rudi001

Table 1 Crystal data and structure refinement for rudi001.
Identification code rudi001
Empirical formula C14H20B22Cl22N6Ni
Formula weight 1348.79
Temperature/K 100.00
Crystal system orthorhombic
Space group Pnma
a/Å 10.3212(3)
b/Å 13.0627(3)
c/Å 20.4914(5)
α/° 90
β/° 90
γ/° 90
Volume/Å3 2762.71(12)
Z 2
ρcalcg/cm3 1.621
μ/mm‑1 10.516
F(000) 1316.0
Crystal size/mm3 0.259 × 0.149 × 0.132
Radiation CuKα (λ = 1.54178)
2Θ range for data collection/° 9.594 to 149.166
Index ranges -12 ≤ h ≤ 12, -16 ≤ k ≤ 16, -25 ≤ l ≤ 25
Reflections collected 35499
Independent reflections 2943 [Rint = 0.0506, Rsigma = 0.0225]
Data/restraints/parameters 2943/148/236
Goodness-of-fit on F2 1.206
Final R indexes [I>=2σ (I)] R1 = 0.0417, wR2 = 0.1159
Final R indexes [all data] R1 = 0.0429, wR2 = 0.1166
Largest diff. peak/hole / e Å-3 2.29/-0.44

 

Table 2 Fractional Atomic Coordinates (×104) and Equivalent Isotropic Displacement Parameters (Å2×103) for rudi001. Ueq is defined as 1/3 of the trace of the orthogonalised UIJ tensor.
AtomxyzU(eq)
Ni15494.9(13)-2506(7)2469.2(6)10.8(3)
N16645(7)-2540(40)3296(3)18.2(17)
N26636(5)-1401(4)2031(2)18.8(8)
N34242(7)-2430(20)1682(3)14.1(18)
N44382(5)-1386(4)2913(2)17.5(8)
C17092(9)-2440(30)3804(4)18.1(17)
C27669(17)-2610(30)4460(5)23(5)
C37286(6)-822(4)1769(3)19.2(8)
C48158(13)-111(6)1411(5)21.0(12)
C53549(8)-2570(20)1255(4)14.0(18)
C62627(12)-2633(18)699(5)14(2)
C73820(6)-778(4)3199(3)17.8(8)
C83035(12)13(6)3540(5)19.5(12)
Cl111041.1(10)25003935.5(5)19.8(2)
Cl29193.4(7)273.9(6)3478.9(3)18.83(19)
Cl36247.9(8)1145.2(6)2744.7(3)20.89(19)
Cl49212.7(7)1108.3(6)5227.6(3)20.30(19)
Cl56211.9(7)213.3(6)4457.7(4)19.88(19)
Cl66178.6(10)25005517.6(5)18.7(2)
Cl74312.2(10)25003989.4(6)22.5(3)
C98358(4)25003322.2(19)12.0(8)
B19330(5)25004000(2)13.2(9)
B28419(3)1391(3)3775.3(15)12.5(6)
B36943(3)1815(3)3405.6(15)13.2(6)
B48435(3)1814(3)4601.9(15)13.3(6)
B56953(3)1386(3)4229.8(15)13.1(6)
B66956(5)25004741(2)13.2(9)
B76041(5)25004004(2)14.0(9)

 

