Literature DB >> 29250416

Formation and structural characterization of a europium(II) mono(scorpionate) complex and a sterically crowded pyraza-bole.

Phil Liebing1, Marcel Kühling2, Josef Takats3, Liane Hilfert2, Frank T Edelmann2.   

Abstract

The reaction of EuI2(THF)2 with potassium hydro-tris-(3,5-diiso-propyl-pyrazol-yl)borate (K[HB(3,5- iPr2pz)3] (= KTp iPr2, pz = pyrazol-yl) in a molar ratio of 1:1.5 resulted in extensive ligand fragmentation and formation of the europium(II) mono(scorpionate) complex bis-(3,5-diisopropyl-1H-pyrazole)[hydro-tris-(3,5-diiso-propyl-pyrazol-yl)borato]iodido-europium(II), [Eu(C27H46BN6)I(C9H16N2)2] or (Tp iPr2)(3,5- iPr2pzH)2EuIII, 1, in high yield (78%). As a typical by-product, small amounts of the sterically crowded pyraza-bole derivative trans-4,8-bis-(3,5-diiso-propyl-pyrazol-1-yl)-1,3,5,7-tetra-iso-propyl-pyraza-bole, C36H62B2H8 or trans-{(3,5- iPr2pz)HB(μ-3,5- iPr2pz)}2, 2, were formed. Both title compounds have been structurally characterized through single-crystal X-ray diffraction. In 1, two isopropyl groups are each disordered over two orientations with occupancy ratios of 0.574 (10):0.426 (10) and 0.719 (16):0.281 (16). In 2, one isopropyl group is similarly disordered, occupancy ratio 0.649 (9):0.351 (9).

Entities:  

Keywords:  crystal structure; europium; pyraza­bole; pyrazolylborate; scorpionate

Year:  2017        PMID: 29250416      PMCID: PMC5730253          DOI: 10.1107/S2056989017016498

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Chemical context

The organometallic chemistry of divalent lanthanides provides fascinating structures such as the sandwich complexes Ln(C5Me5)2 (Ln = Sm, Eu, Yb; C5Me5 = η 5-penta­methyl­cyclo­penta­dien­yl). An unusual structural feature of the unsolvated lanthanide sandwich complexes Ln(C5Me5)2 (Fig. 1 ▸ a, Ln = Sm, Eu, Yb) is their bent metallocene structure in the solid state. This opens up the coordination sphere around the central divalent lanthanide ions and accounts for the very high reactivity of these compounds (Evans et al., 1983 ▸, 1988 ▸; Evans, 2007 ▸). It has been demonstrated in the past that Trofimenko’s famous hydro­tris­(pyrazol­yl)borate ligands (‘scorpionates’) represent useful alternatives to the ubiquitous cyclo­penta­dienyl ligands (Pettinari, 2008 ▸; Trofimenko, 1966 ▸, 1993 ▸, 1999 ▸). Like the cyclo­penta­dienyl ligands, these trident­ate, monoanionic ligands can also be largely varied in their steric demand by introducing different substituents in the 3- and 5-positions of the pyrazolyl rings. According to Trofimenko’s nomenclature, the abbreviation Tp stands for the ring-unsubstituted hydro­tris­(pyrazol­yl)borate, whereas e.g. TpMe2 denotes the sterically more demanding hydro­tris­(3,5-di­methyl­pyrazol­yl)borate. The homoleptic divalent lanthanide complexes Ln(TpMe2)2 (Ln = Sm, Eu, Yb) have been found to adopt a highly symmetrical, trigonal–anti­prismatic coordination comprising an almost linear B⋯Ln⋯B arrangement (Marques et al., 2002 ▸). Apparently, the sandwich-like structure of Ln(TpMe2)2 is the result of the much larger cone angle of TpMe2 (239°) as compared to that of the C5Me5 ligand (142°) (Davies et al., 1985 ▸). More recently, these investigations have been successfully extended to the even larger hydro­tris­(3,5-diiso­propyl­pyrazol­yl)borate ligand (Tp) (Kitajima et al., 1992 ▸). Homoleptic complexes of this ligand could be isolated with the ‘classical’ divalent lanthanides samarium, europium, thulium and ytterbium (Momin et al., 2014 ▸; Kühling et al., 2015 ▸). Rather surprisingly, crystal structure determinations revealed a ‘bent sandwich’-like mol­ecular structure like Ln(C5Me5)2 (Fig. 1 ▸ b). Computational studies indicated that steric repulsion between the isopropyl groups forces the Tp ligands apart and permits the formation of unusual inter­ligand C—H⋯N hydrogen-bonding inter­actions that help to stabil­ize the structure (Momin et al., 2014 ▸). The recently reported neon-yellow divalent europium complex Eu(Tp)2 also stands out due to its bright-yellow photoluminescence, which has been investigated in great detail (Kühling et al., 2015 ▸; Suta et al., 2017 ▸). Eu(Tp)2 was easily prepared in 83% yield by treatment of the bis-THF adduct of europium(II) diiodide, EuI2(THF)2, with 2 equiv. of KTp in THF solution (Kühling et al. 2015 ▸). We now report that the use of a significantly smaller amount of KTp led to extensive ligand fragmentation and formation of the first europium(II) mono(scorp­ion­ate) complex, [HB(3,5-pz)](3,5-pzH)2EuIII (1), in addition to a frequently observed by-product, the sterically crowded 4,8-bis­(pyrazol­yl)pyraza­bole derivative trans-{(3,5-pz)HB(μ-3,5-pz)}2 (2). Both products have been structurally characterized through single-crystal X-ray diffraction.
Figure 1

Comparison of the mol­ecular structures of ‘bent sandwich’-like lanthanide(II) cyclo­penta­dienides (a) and tris­(3,5-diiso­propyl­pyrazol­yl)borates (b).

The starting material EuI2(THF)2 was prepared from Eu metal and 1,2-di­iodo­ethane using an established literature procedure (Girard et al., 1980 ▸). The reaction of EuI2(THF)2 with 1.5 equiv. of KTp in THF produced a fluorescent, neon-yellow solution and a white precipitate of potassium iodide. Crystallization from n-pentane solvent afforded bright-yellow, air-sensitive crystals, which turned out to be the unexpected europium(II) mono(scorpionate) complex (Tp)(3,5-pzH)2EuIII (1). The 78% isolated yield of 1 was surprisingly high. The coordinated neutral 3,5-diiso­propyl­yrazole ligands clearly resulted from fragmentation of the Tp ligand. Ln-induced fragmentation of substituted Tp ligands is well documented (Domingos et al., 2002 ▸, and references cited therein), but it seems to be even more prevalent in the sterically highly demanding Tp system, as seen in some recently reported Ln(Tp)-derived polysulfide complexes (Kühling et al., 2016 ▸). Despite its paramagnetic nature, inter­pretable NMR spectra could be obtained for 1. A single resonance at δ −5.3 ppm in the 11B NMR spectrum proved the presence of a single boron-containing species. A high-intensity peak at m/z 769 in the mass spectrum of 1 could be assigned to the fragment ion [Eu(Tp)(pz)]+, while a peak at m/z 616 corresponds to the ion [Eu(Tp)]+. Further work-up of the supernatant solution remaining after isolation of 1 by addition of a large volume of non-polar hexa­methyl­disiloxane (HMDSO) resulted in the formation of well-formed, colorless, cube-like crystals in low yield. These turned out to be another ligand fragmentation product typical for lanthanide Tp chemistry, namely the 4,8-bis­(pyrazol­yl)pyraza­bole derivative trans-{(3,5-pz)HB(μ-3,5-pz)}2 (2). The parent pyraza­bole, {H2B(μ-pz)}2 has been known since 1966 when it was reported by Trofimenko contemporaneously with the discovery of Tp ligands (Trofimenko, 1966 ▸). Since then, numerous substituted pyraza­boles have been prepared and structurally investigated (Alcock & Sawyer, 1974 ▸; Cavero et al., 2008 ▸; Niedenzu & Niedenzu, 1984 ▸; Niedenzu & Nöth, 1983 ▸; Trofimenko, 1966 ▸). In a number of recent studies, it has been demonstrated that certain substituted pyraza­boles possess unique photophysical and electrochemical properties and could thus find promising applications in organic photovoltaics (OPVs) and non-linear optics (Jadhav et al., 2013 ▸, 2015 ▸; Misra et al., 2013 ▸, 2014 ▸; Patil et al., 2017 ▸). Compound 2 belongs to the rather special class of 4,8-bis­(pyrazol­yl)pyraza­boles in which two hydrogen atoms at boron are replaced by pyrazolyl moieties (Niedenzu & Niedenzu, 1984 ▸). Deliberate formation of the parent 4,8-bis­(pyrazol­yl)pyraza­bole, 4,8-trans-{(pz)HB(μ-pz)}2, has been achieved by thermolysis of the free acid of the hydro­tris­(pyrazol­yl)borate anion (Kresínski, 1999 ▸). In lanthanide Tp chemistry, such 4,8-(pyrazol­yl)pyraza­boles normally represent unwanted side-products as they frequently result from ligand fragmentation and are often the first crystalline products to come out of reaction mixtures (Kühling et al., 2015 ▸, 2016 ▸; Lobbia et al., 1992 ▸). Spectroscopic characterization of 2 was in good agreement with the results of the X-ray diffraction study. For instance, the mass spectrum of 2 showed the mol­ecular ion at m/z 627, and the 11B NMR spectrum displayed a single resonance at δ −4.3 ppm.

