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Two copper(I) iodide tetra­mers, namely, [μ2-1,3-bis­(di­phenyl­phosphan­yl)pro­pane-κ2P:P′]di-μ3-iodido-di-μ2-iodido-[1-(pyridin-3-yl)ethan-1-one-κN]tetra­copper(I) di­chloro­methane disolvate, [Cu4I4(C6H7NO)2(C27H26P2)2]·2CH2Cl2 (CuL3), and [μ2-1,3-bis­(di­phenyl­phosphan­yl)propane-κ2P:P′]di-μ3-iodido-di-μ2-iodido-[1-(pyridin-4-yl)ethan-1-one-κN]tetra­copper(I), [Cu4I4(C6H7NO)2(C27H26P2)2] (CuL4), have been synthesized from reactions of CuI, 1,3-bis­(di­phenyl­phosphan­yl)propane (dppp) and 3- or 4-acetyl­pyridine (3/4-acepy). The com­plexes were characterized by elemental analysis, IR spectroscopy, single-crystal X-ray diffraction (XRD), powder XRD and photoluminescence spectroscopy. Both com­plexes possess a stair-step [Cu4I4] cluster structure with a crystallographic inversion centre located in the middle of a Cu2I2 ring (Z′ = 1 \over 2). The dppp ligands each adopt a bidentate coordination mode that bridges two CuI centres on one side of the [Cu4I4] cluster and the acepy ligands act as terminal ligands. The solid-state samples of similar com­plexes show highly efficiency thermally activated delayed fluorescence (TADF) at room temperature. At ambient temperature, both CuL3 and CuL4 exhibit photoluminescence, with a maximum emission in the region 560–580 nm and with short emissive decay times, but only phospho­rescence was observed at 77 K. The narrow gaps between the higher lying singlet state and the triplet state, ΔE(S1T1), also confirm the presence of TADF. Structure analysis and consideration of photoluminescence indicates that the position of the acetyl group on the heterocyclic ligand has an obvious influence on the structural arrangement, on inter­molecular inter­actions and on the observed photophysical properties.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229620016745/ky3202sup1.cif
Contains datablocks CuL3, CuL4, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620016745/ky3202CuL3sup2.hkl
Contains datablock CuL3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620016745/ky3202CuL4sup3.hkl
Contains datablock CuL4

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2053229620016745/ky3202sup4.pdf
Spectra and additional figures

CCDC references: 2052227; 2052226

Computing details top

For both structures, data collection: RAPID AUTO (Rigaku, 1998); cell refinement: RAPID AUTO (Rigaku, 1998); data reduction: RAPID AUTO (Rigaku, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015); molecular graphics: SHELXTL/PC (Sheldrick, 1993); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

2-1,3-Bis(diphenylphosphanyl)propane-κ2P:P']di-µ3-iodido-di-µ2-iodido-[1-(pyridin-3-yl)ethan-1-one-κN]tetracopper(I) dichloromethane disolvate (CuL3) top
Crystal data top
[Cu4I4(C6H7NO)2(C27H26P2)2]·2CH2Cl2Z = 1
Mr = 1998.72F(000) = 976
Triclinic, P1Dx = 1.733 Mg m3
a = 11.950 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 12.443 (3) ÅCell parameters from 6740 reflections
c = 13.060 (3) Åθ = 3.0–25.0°
α = 83.43 (3)°µ = 2.97 mm1
β = 86.30 (3)°T = 293 K
γ = 83.76 (3)°Block, yellowish green
V = 1915.0 (7) Å30.38 × 0.20 × 0.15 mm
Data collection top
Rigaku R-axis RAPID
diffractometer
4522 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.081
Oscillation scansθmax = 25.0°, θmin = 3.0°
Absorption correction: multi-scan
(RAPID AUTO; Rigaku, 1998)
h = 1413
Tmin = 0.363, Tmax = 1.000k = 1414
15188 measured reflectionsl = 1515
6740 independent reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.121H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0453P)2]
where P = (Fo2 + 2Fc2)/3
6740 reflections(Δ/σ)max < 0.001
406 parametersΔρmax = 1.09 e Å3
0 restraintsΔρmin = 0.64 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.17020 (3)0.47605 (3)0.44629 (4)0.04475 (15)
I20.04015 (3)0.20019 (3)0.49130 (4)0.04860 (16)
Cu10.02670 (7)0.59446 (7)0.58304 (8)0.0539 (3)
Cu20.16639 (6)0.25189 (7)0.48718 (8)0.0499 (3)
P10.06505 (14)0.55726 (13)0.75013 (16)0.0411 (4)