Table 3 Anisotropic Displacement Parameters (Å2×103) for rudi001. The Anisotropic displacement factor exponent takes the form: -2π2[h2a*2U11+2hka*b*U12+…].
AtomU11U22U33U23U13U12
Ni111.9(6)14.5(7)6.0(6)-1(4)1.0(5)0(5)
N120(2)18(4)16.5(19)-4(3)0.0(18)0(3)
N222.9(18)16.7(18)16.9(17)-5.0(14)2.8(14)-1.3(15)
N320(2)7(5)15(2)1(3)1.4(18)2(3)
N422.1(18)16.2(18)14.4(17)0.7(14)0.3(13)-1.4(15)
C120(2)18(4)17(2)-4(3)-0.1(19)0(4)
C231(5)19(11)19(3)-4(5)-7(3)0(6)
C323.4(19)16.7(18)17.5(17)-5.2(15)3.5(14)-1.5(15)
C426(2)18(2)20(2)-6(2)6.2(19)-2(2)
C520(2)7(5)15(2)1(3)1.3(18)2(3)
C621(3)7(6)15(3)2(4)0(2)2(4)
C722.1(18)16.3(18)15.0(17)1.0(14)0.0(14)-0.8(15)
C824(2)18(2)17(2)1(2)-1.6(19)1.5(19)
Cl111.1(5)30.5(6)17.8(5)01.8(4)0
Cl224.3(4)15.3(4)16.8(3)0.3(3)6.1(3)5.3(3)
Cl326.3(4)21.8(4)14.5(3)-5.3(3)-4.0(3)-4.8(3)
Cl423.3(4)25.2(4)12.4(3)5.6(3)-2.3(3)5.6(3)
Cl523.3(4)15.4(4)21.0(4)3.0(3)5.2(3)-4.9(3)
Cl622.3(5)22.5(5)11.3(4)07.7(4)0
Cl710.7(5)25.6(6)31.2(6)00.2(4)0
C914.4(19)13.2(19)8.5(17)01.1(15)0
B114(2)17(2)9(2)01.7(17)0
B215.0(15)13.7(15)8.9(14)0.1(12)0.9(12)-1.0(13)
B314.8(15)14.4(15)10.5(14)0.0(12)-0.3(12)-0.5(13)
B414.3(15)15.6(15)9.9(14)0.9(12)2.4(12)-0.4(13)
B514.6(15)13.7(15)10.9(14)-0.1(12)1.8(12)1.2(13)
B613(2)15(2)11(2)03.7(17)0
B714(2)14(2)14(2)0-0.1(18)0

 

Table 4 Bond Lengths for rudi001.
AtomAtomLength/Å AtomAtomLength/Å
Ni1N12.069(5) C9B21.722(4)
Ni1N22.068(6) C9B211.722(4)
Ni1N32.069(5) C9B31.722(5)
Ni1N42.070(6) C9B311.722(5)
N1C11.145(5) B1B21.788(4)
N2C31.145(5) B1B211.788(4)
N3C51.145(5) B1B41.782(5)
N4C71.146(5) B1B411.782(5)
C1C21.487(8) B2B31.790(5)
C3C41.487(8) B2B41.782(4)
C5C61.487(8) B2B51.776(5)
C7C81.487(8) B3B311.789(7)
Cl1B11.771(5) B3B51.780(5)
Cl2B21.771(3) B3B71.780(5)
Cl3B31.765(3) B4B411.793(7)
Cl4B41.771(3) B4B51.798(5)
Cl5B51.775(4) B4B61.793(5)
Cl6B61.783(5) B5B61.793(4)
Cl7B71.785(5) B5B71.794(4)
C9B11.714(6) B6B71.781(7)

1+X,1/2-Y,+Z

 