Structural commentary

Both title compounds 1 and 2 exist as well-separated mol­ecules in the crystal. In the EuII complex 1, one mol­ecule is present in the asymmetric unit (Fig. 2 ▸). The Tp ligand is attached to Eu in a symmetric tridentate mode with an H—B⋯Eu angle of 179.0 (2)°. The three Eu—N bonds cover the range 2.581 (2)–2.633 (2) Å, which resembles that observed in the corresponding homoleptic EuII complex Eu(Tp)2 [2.563 (5)–2.670 (5) Å; Suta et al., 2017 ▸]. The same applies to the B—N bonds, which are in the narrow range 1.547 (4)–1.555 (4) Å [Eu(Tp)2: B—N = 1.531 (8)–1.559 (7) Å]. In 1, the coordination of the iodido ligand relative to the (Tp)− ligand is slightly tilted [I—Eu⋯B = 151.49 (5)°], and an almost linear arrangement of the iodido ligand and one of the Tp N-donor atoms is realized [I—Eu—N2 = 165.92 (5)°]. A strongly distorted octa­hedral coordination is completed by the two neutral (3,5-pzH) ligands, with coordination angles of 138.80 (7)° (N4—Eu—N8) and 137.43 (7)° (N6—Eu—N10). The corresponding Eu—N bond lengths [Eu—N8 = 2.699 (3), Eu—N10 = 2.660 (2) Å] are slightly longer than those to the (Tp)− ligand, which may be due to the absence of negative ligand charge. The NH⋯N distances between the two pyrazole NH moieties and potential hydrogen-acceptor atoms (N2, N4, N6) are in the range 2.512 (2)–2.610 (2) Å, but the groups are not in a proper orientation for efficient hydrogen bonding [N—H⋯N 115.0 (2)–122.0 (2)°]. Consequently, stabilization of the mol­ecular structure by intra­molecular hydrogen bonding is presumably of less importance.
Figure 2

The mol­ecular structure of compound 1 in the crystal, showing orientational disorder of two isopropyl groups. Displacement ellipsoids are drawn at the 40% probability level, H atoms attached to C atoms omitted for clarity.

The pyraza­bol 2 exists as a centrosymmetric dimer in the crystal, which formally results from two HB(3,5-pz)2 monomers (Fig. 3 ▸). The two B atoms are inter­connected by two μ-bridging (3,5-pz) moieties, resulting in a planar, six-membered B2N4 ring. The B—N bonds within this ring are virtually equal at 1.554 (2) Å (B—N1) and 1.557 (2) Å (B—N2′), and therefore similar to that within the (Tp)− ligand in 1. In contrast, the B—N bond to the terminal (3,5-pz) moiety (B—N3) is slightly shortened to 1.532 (2) Å. The B atoms in 2 exhibit a virtually ideal tetra­hedral coordination with bonding angles in the narrow range 108.3 (1)–110.7 (1)°. The mol­ecular structure of 2 is very similar to that of the 3,5-di­methyl­pyrazolyl analog, trans-{(3,5-Me2pz)HB(μ-3,5-Me2pz)}2 [B—N = 1.5419 (2) and 1.5486 (1) Å for μ-(3,5-Me2pz) and 1.5257 (2) Å for terminal 3,5-Me2pz, N—B—N = 108.532 (6)–109.091 (6)°; Alcock & Sawyer, 1974 ▸]. In contrast, the unsubstituted pyraza­bol trans-{(pz)HB(μ-pz)}2 is non-centrosymmetric and features a remarkably puckered B2N4 ring [B—N = 1.546 (3)–1.559 (3) Å for μ-pz and 1.501 (3)–1.533 (3) Å for terminal pz, N—B—N = 105.2 (2)–111.0 (2)°; Kresiński, 1999 ▸].
Figure 3

The mol­ecular structure of compound 2 in the crystal, showing orientational disorder of one isopropyl group. Displacement ellipsoids drawn at the 50% probability level, H atoms attached to C atoms omitted for clarity. [Symmetry code: (′)  − x,  − y, −z.]

Supra­molecular features

In both compounds 1 and 2, no unusually short inter­molecular contacts have been observed. In 1, the bulky Pr groups at the mol­ecule’s surface does not allow for inter­molecular N—H⋯N hydrogen bonding.

Database survey

For selected references on the reactivity of the sandwich complexes Ln(C5Me5)2 (Ln = Sm, Eu, Yb), see: Evans et al. (1983 ▸, 1988 ▸), Evans (2007 ▸). For general information on scorpionate ligands, see: Kitajima et al. (1992 ▸), Pettinari (2008 ▸),Trofimenko (1966 ▸, 1999 ▸). For the chemistry of divalent lanthanide scorpionate complexes, see: Davies et al. (1985 ▸), Domingos et al. (2002 ▸), Hillier et al. (2001 ▸), Kühling et al. (2015 ▸, 2016 ▸), Marques et al. (2002 ▸), Momin et al. (2014 ▸), Suta et al. (2017 ▸). For general information on the chemistry and structures of pyraza­boles, see: Cavero et al. (2008 ▸), Niedenzu & Niedenzu (1984 ▸), Niedenzu & Nöth (1983 ▸), Trofimenko (1966 ▸). For information on practical applications of pyraza­boles, see: Jadhav et al. (2013 ▸, 2015 ▸), Misra et al. (2013 ▸, 2014 ▸), Patil et al. (2017 ▸).

