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1.
Synthesis, Crystal Structures, and Vibrational Spectra of trans ‐[Pt(N3)4(ECN)2]2–, E = S, Se By oxidative addition to (n‐Bu4N)2[Pt(N3)4] with dirhodane in dichloromethane trans‐(n‐Bu4N)2[Pt(N3)4(SCN)2] and by ligand exchange of trans(n‐Bu4N)2[Pt(N3)4I2] with Pb(SeCN)2 trans‐(n‐Bu4N)2[Pt(N3)4(SeCN)2] are formed. X‐ray structure determinations on single crystals of trans‐(Ph4P)2[Pt(N3)4(SCN)2] (triclinic, space group P 1, a = 10.309(3), b = 11.228(2), c = 11.967(2) Å, α = 87.267(13), β = 75.809(16), γ = 65.312(17)°, Z = 1) and trans‐(Ph4P)2[Pt(N3)4(SeCN)2] (triclinic, space group P 1, a = 9.1620(10), b = 10.8520(10), c = 12.455(2) Å, α = 90.817(10), β = 102.172(10), γ = 92.994(9)°, Z = 1) reveal, that the compounds crystallize isotypically with octahedral centrosymmetric complex anions. The bond lengths are Pt–S = 2.337, Pt–Se = 2.490 and Pt–N = 2.083 (S), 2.053 Å (Se). The approximate linear Azidoligands with Nα–Nβ–Nγ‐angles = 172,1–175,0° are bonded with Pt–Nα–Nβ‐angles = 116,7–120,5°. In the vibrational spectra the platinum chalcogen stretching vibrations of trans‐(n‐Bu4N)2[Pt(N3)4(ECN)2] are observed at 296 (E = S) and in the range of 186–203 cm–1 (Se). The platinum azide stretching modes of the complex salts are in the range of 402–425 cm–1. Based on the molecular parameters of the X‐ray determinations the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants are fd(PtS) = 1.64, fd(PtSe) = 1.36, fd(PtNα) = 2.33 (S), 2.40 (Se) and fd(NαNβ, NβNγ) = 12.43 (S), 12.40 mdyn/Å (Se). 相似文献
2.
Synthesis, Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of trans ‐( n ‐Bu4N)4[Pt(ECN)2(ox)2], E = S, Se By reaction of (n‐Bu4N)2[Pt(ox)2] with (SCN)2 and (SeCN)2 in dichloromethane trans‐(n‐Bu4N)2[Pt(SCN)2(ox)2] ( 1 ) und trans‐(n‐Bu4N)2[Pt(SeCN)2(ox)2] ( 2 ) are formed. The crystal structures of 1 (triclinic, space group P1, a = 10.219(2), b = 11.329(2), c = 12.010(3) Å, α = 114.108(15), β = 104.797(20), γ = 102.232(20)°, Z = 1) and 2 (triclinic, space group P1, a = 10.288(1), b = 11.332(1), c = 12.048(1) Å, α = 114.391(9), β = 103.071(10), γ = 102.466(12)°, Z = 1) reveal, that the compounds crystallize isotypically with centrosymmetric complex anions. The bond lengths are Pt–S = 2.357, Pt–Se = 2.480 and Pt–O = 2.011 ( 1 ) und 2.006 Å ( 2 ). The oxalato ligands are nearly plane with O–C–C–O torsion angles of 1.7–3.6°. The via S or Se coordinated linear groups are inclined between both oxalato ligands with Pt–E–C angles of 100.4 (E = S) and 97.4° (Se). In the vibrational spectra the PtE stretching vibrations are observed at 299–314 ( 1 ) and 189–200 cm–1 ( 2 ). The PtO stretching vibrations are coupled with internal vibrations of the oxalato ligands and appear in the range of 400–800 cm–1. Based on the molecular parameters of the X‐ray determinations the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants are fd(PtS) = 1.75, fd(PtSe) = 1.35 and fd(PtO) = 2.77 mdyn/Å. The NMR shifts are δ(195Pt) = 5435.2 ( 1 ), 5373.7 ( 2 ) and δ(77Se) = 353.2 ppm with the coupling constant 1J(SePt) = 37.4 Hz. 相似文献
3.