Table 5 Bond Angles for rudi001.
AtomAtomAtomAngle/˚ AtomAtomAtomAngle/˚
N1Ni1N488.5(9) B5B3B31108.37(15)
N2Ni1N192.5(9) B7B3B2108.0(2)
N2Ni1N389.1(7) B7B3B3159.84(13)
N2Ni1N490.8(4) B7B3B560.53(19)
N3Ni1N1176.0(5) Cl4B4B1121.8(2)
N3Ni1N487.8(7) Cl4B4B2122.1(2)
C1N1Ni1167(3) Cl4B4B41121.36(11)
C3N2Ni1176.9(5) Cl4B4B5122.0(2)
C5N3Ni1168(3) Cl4B4B6122.1(2)
C7N4Ni1174.9(5) B1B4B4159.81(13)
N1C1C2165(4) B1B4B5107.7(2)
N2C3C4177.3(8) B1B4B6107.4(2)
N3C5C6174(3) B2B4B160.21(18)
N4C7C8176.7(7) B2B4B41108.06(15)
B1C9B2162.71(17) B2B4B559.50(18)
B1C9B262.71(17) B2B4B6107.3(2)
B1C9B31114.6(3) B41B4B5108.11(15)
B1C9B3114.6(3) B6B4B4160.00(13)
B21C9B2114.6(3) B6B4B559.90(19)
B31C9B2162.63(18) Cl5B5B2120.6(2)
B3C9B262.63(18) Cl5B5B3121.3(2)
B31C9B2114.5(3) Cl5B5B4121.6(2)
B3C9B21114.5(3) Cl5B5B6123.2(2)
B31C9B362.6(3) Cl5B5B7122.8(2)
Cl1B1B21120.35(18) B2B5B360.43(18)
Cl1B1B2120.35(18) B2B5B459.79(18)
Cl1B1B41124.7(3) B2B5B6107.6(3)
Cl1B1B4124.7(3) B2B5B7108.0(3)
C9B1Cl1121.5(3) B3B5B4108.0(2)
C9B1B258.87(17) B3B5B6107.4(2)
C9B1B2158.87(17) B3B5B759.7(2)
C9B1B4104.9(3) B6B5B459.9(2)
C9B1B41104.9(3) B6B5B759.5(2)
B2B1B21108.3(3) B7B5B4107.7(2)
B41B1B2108.3(3) Cl6B6B4121.7(2)
B41B1B2159.88(18) Cl6B6B41121.7(3)
B4B1B259.88(18) Cl6B6B5121.37(18)
B4B1B21108.3(3) Cl6B6B51121.37(18)
B41B1B460.4(3) B41B6B460.0(3)
Cl2B2B1121.2(2) B41B6B5108.3(3)
Cl2B2B3119.6(2) B4B6B560.19(18)
Cl2B2B4125.3(2) B41B6B5160.20(18)
Cl2B2B5124.1(2) B4B6B51108.3(3)
C9B2Cl2121.6(2) B5B6B51108.5(3)
C9B2B158.4(2) B7B6Cl6121.2(3)
C9B2B358.7(2) B7B6B41108.5(3)
C9B2B4104.6(2) B7B6B4108.5(3)
C9B2B5104.8(2) B7B6B560.27(18)
B1B2B3107.8(2) B7B6B5160.27(18)
B4B2B159.9(2) Cl7B7B5121.94(19)
B4B2B3108.3(2) Cl7B7B51121.93(19)
B5B2B1108.4(2) B31B7Cl7120.8(3)
B5B2B359.87(18) B3B7Cl7120.8(3)
B5B2B460.70(18) B31B7B360.3(3)
Cl3B3B2121.1(2) B3B7B51108.1(3)
Cl3B3B31119.73(11) B3B7B559.72(18)
Cl3B3B5125.1(2) B31B7B5108.1(3)
Cl3B3B7124.4(2) B31B7B5159.72(18)
C9B3Cl3121.8(2) B3B7B6107.8(3)
C9B3B258.70(18) B31B7B6107.8(3)
C9B3B3158.70(13) B5B7B51108.4(3)
C9B3B5104.6(2) B6B7Cl7123.0(3)
C9B3B7104.5(2) B6B7B5160.19(18)
B31B3B2108.05(15) B6B7B560.19(18)
B5B3B259.70(18)     

1+X,1/2-Y,+Z

 