Synthesis and crystallization

All operations were performed under an argon atmosphere using standard Schlenk techniques. THF, hexa­methyl­disiloxane (HMDSO), and n-pentane were distilled from sodium/benzo­phenone under argon prior to use. NMR spectra were recorded on a Bruker DPX400 (1H: 400 MHz) spectrom­eter in THF-D 8 at 295 (2) K. The 11B NMR spectra were obtained by using inverse gated decoupling on a Bruker Avance 400 NMR spectrometer, operating at 128.4 MHz. The external standard was 15 wt-% BF3·OEt2 in CDCl3 (δB = 0 ppm). IR spectra were measured on a Bruker Vertex V70 spectrometer equipped with a diamond ATR unit, electron impact mass spectra on a MAT95 spectrometer with an ioniz­ation energy of 70 eV. Elemental analyses (C, H and N) were performed using a VARIO EL cube apparatus. The starting materials EuI2(THF)2 (Girard et al. 1980 ▸) and KTp (Kitajima et al. 1992 ▸) were prepared according to published procedures. Preparation of (Tp)(3,5-Hpz)2EuIII (1) and trans-{(3,5-pz)HB(μ-3,5-pz)}2 (2): In a 250 mL Schlenk flask, THF (150 mL) was added to a mixture of EuI2(THF)2 (2.36 g, 4.29 mmol) and KTp (3.20 g, 6.33 mmol), and the resulting suspension was stirred for 12 h at r.t. A white precipitate (KI) was removed by filtration and the neon-yellow, fluorescent filtrate was evaporated to dryness. The residue was extracted with n-pentane (3 × 50 mL), the combined extracts filtered again and concentrated in vacuo to a total volume of ca 30 mL. Cooling to 277 K afforded bright-yellow, air-sensitive crystals of 1 (3.64 g, 78%), which were suitable for X-ray diffraction. The mother liquid was taken to dryness, and the slightly sticky residue was redissolved in ca 5 mL of THF. Addition of dry hexa­methyl­disiloxane (ca 50 mL) followed by cooling to 277 K for several days afforded ca 0.5 g of 2 as colorless, cube-like single-crystals. 1: Analysis calculated for C45H78BEuIN10, M = 1049.86 g mol−1: C 51.48, H 7.58, N 13.34%. Found: C 50.88, H 7.77, N 12.59%. M.p. ca 353 K (dec.). IR: ν 3173 w, 3096 w (ν C—H pyrazol­yl), 2961 s, 2929 m, 2869 m (ν CH3), 2550 w (νB—H), 1565 w, 1534 m, 1460 s, 1426 m, 1379 s, 1361 s, 1295 m, 1170 vs, 1104 m, 1046 s, 1012 s, 958 w, 923 w, 878 w, 787 vs, 767 s, 716 m, 659 s, 587 w, 511 w, 462 w, 389 w, 362 w, 306 w, 258 w, 219 w, 109 s, 75 m cm−1. 1H NMR (400.1 MHz, THF-D, 300 K): δ 11.6 (s br, B—H), 5.70 (s br, 5H, C-H pyrazol­yl), 2.88 δ 153.8 (br, q-C pyrazol­yl), 98.7, 99.3 (C—H pyrazol­yl), 27.9, 32.1 (C—H Pr), 23.2 (CH3 Pr). 11B NMR (300 K, THF-D, 128.4 MHz): δ −5.3 (s, br) ppm. MS: m/z (%) 769 (98) [Eu(TpPr2)(pz)]+, 616 (92) [Eu(Tp)]+, 477 (85), 321 (100), 302 (55) [EuBH(pz-CH3)]+, 152 (21) [pz]+, 137 (63). 2: Analysis calculated for C36H62B2N8, M = 628.56 g mol−1: C 68.79, H 9.94, N 17.83%. Found: C 68.50, H 10.10, N 17.53%. M.p. 553 K. IR: ν 3176 w, 3094 w (ν C—H pyrazol­yl), 2966 s, 2928 m, 2869 m, 2825 w (ν CH3), 2467 w (ν B—H), 1576 w, 1541 m, 1497 m, 1461 m, 1369 m, 1301 s, 1233 vs, 1169 vs, 1134 vs, 1090 s, 1063 s, 1041 m, 1015 m, 982 s, 919 w, 879 w, 832 s, 788 s, 751 m, 723 m, 675 m, 566 m, 508 m, 473 w, 365 m, 302 m, 246 m, 137 m, 106 m, 75 m cm−1. 1H NMR (400.1 MHz, THF-D, 300 K): δ 11.0 (s br, 2H, B—H), 5.75 (s br, 4H, C-H pyrazol­yl), 2.87–2.91 (m, 4H, C—H Pr), 1.15–1.27 (m, 48H, CH 3 iPr) ppm. 13C NMR (300 K, THF-D, 100 MHz): δ 160.7 (br, q-C pyrazol­yl), 97.5 (C—H pyrazol­yl), 28.5 (C—H Pr), 23.5 (CH3 Pr). 11B NMR (300 K, THF-D, 128.4 MHz): δ −4.3 (s, br) ppm. MS: m/z (%) 627 (62) [M]+, 476 (100) [C27H46B2N6]+, 461 (75) [C26H43B2N6]+, 325 (66) [C18H31B2N4]+, 152 (74) [C6H2B2N4]+, 137 (89) [pz2].

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 1 ▸. All H atoms were refined as riding atoms with B—H = 1.00 Å and C—H = 0.98–1.00 Å and U iso(H) = 1.5U eq(C) for methyl H atoms and U iso(H) = 1.2U eq(B,C) for all others. In 1, two isopropyl groups are each disordered over two orientations with occupancy ratios of 0.574 (10):0.426 (10) and 0.719 (16):0.281 (16). In 2, one isopropyl group is similarly disordered, occupancy ratio 0.649 (9):0.351 (9).
Table 1

Experimental details

  1 2
Crystal data
Chemical formula[Eu(C27H46BN6)I(C9H16N2)2]C36H62B2N8
M r 1048.84628.55
Crystal system, space groupOrthorhombic, P b c a Monoclinic, C2/c
Temperature (K)153153
a, b, c (Å)19.5319 (4), 26.6614 (4), 19.8681 (3)25.7646 (11), 11.2134 (3), 15.0968 (7)
α, β, γ (°)90, 90, 9090, 118.792 (3), 90
V3)10346.3 (3)3822.4 (3)
Z 84
Radiation typeMo KαMo Kα
μ (mm−1)1.850.07
Crystal size (mm)0.49 × 0.27 × 0.210.33 × 0.29 × 0.13
 
Data collection
DiffractometerStoe IPDS 2TStoe IPDS 2T
Absorption correctionNumerical (X-AREA and X-RED; Stoe & Cie, 2002)
T min, T max 0.535, 0.716
No. of measured, independent and observed [I > 2σ(I)] reflections43898, 10158, 822910509, 3367, 2594
R int 0.0450.046
(sin θ/λ)max−1)0.6170.595
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.031, 0.063, 1.040.044, 0.104, 1.02
No. of reflections101583367
No. of parameters576238
No. of restraints240
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å−3)1.24, −1.270.25, −0.21

Computer programs: X-AREA and X-RED (Stoe & Cie, 2002 ▸), SIR97 (Altomare et al., 1999 ▸), SHELXL2016 (Sheldrick, 2015 ▸), DIAMOND (Brandenburg, 1999 ▸) and publCIF (Westrip, 2010 ▸).