P20.25866 (13)0.22199 (13)0.63184 (16)0.0388 (4)
N10.2482 (5)0.1833 (5)0.3645 (5)0.0523 (16)
O10.2597 (9)0.0651 (7)0.1147 (7)0.140 (4)
C10.0242 (7)0.6409 (5)0.8366 (7)0.060 (2)
C20.1392 (7)0.6325 (7)0.8465 (8)0.074 (3)
H2A0.1708570.5847640.8096330.089*
C30.2062 (9)0.6950 (9)0.9110 (9)0.093 (4)
H3A0.2828660.6869290.9181050.112*
C40.1662 (13)0.7670 (9)0.9643 (10)0.110 (5)
H4A0.2141160.8086681.0068590.132*
C50.0526 (13)0.7778 (8)0.9546 (9)0.104 (4)
H5A0.0232310.8276980.9905270.125*
C60.0189 (8)0.7148 (6)0.8914 (7)0.071 (3)
H6A0.0957140.7222440.8858620.085*
C70.2108 (6)0.5704 (5)0.7794 (7)0.0478 (19)
C80.2562 (8)0.5379 (7)0.8740 (8)0.073 (3)
H8A0.2107310.5109650.9293950.088*
C90.3668 (10)0.5451 (7)0.8865 (10)0.096 (4)
H9A0.3960420.5235020.9507580.116*
C100.4361 (8)0.5833 (8)0.8065 (12)0.094 (4)
H10A0.5121440.5860340.8162800.112*
C110.3942 (7)0.6177 (7)0.7121 (9)0.078 (3)
H11A0.4408920.6441900.6574770.094*
C120.2804 (6)0.6123 (6)0.6992 (7)0.057 (2)
H12A0.2506250.6372290.6357500.068*
C130.0390 (5)0.4192 (5)0.8117 (6)0.0470 (19)
H13A0.0739130.4065670.8775630.056*
H13B0.0415530.4169330.8251470.056*
C140.0837 (5)0.3276 (5)0.7470 (7)0.050 (2)
H14A0.0456680.3378090.6826860.060*
H14B0.0655660.2589350.7837340.060*
C150.2114 (5)0.3217 (5)0.7226 (6)0.0435 (18)
H15A0.2502120.3020850.7861460.052*
H15B0.2312310.3928100.6933600.052*
C160.2604 (5)0.0917 (5)0.7096 (6)0.0393 (16)
C170.2148 (6)0.0068 (5)0.6740 (7)0.061 (2)
H17A0.1812170.0174830.6108320.073*
C180.2185 (8)0.0935 (7)0.7308 (10)0.088 (4)
H18A0.1881840.1501330.7051360.106*
C190.2658 (7)0.1113 (6)0.8241 (9)0.080 (3)
H19A0.2683790.1798510.8611880.095*
C200.3095 (7)0.0284 (6)0.8632 (7)0.066 (2)
H20A0.3408470.0394800.9274080.080*
C210.3062 (6)0.0723 (6)0.8057 (7)0.056 (2)
H21A0.3355400.1288060.8323940.068*
C220.4103 (5)0.2382 (6)0.6101 (6)0.0481 (19)
C230.4474 (6)0.3423 (6)0.6006 (7)0.060 (2)
H23A0.3956530.4024690.6089490.072*
C240.5591 (6)0.3563 (8)0.5792 (8)0.084 (3)
H24A0.5828860.4256030.5725340.101*
C250.6333 (7)0.2699 (10)0.5681 (8)0.087 (3)
H25A0.7094040.2794670.5565740.104*
C260.5995 (7)0.1653 (9)0.5732 (9)0.095 (4)
H26A0.6518380.1063720.5617750.114*
C270.4852 (6)0.1506 (7)0.5959 (8)0.069 (3)
H27A0.4612030.0814150.6011710.082*
C280.2029 (6)0.1121 (6)0.3151 (7)0.054 (2)
H28A0.1280680.1003490.3319620.065*
C290.2607 (7)0.0547 (6)0.2405 (7)0.062 (2)
C300.3714 (8)0.0717 (8)0.2161 (9)0.087 (3)
H30A0.4125700.0341460.1661040.104*
C310.4212 (8)0.1442 (9)0.2658 (10)0.091 (3)
H31A0.4960730.1565690.2501360.110*
C320.3572 (6)0.1981 (7)0.3394 (8)0.071 (3)
H32A0.3907280.2470710.3733100.086*
C330.2057 (10)0.0206 (7)0.1837 (9)0.084 (3)
C340.0910 (11)0.0454 (8)0.2156 (10)0.116 (4)
H34A0.0621810.0029800.2703220.174*
H34B0.0437640.0280290.1580220.174*
H34C0.0915880.1212960.2395070.174*
C410.4199 (12)0.7138 (11)0.1522 (12)0.139 (5)
H41A0.3936620.7795140.1836210.166*
H41B0.4709280.6696890.1986670.166*
Cl10.4928 (3)0.7487 (3)0.0406 (4)0.1445 (14)
Cl20.3071 (4)0.6443 (4)0.1413 (5)0.197 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0350 (2)0.0434 (2)0.0553 (4)0.00649 (19)0.0002 (2)0.0020 (2)
I20.0338 (2)0.0445 (3)0.0661 (4)0.00487 (19)0.0020 (2)0.0007 (2)
Cu10.0487 (5)0.0606 (5)0.0512 (7)0.0090 (4)0.0085 (4)0.0063 (5)
Cu20.0386 (4)0.0590 (5)0.0522 (7)0.0033 (4)0.0032 (4)0.0083 (5)
P10.0429 (9)0.0343 (8)0.0433 (13)0.0005 (7)0.0036 (8)0.0007 (8)
P20.0314 (8)0.0359 (8)0.0489 (13)0.0013 (7)0.0039 (8)0.0050 (8)
N10.046 (3)0.059 (4)0.052 (5)0.001 (3)0.007 (3)0.014 (3)
O10.212 (10)0.122 (7)0.092 (8)0.009 (6)0.032 (7)0.061 (6)
C10.089 (6)0.034 (4)0.050 (6)0.007 (4)0.009 (4)0.001 (4)
C20.061 (5)0.070 (5)0.077 (8)0.021 (4)0.015 (5)0.018 (5)
C30.096 (7)0.079 (7)0.080 (9)0.042 (6)0.038 (6)0.022 (6)
C40.182 (14)0.069 (7)0.056 (8)0.041 (8)0.036 (9)0.014 (6)
C50.191 (13)0.049 (5)0.065 (9)0.007 (7)0.016 (9)0.010 (5)
C60.106 (7)0.043 (4)0.060 (7)0.001 (4)0.013 (5)0.008 (4)
C70.054 (4)0.039 (3)0.054 (6)0.014 (3)0.008 (4)0.009 (4)
C80.091 (6)0.076 (6)0.055 (7)0.018 (5)0.030 (5)0.006 (5)
