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N,N′-Bis­(pyridin-4-yl)formamidine (4-pyfH) was reacted with AuI and AgI metal salts to form a novel tetra­nuclear complex, tetra­kis­[μ-N,N′-bis­(pyridin-4-yl)formamidinato]digold(I)disilver(I), [Ag2Au2(C11H9N4)2] or [AuxAg4–x(4-pyf)4] (x = 0–4), 1, which is supported by its metallophilicity. Due to the potential permutation of the coordinated metal ions, six different canonical structures of 1 can be obtained. Complex 1 shows an emission at 501 nm upon excitation at 375 nm in the solid state and an emission at 438 nm upon excitation at 304 nm when dispersed in methanol. Time-dependent density functional theory (TD-DFT) calculations confirmed that these emissions can be ascribed to metal-to-ligand charge transfer (MLCT) processes. Moreover, the calculations of the optimized structural conformations of the S0 ground state, and the S1 and T1 excited states are discussed and suggest a distorted planar conformation for the tetra­nuclear Au2Ag2 complex.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229619008581/qs3083sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229619008581/qs3083Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2053229619008581/qs3083sup3.pdf
Additional experimental information, figures and tables

CCDC reference: 1896371

Computing details top

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT (Bruker, 2008); program(s) used to solve structure: olex2.solve (Bourhis et al., 2015); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).

Tetrakis[µ-N,N'-bis(pyridin-4-yl)formamidinato]digold(I)disilver(I) top
Crystal data top
[AgAu(C11H9N4)2]Dx = 1.876 Mg m3
Mr = 699.28Mo Kα radiation, λ = 0.71073 Å
Tetragonal, P4n2Cell parameters from 9407 reflections
a = 16.5350 (4) Åθ = 2.9–28.3°
c = 18.1127 (4) ŵ = 6.73 mm1
V = 4952.1 (3) Å3T = 296 K
Z = 8Plate, colourless
F(000) = 26560.35 × 0.25 × 0.2 mm
Data collection top
Bruker APEXII CCD
diffractometer
4918 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.049
φ and ω scansθmax = 28.3°, θmin = 1.7°
Absorption correction: multi-scan
(SADABS; Bruker, 2008)
h = 1621
Tmin = 0.385, Tmax = 0.746k = 2221
23337 measured reflectionsl = 2423
5627 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.032 w = 1/[σ2(Fo2) + (0.0347P)2 + 5.3324P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.080(Δ/σ)max < 0.001
S = 1.05Δρmax = 1.22 e Å3
5627 reflectionsΔρmin = 0.76 e Å3
299 parametersAbsolute structure: Flack x determined using 1780 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
0 restraintsAbsolute structure parameter: 0.070 (14)
Primary atom site location: iterative
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.