Crystal structure: contains datablock(s) 1, 2. DOI: 10.1107/S2056989017016498/zl2718sup1.cif Structure factors: contains datablock(s) 1. DOI: 10.1107/S2056989017016498/zl27181sup2.hkl Structure factors: contains datablock(s) 2. DOI: 10.1107/S2056989017016498/zl27182sup3.hkl CCDC references: 1585878, 1585877 Additional supporting information: crystallographic information; 3D view; checkCIF report
[Eu(C27H46BN6)I(C9H16N2)2]Dx = 1.347 Mg m3
Mr = 1048.84Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 44511 reflections
a = 19.5319 (4) Åθ = 2.2–26.2°
b = 26.6614 (4) ŵ = 1.85 mm1
c = 19.8681 (3) ÅT = 153 K
V = 10346.3 (3) Å3Block, yellow
Z = 80.49 × 0.27 × 0.21 mm
F(000) = 4312
Stoe IPDS 2T diffractometer10158 independent reflections
Radiation source: fine-focus sealed tube8229 reflections with I > 2σ(I)
Detector resolution: 6.67 pixels mm-1Rint = 0.045
area detector scansθmax = 26.0°, θmin = 2.2°
Absorption correction: numerical (X-AREA and X-RED; Stoe & Cie, 2002)h = −23→24
Tmin = 0.535, Tmax = 0.716k = −32→32
43898 measured reflectionsl = −21→24
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.031H-atom parameters constrained
wR(F2) = 0.063w = 1/[σ2(Fo2) + (0.0226P)2 + 10.682P] where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.002
10158 reflectionsΔρmax = 1.24 e Å3
576 parametersΔρmin = −1.27 e Å3
24 restraintsExtinction correction: SHELXL2016 (Sheldrick, 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: heavy-atom methodExtinction coefficient: 0.00019 (2)
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.
xyzUiso*/UeqOcc. (<1)
C10.23921 (15)0.19065 (10)0.45330 (14)0.0232 (6)
C20.21068 (16)0.19034 (11)0.38902 (14)0.0273 (6)
H40.1832760.2157460.3690570.033*
C30.23046 (15)0.14552 (10)0.36038 (14)0.0238 (6)
C40.23355 (17)0.23068 (11)0.50638 (15)0.0283 (6)
H50.2639080.2210370.5447890.034*
C50.25808 (19)0.28129 (12)0.47934 (18)0.0384 (8)
H80.2554170.3064930.5151430.058*
H60.2289810.2915440.4415890.058*
H70.3055750.2782520.4639530.058*
C60.16048 (18)0.23508 (12)0.53306 (17)0.0381 (8)
H100.1587950.2607250.5683520.057*
H90.1460110.2027460.5517240.057*
H110.1297350.2445810.4962240.057*
C70.21582 (15)0.12724 (11)0.29037 (14)0.0291 (6)
H120.2186470.0897890.2902760.035*
C80.14350 (19)0.14246 (15)0.26872 (18)0.0492 (9)
H140.1337310.1285340.2240960.074*
H130.1402940.1791210.2669700.074*
H150.1102060.1294740.3012420.074*
C90.2686 (2)0.14745 (12)0.24108 (16)0.0392 (8)
H170.2590150.1344090.1959490.059*
H180.3144710.1368030.2551550.059*
H160.2664400.1841720.2403950.059*
C100.48118 (14)0.09139 (11)0.45682 (14)0.0244 (6)
C110.49553 (15)0.07902 (11)0.39050 (14)0.0274 (6)
H190.5393990.0779250.3699110.033*
C120.43383 (15)0.06867 (10)0.36050 (14)0.0238 (6)
C130.52990 (15)0.10295 (12)0.51323 (15)0.0309 (7)
H200.5023090.1140620.5529280.037*
C140.56970 (19)0.05623 (13)0.53359 (17)0.0432 (8)
H210.6003010.0643300.5711370.065*
H220.5968050.0443720.4952500.065*
H230.5376140.0299380.5474690.065*
C150.57849 (19)0.14513 (14)0.4948 (2)0.0483 (9)
H240.6073700.1532130.5336680.073*
H250.5520760.1748280.4817850.073*
H260.6074490.1345940.4570930.073*
C160.42087 (16)0.04955 (11)0.29062 (14)0.0287 (6)
H270.3746540.0614150.2759380.034*
C170.4208 (2)−0.00760 (12)0.29044 (17)0.0436 (9)
H300.412317−0.0197690.2446420.065*
H280.384677−0.0198800.3204680.065*
H290.465295−0.0199210.3060870.065*
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C4—C5—H6109.5C36b—C34b—C30116.2 (5)
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C8—C7—H12108.4H62a—C36a—H63A109.5
C7—C8—H14109.5C34b—C36b—H61B109.5
C7—C8—H13109.5C34b—C36b—H62B109.5
H14—C8—H13109.5H61b—C36b—H62B109.5
C7—C8—H15109.5C34b—C36b—H63B109.5
H14—C8—H15109.5H61b—C36b—H63B109.5
H13—C8—H15109.5H62b—C36b—H63B109.5
C7—C9—H17109.5N10—C37—C38110.5 (3)
C7—C9—H18109.5N10—C37—C40121.5 (3)
H17—C9—H18109.5C38—C37—C40128.0 (3)
C7—C9—H16109.5C39—C38—C37106.4 (3)
H17—C9—H16109.5C39—C38—H64126.8
H18—C9—H16109.5C37—C38—H64126.8
N4—C10—C11110.0 (2)N9—C39—C38105.5 (3)
N4—C10—C13120.9 (3)N9—C39—C43A122.8 (3)
C11—C10—C13129.0 (3)C38—C39—C43A131.7 (3)
C12—C11—C10106.4 (3)N9—C39—C43B122.8 (3)
C12—C11—H19126.8C38—C39—C43B131.7 (3)
C10—C11—H19126.8C37—C40—C41110.0 (3)
N3—C12—C11107.6 (2)C37—C40—C42109.6 (3)
N3—C12—C16124.1 (3)C41—C40—C42111.7 (4)
C11—C12—C16128.2 (3)C37—C40—H65108.5
C10—C13—C15111.6 (3)C41—C40—H65108.5
C10—C13—C14110.7 (3)C42—C40—H65108.5
C15—C13—C14110.5 (3)C40—C41—H67109.5
C10—C13—H20107.9C40—C41—H68109.5
C15—C13—H20107.9H67—C41—H68109.5
C14—C13—H20107.9C40—C41—H66109.5
C13—C14—H21109.5H67—C41—H66109.5
C13—C14—H22109.5H68—C41—H66109.5
H21—C14—H22109.5C40—C42—H69109.5
C13—C14—H23109.5C40—C42—H71109.5
H21—C14—H23109.5H69—C42—H71109.5
H22—C14—H23109.5C40—C42—H70109.5
C13—C15—H24109.5H69—C42—H70109.5
C13—C15—H25109.5H71—C42—H70109.5
H24—C15—H25109.5C44a—C43a—C39114.0 (4)
C13—C15—H26109.5C44a—C43a—C45A116.9 (5)
H24—C15—H26109.5C39—C43a—C45A112.6 (4)
H25—C15—H26109.5C44a—C43a—H72A103.8
C12—C16—C18111.1 (3)C39—C43a—H72A103.8
C12—C16—C17110.0 (2)C45a—C43a—H72A103.8
C18—C16—C17110.6 (3)C45b—C43b—C39114.5 (8)
C12—C16—H27108.3C45b—C43b—C44B122.4 (12)
C18—C16—H27108.3C39—C43b—C44B104.1 (7)
C17—C16—H27108.3C45b—C43b—H72B104.7
C16—C17—H30109.5C39—C43b—H72B104.7
C16—C17—H28109.5C44b—C43b—H72B104.7
H30—C17—H28109.5C43a—C44a—H73A109.5
C16—C17—H29109.5C43a—C44a—H74A109.5