C90.114 (8)0.066 (6)0.114 (12)0.006 (6)0.067 (8)0.000 (6)
C100.067 (6)0.084 (7)0.139 (13)0.018 (5)0.051 (7)0.014 (7)
C110.055 (5)0.082 (6)0.104 (9)0.032 (5)0.015 (5)0.010 (6)
C120.056 (4)0.050 (4)0.068 (7)0.011 (4)0.016 (4)0.005 (4)
C130.042 (3)0.039 (3)0.057 (6)0.005 (3)0.016 (3)0.002 (4)
C140.041 (3)0.041 (4)0.071 (6)0.007 (3)0.011 (4)0.017 (4)
C150.034 (3)0.036 (3)0.061 (6)0.004 (3)0.000 (3)0.012 (3)
C160.035 (3)0.034 (3)0.047 (5)0.004 (3)0.003 (3)0.001 (3)
C170.061 (4)0.045 (4)0.079 (7)0.005 (4)0.027 (5)0.004 (4)
C180.088 (6)0.050 (5)0.130 (11)0.015 (5)0.042 (7)0.010 (6)
C190.070 (5)0.046 (5)0.114 (10)0.004 (4)0.016 (6)0.026 (5)
C200.074 (5)0.057 (5)0.058 (7)0.015 (4)0.003 (5)0.011 (4)
C210.060 (4)0.043 (4)0.065 (7)0.003 (3)0.003 (4)0.013 (4)
C220.031 (3)0.068 (5)0.043 (5)0.002 (3)0.008 (3)0.003 (4)
C230.042 (4)0.061 (5)0.077 (7)0.013 (4)0.001 (4)0.003 (5)
C240.030 (4)0.108 (7)0.106 (10)0.008 (5)0.003 (5)0.016 (7)
C250.040 (4)0.137 (9)0.072 (8)0.014 (6)0.008 (4)0.040 (7)
C260.057 (5)0.114 (8)0.091 (9)0.037 (6)0.016 (5)0.029 (7)
C270.043 (4)0.065 (5)0.090 (8)0.009 (4)0.010 (4)0.004 (5)
C280.053 (4)0.052 (4)0.052 (6)0.008 (4)0.004 (4)0.003 (4)
C290.077 (5)0.049 (4)0.053 (6)0.008 (4)0.004 (5)0.001 (4)
C300.084 (7)0.090 (7)0.072 (8)0.037 (6)0.019 (6)0.001 (6)
C310.057 (5)0.115 (8)0.095 (10)0.008 (6)0.019 (6)0.006 (7)
C320.050 (4)0.084 (6)0.078 (8)0.001 (4)0.008 (5)0.009 (6)
C330.135 (9)0.057 (5)0.060 (8)0.016 (6)0.011 (7)0.009 (5)
C340.184 (12)0.094 (7)0.087 (10)0.072 (8)0.014 (9)0.032 (7)
C410.162 (12)0.138 (11)0.105 (13)0.008 (10)0.024 (10)0.006 (9)
Cl10.118 (2)0.163 (3)0.150 (4)0.006 (2)0.002 (2)0.018 (3)
Cl20.164 (4)0.198 (4)0.233 (7)0.057 (4)0.040 (4)0.028 (4)
Geometric parameters (Å, º) top
I1—Cu1i2.6636 (11)C14—H14A0.9700
I1—Cu22.7840 (11)C14—H14B0.9700
I1—Cu12.8212 (15)C15—H15A0.9700
I2—Cu22.6132 (10)C15—H15B0.9700
I2—Cu1i2.6455 (12)C16—C171.378 (9)
Cu1—P12.245 (2)C16—C211.387 (11)
Cu1—Cu2i2.9552 (16)C17—C181.376 (11)
Cu2—N12.044 (6)C17—H17A0.9300
Cu2—P22.223 (2)C18—C191.360 (13)
P1—C11.835 (8)C18—H18A0.9300
P1—C71.835 (7)C19—C201.368 (11)
P1—C131.861 (6)C19—H19A0.9300
P2—C161.811 (7)C20—C211.382 (10)
P2—C151.834 (7)C20—H20A0.9300
P2—C221.846 (6)C21—H21A0.9300
N1—C281.332 (9)C22—C271.354 (10)
N1—C321.350 (9)C22—C231.404 (10)
O1—C331.223 (12)C23—C241.372 (9)
C1—C61.387 (11)C23—H23A0.9300
C1—C21.386 (11)C24—C251.332 (13)
C2—C31.372 (13)C24—H24A0.9300
C2—H2A0.9300C25—C261.397 (13)
C3—C41.340 (16)C25—H25A0.9300
C3—H3A0.9300C26—C271.407 (11)
C4—C51.375 (16)C26—H26A0.9300
C4—H4A0.9300C27—H27A0.9300
C5—C61.392 (14)C28—C291.380 (11)
C5—H5A0.9300C28—H28A0.9300
C6—H6A0.9300C29—C301.373 (12)
C7—C81.382 (11)C29—C331.489 (12)
C7—C121.385 (11)C30—C311.375 (13)
C8—C91.356 (12)C30—H30A0.9300
C8—H8A0.9300C31—C321.379 (13)
C9—C101.366 (16)C31—H31A0.9300
C9—H9A0.9300C32—H32A0.9300
C10—C111.366 (15)C33—C341.462 (14)
C10—H10A0.9300C34—H34A0.9600
C11—C121.390 (10)C34—H34B0.9600
C11—H11A0.9300C34—H34C0.9600
C12—H12A0.9300C41—Cl11.687 (14)
C13—C141.525 (9)C41—Cl21.700 (13)
C13—H13A0.9700C41—H41A0.9700
C13—H13B0.9700C41—H41B0.9700
C14—C151.535 (8)
Cu1i—I1—Cu265.66 (4)H13A—C13—H13B107.6
Cu1i—I1—Cu179.47 (4)C13—C14—C15113.4 (5)
Cu2—I1—Cu1113.32 (4)C13—C14—H14A108.9
Cu2—I2—Cu1i68.38 (4)C15—C14—H14A108.9
P1—Cu1—I2i114.11 (6)C13—C14—H14B108.9
P1—Cu1—I1i109.28 (6)C15—C14—H14B108.9
I2i—Cu1—I1i113.31 (4)H14A—C14—H14B107.7
P1—Cu1—I1114.97 (6)C14—C15—P2111.8 (4)
I2i—Cu1—I1103.87 (4)C14—C15—H15A109.2
I1i—Cu1—I1100.53 (4)P2—C15—H15A109.2
P1—Cu1—Cu2i122.44 (7)C14—C15—H15B109.2
I2i—Cu1—Cu2i55.29 (3)P2—C15—H15B109.2
I1i—Cu1—Cu2i59.13 (3)H15A—C15—H15B107.9
I1—Cu1—Cu2i122.52 (5)C17—C16—C21117.2 (6)
N1—Cu2—P2114.48 (18)C17—C16—P2120.1 (6)
N1—Cu2—I2105.40 (16)C21—C16—P2122.7 (5)
P2—Cu2—I2118.77 (7)C18—C17—C16120.7 (8)
N1—Cu2—I1107.22 (18)C18—C17—H17A119.7
P2—Cu2—I199.97 (6)C16—C17—H17A119.7
I2—Cu2—I1110.48 (4)C19—C18—C17121.0 (8)
N1—Cu2—Cu1i110.15 (19)C19—C18—H18A119.5
P2—Cu2—Cu1i133.95 (7)C17—C18—H18A119.5