Refinement. The diffraction data of this complex was collected on a Bruker SMART APEXII diffractometer equipped with a graphite-monochromatic Mo Kα (λα = 0.71073 Å) radiation at 296.15 K. Data reduction carried by standard methods with use of well-established computational procedures (Bruker & SHELXTL V6.14; Sheldrick, 2008). The structure factors were obtained after Lorentz and polarization correction.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Au10.3983 (2)0.4864 (3)0.24374 (17)0.0202 (7)0.5
Au20.5000000.5000000.37619 (3)0.01540 (15)0.5
Au30.5000000.5000000.11049 (3)0.01605 (16)0.5
Ag10.3991 (4)0.4910 (5)0.2442 (2)0.0098 (10)0.5
Ag20.5000000.5000000.37619 (3)0.01540 (15)0.5
Ag30.5000000.5000000.11049 (3)0.01605 (16)0.5
N10.2597 (9)0.7481 (8)0.3844 (6)0.082 (4)
N20.3841 (5)0.6071 (5)0.2241 (4)0.037 (2)
N30.4581 (6)0.6156 (5)0.1116 (4)0.035 (2)
N40.5262 (8)0.7869 (7)0.0518 (7)0.061 (3)
N50.2953 (9)0.2021 (6)0.1164 (5)0.066 (3)
N60.4058 (5)0.3680 (5)0.2659 (5)0.037 (2)
N70.4811 (5)0.3776 (5)0.3785 (5)0.034 (2)
N80.5755 (8)0.2375 (6)0.5546 (7)0.063 (3)
C10.2402 (11)0.6697 (10)0.3687 (10)0.100 (7)
H10.1972000.6467040.3942620.120*
C20.2800 (9)0.6221 (8)0.3171 (9)0.078 (5)
H20.2638220.5687850.3099010.093*
C30.3433 (7)0.6532 (7)0.2765 (7)0.051 (3)
C40.3689 (8)0.7351 (8)0.2945 (6)0.050 (3)
H40.4122160.7596690.2707230.060*
C50.3242 (9)0.7751 (8)0.3500 (7)0.061 (4)
H50.3424980.8260860.3637700.073*
C60.4131 (7)0.6464 (6)0.1658 (6)0.036 (2)
H60.4006310.7011020.1624780.044*
C70.5748 (9)0.7292 (8)0.0293 (8)0.063 (4)
H70.6266030.7281070.0491690.075*
C80.5551 (7)0.6690 (7)0.0224 (6)0.043 (3)
H80.5924080.6291700.0350050.051*
C90.4761 (8)0.6703 (8)0.0554 (6)0.037 (3)
C100.4234 (8)0.7308 (7)0.0302 (6)0.045 (3)
H100.3707780.7329820.0483010.054*
C110.4487 (9)0.7877 (8)0.0215 (7)0.047 (3)
H110.4126270.8276330.0364080.057*
C120.2673 (9)0.2792 (8)0.1298 (8)0.072 (5)
H120.2206640.2949510.1049690.087*
C130.3025 (8)0.3359 (9)0.1773 (7)0.062 (4)
H130.2799660.3870290.1830720.074*
C140.3720 (7)0.3138 (7)0.2156 (6)0.041 (3)
C150.4068 (7)0.2360 (7)0.2012 (6)0.042 (3)
H150.4543400.2205530.2246750.050*
C160.3690 (9)0.1838 (8)0.1520 (7)0.059 (4)
H160.3935410.1343690.1419690.071*
C170.4425 (6)0.3366 (7)0.3256 (6)0.037 (3)
H170.4409520.2806530.3305360.044*
C180.5081 (8)0.2154 (9)0.5179 (7)0.048 (4)
H180.4832150.1674270.5320460.057*
C190.4734 (7)0.2584 (7)0.4612 (6)0.040 (3)
H190.4261650.2399280.4390040.048*
C200.5088 (7)0.3286 (8)0.4378 (7)0.034 (3)
C210.5815 (8)0.3526 (7)0.4742 (6)0.048 (3)
H210.6085300.3994810.4600390.057*
C220.6108 (9)0.3055 (8)0.5303 (7)0.060 (4)
H220.6584880.3217070.5531440.072*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Au10.0131 (12)0.0101 (8)0.0372 (13)0.0016 (7)0.0029 (10)0.0014 (10)
Au20.0128 (4)0.0094 (4)0.0241 (3)0.0002 (3)0.0000.000
Au30.0133 (5)0.0102 (4)0.0246 (3)0.0027 (3)0.0000.000
Ag10.010 (2)0.0118 (19)0.0072 (15)0.0004 (14)0.0050 (14)0.0039 (15)
Ag20.0128 (4)0.0094 (4)0.0241 (3)0.0002 (3)0.0000.000
Ag30.0133 (5)0.0102 (4)0.0246 (3)0.0027 (3)0.0000.000
N10.121 (14)0.043 (8)0.080 (8)0.021 (7)0.059 (8)0.003 (6)