Crystal Structures, Spectroscopic Analysis, and Normal Coordinate Analysis of ( n ‐Bu4N)2[M(ECN)4] (M = Pd, Pt; E = S, Se) The reaction of (NH4)2[PdCl4] or K2[PtCl4] with KSCN or KSeCN in aqueous solutions yields the complex anions [Pd(SCN)4]2–, [Pt(SCN)4]2– and [Pt(SeCN)4]2–, which are converted into (n‐Bu4N) salts with (n‐Bu4N)HSO4. (n‐Bu4N)2[Pd(SeCN)4] is formed by treatment of (n‐Bu4N)2[PdCl4] with (n‐Bu4N)SeCN in acetone. X‐ray structure determinations on single crystals of (n‐Bu4N)2[Pd(SCN)4] (monoclinic, space group P21/n, a = 13.088(3), b = 12.481(2), c = 13.574(3) Å, β = 91.494(15)°, Z = 2), (n‐Bu4N)2[Pd(SeCN)4] (monoclinic, space group P21/n, a = 13.171(2), b = 12.644(2), c = 13.560(2) Å, β = 91.430(11)°, Z = 2) and (n‐Bu4N)2[Pt(SeCN)4] (monoclinic, space group P21/n, a = 13.167(2), b = 12.641(1), c = 13.563(2) Å, β = 91.516(18)°, Z = 2) reveal, that the compounds crystallize isotypically and the complex anions are centrosymmetric and approximate planar. In the Raman spectra the metal ligand stretching modes of (n‐Bu4N)2[Pd(SCN)4] ( 1 ) and (n‐Bu4N)2[Pt(SCN)4] ( 3 ) are observed in the range of 260–303 cm–1 and of (n‐Bu4N)2[Pd(SeCN)4] ( 2 ) and (n‐Bu4N)2[Pt(SeCN)4] ( 4 ) in the range of 171–195 cm–1. The IR and Raman spectra are assigned by normal coordinate analysis using the molecular parameters of the X‐ray determination. The valence force constants are fd(PdS) = 1.17, fd(PdSe) = 1.17, fd(PtS) = 1.44 and fd(PtSe) = 1.42 mdyn/Å. The 77Se NMR resonances are 23 for 2 , –3 for 4 and the 195Pt NMR resonances 549 for 3 and 130 ppm for 4 . 相似文献
4.
Synthesis, Crystal Structures, and Vibrational Spectra of [Pt(N3)6]2– and [Pt(N3)Cl5]2–, 195Pt and 15N NMR Spectra of [Pt(N3)nCl6–n]2– and [Pt(15NN2)n(N215N)6–n]2–, n = 0–6 By ligand exchange of [PtCl6]2– with sodium azide mixed complexes of the series [Pt(N3)nCl6–n]2– and with 15N‐labelled sodium azide (Na15NN2) mixtures of the isotopomeres [Pt(15NN2)n(N215N)6–n]2–, n = 0–6 and the pair [Pt(15NN2)Cl5]2–/[Pt(N215N)Cl5]2– are formed. X‐ray structure determinations on single crystals of (Ph4P)2[Pt(N3)6] ( 1 ) (triclinic, space group P1, a = 10.175(1), b = 10.516(1), c = 12.380(2) Å, α = 87.822(9), β = 73.822(9), γ = 67.987(8)°, Z = 1) and (Ph4As)2[Pt(N3)Cl5] · HCON(CH3)2 ( 2 ) (triclinic, space group P1, a = 10.068(2), b = 11.001(2), c = 23.658(5) Å, α = 101.196(14), β = 93.977(15), γ = 101.484(13)°, Z = 2) have been performed. The bond lengths are Pt–N = 2.088 ( 1 ), 2.105 ( 2 ) and Pt–Cl = 2.318 Å ( 2 ). The approximate linear azido ligands with Nα–Nβ–Nγ‐angles = 173.5–174.6° are bonded with Pt–Nα–Nβ‐angles = 116.4–121.0°. In the vibrational spectra the PtCl stretching vibrations of (n‐Bu4N)2[Pt(N3)Cl5] are observed at 318–345, the PtN stretching modes of (n‐Bu4N)2[Pt(N3)6] at 401–428 and of (n‐Bu4N)2[Pt(N3)Cl5] at 408–413 cm–1. The mixtures (n‐Bu4N)2[Pt(15NN2)n(N215N)6–n], n = 0–6 and (n‐Bu4N)2[Pt(15NN2)Cl5]/(n‐Bu4N)2[Pt(N215N)Cl5] exhibit 15N‐isotopic shifts up to 20 cm–1. Based on the molecular parameters of the X‐ray determinations the vibrational spectra are assigned by normal coordinate analysis. The average valence force constants are fd(PtCl) = 1.93, fd(PtNα) = 2.38 and fd(NαNβ, NβNγ) = 12.39 mdyn/Å. In the 195Pt NMR spectrum of [Pt(N3)nCl6–n]2–, n = 0–6 downfield shifts with the increasing number of azido ligands are observed in the range 4766–5067 ppm. The 15N NMR spectrum of (n‐Bu4N)2[Pt(15NN2)n(N215N)6–n], n = 0–6 exhibits by 15N–195Pt coupling a pseudotriplett at –307.5 ppm. Due to the isotopomeres n = 0–5 for terminal 15N six well‐resolved signals with distances of 0.03 ppm are observed in the low field region at –201 to –199 ppm. 相似文献
5.