I2—Cu2—Cu1i56.33 (3)C18—C19—C20120.0 (8)
I1—Cu2—Cu1i55.21 (3)C18—C19—H19A120.0
C1—P1—C7105.7 (4)C20—C19—H19A120.0
C1—P1—C1399.9 (3)C19—C20—C21118.8 (8)
C7—P1—C13104.0 (3)C19—C20—H20A120.6
C1—P1—Cu1114.1 (3)C21—C20—H20A120.6
C7—P1—Cu1115.2 (3)C20—C21—C16122.2 (7)
C13—P1—Cu1116.2 (3)C20—C21—H21A118.9
C16—P2—C15104.5 (3)C16—C21—H21A118.9
C16—P2—C22102.1 (3)C27—C22—C23119.8 (6)
C15—P2—C22102.7 (3)C27—C22—P2120.0 (5)
C16—P2—Cu2120.3 (2)C23—C22—P2120.0 (5)
C15—P2—Cu2112.5 (2)C24—C23—C22120.8 (8)
C22—P2—Cu2112.9 (3)C24—C23—H23A119.6
C28—N1—C32117.0 (7)C22—C23—H23A119.6
C28—N1—Cu2122.3 (5)C25—C24—C23119.5 (9)
C32—N1—Cu2120.1 (6)C25—C24—H24A120.2
C6—C1—C2118.2 (8)C23—C24—H24A120.2
C6—C1—P1122.3 (7)C24—C25—C26121.5 (8)
C2—C1—P1119.5 (7)C24—C25—H25A119.2
C3—C2—C1119.6 (10)C26—C25—H25A119.2
C3—C2—H2A120.2C25—C26—C27119.0 (9)
C1—C2—H2A120.2C25—C26—H26A120.5
C4—C3—C2123.0 (11)C27—C26—H26A120.5
C4—C3—H3A118.5C22—C27—C26119.3 (8)
C2—C3—H3A118.5C22—C27—H27A120.4
C3—C4—C5118.3 (12)C26—C27—H27A120.4
C3—C4—H4A120.9N1—C28—C29123.7 (7)
C5—C4—H4A120.8N1—C28—H28A118.2
C4—C5—C6120.7 (11)C29—C28—H28A118.2
C4—C5—H5A119.7C30—C29—C28118.1 (8)
C6—C5—H5A119.7C30—C29—C33119.8 (9)
C1—C6—C5120.1 (10)C28—C29—C33122.1 (8)
C1—C6—H6A119.9C29—C30—C31119.9 (9)
C5—C6—H6A119.9C29—C30—H30A120.1
C8—C7—C12118.3 (7)C31—C30—H30A120.1
C8—C7—P1124.7 (7)C30—C31—C32118.2 (9)
C12—C7—P1117.0 (6)C30—C31—H31A120.9
C9—C8—C7120.3 (10)C32—C31—H31A120.9
C9—C8—H8A119.8N1—C32—C31123.1 (9)
C7—C8—H8A119.8N1—C32—H32A118.4
C8—C9—C10121.3 (10)C31—C32—H32A118.4
C8—C9—H9A119.4O1—C33—C34121.2 (10)
C10—C9—H9A119.4O1—C33—C29119.2 (11)
C9—C10—C11120.2 (9)C34—C33—C29119.5 (9)
C9—C10—H10A119.9C33—C34—H34A109.5
C11—C10—H10A119.9C33—C34—H34B109.5
C10—C11—C12118.9 (10)H34A—C34—H34B109.5
C10—C11—H11A120.6C33—C34—H34C109.5
C12—C11—H11A120.6H34A—C34—H34C109.5
C7—C12—C11121.0 (9)H34B—C34—H34C109.5
C7—C12—H12A119.5Cl1—C41—Cl2115.5 (9)
C11—C12—H12A119.5Cl1—C41—H41A108.4
C14—C13—P1114.1 (5)Cl2—C41—H41A108.4
C14—C13—H13A108.7Cl1—C41—H41B108.4
P1—C13—H13A108.7Cl2—C41—H41B108.4
C14—C13—H13B108.7H41A—C41—H41B107.5
P1—C13—H13B108.7
C7—P1—C1—C613.1 (8)C15—P2—C16—C2145.4 (6)
C13—P1—C1—C6120.8 (7)C22—P2—C16—C2161.3 (7)
Cu1—P1—C1—C6114.5 (7)Cu2—P2—C16—C21172.9 (5)
C7—P1—C1—C2168.4 (7)C21—C16—C17—C182.1 (12)
C13—P1—C1—C260.7 (7)P2—C16—C17—C18178.1 (7)
Cu1—P1—C1—C264.0 (7)C16—C17—C18—C190.9 (15)
C6—C1—C2—C31.4 (13)C17—C18—C19—C200.8 (16)
P1—C1—C2—C3179.9 (7)C18—C19—C20—C211.0 (14)
C1—C2—C3—C41.6 (15)C19—C20—C21—C160.3 (12)
C2—C3—C4—C50.7 (17)C17—C16—C21—C201.8 (11)
C3—C4—C5—C60.4 (17)P2—C16—C21—C20178.4 (6)
C2—C1—C6—C50.3 (13)C16—P2—C22—C2736.8 (8)
P1—C1—C6—C5178.8 (8)C15—P2—C22—C27144.9 (7)
C4—C5—C6—C10.6 (16)Cu2—P2—C22—C2793.8 (7)
C1—P1—C7—C862.0 (7)C16—P2—C22—C23147.9 (7)
C13—P1—C7—C842.7 (8)C15—P2—C22—C2339.8 (8)
Cu1—P1—C7—C8171.1 (6)Cu2—P2—C22—C2381.5 (7)
C1—P1—C7—C12120.5 (6)C27—C22—C23—C241.3 (13)
C13—P1—C7—C12134.8 (6)P2—C22—C23—C24176.7 (7)
Cu1—P1—C7—C126.5 (6)C22—C23—C24—C250.5 (15)
C12—C7—C8—C91.4 (12)C23—C24—C25—C262.8 (16)
P1—C7—C8—C9176.1 (7)C24—C25—C26—C273.3 (17)
C7—C8—C9—C100.6 (15)C23—C22—C27—C260.8 (14)
C8—C9—C10—C111.5 (16)P2—C22—C27—C26176.1 (8)
C9—C10—C11—C120.4 (15)C25—C26—C27—C221.4 (15)
C8—C7—C12—C112.5 (11)C32—N1—C28—C290.6 (12)
P1—C7—C12—C11175.2 (6)Cu2—N1—C28—C29172.0 (7)
C10—C11—C12—C71.7 (13)N1—C28—C29—C300.3 (13)
C1—P1—C13—C14168.9 (6)N1—C28—C29—C33177.2 (8)
C7—P1—C13—C1482.0 (6)C28—C29—C30—C310.0 (14)
Cu1—P1—C13—C1445.7 (6)C33—C29—C30—C31177.6 (9)
P1—C13—C14—C1559.7 (8)C29—C30—C31—C320.0 (16)
C13—C14—C15—P2172.9 (5)C28—N1—C32—C310.5 (14)
C16—P2—C15—C1477.3 (6)Cu2—N1—C32—C31172.1 (8)
C22—P2—C15—C14176.4 (5)C30—C31—C32—N10.2 (16)
Cu2—P2—C15—C1454.8 (6)C30—C29—C33—O11.2 (15)
C15—P2—C16—C17134.4 (6)C28—C29—C33—O1176.4 (10)
C22—P2—C16—C17119.0 (6)C30—C29—C33—C34174.9 (9)
Cu2—P2—C16—C176.9 (7)C28—C29—C33—C347.5 (14)
Symmetry code: (i) x, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C28—H28A···I20.933.073.735 (8)130
C41—H41A···O1ii0.972.503.185 (17)128
Symmetry code: (ii) x, y+1, z.