Table 6 Torsion Angles for rudi001.
ABCDAngle/˚ ABCDAngle/˚
Ni1N1C1C2123(17) B2B3B5B7137.9(3)
Cl1B1B2Cl2-0.4(4) B2B3B7Cl7-148.9(2)
Cl1B1B2C9-110.7(3) B2B3B7B31100.8(2)
Cl1B1B2B3-143.8(3) B2B3B7B5163.7(3)
Cl1B1B2B4115.0(3) B2B3B7B5-37.5(2)
Cl1B1B2B5152.9(3) B2B3B7B60.0(3)
Cl1B1B4Cl43.4(4) B2B4B5Cl5109.4(3)
Cl1B1B4B2-108.0(2) B2B4B5B3-37.8(2)
Cl1B1B4B41113.7(3) B2B4B5B6-137.8(2)
Cl1B1B4B5-145.2(2) B2B4B5B7-100.9(3)
Cl1B1B4B6151.6(2) B2B4B6Cl6147.9(2)
Cl2B2B3Cl3-0.5(3) B2B4B6B41-101.2(2)
Cl2B2B3C9-111.1(3) B2B4B6B537.3(2)
Cl2B2B3B31-144.24(16) B2B4B6B51-64.0(3)
Cl2B2B3B5114.6(3) B2B4B6B7-0.1(3)
Cl2B2B3B7152.5(2) B2B5B6Cl6-148.6(3)
Cl2B2B4Cl4-2.1(4) B2B5B6B4-37.5(2)
Cl2B2B4B1108.9(3) B2B5B6B41-0.3(3)
Cl2B2B4B41146.17(19) B2B5B6B5163.5(4)
Cl2B2B4B5-113.0(3) B2B5B6B7100.9(3)
Cl2B2B4B6-150.5(2) B2B5B7Cl7147.3(3)
Cl2B2B5Cl53.7(4) B2B5B7B310.4(3)
Cl2B2B5B3-107.3(3) B2B5B7B337.8(2)
Cl2B2B5B4114.8(3) B2B5B7B51-62.8(4)
Cl2B2B5B6152.3(2) B2B5B7B6-100.2(3)
Cl2B2B5B7-144.8(2) B3C9B1Cl1145.15(18)
Cl3B3B5Cl5-1.1(4) B31C9B1Cl1-145.16(18)
Cl3B3B5B2108.8(3) B31C9B1B21-36.4(2)
Cl3B3B5B4146.3(2) B3C9B1B21-106.1(3)
Cl3B3B5B6-150.5(3) B31C9B1B2106.1(3)
Cl3B3B5B7-113.4(3) B3C9B1B236.4(2)
Cl3B3B7Cl72.9(3) B31C9B1B466.2(2)
Cl3B3B7B31-107.3(2) B3C9B1B4-3.5(3)
Cl3B3B7B5114.4(3) B31C9B1B413.5(3)
Cl3B3B7B51-144.4(3) B3C9B1B41-66.2(2)
Cl3B3B7B6151.9(2) B31C9B2Cl2144.1(2)
Cl4B4B5Cl5-1.6(4) B3C9B2Cl2107.7(3)
Cl4B4B5B2-111.0(3) B31C9B2B1-106.2(3)
Cl4B4B5B3-148.8(2) B3C9B2B1-142.6(3)
Cl4B4B5B6111.2(3) B31C9B2B336.4(2)
Cl4B4B5B7148.1(2) B3C9B2B4-102.8(2)
Cl4B4B6Cl6-0.5(3) B31C9B2B4-66.4(3)
Cl4B4B6B41110.3(2) B31C9B2B5-3.5(3)
Cl4B4B6B51147.6(2) B3C9B2B5-39.8(2)
Cl4B4B6B5-111.1(3) B31C9B3Cl3107.8(2)
Cl4B4B6B7-148.6(2) B31C9B3B2-142.57(19)
Cl5B5B6Cl6-0.9(5) B31C9B3B5-102.9(2)
Cl5B5B6B41147.3(2) B31C9B3B7-40.1(3)
Cl5B5B6B4110.1(3) B3B2B4Cl4148.6(2)
Cl5B5B6B51-148.91(17) B3B2B4B1-100.4(3)
Cl5B5B6B7-111.5(3) B3B2B4B41-63.2(2)
Cl5B5B7Cl7-0.3(4) B3B2B4B537.6(2)
Cl5B5B7B3-109.8(3) B3B2B4B60.1(3)
Cl5B5B7B31-147.2(2) B3B2B5Cl5111.0(3)