Crystal Structures, Normal Coordinate Analyses, and 15N NMR and 77Se NMR Chemical Shifts of trans ‐[OsO2(NCO)4]2–, trans ‐[OsO2(NCS)4]2–, and trans ‐[OsO2(SeCN)4]2– The crystal structures of trans‐(Ph3PNPPh3)2[OsO2(NCO)4] ( 1 ) (orthorhombic, space group Pbca, a = 19.278(3), b = 16.674(4), c = 19.982(2) Å, Z = 4), trans(n‐Bu4N)2[OsO2(NCS)4] ( 2 ) (triclinic, space group P1, a = 12.728(3), b = 12.953(3), c = 16.255(6) Å, α = 97.39(4), β = 105.62(2), γ = 95.25(3)°, Z = 2) and trans‐(n‐Bu4N)2[OsO2(SeCN)4] ( 3 ) (tetragonal, space group I4/m, a = 13.406(2), c = 12.871(1) Å, Z = 2) have been determined by single‐crystal X‐ray diffraction analysis, showing the bonding of NCO and NCS via the N atom but the coordination of SeCN via the Se atom to osmium. Based on the molecular parameters of the X‐ray determinations the vibrational spectra have been assigned by normal coordinate analyses. The valence force constants are for 1 fd(OsO) = 6.43, fd(OsN) = 3.32, fd(NC) = 14.50, fd(CO) = 12.80, for 2 fd(OsO) = 6.56, fd(OsN) = 1.75, fd(NC) = 15.00, fd(CS) = 5.50, and for 3 fd(OsO) = 6.75, fd(OsSe) = 0.99, fd(SeC) = 3.23, fd(CN) = 15.95 mdyn/Å. The observed NMR shifts are δ(15N) = –386.6 ( 1 ), δ(15N) = –294.7 ( 2 ) and δ(77Se) = 108.8 ppm ( 3 ). 相似文献
6.
Synthesis, Crystal Structure, and Vibrational Spectra of cis ‐(CH2Py2)[ReBr4Py2]2 · (CH3)2CO By reaction of (n‐Bu4N)2[ReBr6] with pyridine and (n‐Bu4N)BH4 in dichloromethane halogeno‐pyridine‐rhenium(III)complexes are formed and purified by chromatography. X‐ray structure determination on a single crystal has been performed of cis‐(CH2Py2)[ReBr4Py2]2 · (CH3)2CO (monoclinic, space group P21/c, a = 15.0690(9), b = 8.3337(8), c = 35.588(4) Å, β = 96.409(7), Z = 4). Based on the molecular parameters of the X‐ray structure determination and assuming C2 point symmetry for the anion cis‐[ReBr4Py2]– the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants are in the Br–Re–Br axis fd(ReBr) = 1.49, in the asymmetrically coordinated N′–Re–Br · axes fd(ReBr · ) = 1.03 und fd(ReN′) = 2.52 mdyn/Å. 相似文献
7.