2-1,3-Bis(diphenylphosphanyl)propane-κ2P:P']di-µ3-iodido-di-µ2-iodido-[1-(pyridin-4-yl)ethan-1-one-κN]tetracopper(I) (CuL4) top
Crystal data top
[Cu4I4(C6H7NO)2(C27H26P2)2]Z = 1
Mr = 1828.86F(000) = 892
Triclinic, P1Dx = 1.794 Mg m3
a = 11.981 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 12.996 (3) ÅCell parameters from 5949 reflections
c = 13.230 (3) Åθ = 3.0–25.0°
α = 62.49 (3)°µ = 3.20 mm1
β = 68.32 (3)°T = 293 K
γ = 83.71 (3)°Block, yellow
V = 1693.2 (8) Å30.26 × 0.25 × 0.18 mm
Data collection top
Rigaku R-axis RAPID
diffractometer
3380 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.112
Oscillation scansθmax = 25.0°, θmin = 3.0°
Absorption correction: multi-scan
(RAPID AUTO; Rigaku, 1998)
h = 1413
Tmin = 0.410, Tmax = 1.000k = 1515
13417 measured reflectionsl = 1515
5949 independent reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.064Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.154H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.027P)2]
where P = (Fo2 + 2Fc2)/3
5949 reflections(Δ/σ)max < 0.001
379 parametersΔρmax = 1.05 e Å3
0 restraintsΔρmin = 1.31 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.84534 (6)0.40748 (6)0.04377 (6)0.0454 (2)
I20.83888 (7)0.57809 (6)0.26992 (6)0.0516 (2)
Cu11.09434 (13)0.39277 (12)0.04689 (12)0.0591 (4)
Cu20.74647 (11)0.40079 (11)0.26659 (11)0.0480 (4)
P11.1371 (2)0.2260 (2)0.0895 (2)0.0413 (7)
P20.7798 (2)0.2409 (2)0.4168 (2)0.0402 (6)
N10.5717 (8)0.4382 (8)0.2837 (8)0.052 (2)
C11.2893 (9)0.2244 (8)0.0921 (8)0.037 (2)
C21.3668 (10)0.3214 (10)0.0162 (10)0.060 (3)
H2A1.3413160.3893920.0341450.072*
C31.4817 (11)0.3188 (11)0.0142 (10)0.068 (4)
H3A1.5338740.3853330.0393620.082*
C41.5223 (11)0.2233 (12)0.0869 (12)0.070 (4)
H4A1.6006880.2236030.0849630.084*
C51.4458 (15)0.1272 (12)0.1628 (15)0.098 (5)
H5A1.4724880.0597740.2125530.118*
C61.3271 (12)0.1270 (11)0.1680 (12)0.087 (5)
H6A1.2744630.0609730.2227340.104*
C71.1240 (9)0.0931 (9)0.0794 (9)0.044 (3)
C81.1918 (12)0.0883 (10)0.0269 (10)0.063 (3)
H8A1.2410000.1532710.0920660.076*
C91.1889 (13)0.0102 (13)0.0399 (12)0.084 (4)
H9A1.2383940.0117800.1122750.101*
C101.1132 (14)0.1074 (12)0.0534 (14)0.079 (4)
H10A1.1081790.1725100.0428460.094*
C111.0481 (13)0.1051 (11)0.1582 (12)0.078 (4)
H11A0.9996120.1704540.2234440.093*
C121.0526 (12)0.0029 (10)0.1707 (11)0.067 (3)
H12A1.0048810.0021030.2439100.080*
C131.0366 (10)0.1873 (9)0.2450 (9)0.053 (3)
H13A0.9563370.1691340.2531790.063*
H13B1.0622120.1171210.2995620.063*
C141.0297 (9)0.2789 (8)0.2861 (8)0.042 (2)
H14A1.0124560.3517060.2272130.051*
H14B1.1074090.2906510.2878730.051*
C150.9337 (10)0.2470 (9)0.4120 (9)0.051 (3)
H15A0.9411610.3038590.4378860.061*
H15B0.9482740.1718580.4698060.061*
C160.7524 (8)0.0986 (8)0.4300 (8)0.039 (2)
C170.7994 (12)0.0014 (9)0.4917 (11)0.069 (4)
H17A0.8491000.0010060.5305730.083*
C180.7754 (14)0.1036 (11)0.4974 (13)0.086 (5)
H18A0.8064410.1709070.5419310.104*
C190.7052 (13)0.1083 (11)0.4377 (12)0.076 (4)
H19A0.6916180.1780940.4391480.092*
C200.6551 (13)0.0108 (10)0.3761 (11)0.074 (4)
H20A0.6049600.0139150.3380650.089*
C210.6809 (11)0.0915 (9)0.3720 (10)0.061 (3)
H21A0.6488900.1586600.3284990.073*
C220.6836 (9)0.2185 (8)0.5715 (8)0.038 (2)
C230.7248 (11)0.1871 (9)0.6658 (9)0.059 (3)
H23A0.8064620.1785940.6517420.071*
C240.6458 (12)0.1682 (10)0.7810 (10)0.065 (3)