H30—C17—H29109.5H73a—C44a—H74A109.5
H28—C17—H29109.5C43a—C44a—H75A109.5
C16—C18—H32109.5H73a—C44a—H75A109.5
C16—C18—H33109.5H74a—C44a—H75A109.5
H32—C18—H33109.5C43b—C44b—H73B109.5
C16—C18—H31109.5C43b—C44b—H74B109.5
H32—C18—H31109.5H73b—C44b—H74B109.5
H33—C18—H31109.5C43b—C44b—H75B109.5
N6—C19—C20110.2 (3)H73b—C44b—H75B109.5
N6—C19—C22119.7 (3)H74b—C44b—H75B109.5
C20—C19—C22130.1 (3)C43a—C45a—H76A109.5
C21—C20—C19106.1 (3)C43a—C45a—H77A109.5
C21—C20—H34127.0H76a—C45a—H77A109.5
C19—C20—H34127.0C43a—C45a—H78A109.5
N5—C21—C20107.4 (3)H76a—C45a—H78A109.5
N5—C21—C25124.2 (3)H77a—C45a—H78A109.5
C20—C21—C25128.4 (3)C43b—C45b—H76B109.5
C19—C22—C24111.9 (3)C43b—C45b—H77B109.5
C19—C22—C23110.8 (3)H76b—C45b—H77B109.5
C24—C22—C23111.8 (3)C43b—C45b—H78B109.5
C19—C22—H35107.4H76b—C45b—H78B109.5
C24—C22—H35107.4H77b—C45b—H78B109.5
C23—C22—H35107.4N3—B—N5110.3 (2)
C22—C23—H37109.5N3—B—N1110.1 (2)
C22—C23—H38109.5N5—B—N1110.3 (2)
H37—C23—H38109.5N3—B—H1108.7
C22—C23—H36109.5N5—B—H1108.7
H37—C23—H36109.5N1—B—H1108.7
H38—C23—H36109.5C3—N1—N2109.2 (2)
C22—C24—H39109.5C3—N1—B130.6 (2)
C22—C24—H41109.5N2—N1—B120.2 (2)
H39—C24—H41109.5C1—N2—N1106.6 (2)
C22—C24—H40109.5C1—N2—EU128.40 (18)
H39—C24—H40109.5N1—N2—EU124.87 (16)
H41—C24—H40109.5C12—N3—N4109.3 (2)
C21—C25—C27111.5 (3)C12—N3—B129.4 (2)
C21—C25—C26110.5 (3)N4—N3—B121.3 (2)
C27—C25—C26110.5 (3)C10—N4—N3106.6 (2)
C21—C25—H42108.1C10—N4—EU127.79 (18)
C27—C25—H42108.1N3—N4—EU124.67 (17)
C26—C25—H42108.1C21—N5—N6109.7 (2)
C25—C26—H45109.5C21—N5—B130.1 (2)
C25—C26—H44109.5N6—N5—B120.1 (2)
H45—C26—H44109.5C19—N6—N5106.6 (2)
C25—C26—H43109.5C19—N6—EU126.86 (19)
H45—C26—H43109.5N5—N6—EU126.29 (16)
H44—C26—H43109.5C30—N7—N8113.1 (3)
C25—C27—H47109.5C30—N7—H2123.5
C25—C27—H46109.5N8—N7—H2123.5
H47—C27—H46109.5C28—N8—N7104.0 (2)
C25—C27—H48109.5C28—N8—EU145.8 (2)
H47—C27—H48109.5N7—N8—EU109.68 (17)
H46—C27—H48109.5C39—N9—N10113.3 (2)
N8—C28—C29110.7 (3)C39—N9—H3123.4
N8—C28—C31120.3 (3)N10—N9—H3123.4
C29—C28—C31129.1 (3)C37—N10—N9104.3 (2)
C30—C29—C28106.2 (3)C37—N10—EU142.21 (19)
C30—C29—H49126.9N9—N10—EU113.47 (18)
C28—C29—H49126.9N6—EU—N468.39 (7)
N7—C30—C29106.0 (3)N6—EU—N272.16 (7)
N7—C30—C34A121.4 (3)N4—EU—N273.92 (7)
C29—C30—C34A132.6 (3)N6—EU—N10137.43 (7)
N7—C30—C34B121.4 (3)N4—EU—N1076.75 (7)
C29—C30—C34B132.6 (3)N2—EU—N1075.37 (7)
C28—C31—C32110.7 (3)N6—EU—N875.95 (7)
C28—C31—C33111.8 (3)N4—EU—N8138.80 (7)
C32—C31—C33110.7 (3)N2—EU—N876.11 (7)
C28—C31—H50107.8N10—EU—N8121.58 (8)
C32—C31—H50107.8N6—EU—I119.00 (5)
C33—C31—H50107.8N4—EU—I117.23 (5)
C31—C32—H53109.5N2—EU—I165.92 (5)
C31—C32—H51109.5N10—EU—I98.11 (5)
H53—C32—H51109.5N8—EU—I97.58 (5)
N2—C1—C2—C3−0.7 (3)N9—C39—C43b—C44b−75.4 (13)
C4—C1—C2—C3−179.8 (3)C38—C39—C43b—C44b105.1 (13)
C1—C2—C3—N10.4 (3)C2—C3—N1—N20.0 (3)
C1—C2—C3—C7−177.4 (3)C7—C3—N1—N2177.9 (3)
N2—C1—C4—C6−111.6 (3)C2—C3—N1—B−178.4 (3)
C2—C1—C4—C667.4 (4)C7—C3—N1—B−0.5 (5)
N2—C1—C4—C5125.1 (3)N3—B—N1—C3116.0 (3)
C2—C1—C4—C5−55.9 (4)N5—B—N1—C3−121.9 (3)
N1—C3—C7—C9−92.6 (3)N3—B—N1—N2−62.2 (3)
C2—C3—C7—C984.9 (4)N5—B—N1—N259.8 (3)
N1—C3—C7—C8144.6 (3)C2—C1—N2—N10.7 (3)
C2—C3—C7—C8−37.9 (4)C4—C1—N2—N1179.8 (3)
N4—C10—C11—C12−1.7 (3)C2—C1—N2—EU176.38 (19)
C13—C10—C11—C12175.9 (3)C4—C1—N2—EU−4.5 (4)
C10—C11—C12—N31.3 (3)C3—N1—N2—C1−0.4 (3)
C10—C11—C12—C16−174.9 (3)B—N1—N2—C1178.2 (2)
N4—C10—C13—C15−127.3 (3)C3—N1—N2—EU−176.29 (17)
C11—C10—C13—C1555.3 (4)B—N1—N2—EU2.3 (3)
N4—C10—C13—C14109.1 (3)C11—C12—N3—N4−0.6 (3)
C11—C10—C13—C14−68.3 (4)C16—C12—N3—N4175.8 (2)
N3—C12—C16—C18150.9 (3)C11—C12—N3—B−178.8 (3)
C11—C12—C16—C18−33.5 (4)C16—C12—N3—B−2.4 (4)
N3—C12—C16—C17−86.3 (4)N5—B—N3—C12125.1 (3)
C11—C12—C16—C1789.4 (4)N1—B—N3—C12−112.9 (3)
N6—C19—C20—C210.2 (4)N5—B—N3—N4−52.9 (3)
C22—C19—C20—C21−177.3 (3)N1—B—N3—N469.1 (3)
C19—C20—C21—N5−0.3 (4)C11—C10—N4—N31.3 (3)
C19—C20—C21—C25−177.6 (3)C13—C10—N4—N3−176.5 (2)
N6—C19—C22—C24139.4 (3)C11—C10—N4—EU−168.18 (19)
C20—C19—C22—C24−43.4 (5)C13—C10—N4—EU14.0 (4)
N6—C19—C22—C23−95.2 (4)C12—N3—N4—C10−0.5 (3)
C20—C19—C22—C2382.1 (5)B—N3—N4—C10177.9 (2)
N5—C21—C25—C27−75.4 (4)C12—N3—N4—EU169.45 (17)
C20—C21—C25—C27101.5 (4)B—N3—N4—EU−12.2 (3)
N5—C21—C25—C26161.3 (3)C20—C21—N5—N60.2 (3)
C20—C21—C25—C26−21.8 (5)C25—C21—N5—N6177.7 (3)
N8—C28—C29—C30−0.3 (4)C20—C21—N5—B177.7 (3)
C31—C28—C29—C30179.0 (3)C25—C21—N5—B−4.8 (5)
C28—C29—C30—N70.1 (4)N3—B—N5—C21−121.5 (3)
C28—C29—C30—C34a178.3 (4)N1—B—N5—C21116.6 (3)
C28—C29—C30—C34b178.3 (4)N3—B—N5—N655.8 (3)
N8—C28—C31—C3266.9 (4)N1—B—N5—N6−66.1 (3)
C29—C28—C31—C32−112.3 (4)C20—C19—N6—N50.0 (3)
N8—C28—C31—C33−169.1 (3)C22—C19—N6—N5177.7 (3)
C29—C28—C31—C3311.6 (5)C20—C19—N6—EU174.9 (2)
N7—C30—C34a—C36a107.3 (6)C22—C19—N6—EU−7.3 (4)
C29—C30—C34a—C36a−70.6 (7)C21—N5—N6—C19−0.1 (3)
N7—C30—C34a—C35−32.9 (5)B—N5—N6—C19−177.9 (2)
C29—C30—C34a—C35149.1 (4)C21—N5—N6—EU−175.07 (18)
N7—C30—C34b—C36b−178.2 (7)B—N5—N6—EU7.1 (3)
C29—C30—C34b—C36b3.8 (9)C29—C30—N7—N80.1 (4)
N7—C30—C34b—C35−32.9 (5)C34a—C30—N7—N8−178.3 (3)
C29—C30—C34b—C35149.1 (4)C34b—C30—N7—N8−178.3 (3)
N10—C37—C38—C390.8 (4)C29—C28—N8—N70.4 (3)
C40—C37—C38—C39−178.8 (4)C31—C28—N8—N7−179.0 (3)
C37—C38—C39—N9−0.8 (4)C29—C28—N8—EU−170.2 (3)
C37—C38—C39—C43a178.8 (4)C31—C28—N8—EU10.4 (5)
C37—C38—C39—C43b178.8 (4)C30—N7—N8—C28−0.3 (3)
N10—C37—C40—C41117.8 (4)C30—N7—N8—EU174.1 (2)