Synthesis, Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of (Ph4P)2[OsN(N3)5] and 15N NMR Chemical Shifts of Nitridoosmates(VI, VIII) The treatment of (Ph4P)[OsNCl4] with NaN3 yields (Ph4P)2[OsN(N3)5], which crystal structure has been determined by single crystal X‐ray diffraction analysis (monoclinic, space group P 21/a, a = 20.484(6), b = 11.168(1), c = 20.666(4) Å, β = 97.35(3)°, Z = 4). The IR and Raman vibrations were assigned by a normal coordinate analysis based on the molecular parameters of the X‐ray determination. The valence force constants are fd(Os≡N) = 8.52, fd(Os–Nα) = 1.99, fd(Nα–Nβ) = 12.42, fd(Nβ–Nγ) = 12.73 and for the azido ligand in trans‐position to the nitrido group fd(Os–Nα · ) = 1.84, fd(Nα · –Nβ · ) = 11.91, fd(Nβ · –Nγ · ) = 12.18 mdyn/Å. The 15N NMR spectra of various nitridoosmates reveal the chemical shifts δ(15N) for K[OsO315N] = 387.6, K2[Os15NCl5] = 446.7, (Ph4P)[Os15NCl4] = 352.9, [(n‐C6H13)4N]2[Os15N(N3)5] = 307.3 and for [(n‐Pr)4N]2[Os15N(15NCO)5] = 483,7 (Os≡N), –417,7 (OsNCOeq) und –392,8 ppm (OsNCOax). 相似文献
8.
Synthesis, Crystal Structures, Vibrational Spectra, and Normal Coordinate Analyses of the Tetrahalogeno‐bis‐Pyridine‐Osmium(III) Complexes cis ‐( n ‐Bu4N)[OsCl4Py2] and trans ‐( n ‐Bu4N)[OsX4Py2], X = Cl, Br By reaction of (n‐Bu4N)2[OsX6], X = Cl, Br, with pyridine and (n‐Bu4N)[BH4] tetrahalogeno‐bis‐pyridine‐osmium(III) complexes are formed and purified by chromatography. X‐ray structure determinations on single crystals have been performed of cis‐(n‐Bu4N)[OsCl4Py2] ( 1 ) (triclinic, space group P1, a = 9.4047(9), b = 10.8424(18), c = 17.007(2) Å, α = 71.833(2), β = 81.249(10), γ = 67.209(12)°, Z = 2), trans‐(n‐Bu4N)[OsCl4Py2] ( 2 ) (orthorhombic, space group P212121, a = 8.7709(12), b = 20.551(4), c = 17.174(4) Å, Z = 4) and trans‐(n‐Bu4N)[OsBr4Py2] ( 3 ) (triclinic, space group P1, a = 9.132(3), b = 12.053(3), c = 15.398(2) Å, α = 95.551(18), β = 94.12(2), γ = 106.529(19)°, Z = 2). Based on the molecular parameters of the X‐ray structure determinations and assuming C2 point symmetry for the anion of 1 and D2h point symmetry for the anions of 2 and 3 the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants of 1 are in the Cl–Os–Cl axis fd(OsCl) = 1.58, in the asymmetrically coordinated N′–Os–Cl · axes fd(OsCl · ) = 1.45, fd(OsN′) = 2.48, of 2 fd(OsCl) = 1.62, fd(OsN) = 2.42 and of 3 fd(OsBr) = 1.39 and fd(OsN) = 2.34 mdyn/Å. 相似文献
9.