H24A0.6743280.1485420.8437640.079*
C250.5257 (12)0.1787 (11)0.8016 (11)0.067 (3)
H25A0.4725930.1632100.8797770.081*
C260.4810 (10)0.2117 (10)0.7095 (10)0.057 (3)
H26A0.3994310.2211980.7236750.068*
C270.5611 (9)0.2299 (9)0.5964 (9)0.051 (3)
H27A0.5321470.2507770.5337240.061*
C280.5062 (11)0.3863 (9)0.2575 (10)0.059 (3)
H28A0.5458050.3411200.2191480.070*
C290.3850 (10)0.3927 (9)0.2815 (10)0.057 (3)
H29A0.3447300.3551540.2582310.068*
C300.3252 (10)0.4567 (9)0.3412 (9)0.048 (3)
C310.3895 (10)0.5117 (11)0.3704 (11)0.072 (4)
H31A0.3522620.5577650.4084700.087*
C320.5120 (10)0.4975 (9)0.3422 (9)0.052 (3)
H32A0.5544680.5322590.3661310.062*
C330.1870 (12)0.4610 (11)0.3796 (12)0.068 (3)
C340.1407 (13)0.5749 (12)0.3487 (17)0.138 (8)
H34A0.2065770.6330030.3073920.208*
H34B0.0969370.5891400.2962250.208*
H34C0.0880700.5781190.4221020.208*
O10.1274 (9)0.3734 (8)0.4305 (11)0.110 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0362 (4)0.0478 (4)0.0510 (4)0.0082 (3)0.0109 (3)0.0264 (3)
I20.0500 (5)0.0536 (5)0.0541 (5)0.0027 (4)0.0155 (4)0.0290 (4)
Cu10.0610 (10)0.0557 (9)0.0550 (8)0.0216 (7)0.0237 (7)0.0224 (7)
Cu20.0399 (8)0.0461 (8)0.0538 (8)0.0116 (6)0.0169 (6)0.0213 (6)
P10.0362 (16)0.0418 (15)0.0413 (15)0.0142 (12)0.0112 (12)0.0197 (12)
P20.0348 (16)0.0448 (15)0.0425 (15)0.0088 (12)0.0120 (12)0.0238 (12)
N10.044 (6)0.054 (6)0.060 (6)0.016 (5)0.018 (5)0.030 (5)
C10.038 (6)0.042 (6)0.033 (5)0.006 (5)0.013 (4)0.021 (4)
C20.037 (7)0.054 (7)0.066 (7)0.010 (6)0.010 (6)0.017 (6)
C30.040 (8)0.080 (9)0.063 (8)0.006 (7)0.007 (6)0.022 (6)
C40.039 (8)0.089 (10)0.109 (10)0.029 (7)0.037 (7)0.064 (8)
C50.098 (13)0.052 (8)0.160 (14)0.023 (8)0.091 (12)0.030 (9)
C60.058 (9)0.067 (9)0.106 (11)0.006 (7)0.046 (8)0.004 (8)
C70.036 (6)0.046 (6)0.056 (7)0.019 (5)0.020 (5)0.030 (5)
C80.082 (10)0.060 (8)0.050 (7)0.014 (7)0.020 (6)0.032 (6)
C90.081 (11)0.102 (11)0.084 (10)0.022 (9)0.013 (8)0.068 (9)
C100.089 (12)0.078 (10)0.118 (13)0.028 (9)0.060 (10)0.071 (10)
C110.093 (12)0.058 (8)0.085 (10)0.003 (8)0.034 (9)0.031 (7)
C120.067 (9)0.060 (8)0.076 (8)0.010 (7)0.026 (7)0.034 (7)
C130.046 (7)0.046 (6)0.052 (6)0.020 (5)0.016 (5)0.016 (5)
C140.029 (6)0.047 (6)0.051 (6)0.009 (5)0.014 (5)0.024 (5)
C150.056 (8)0.050 (6)0.050 (6)0.001 (6)0.015 (5)0.029 (5)
C160.027 (6)0.042 (6)0.047 (6)0.000 (5)0.011 (5)0.021 (5)
C170.087 (10)0.044 (7)0.081 (9)0.004 (7)0.045 (8)0.021 (6)
C180.107 (13)0.049 (8)0.105 (11)0.006 (8)0.058 (10)0.021 (7)
C190.095 (12)0.051 (8)0.085 (9)0.002 (7)0.028 (8)0.035 (7)
C200.111 (12)0.056 (8)0.080 (9)0.013 (8)0.059 (9)0.035 (7)
C210.082 (10)0.040 (6)0.066 (8)0.002 (6)0.041 (7)0.017 (6)
C220.039 (6)0.039 (5)0.043 (6)0.013 (5)0.009 (5)0.030 (5)
C230.057 (8)0.074 (8)0.045 (7)0.019 (6)0.024 (6)0.025 (6)
C240.067 (9)0.077 (9)0.057 (8)0.015 (7)0.025 (7)0.035 (6)
C250.058 (9)0.082 (9)0.057 (8)0.002 (7)0.006 (6)0.039 (6)
C260.033 (7)0.075 (8)0.061 (7)0.005 (6)0.002 (6)0.042 (6)
C270.031 (6)0.067 (7)0.047 (6)0.003 (5)0.004 (5)0.027 (5)
C280.048 (8)0.051 (7)0.060 (7)0.011 (6)0.007 (6)0.023 (6)
C290.047 (8)0.054 (7)0.088 (8)0.005 (6)0.019 (6)0.051 (6)
C300.042 (7)0.042 (6)0.067 (7)0.015 (5)0.021 (6)0.032 (5)
C310.038 (8)0.099 (10)0.117 (10)0.021 (7)0.025 (7)0.084 (9)
C320.047 (7)0.062 (7)0.067 (7)0.009 (6)0.022 (6)0.046 (6)
C330.044 (8)0.061 (8)0.117 (10)0.027 (7)0.029 (7)0.059 (8)