Cl5B5B7B51149.52(17) B3B2B5B4-137.9(2)
Cl5B5B7B6112.1(3) B3B2B5B6-100.4(3)
Cl6B6B7Cl70.000(1) B3B2B5B7-37.5(2)
Cl6B6B7B3-148.14(16) B31B3B5Cl5149.57(17)
Cl6B6B7B31148.14(16) B31B3B5B2-100.60(16)
Cl6B6B7B5-110.79(17) B31B3B5B4-63.1(2)
Cl6B6B7B51110.79(17) B31B3B5B60.1(3)
C9B1B2Cl2110.3(3) B31B3B5B737.27(18)
C9B1B2B3-33.0(2) B31B3B7Cl7110.2(2)
C9B1B2B4-134.3(3) B31B3B7B51-37.16(16)
C9B1B2B5-96.4(3) B31B3B7B5-138.3(2)
C9B1B4Cl4150.8(2) B31B3B7B6-100.8(2)
C9B1B4B239.36(19) B3B5B6Cl6147.8(3)
C9B1B4B41-98.92(19) B3B5B6B41-64.0(3)
C9B1B4B52.1(3) B3B5B6B4-101.2(2)
C9B1B4B6-61.0(2) B3B5B6B51-0.2(4)
C9B2B3Cl3110.6(3) B3B5B6B737.2(3)
C9B2B3B31-33.11(16) B3B5B7Cl7109.5(3)
C9B2B3B5-134.3(2) B3B5B7B31-37.4(2)
C9B2B3B7-96.4(2) B3B5B7B51-100.7(3)
C9B2B4Cl4-150.1(2) B3B5B7B6-138.0(3)
C9B2B4B1-39.1(2) B4B1B2Cl2-115.4(3)
C9B2B4B41-1.8(2) B41B1B2Cl2-152.9(2)
C9B2B4B599.0(3) B4B1B2C9134.3(3)
C9B2B4B661.5(3) B41B1B2C996.7(3)
C9B2B5Cl5150.2(2) B4B1B2B3101.3(2)
C9B2B5B339.2(2) B41B1B2B363.7(3)
C9B2B5B4-98.7(2) B41B1B2B4-37.5(2)
C9B2B5B6-61.1(3) B4B1B2B537.9(2)
C9B2B5B71.7(3) B41B1B2B50.4(3)
C9B3B5Cl5-149.1(2) B41B1B4Cl4-110.3(2)
C9B3B5B2-39.2(2) B41B1B4B2138.3(2)
C9B3B5B4-1.7(3) B41B1B4B5101.1(2)
C9B3B5B661.5(3) B41B1B4B637.9(3)
C9B3B5B798.6(2) B4B2B3Cl3-153.1(2)
C9B3B7Cl7149.7(2) B4B2B3C996.3(3)
C9B3B7B3139.5(3) B4B2B3B3163.2(2)
C9B3B7B512.4(3) B4B2B3B5-38.0(2)
C9B3B7B5-98.8(2) B4B2B3B7-0.1(3)
C9B3B7B6-61.3(2) B4B2B5Cl5-111.1(3)
B1C9B2Cl2-109.7(3) B4B2B5B3137.9(2)
B1C9B2B3142.6(3) B4B2B5B637.5(2)
B1C9B2B439.8(2) B4B2B5B7100.4(3)
B1C9B2B5102.8(3) B41B4B5Cl5-149.86(17)
B1C9B3Cl3-146.0(2) B41B4B5B2100.72(16)
B1C9B3B2-36.4(2) B41B4B5B362.9(2)
B1C9B3B31106.2(2) B41B4B5B6-37.10(17)
B1C9B3B53.3(3) B41B4B5B7-0.2(2)
B1C9B3B766.1(3) B41B4B6Cl6-110.9(3)
B1B2B3Cl3143.5(2) B41B4B6B5137.23(16)
B1B2B3C932.9(2) B41B4B6B5138.6(2)
B1B2B3B31-0.2(2) B41B4B6B7101.13(19)
B1B2B3B5-101.4(3) B4B5B6Cl6-111.1(3)
B1B2B3B7-63.5(3) B4B5B6B4137.2(2)
B1B2B4Cl4-111.0(3) B4B5B6B51101.0(3)
B1B2B4B4137.23(18) B4B5B6B7138.4(3)