N20.030 (5)0.038 (5)0.044 (5)0.002 (4)0.005 (4)0.000 (4)
N30.041 (6)0.032 (5)0.031 (4)0.008 (4)0.004 (4)0.003 (4)
N40.062 (8)0.037 (7)0.084 (9)0.001 (6)0.007 (7)0.016 (6)
N50.123 (13)0.015 (6)0.061 (7)0.016 (5)0.037 (7)0.001 (5)
N60.035 (4)0.025 (4)0.051 (6)0.003 (3)0.013 (4)0.007 (4)
N70.027 (5)0.031 (5)0.044 (5)0.001 (4)0.010 (4)0.005 (4)
N80.083 (10)0.032 (6)0.073 (8)0.012 (6)0.028 (7)0.002 (6)
C10.096 (14)0.062 (11)0.141 (16)0.037 (9)0.077 (12)0.022 (11)
C20.066 (10)0.040 (8)0.127 (14)0.013 (7)0.054 (10)0.009 (8)
C30.052 (7)0.036 (7)0.065 (8)0.024 (5)0.008 (6)0.008 (6)
C40.049 (8)0.060 (9)0.041 (6)0.026 (6)0.004 (6)0.005 (6)
C50.080 (11)0.057 (9)0.046 (7)0.039 (7)0.008 (7)0.006 (6)
C60.038 (6)0.028 (6)0.044 (6)0.005 (5)0.004 (5)0.005 (5)
C70.073 (10)0.036 (7)0.078 (10)0.006 (7)0.026 (8)0.010 (7)
C80.038 (7)0.038 (7)0.052 (7)0.008 (5)0.009 (5)0.003 (5)
C90.039 (8)0.028 (7)0.042 (6)0.006 (5)0.001 (5)0.007 (5)
C100.042 (7)0.037 (7)0.057 (8)0.004 (5)0.005 (6)0.000 (6)
C110.052 (9)0.030 (7)0.060 (8)0.010 (6)0.008 (6)0.006 (6)
C120.081 (11)0.044 (8)0.092 (10)0.019 (7)0.050 (9)0.004 (8)
C130.059 (9)0.049 (8)0.078 (10)0.014 (7)0.033 (7)0.004 (7)
C140.036 (6)0.037 (6)0.050 (7)0.010 (5)0.008 (5)0.007 (5)
C150.036 (6)0.041 (7)0.049 (7)0.008 (5)0.003 (5)0.002 (5)
C160.072 (10)0.049 (8)0.058 (8)0.010 (7)0.006 (7)0.004 (6)
C170.030 (6)0.034 (6)0.048 (7)0.003 (4)0.001 (5)0.001 (5)
C180.042 (8)0.043 (8)0.057 (8)0.006 (6)0.002 (6)0.012 (6)
C190.041 (7)0.034 (7)0.045 (6)0.007 (5)0.002 (5)0.001 (5)
C200.031 (7)0.025 (7)0.046 (6)0.001 (5)0.003 (5)0.003 (5)
C210.058 (9)0.030 (6)0.055 (7)0.008 (6)0.019 (6)0.004 (5)
C220.074 (10)0.047 (8)0.058 (8)0.005 (7)0.019 (7)0.005 (7)
Geometric parameters (Å, º) top
Au1—Au22.938 (3)C1—C21.388 (18)
Au1—Au32.950 (4)C2—H20.9300
Au1—N22.041 (9)C2—C31.379 (17)
Au1—N62.001 (9)C3—C41.455 (17)
Au2—N72.048 (9)C4—H40.9300
Au2—N7i2.048 (9)C4—C51.413 (16)
Au3—N32.033 (8)C5—H50.9300
Au3—N3i2.033 (8)C6—H60.9300
Ag1—Ag22.920 (5)C7—H70.9300
Ag1—Ag32.944 (6)C7—C81.405 (16)
Ag1—N21.969 (11)C8—H80.9300
Ag1—N62.074 (11)C8—C91.437 (16)
Ag2—N7i2.048 (9)C9—C101.405 (16)
Ag2—N72.048 (9)C10—H100.9300
Ag3—N32.033 (8)C10—C111.391 (16)
Ag3—N3i2.033 (8)C11—H110.9300
N1—C11.37 (2)C12—H120.9300
N1—C51.313 (17)C12—C131.399 (16)
N2—C31.393 (13)C13—H130.9300
N2—C61.329 (12)C13—C141.391 (16)
N3—C61.334 (12)C14—C151.433 (16)
N3—C91.393 (15)C15—H150.9300
N4—C71.312 (16)C15—C161.389 (16)
N4—C111.394 (18)C16—H160.9300
N5—C121.377 (16)C17—H170.9300
N5—C161.412 (17)C18—H180.9300
N6—C141.396 (12)C18—C191.375 (17)
N6—C171.345 (12)C19—H190.9300
N7—C171.336 (12)C19—C201.368 (17)
N7—C201.420 (15)C20—C211.428 (16)
N8—C181.348 (16)C21—H210.9300
N8—C221.340 (17)C21—C221.370 (16)
C1—H10.9300C22—H220.9300
Au2—Au1—Au3109.63 (13)N2—C3—C4121.4 (11)
N2—Au1—Au297.7 (3)C2—C3—N2121.8 (12)
N2—Au1—Au381.3 (3)C2—C3—C4116.7 (11)
N6—Au1—Au282.9 (3)C3—C4—H4121.9
N6—Au1—Au3101.7 (3)C5—C4—C3116.3 (13)