C340.052 (10)0.080 (11)0.25 (2)0.025 (9)0.051 (12)0.060 (12)
O10.053 (6)0.067 (6)0.213 (12)0.009 (5)0.039 (7)0.071 (7)
Geometric parameters (Å, º) top
I1—Cu22.7032 (17)C14—C151.523 (13)
I1—Cu1i2.7920 (18)C14—H14A0.9700
I1—Cu12.7962 (18)C14—H14B0.9700
I2—Cu1i2.6039 (17)C15—H15A0.9700
I2—Cu22.6881 (17)C15—H15B0.9700
Cu1—P12.246 (3)C16—C171.368 (13)
Cu1—Cu2i3.017 (3)C16—C211.379 (13)
Cu2—N12.050 (9)C17—C181.353 (17)
Cu2—P22.240 (3)C17—H17A0.9300
P1—C131.811 (10)C18—C191.371 (17)
P1—C71.820 (11)C18—H18A0.9300
P1—C11.835 (10)C19—C201.367 (15)
P2—C161.830 (10)C19—H19A0.9300
P2—C151.831 (11)C20—C211.370 (15)
P2—C221.839 (9)C20—H20A0.9300
N1—C321.313 (13)C21—H21A0.9300
N1—C281.313 (14)C22—C231.382 (13)
C1—C61.360 (13)C22—C271.387 (13)
C1—C21.363 (13)C23—C241.385 (15)
C2—C31.364 (15)C23—H23A0.9300
C2—H2A0.9300C24—C251.366 (16)
C3—C41.347 (15)C24—H24A0.9300
C3—H3A0.9300C25—C261.380 (15)
C4—C51.350 (17)C25—H25A0.9300
C4—H4A0.9300C26—C271.370 (14)
C5—C61.399 (18)C26—H26A0.9300
C5—H5A0.9300C27—H27A0.9300
C6—H6A0.9300C28—C291.369 (15)
C7—C121.351 (15)C28—H28A0.9300
C7—C81.367 (14)C29—C301.375 (14)
C8—C91.373 (16)C29—H29A0.9300
C8—H8A0.9300C30—C311.360 (15)
C9—C101.387 (18)C30—C331.546 (16)
C9—H9A0.9300C31—C321.388 (15)
C10—C111.329 (18)C31—H31A0.9300
C10—H10A0.9300C32—H32A0.9300
C11—C121.420 (17)C33—O11.172 (14)
C11—H11A0.9300C33—C341.447 (17)
C12—H12A0.9300C34—H34A0.9600
C13—C141.505 (14)C34—H34B0.9600
C13—H13A0.9700C34—H34C0.9600
C13—H13B0.9700
Cu2—I1—Cu1i66.59 (6)P1—C13—H13A108.4
Cu2—I1—Cu1117.54 (5)C14—C13—H13B108.4
Cu1i—I1—Cu184.66 (6)P1—C13—H13B108.4
Cu1i—I2—Cu269.51 (6)H13A—C13—H13B107.5
P1—Cu1—I2i117.05 (10)C13—C14—C15112.9 (8)
P1—Cu1—I1i114.46 (10)C13—C14—H14A109.0
I2i—Cu1—I1i111.04 (6)C15—C14—H14A109.0
P1—Cu1—I1107.26 (10)C13—C14—H14B109.0
I2i—Cu1—I1109.28 (6)C15—C14—H14B109.0
I1i—Cu1—I195.34 (6)H14A—C14—H14B107.8
P1—Cu1—Cu2i131.81 (10)C14—C15—P2113.6 (7)
I2i—Cu1—Cu2i56.56 (5)C14—C15—H15A108.8
I1i—Cu1—Cu2i55.30 (5)P2—C15—H15A108.8
I1—Cu1—Cu2i120.02 (6)C14—C15—H15B108.8
N1—Cu2—P2118.3 (3)P2—C15—H15B108.8
N1—Cu2—I2104.2 (3)H15A—C15—H15B107.7
P2—Cu2—I2104.59 (9)C17—C16—C21117.3 (10)
N1—Cu2—I1104.0 (3)C17—C16—P2124.8 (8)
P2—Cu2—I1114.27 (9)C21—C16—P2117.9 (7)
I2—Cu2—I1111.23 (6)C18—C17—C16121.5 (12)
N1—Cu2—Cu1i107.2 (2)C18—C17—H17A119.2
P2—Cu2—Cu1i133.85 (9)C16—C17—H17A119.2
I2—Cu2—Cu1i53.93 (5)C17—C18—C19120.1 (12)
I1—Cu2—Cu1i58.12 (5)C17—C18—H18A120.0
C13—P1—C7101.4 (5)C19—C18—H18A120.0
C13—P1—C1105.2 (5)C20—C19—C18120.4 (12)
C7—P1—C1102.4 (4)C20—C19—H19A119.8
C13—P1—Cu1112.4 (3)C18—C19—H19A119.8
C7—P1—Cu1118.1 (3)C19—C20—C21118.2 (12)
C1—P1—Cu1115.6 (3)C19—C20—H20A120.9
C16—P2—C15106.5 (5)C21—C20—H20A120.9
C16—P2—C2299.8 (4)C20—C21—C16122.4 (10)
C15—P2—C22104.5 (5)C20—C21—H21A118.8
C16—P2—Cu2118.7 (3)C16—C21—H21A118.8
C15—P2—Cu2111.6 (3)C23—C22—C27117.8 (9)
C22—P2—Cu2114.2 (3)C23—C22—P2124.2 (8)
C32—N1—C28115.3 (10)C27—C22—P2118.0 (7)
C32—N1—Cu2122.1 (8)C22—C23—C24120.7 (11)
C28—N1—Cu2121.4 (8)C22—C23—H23A119.6
C6—C1—C2119.1 (10)C24—C23—H23A119.6
C6—C1—P1120.9 (8)C25—C24—C23119.3 (11)
C2—C1—P1119.9 (7)C25—C24—H24A120.3
C3—C2—C1120.0 (10)C23—C24—H24A120.3
C3—C2—H2A120.0C24—C25—C26121.8 (11)
C1—C2—H2A120.0C24—C25—H25A119.1
C4—C3—C2122.3 (11)C26—C25—H25A119.1
C4—C3—H3A118.8C27—C26—C25117.6 (11)
C2—C3—H3A118.8C27—C26—H26A121.2
C3—C4—C5118.0 (11)C25—C26—H26A121.2