C38—C37—C40—C41−62.6 (5)C38—C39—N9—N100.6 (4)
N10—C37—C40—C42−119.1 (4)C43a—C39—N9—N10−179.1 (3)
C38—C37—C40—C4260.5 (5)C43b—C39—N9—N10−179.1 (3)
N9—C39—C43a—C44a−111.9 (7)C38—C37—N10—N9−0.5 (4)
C38—C39—C43a—C44a68.5 (8)C40—C37—N10—N9179.2 (3)
N9—C39—C43a—C45a24.2 (7)C38—C37—N10—EU179.1 (2)
C38—C39—C43a—C45a−155.3 (6)C40—C37—N10—EU−1.2 (6)
N9—C39—C43b—C45b60.8 (14)C39—N9—N10—C37−0.1 (4)
C38—C39—C43b—C45b−118.7 (13)C39—N9—N10—EU−179.8 (2)
C36H62B2N8F(000) = 1376
Mr = 628.55Dx = 1.092 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 25.7646 (11) ÅCell parameters from 11890 reflections
b = 11.2134 (3) Åθ = 2.0–26.2°
c = 15.0968 (7) ŵ = 0.07 mm1
β = 118.792 (3)°T = 153 K
V = 3822.4 (3) Å3Plate, colorless
Z = 40.33 × 0.29 × 0.13 mm
Stoe IPDS 2T diffractometer2594 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.046
Detector resolution: 6.67 pixels mm-1θmax = 25.0°, θmin = 2.0°
area detector scansh = −30→29
10509 measured reflectionsk = −12→13
3367 independent reflectionsl = −17→17
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.044H-atom parameters constrained
wR(F2) = 0.104w = 1/[σ2(Fo2) + (0.050P)2 + 1.3932P] where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
3367 reflectionsΔρmax = 0.25 e Å3
238 parametersΔρmin = −0.20 e Å3
0 restraintsExtinction correction: SHELXL2016 (Sheldrick, 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0022 (4)
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.
xyzUiso*/UeqOcc. (<1)
C10.32091 (7)0.43231 (14)0.12232 (11)0.0228 (3)
C20.31092 (7)0.42821 (15)0.20414 (12)0.0275 (4)
H20.3281760.4783830.2619670.033*
C30.27098 (7)0.33708 (14)0.18577 (11)0.0239 (3)
C40.36140 (7)0.51263 (14)0.10426 (12)0.0255 (4)
H30.3508660.5069560.0314000.031*
C50.42566 (7)0.47407 (17)0.16846 (13)0.0361 (4)
H50.4514500.5275730.1558100.054*
H60.4304550.3922530.1507390.054*
H40.4363890.4775730.2401280.054*
C60.35282 (9)0.64149 (16)0.12723 (15)0.0390 (4)
H90.3787210.6938910.1139010.059*
H80.3627810.6483660.1983970.059*
H70.3114530.6649420.0841520.059*
C70.24394 (7)0.29648 (16)0.24900 (12)0.0302 (4)
H100.2239570.2180980.2223170.036*
C80.29206 (10)0.2793 (2)0.35783 (14)0.0543 (6)
H110.2740680.2536110.3989450.081*
H120.3130650.3547940.3842370.081*
H130.3200740.2184560.3604670.081*
C90.19746 (9)0.38648 (18)0.24156 (16)0.0451 (5)
H150.1791270.3581610.2814490.068*
H140.1670060.3952180.1707350.068*
H160.2164350.4637800.2677400.068*
C100.06813 (7)0.23099 (14)0.02850 (12)0.0257 (4)
C110.06359 (7)0.32593 (15)−0.03555 (13)0.0290 (4)
H170.0314640.379970−0.0683150.035*
C120.11522 (7)0.32426 (14)−0.04087 (11)0.0242 (3)
C130.02374 (7)0.19290 (17)0.06011 (13)0.0322 (4)
H180.0396840.1203550.1034670.039*
C140.01516 (10)0.2889 (2)0.12299 (18)0.0527 (6)
H20−0.0114350.2591680.1474520.079*
H19−0.0021670.3599660.0813170.079*
H210.0535470.3093030.1807520.079*
C15−0.03477 (8)0.1591 (2)−0.03071 (16)0.0520 (6)
H24−0.0615590.126983−0.0075830.078*
H23−0.0278730.098683−0.0707610.078*
H22−0.0526620.229990−0.0724240.078*
C16A0.13485 (7)0.40591 (15)−0.09797 (13)0.0292 (4)0.649 (9)
H25A0.1688070.367438−0.1015620.035*0.649 (9)
C17A0.1569 (3)0.5251 (3)−0.0392 (4)0.0435 (11)0.649 (9)
H26A0.1716750.577049−0.0743760.065*0.649 (9)
H27A0.1888760.5088640.0292620.065*0.649 (9)
H28A0.1240790.564576−0.0355020.065*0.649 (9)
C18A0.0865 (2)0.4274 (6)−0.2035 (3)0.0535 (14)0.649 (9)
H29A0.1019680.474541−0.2403130.080*0.649 (9)
H30A0.0540760.470950−0.2015810.080*0.649 (9)
H31A0.0717600.350805−0.2377780.080*0.649 (9)
C16B0.13485 (7)0.40591 (15)−0.09797 (13)0.0292 (4)0.351 (9)
H25B0.1787890.399759−0.0688500.035*0.351 (9)
C17B0.1037 (4)0.3646 (8)−0.2133 (5)0.045 (2)0.351 (9)
H26B0.1152400.418278−0.2519170.067*0.351 (9)
H27B0.0605620.366928−0.2412310.067*0.351 (9)
H28B0.1160130.283030−0.2174590.067*0.351 (9)
C18B0.1187 (6)0.5326 (6)−0.0920 (9)0.053 (3)0.351 (9)
H29B0.1322040.583712−0.1294470.079*0.351 (9)
H30B0.1376250.557807−0.0210630.079*0.351 (9)
H31B0.0755800.539310−0.1214280.079*0.351 (9)
B0.21039 (7)0.18853 (16)0.04185 (12)0.0209 (4)
H10.2209470.1171810.0869850.025*
N10.25728 (5)0.28776 (11)0.09607 (9)0.0205 (3)
N20.28824 (5)0.34639 (11)0.05681 (9)0.0198 (3)
N30.14859 (5)0.23196 (11)0.01778 (9)0.0207 (3)
N40.11934 (6)0.17386 (12)0.06116 (9)0.0235 (3)
U11U22U33U12U13U23
C10.0190 (8)0.0221 (8)0.0248 (8)−0.0002 (6)0.0085 (6)−0.0021 (6)
C20.0270 (9)0.0295 (9)0.0254 (8)−0.0041 (7)0.0121 (7)−0.0077 (7)
C30.0220 (8)0.0275 (8)0.0210 (7)−0.0009 (7)0.0095 (6)−0.0027 (6)
C40.0244 (8)0.0246 (8)0.0256 (8)−0.0043 (7)0.0105 (7)−0.0019 (7)
C50.0250 (9)0.0431 (10)0.0374 (10)−0.0067 (8)0.0128 (8)−0.0010 (8)
C60.0451 (11)0.0273 (9)0.0485 (11)−0.0060 (8)0.0255 (10)−0.0046 (8)
C70.0306 (9)0.0372 (10)0.0262 (8)−0.0092 (8)0.0165 (7)−0.0063 (7)
C80.0474 (12)0.0863 (17)0.0293 (10)−0.0183 (12)0.0185 (9)0.0022 (10)
C90.0496 (12)0.0469 (12)0.0550 (12)−0.0104 (10)0.0382 (10)−0.0136 (10)
C100.0213 (8)0.0295 (9)0.0277 (8)−0.0015 (7)0.0130 (7)−0.0006 (7)
C110.0234 (8)0.0294 (9)0.0350 (9)0.0046 (7)0.0147 (7)0.0040 (7)
C120.0234 (8)0.0229 (8)0.0265 (8)0.0023 (7)0.0122 (7)0.0009 (6)
C130.0262 (9)0.0385 (10)0.0368 (9)−0.0005 (8)0.0190 (8)0.0045 (8)
C140.0529 (13)0.0612 (14)0.0649 (14)−0.0020 (11)0.0450 (12)−0.0062 (11)
C150.0312 (10)0.0748 (15)0.0488 (12)−0.0145 (10)0.0184 (9)0.0055 (11)
C16A0.0271 (9)0.0287 (9)0.0360 (9)0.0053 (7)0.0183 (8)0.0086 (7)
