2400.14011.1060.01090.0463
Dy3+−0.04236.038−0.12482.2440.13591.2000.01880.0350
Ho2+−0.07256.045−0.03182.2430.07381.2020.02520.0634
Ho3+−0.02896.050−0.15452.2300.15501.2600.01770.0351
Er2+0.06486.056−0.05152.2300.08251.2640.02500.0409
Er3+−0.01106.061−0.19542.2240.18181.2960.01490.0455
Tm2+0.08424.0700.08070.849−0.20870.0390.20950.0360
Tm3+0.07274.0730.02430.6893.94590.002−3.90760.0502
Yb2+−0.07395.0310.01402.0300.03510.5080.01740.0434
Yb3+−0.03455.007−0.06772.0200.09850.549−0.00760.0359

Table 4.4.5.14| top | pdf |
j6〉 form factors for actinide ions

IonAaBbCcDe
U3+−0.37979.9530.04595.0380.27481.6070.00160.0345
U4+−0.179311.896−0.22695.4280.32911.7010.00300.0472
U5+−0.039911.891−0.34585.5800.33401.6450.00290.0444
Np3+−0.242711.844−0.11295.3770.28481.5680.00220.0368
Np4+−0.24369.599−0.13174.1010.30291.5450.00190.0500
Np5+−0.11579.565−0.26544.2600.32981.5490.00250.0495
Np6+−0.01289.569−0.36114.3040.34191.5410.00320.0520
Pu3+−0.03649.572−0.31814.3420.32101.5230.00410.0496
Pu4+−0.23947.837−0.07854.0240.26431.3780.00120.0414
Pu5+−0.10907.819−0.22434.1000.29471.4040.00150.0477
Pu6+−0.00017.820−0.33544.1440.30971.4030.00200.0513
Am2+−0.31767.8640.07714.1610.21941.3390.00180.0374
Am3+−0.31596.9820.06823.9950.21411.188−0.00150.0281
Am4+−0.17877.880−0.12744.0900.25651.3150.00170.0419
Am5+−0.09276.073−0.22273.7840.29161.3720.00260.0485
Am6+0.01526.079−0.35493.8610.31251.4030.00360.0732
Am7+0.12926.082−0.46893.8790.32341.3930.00420.0475

For the transition-metal series, the coefficients of the approximation have been obtained by fitting to form factors calculated from the Hartree–Fock wavefunctions given by Clementi & Roetti (1974[link]) in terms of Slater-type functions in the form [U(r)=\textstyle\sum\limits_{nj}\,N_{nl}\,r^2A_{nlj}\exp(-a_{nlj}\,r) \eqno (4.4.5.4)]by using the identity: [\eqalignno{ &\int^\infty_0\,j_l(kr) r^n\exp(-pr)4\pi r^2\,{\rm d} r \cr &\quad ={\pi^{3/2}\Gamma(n+l+3)k^l \over 2^{l-1}\Gamma(l+3/2)(k^2+p^2)^{(n+l+3)/2}} \cr &\qquad\times {_2}F_1\left({n+l+3\over 2};\, {l-n+3\over 2};\, l+{3\over2};\, {k^2\over k^2+p^2}\right). \cr&& (4.4.5.5)}]

The form factors have been calculated from these relationships in the range [(\sin\theta)/\lambda=0] to 1.5 Å−1 at intervals of 0.05 Å−1, and the coefficients of the exponential expansion fitted by a least-squares procedure at the calculated points.

For the atoms of the rare-earth and actinide series, the wavefunctions and form factors have been calculated by Freeman & Desclaux (1979[link]) and Desclaux & Freeman (1978[link]) using Dirac–Fock theory. The constants given in Tables 4.4.5.3[link], 4.4.5.4[link], 4.4.5.7[link], 4.4.5.8[link], and 4.4.5.11[link][link][link]–4.4.5.14[link] have been fitted to the results of these calculations. For the rare-earth ions, the form factors are given in the range [(\sin\theta)/\lambda=0] to 0.5 Å−1 at intervals of 0.5 Å−1 and in the range 0.5 to 1.2 Å−1 at intervals of 0.1 Å−1. For the actinide ions, the calculations extend to 1.5 Å−1. All the values given in the publications cited were included in the fitting procedure. The accuracy with which the exponential expansions fit the theoretical form factors can be judged from the value of the parameter e given in the tables, and defined by: [e=100\left(\,{\sum_i\delta^2_i \over N}\,\right)^{1/2}, \eqno (4.4.5.6)]where [\delta_i] is the difference between the ith fitted point and its theoretical value. The sum is over the N points included in the fitting procedure.

References

First citation Clementi, E. & Roetti, C. (1974). Roothan–Hartree–Fock atomic wave functions. At. Data Nucl. Data Tables, 14, 177–478.Google Scholar
First citation Desclaux, J. P. & Freeman, A. J. (1978). Dirac–Fock studies of some electronic properties of actinide ions. J. Magn. Magn. Mater. 8, 119–129.Google Scholar
First citation Forsyth, J. B. & Wells, M. (1959). On an analytic approximation to the atomic scattering factor. Acta Cryst. 12, 412–414.Google Scholar
First citation Freeman, A. J. & Desclaux, J. P. (1979). Dirac–Fock studies of some electronic properties of rare-earth ions. J. Magn. Magn. Mater. 12, 11–21.Google Scholar
First citation Lisher, E. J. & Forsyth, J. B. (1971). Analytic approximations to form factors. Acta Cryst. A27, 545–549.Google Scholar








































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