C3—C4—H4A121.0C26—C27—C22122.7 (10)
C5—C4—H4A121.0C26—C27—H27A118.6
C4—C5—C6121.3 (11)C22—C27—H27A118.6
C4—C5—H5A119.4N1—C28—C29126.0 (11)
C6—C5—H5A119.4N1—C28—H28A117.0
C1—C6—C5119.3 (12)C29—C28—H28A117.0
C1—C6—H6A120.4C28—C29—C30117.3 (11)
C5—C6—H6A120.4C28—C29—H29A121.3
C12—C7—C8117.0 (11)C30—C29—H29A121.3
C12—C7—P1124.6 (9)C31—C30—C29118.6 (11)
C8—C7—P1118.4 (9)C31—C30—C33120.9 (10)
C7—C8—C9121.6 (11)C29—C30—C33120.4 (10)
C7—C8—H8A119.2C30—C31—C32118.5 (11)
C9—C8—H8A119.2C30—C31—H31A120.7
C8—C9—C10121.0 (12)C32—C31—H31A120.7
C8—C9—H9A119.5N1—C32—C31124.1 (11)
C10—C9—H9A119.5N1—C32—H32A117.9
C11—C10—C9118.3 (13)C31—C32—H32A117.9
C11—C10—H10A120.9O1—C33—C34124.8 (13)
C9—C10—H10A120.9O1—C33—C30118.6 (11)
C10—C11—C12120.1 (13)C34—C33—C30116.6 (12)
C10—C11—H11A119.9C33—C34—H34A109.5
C12—C11—H11A119.9C33—C34—H34B109.5
C7—C12—C11122.0 (12)H34A—C34—H34B109.5
C7—C12—H12A119.0C33—C34—H34C109.5
C11—C12—H12A119.0H34A—C34—H34C109.5
C14—C13—P1115.4 (7)H34B—C34—H34C109.5
C14—C13—H13A108.4
C13—P1—C1—C657.6 (11)C15—P2—C16—C21145.3 (9)
C7—P1—C1—C648.0 (11)C22—P2—C16—C21106.3 (9)
Cu1—P1—C1—C6177.8 (9)Cu2—P2—C16—C2118.4 (10)
C13—P1—C1—C2123.1 (9)C21—C16—C17—C181.0 (18)
C7—P1—C1—C2131.2 (9)P2—C16—C17—C18179.9 (11)
Cu1—P1—C1—C21.4 (10)C16—C17—C18—C192 (2)
C6—C1—C2—C32.1 (18)C17—C18—C19—C203 (2)
P1—C1—C2—C3177.1 (10)C18—C19—C20—C212 (2)
C1—C2—C3—C41 (2)C19—C20—C21—C162 (2)
C2—C3—C4—C51 (2)C17—C16—C21—C200.9 (18)
C3—C4—C5—C61 (2)P2—C16—C21—C20179.9 (10)
C2—C1—C6—C53 (2)C16—P2—C22—C2397.0 (9)
P1—C1—C6—C5176.6 (12)C15—P2—C22—C2313.0 (10)
C4—C5—C6—C12 (3)Cu2—P2—C22—C23135.2 (8)
C13—P1—C7—C121.0 (10)C16—P2—C22—C2780.7 (9)
C1—P1—C7—C12109.5 (10)C15—P2—C22—C27169.2 (8)
Cu1—P1—C7—C12122.2 (9)Cu2—P2—C22—C2747.0 (9)
C13—P1—C7—C8178.1 (9)C27—C22—C23—C240.2 (16)
C1—P1—C7—C869.6 (9)P2—C22—C23—C24177.9 (9)
Cu1—P1—C7—C858.6 (9)C22—C23—C24—C251.2 (18)
C12—C7—C8—C91.0 (18)C23—C24—C25—C262 (2)
P1—C7—C8—C9178.2 (10)C24—C25—C26—C272.2 (19)
C7—C8—C9—C102 (2)C25—C26—C27—C221.2 (18)
C8—C9—C10—C113 (2)C23—C22—C27—C260.2 (17)
C9—C10—C11—C123 (2)P2—C22—C27—C26178.0 (9)
C8—C7—C12—C110.5 (17)C32—N1—C28—C292.6 (16)
P1—C7—C12—C11178.6 (10)Cu2—N1—C28—C29170.4 (8)
C10—C11—C12—C72 (2)N1—C28—C29—C301.8 (17)
C7—P1—C13—C14177.7 (7)C28—C29—C30—C311.5 (16)
C1—P1—C13—C1471.3 (8)C28—C29—C30—C33175.7 (10)
Cu1—P1—C13—C1455.2 (8)C29—C30—C31—C322.1 (17)
P1—C13—C14—C15173.5 (7)C33—C30—C31—C32175.0 (10)
C13—C14—C15—P266.3 (10)C28—N1—C32—C313.3 (16)
C16—P2—C15—C1481.4 (8)Cu2—N1—C32—C31171.0 (9)
C22—P2—C15—C14173.5 (7)C30—C31—C32—N13.2 (18)
Cu2—P2—C15—C1449.7 (8)C31—C30—C33—O1128.9 (15)
C15—P2—C16—C1733.5 (11)C29—C30—C33—O148.2 (18)
C22—P2—C16—C1774.9 (10)C31—C30—C33—C3451.3 (18)
Cu2—P2—C16—C17160.4 (9)C29—C30—C33—C34131.6 (14)
Symmetry code: (i) x+2, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2A···I1i0.933.254.056 (11)146
C14—H14B···O1ii0.972.653.265 (15)121
C15—H15A···O1ii0.972.453.125 (14)126
C32—H32A···I20.933.183.815 (11)127
C34—H34B···I2iii0.963.264.109 (16)148
Symmetry codes: (i) x+2, y+1, z; (ii) x+1, y, z; (iii) x1, y, z.
Emission properties of CuL3 and CuL4 in the solid state at 298 and 77 K top
Emission prppertiesCuL3CuL4
λmax (298 K) (nm)562580
τ (298 K) (µs)2.5210.78
ΦPL (298 K) (%)26.330.6
λmax (77 K) (nm)572588
τ (77 K) (µs)95.9046.33
ΔE(S1 - T1) (cm-1)290280
 

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