C17A0.054 (3)0.0287 (17)0.056 (2)−0.0048 (18)0.033 (2)0.0051 (16)
C18A0.045 (2)0.067 (3)0.0401 (19)−0.010 (2)0.0142 (17)0.020 (2)
C16B0.0271 (9)0.0287 (9)0.0360 (9)0.0053 (7)0.0183 (8)0.0086 (7)
C17B0.048 (4)0.053 (5)0.036 (3)0.001 (3)0.022 (3)0.012 (3)
C18B0.079 (7)0.030 (3)0.075 (6)0.009 (4)0.058 (6)0.013 (3)
B0.0200 (9)0.0204 (9)0.0215 (8)−0.0001 (7)0.0093 (7)0.0012 (7)
N10.0186 (6)0.0228 (7)0.0205 (6)−0.0007 (5)0.0098 (5)−0.0005 (5)
N20.0167 (6)0.0214 (7)0.0215 (6)−0.0011 (5)0.0095 (5)0.0001 (5)
N30.0199 (7)0.0215 (7)0.0226 (6)−0.0008 (5)0.0117 (5)0.0009 (5)
N40.0224 (7)0.0261 (7)0.0250 (7)−0.0028 (6)0.0138 (6)−0.0002 (5)
C1—N21.3464 (19)C13—C141.520 (3)
C1—C21.379 (2)C13—H181.0000
C1—C41.499 (2)C14—H200.9800
C2—C31.380 (2)C14—H190.9800
C2—H20.9500C14—H210.9800
C3—N11.3431 (19)C15—H240.9800
C3—C71.498 (2)C15—H230.9800
C4—C51.524 (2)C15—H220.9800
C4—C61.527 (2)C16a—C18A1.496 (4)
C4—H31.0000C16a—C17A1.552 (4)
C5—H50.9800C16a—H25A1.0000
C5—H60.9800C17a—H26A0.9800
C5—H40.9800C17a—H27A0.9800
C6—H90.9800C17a—H28A0.9800
C6—H80.9800C18a—H29A0.9800
C6—H70.9800C18a—H30A0.9800
C7—C81.520 (3)C18a—H31A0.9800
C7—C91.528 (3)C16b—C18B1.496 (7)
C7—H101.0000C16b—C17B1.595 (7)
C8—H110.9800C16b—H25B1.0000
C8—H120.9800C17b—H26B0.9800
C8—H130.9800C17b—H27B0.9800
C9—H150.9800C17b—H28B0.9800
C9—H140.9800C18b—H29B0.9800
C9—H160.9800C18b—H30B0.9800
C10—N41.330 (2)C18b—H31B0.9800
C10—C111.405 (2)B—N31.532 (2)
C10—C131.498 (2)B—N11.554 (2)
C11—C121.371 (2)B—N2i1.557 (2)
C11—H170.9500B—H11.0000
C12—N31.364 (2)N1—N21.3693 (16)
C12—C16A1.502 (2)N2—Bi1.557 (2)
C12—C16B1.502 (2)N3—N41.3772 (17)
C13—C151.518 (3)
N2—C1—C2108.29 (13)C13—C14—H19109.5
N2—C1—C4122.67 (13)H20—C14—H19109.5
C2—C1—C4129.02 (14)C13—C14—H21109.5
C1—C2—C3106.71 (14)H20—C14—H21109.5
C1—C2—H2126.6H19—C14—H21109.5
C3—C2—H2126.6C13—C15—H24109.5
N1—C3—C2108.41 (13)C13—C15—H23109.5
N1—C3—C7122.71 (14)H24—C15—H23109.5
C2—C3—C7128.86 (14)C13—C15—H22109.5
C1—C4—C5110.60 (13)H24—C15—H22109.5
C1—C4—C6109.73 (13)H23—C15—H22109.5
C5—C4—C6110.85 (14)C18a—C16a—C12111.80 (19)
C1—C4—H3108.5C18a—C16a—C17A111.0 (3)
C5—C4—H3108.5C12—C16a—C17A109.18 (17)
C6—C4—H3108.5C18a—C16a—H25A108.3
C4—C5—H5109.5C12—C16a—H25A108.3
C4—C5—H6109.5C17a—C16a—H25A108.3
H5—C5—H6109.5C16a—C17a—H26A109.5
C4—C5—H4109.5C16a—C17a—H27A109.5
H5—C5—H4109.5H26a—C17a—H27A109.5
H6—C5—H4109.5C16a—C17a—H28A109.5
C4—C6—H9109.5H26a—C17a—H28A109.5
C4—C6—H8109.5H27a—C17a—H28A109.5
H9—C6—H8109.5C16a—C18a—H29A109.5
C4—C6—H7109.5C16a—C18a—H30A109.5
H9—C6—H7109.5H29a—C18a—H30A109.5
H8—C6—H7109.5C16a—C18a—H31A109.5
C3—C7—C8109.85 (14)H29a—C18a—H31A109.5
C3—C7—C9109.93 (14)H30a—C18a—H31A109.5
C8—C7—C9111.42 (16)C18b—C16b—C12111.3 (3)
C3—C7—H10108.5C18b—C16b—C17B109.5 (5)
C8—C7—H10108.5C12—C16b—C17B108.5 (3)
C9—C7—H10108.5C18b—C16b—H25B109.2
C7—C8—H11109.5C12—C16b—H25B109.2
C7—C8—H12109.5C17b—C16b—H25B109.2
H11—C8—H12109.5C16b—C17b—H26B109.5
C7—C8—H13109.5C16b—C17b—H27B109.5
H11—C8—H13109.5H26b—C17b—H27B109.5
H12—C8—H13109.5C16b—C17b—H28B109.5
C7—C9—H15109.5H26b—C17b—H28B109.5
C7—C9—H14109.5H27b—C17b—H28B109.5
H15—C9—H14109.5C16b—C18b—H29B109.5
C7—C9—H16109.5C16b—C18b—H30B109.5
H15—C9—H16109.5H29b—C18b—H30B109.5
H14—C9—H16109.5C16b—C18b—H31B109.5
N4—C10—C11111.05 (13)H29b—C18b—H31B109.5
N4—C10—C13121.20 (14)H30b—C18b—H31B109.5
C11—C10—C13127.74 (15)N3—B—N1110.66 (12)
C12—C11—C10105.58 (14)N3—B—N2i110.67 (12)
C12—C11—H17127.2N1—B—N2i108.29 (12)
C10—C11—H17127.2N3—B—H1109.1
N3—C12—C11107.36 (13)N1—B—H1109.1
N3—C12—C16A123.61 (13)N2i—B—H1109.1
C11—C12—C16A129.03 (15)C3—N1—N2108.29 (12)
N3—C12—C16B123.61 (13)C3—N1—B125.87 (12)
C11—C12—C16B129.03 (15)N2—N1—B125.66 (11)
C10—C13—C15111.21 (14)C1—N2—N1108.30 (11)
C10—C13—C14111.11 (15)C1—N2—Bi126.05 (12)
C15—C13—C14111.14 (17)N1—N2—Bi125.43 (12)
C10—C13—H18107.7C12—N3—N4110.45 (12)
C15—C13—H18107.7C12—N3—B130.79 (12)
C14—C13—H18107.7N4—N3—B118.75 (12)
C13—C14—H20109.5C10—N4—N3105.56 (12)
N2—C1—C2—C3−0.15 (18)C7—C3—N1—N2178.58 (14)
C4—C1—C2—C3−178.52 (15)C2—C3—N1—B−175.10 (14)
C1—C2—C3—N10.01 (18)C7—C3—N1—B3.3 (2)
C1—C2—C3—C7−178.32 (16)N3—B—N1—C361.64 (19)
N2—C1—C4—C5−103.02 (17)N2i—B—N1—C3−176.89 (13)
C2—C1—C4—C575.1 (2)N3—B—N1—N2−112.79 (14)
N2—C1—C4—C6134.38 (16)N2i—B—N1—N28.7 (2)
C2—C1—C4—C6−47.5 (2)C2—C1—N2—N10.23 (16)
N1—C3—C7—C8132.58 (18)C4—C1—N2—N1178.73 (13)
C2—C3—C7—C8−49.3 (2)C2—C1—N2—Bi−174.58 (14)
N1—C3—C7—C9−104.46 (18)C4—C1—N2—Bi3.9 (2)
C2—C3—C7—C973.6 (2)C3—N1—N2—C1−0.23 (16)
N4—C10—C11—C120.08 (19)B—N1—N2—C1175.02 (13)
C13—C10—C11—C12179.94 (16)C3—N1—N2—Bi174.62 (13)
C10—C11—C12—N30.00 (18)B—N1—N2—Bi−10.1 (2)
C10—C11—C12—C16a−179.54 (16)C11—C12—N3—N4−0.08 (17)
C10—C11—C12—C16b−179.54 (16)C16a—C12—N3—N4179.49 (14)
N4—C10—C13—C15−120.42 (18)C16b—C12—N3—N4179.49 (14)
C11—C10—C13—C1559.7 (2)C11—C12—N3—B−178.88 (14)
N4—C10—C13—C14115.21 (18)C16a—C12—N3—B0.7 (2)
C11—C10—C13—C14−64.6 (2)C16b—C12—N3—B0.7 (2)
N3—C12—C16a—C18a135.3 (3)N1—B—N3—C1260.88 (19)
C11—C12—C16a—C18a−45.3 (4)N2i—B—N3—C12−59.2 (2)
N3—C12—C16a—C17a−101.6 (3)N1—B—N3—N4−117.84 (14)
C11—C12—C16a—C17a77.9 (3)N2i—B—N3—N4122.10 (13)
N3—C12—C16b—C18b−139.2 (6)C11—C10—N4—N3−0.13 (17)
C11—C12—C16b—C18b40.3 (6)C13—C10—N4—N3−179.99 (14)
N3—C12—C16b—C17b100.3 (4)C12—N3—N4—C100.13 (16)
C11—C12—C16b—C17b−80.2 (5)B—N3—N4—C10179.09 (13)
C2—C3—N1—N20.14 (17)
  10 in total