N6—Au1—N2176.6 (4)C5—C4—H4121.9
Au1i—Au2—Au170.54 (15)N1—C5—C4127.1 (14)
N7i—Au2—Au1i81.6 (3)N1—C5—H5116.4
N7—Au2—Au1i100.4 (3)C4—C5—H5116.4
N7—Au2—Au181.6 (3)N2—C6—N3126.9 (10)
N7i—Au2—Au1100.4 (3)N2—C6—H6116.6
N7i—Au2—N7177.7 (5)N3—C6—H6116.6
Au1—Au3—Au1i70.21 (14)N4—C7—H7117.2
N3—Au3—Au182.5 (2)N4—C7—C8125.5 (14)
N3—Au3—Au1i96.6 (3)C8—C7—H7117.2
N3i—Au3—Au1i82.5 (2)C7—C8—H8120.8
N3i—Au3—Au196.6 (3)C7—C8—C9118.5 (12)
N3—Au3—N3i178.9 (4)C9—C8—H8120.8
Ag2—Ag1—Ag3110.3 (2)N3—C9—C8119.2 (11)
N2—Ag1—Ag2100.0 (4)N3—C9—C10124.6 (11)
N2—Ag1—Ag382.5 (3)C10—C9—C8116.1 (11)
N2—Ag1—N6175.8 (5)C9—C10—H10119.5
N6—Ag1—Ag282.2 (3)C11—C10—C9120.9 (12)
N6—Ag1—Ag3100.1 (3)C11—C10—H10119.5
N7—Ag2—Ag183.1 (3)N4—C11—H11118.8
N7i—Ag2—Ag198.9 (3)C10—C11—N4122.4 (12)
N7i—Ag2—N7177.7 (5)C10—C11—H11118.8
N3—Ag3—Ag181.2 (3)N5—C12—H12117.0
N3i—Ag3—Ag197.9 (3)N5—C12—C13126.1 (13)
N3—Ag3—N3i178.9 (4)C13—C12—H12117.0
C5—N1—C1114.5 (12)C12—C13—H13120.8
C3—N2—Au1118.2 (7)C14—C13—C12118.3 (13)
C3—N2—Ag1117.9 (7)C14—C13—H13120.8
C6—N2—Au1125.1 (7)N6—C14—C15122.3 (10)
C6—N2—Ag1125.3 (7)C13—C14—N6119.2 (10)
C6—N2—C3116.7 (9)C13—C14—C15118.4 (10)
C6—N3—Au3123.8 (7)C14—C15—H15120.2
C6—N3—Ag3123.8 (7)C16—C15—C14119.6 (11)
C6—N3—C9114.1 (9)C16—C15—H15120.2
C9—N3—Au3122.1 (7)N5—C16—H16118.4
C9—N3—Ag3122.1 (7)C15—C16—N5123.2 (12)
C7—N4—C11116.6 (12)C15—C16—H16118.4
C12—N5—C16114.1 (10)N6—C17—H17116.7
C14—N6—Au1118.2 (7)N7—C17—N6126.6 (10)
C14—N6—Ag1119.0 (7)N7—C17—H17116.7
C17—N6—Au1124.5 (7)N8—C18—H18117.5
C17—N6—Ag1123.8 (7)N8—C18—C19125.0 (13)
C17—N6—C14117.3 (8)C19—C18—H18117.5
C17—N7—Au2124.0 (7)C18—C19—H19120.3
C17—N7—Ag2124.0 (7)C20—C19—C18119.5 (12)
C17—N7—C20114.0 (9)C20—C19—H19120.3
C20—N7—Au2122.0 (7)N7—C20—C21117.5 (11)
C20—N7—Ag2122.0 (7)C19—C20—N7125.5 (11)
C22—N8—C18115.1 (12)C19—C20—C21116.9 (11)
N1—C1—H1117.7C20—C21—H21120.6
N1—C1—C2124.6 (15)C22—C21—C20118.8 (12)
C2—C1—H1117.7C22—C21—H21120.6
C1—C2—H2119.8N8—C22—C21124.6 (13)
C3—C2—C1120.5 (14)N8—C22—H22117.7
C3—C2—H2119.8C21—C22—H22117.7
Symmetry code: (i) x+1, y+1, z.
Selected experimental and theoretical distances (Å) and angles (°) for complex 1 modelled in the ground S0, excited S1 and excited T1 states top
ExperimentalS0S1T1
Au1/Ag1—Au2/Ag22.920 (5)–2.938 (3)2.9893.010–3.0332.959–3.055
Au3/Ag3—Au1A/Ag1A2.944 (6)–2.950 (4)2.9892.964–2.9922.923–2.993
Au1/Ag1—N21.969 (11)–2.041 (9)2.0442.170–2.1432.010–2.044
Au1/Ag1—N62.074 (11)–2.001 (9)2.0442.110–2.1452.045–2.046
Au2/Ag2—N7/N7A2.048 (9)2.1422.0322.137–2.146
Au3/Ag3—N3/N3A2.033 (8)2.0442.0392.143–2.154
N2—Au1/Ag1—N6175.8 (5)–176.6 (4)176.6175.5–178.0175.8–175.6
N7—Au2/Ag2—N7A177.7 (5)171.4167.0169.8
N3—Au3/Ag3—N3A178.9 (4)171.4169.1167.1
Acute angles in the M4 plane70.21 (14), 70.54 (15)75.571.6, 72.875.0, 76.4
Obtuse angles in the M4 plane109.63 (13), 110.3 (2)104.5107.7, 107.8103.5, 104.1
Symmetry code: (A) -x+1, -y+1, z.
 

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