B1B2B4B5138.0(3) B4B5B7Cl7-149.5(3)
B1B2B4B6100.5(2) B4B5B7B3101.0(2)
B1B2B5Cl5-148.7(2) B4B5B7B3163.6(3)
B1B2B5B3100.4(3) B4B5B7B510.3(4)
B1B2B5B4-37.6(2) B4B5B7B6-37.1(2)
B1B2B5B60.0(3) B41B6B7Cl7-148.18(16)
B1B2B5B762.8(3) B4B6B7Cl7148.18(16)
B1B4B5Cl5147.0(2) B4B6B7B30.0(3)
B1B4B5B237.5(2) B41B6B7B363.7(2)
B1B4B5B3-0.3(3) B41B6B7B310.0(3)
B1B4B5B6-100.3(2) B4B6B7B31-63.7(2)
B1B4B5B7-63.4(3) B41B6B7B5101.0(3)
B1B4B6Cl6-148.7(2) B41B6B7B51-37.4(2)
B1B4B6B41-37.8(3) B4B6B7B51-101.0(3)
B1B4B6B5100.7(2) B4B6B7B537.4(2)
B1B4B6B51-0.6(3) B5B2B3Cl3-115.1(3)
B1B4B6B763.3(3) B5B2B3C9134.3(2)
B21C9B1Cl1-108.78(16) B5B2B3B31101.16(16)
B2C9B1Cl1108.78(16) B5B2B3B737.9(2)
B21C9B1B2142.4(3) B5B2B4Cl4111.0(3)
B2C9B1B21-142.4(3) B5B2B4B1-138.0(3)
B21C9B1B4139.86(19) B5B2B4B41-100.80(16)
B21C9B1B4102.6(3) B5B2B4B6-37.5(2)
B2C9B1B4-39.86(19) B5B3B7Cl7-111.4(2)
B2C9B1B41-102.6(3) B5B3B7B31138.3(2)
B21C9B2Cl2-146.22(18) B5B3B7B51101.2(3)
B21C9B2B1-36.6(3) B5B3B7B637.55(19)
B21C9B2B3106.0(3) B5B4B6Cl6110.6(2)
B21C9B2B43.2(4) B5B4B6B41-138.6(2)
B21C9B2B566.2(4) B5B4B6B51-101.3(3)
B21C9B3Cl3144.2(2) B5B4B6B7-37.42(19)
B2C9B3Cl3-109.6(3) B5B6B7Cl7110.79(17)
B21C9B3B2-106.2(3) B51B6B7Cl7-110.79(17)
B21C9B3B3136.38(16) B51B6B7B3137.3(2)
B2C9B3B31142.57(19) B5B6B7B3-37.3(2)
B2C9B3B539.7(2) B5B6B7B31-101.1(3)
B21C9B3B5-66.5(3) B51B6B7B3101.1(3)
B2C9B3B7102.5(2) B51B6B7B5138.4(3)
B21C9B3B7-3.7(3) B5B6B7B51-138.4(3)
B21B1B2Cl2143.66(18) B6B4B5Cl5-112.8(3)
B21B1B2C933.3(3) B6B4B5B2137.8(2)
B21B1B2B30.3(4) B6B4B5B3100.0(3)
B21B1B2B4-100.9(3) B6B4B5B736.9(2)
B21B1B2B5-63.0(3) B6B5B7Cl7-112.5(4)
B2B1B4Cl4111.4(3) B6B5B7B3138.0(3)
B21B1B4Cl4-147.6(2) B6B5B7B31100.6(3)
B21B1B4B2101.0(3) B6B5B7B5137.4(3)
B21B1B4B41-37.31(15) B7B3B5Cl5112.3(3)
B2B1B4B41-138.3(2) B7B3B5B2-137.9(3)
B21B1B4B563.8(3) B7B3B5B4-100.4(3)
B2B1B4B5-37.2(2) B7B3B5B6-37.1(3)
B21B1B4B60.6(3) B7B5B6Cl6110.5(4)
B2B1B4B6-100.4(3) B7B5B6B4-138.4(3)
B2B3B5Cl5-109.8(3) B7B5B6B41-101.3(3)
B2B3B5B437.5(2) B7B5B6B51-37.4(3)
B2B3B5B6100.7(3)      