1.  Chemistry of the lanthanides using pyrazolylborate ligands.

Authors:  Noémia Marques; Andrea Sella; Josef Takats
Journal:  Chem Rev       Date:  2002-06       Impact factor: 60.622

2.  The importance of questioning scientific assumptions: some lessons from f element chemistry.

Authors:  William J Evans
Journal:  Inorg Chem       Date:  2007-04-12       Impact factor: 5.165

3.  Facile pyrazolylborate ligand degradation at lanthanide centers: X-ray crystal structures of pyrazolylborinate-bridged bimetallics.

Authors:  Angela Domingos; Mark R J Elsegood; Anna C Hillier; Guanyang Lin; Sung Ying Liu; Irene Lopes; Noémia Marques; Graham H Maunder; Robert McDonald; Andrea Sella; Jonathan W Steed; Josef Takats
Journal:  Inorg Chem       Date:  2002-12-16       Impact factor: 5.165

4.  Stabilization of molecular lanthanide polysulfides by bulky scorpionate ligands.

Authors:  Marcel Kühling; Robert McDonald; Phil Liebing; Liane Hilfert; Michael J Ferguson; Josef Takats; Frank T Edelmann
Journal:  Dalton Trans       Date:  2016-05-06       Impact factor: 4.390

5.  To bend or not to bend: experimental and computational studies of structural preference in Ln(Tp(iPr)2)2 (Ln = Sm, Tm).

Authors:  Aurélien Momin; Lee Carter; Yi Yang; Robert McDonald; Stéphanie Essafi Labouille; François Nief; Iker Del Rosal; Andrea Sella; Laurent Maron; Josef Takats
Journal:  Inorg Chem       Date:  2014-10-27       Impact factor: 5.165

6.  Synthesis and structural comparison of a series of divalent Ln(Tp(R,R)')2 (Ln = Sm, Eu, Yb) and trivalent Sm(Tp(Me2))2X (X = F, Cl, I, BPh4) complexes.

Authors:  A C Hillier; X Zhang; G H Maunder; S Y Liu; T A Eberspacher; M V Metz; R McDonald; A Domingos; N Marques; V W Day; A Sella; J Takats
Journal:  Inorg Chem       Date:  2001-09-24       Impact factor: 5.165

7.  Aryl pyrazaboles: a new class of tunable and highly fluorescent materials.

Authors:  Rajneesh Misra; Thaksen Jadhav; Shaikh M Mobin
Journal:  Dalton Trans       Date:  2013-12-21       Impact factor: 4.390

8.  Design and synthesis of donor-acceptor pyrazabole derivatives for multiphoton absorption.

Authors:  Thaksen Jadhav; Ramesh Maragani; Rajneesh Misra; V Sreeramulu; D Narayana Rao; Shaikh M Mobin
Journal:  Dalton Trans       Date:  2013-04-07       Impact factor: 4.390

9.  Ferrocenyl pyrazaboles: design, synthesis, structure, and properties.

Authors:  Rajneesh Misra; Thaksen Jadhav; Shaikh M Mobin
Journal:  Dalton Trans       Date:  2014-02-07       Impact factor: 4.390

10.  Crystal structure refinement with SHELXL.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr C Struct Chem       Date:  2015-01-01       Impact factor: 1.172

  10 in total

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