1+X,1/2-Y,+Z

 

Table 7 Hydrogen Atom Coordinates (Å×104) and Isotropic Displacement Parameters (Å2×103) for rudi001.
AtomxyzU(eq)
H2A8140.27-3262.644463.6735
H2B6978.3-2631.194788.2635
H2C8267.64-2051.34561.2735
H4A8672.01-497.521093.2532
H4B8738.34229.61720.9232
H4C7637.58404.351182.2932
H6A2729.92-2026.71421.9221
H6B1738.11-2660.82865.7421
H6C2806.47-3249.91442.2621
H8A3314.66695.083400.3629
H8B3155.38-54.444012.929
H8C2117.54-81.853432.9329
H98842.0425002832.914

 

Table 8 Atomic Occupancy for rudi001.
AtomOccupancy AtomOccupancy AtomOccupancy
Ni10.25 N10.25 N20.5
N30.25 N40.5 C10.25
C20.25 H2A0.25 H2B0.25
H2C0.25 C30.5 C40.5
H4A0.5 H4B0.5 H4C0.5
C50.25 C60.25 H6A0.25
H6B0.25 H6C0.25 C70.5
C80.5 H8A0.5 H8B0.5
H8C0.5     

Experimental

Single crystals of C14H20B22Cl22N6Ni [rudi001] were []. A suitable crystal was selected and [] on a Bruker Venture Photon III diffractometer. The crystal was kept at 100.00 K during data collection. Using Olex2 [1], the structure was solved with the XS [2] structure solution program using Direct Methods and refined with the XL [3] refinement package using Least Squares minimisation.

  1. Dolomanov, O.V., Bourhis, L.J., Gildea, R.J, Howard, J.A.K. & Puschmann, H. (2009), J. Appl. Cryst. 42, 339-341.
  2. Sheldrick, G.M. (2008). Acta Cryst. A64, 112-122.
  3. Sheldrick, G.M. (2008). Acta Cryst. A64, 112-122.

Crystal structure determination of [rudi001]

Crystal Data for C14H20B22Cl22N6Ni (=1348.79 g/mol): orthorhombic, space group Pnma (no. 62), a = 10.3212(3) Å, b = 13.0627(3) Å, c = 20.4914(5) Å, = 2762.71(12) Å3, Z = 2, T = 100.00 K, μ(CuKα) = 10.516 mm-1, Dcalc = 1.621 g/cm3, 35499 reflections measured (9.594° ≤ 2Θ ≤ 149.166°), 2943 unique (Rint = 0.0506, Rsigma = 0.0225) which were used in all calculations. The final R1 was 0.0417 (I > 2σ(I)) and wR2 was 0.1166 (all data).

Refinement model description

Number of restraints - 148, number of constraints - unknown.

Details:

1. Fixed Uiso
At 1.2 times of:
All C(H) groups
At 1.5 times of:
All C(H,H,H) groups
2. Restrained distances
Ni1-N4 ≈ Ni1-N1 ≈ Ni1-N3 ≈ Ni1-N2
with sigma of 0.002
N4-C7 ≈ N1-C1 ≈ N3-C5 ≈ N2-C3
with sigma of 0.002
C2-C1 ≈ C8-C7 ≈ C4-C3 ≈ C6-C5
with sigma of 0.002
3. Uiso/Uaniso restraints and constraints
Ni1 ≈ C7 ≈ C8 ≈ N4 ≈ N1 ≈ C1 ≈ N2 ≈ C3 ≈ C4
≈ N3 ≈ C5 ≈ C6: within 2A with sigma of 0.001 and sigma for
terminal atoms of 0.002 within 2A
Uanis(C2) ≈ Ueq, Uanis(N1) ≈ Ueq, Uanis(Ni1) ≈ Ueq: with sigma of
0.005 and sigma for terminal atoms of 0.01
4. Rigid body (RIGU) restrains
Ni1, C2, C1, N1, C8, C7, N4, N2, C3, C4, N3, C5, C6
with sigma for 1-2 distances of 0.001 and sigma for 1-3 distances of 0.001
5. Others
Fixed Sof: Ni1(0.25) N1(0.25) N2(0.5) N3(0.25) N4(0.5) C1(0.25) C2(0.25)
H2A(0.25) H2B(0.25) H2C(0.25) C3(0.5) C4(0.5) H4A(0.5) H4B(0.5) H4C(0.5)
C5(0.25) C6(0.25) H6A(0.25) H6B(0.25) H6C(0.25) C7(0.5) C8(0.5) H8A(0.5)
H8B(0.5) H8C(0.5)
6.a Idealised Me refined as rotating group:
C2(H2A,H2B,H2C), C4(H4A,H4B,H4C), C6(H6A,H6B,H6C), C8(H8A,H8B,H8C)
6.b Boron cage BH refined with riding coordinates:
C9(H9)

This report has been created with Olex2, compiled on 2025.07.13 svn.rb7424aed for OlexSys. Please let us know if there are any errors or if you would like to have additional features.