Synthesis and Properties of trans -Di(fluoro)phthalocyaninatorhenate(III); Crystal Structure of the linear -Bis(triphenylphosphine)iminium Double Salt l (PNP) trans[Re(F)2pc2–] · 0.33l (PNP)F · 2 H2O trans-Bis(triphenylphosphine)phthalocyaninato(2–)rhenium(II) reacts with (nBu4N)F · 3 H2O in acetone on air yielding trans-di(fluoro)phthalocyaninato(2–)rhenate(III), trans[Re(F)2pc2–]–. The complex anion is precipitated as tetra(n-butyl)ammonium (nBu4N), or after addition of (PNP)HSO4 as linear-bis(triphenylphosphine)iminium (l(PNP)) salt. The latter crystallizes as a double salt of formula l(PNP)trans[Re(F)2pc2–] · 0.33l(PNP)F · 2 H2O in the cubic space group I23 (no. 197) with the cell parameter a = 21.836(2) Å; V = 10412(2) Å3; Z = 6. The Re atom is located in the centre of the (Niso)4 plane (Niso: isoindole-N atom) and coordinates axially two fluorine atoms in a mutual trans position. The Re–N and Re–F distance is 2.035(6) and 1.798(7) Å, respectively. According to the short Re–F distance the asymmetric Re–F stretching vibration is observed in the MIR spectrum at 746 cm–1. Obviously due to a large spin-orbit coupling, the complex salt with an electronic low-spin d4 ground state of ReIII (S = 1) is diamagnetic. Hence a sharp signal is observed at –126.1 ppm in the 19F NMR spectrum. The UV-VIS-NIR spectrum shows the typical π-π* transitions at 15000 (B), 29500 (Q) and 36900 cm–1 (N) and trip-multiplet transitions at 9500/10500 cm–1 and 13200/14100 cm–1. 相似文献
10.
Synthesis, Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of cis‐(n‐Bu4N)2[PtX2(ox)2], X = Cl, Br, I By treatment of [PtCl6]2— with C2O42— (ox2—) in water cis‐(n‐Bu4N)2[PtCl2(ox)2] ( 1 ) is formed which has been isolated by ion exchange chromatography on diethylaminoethyl cellulose. Exposure of trans‐(n‐Bu4N)2[PtX2(ox)2], X = Br and I, in dichloromethane yields cis‐(n‐Bu4N)2[PtBr2(ox)2] ( 2 ) and cis‐(n‐Bu4N)2[PtI2(ox)2] ( 3 ). The crystal structure of 3 (monoclinic, space group P21/c, a = 19.132(1), b = 14.377(1), c = 18.099(1) Å, ß = 113.734(8)°, Z = 4) reveals, that the compound crystallizes as a racemic mixture with C2 point symmetrical complex anions. The bond lengths in both I′‐Pt‐O• axes are Pt‐I′ = 2.599 and Pt‐O• = 2.052 and in the O—Pt—O axis Pt—O = 2.016 Å. The oxalato ligands are nearly plane with O—C—C—O torsion angles of 0.2—3.6°. In the vibrational spectra the PtX′ stretching vibrations are observed at 362 and 365 ( 1 ), 231 and 240 ( 2 ) and 172 and 183 cm—1 ( 3 ). The PtO• and PtO stretching vibrations are coupled with internal modes of the oxalato ligands and appear in the range of 400—800 cm—1. Based on the molecular parameters of the X‐ray determination ( 3 ) and estimated data ( 1 , 2 ) the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants are fd(PtCl′) = 2.35, fd(PtBr′) = 2.20, fd(PtI′) = 1.81 and fd(PtO•) = 2.57 ( 1 ), 2.42 ( 2 ) and 2.15 ( 3 ) and fd(PtO) = 2.65 mdyn/Å. Taking into account increments of the trans influence a good agreement between observed and calculated frequencies is achieved. The NMR shifts are δ(195Pt) = 6438.8 ( 1 ), 5988.8 ( 2 ) and 4917.3 ppm ( 3 ). 相似文献
11.
Crystal Structure, Vibrational Spectrum, and Normal Coordinate Analysis of (PNP)2[ReFBr5] · H2O From the complex mixture obtained by oxidative ligand exchange of [ReBr6]2– with BrF3 [ReFBr5]2– has been isolated by ion exchange chromatography on diethylaminoethyl cellulose with 45% yield. The X-ray structure determination of (PNP)2[ReFBr5] · H2O (monoclinic, space group P21/c with a = 21.498(2), b = 13.314(3), c = 23.945(2) Å, β = 105.235(7)°, Z = 4) reveals a completely ordered anion sublattice resulting from the solvent water linked to the F ligand by a hydrogen bond (O–F: 2.758(6) Å). Due to the stronger trans influence of Br compared with F on the F · –Re–Br′ axis the Re–Br′ distance is shortened by 0.6% with regard to symmetrically coordinated axes. Based on the molecular parameters of the X-Ray determination the low temperature (10 K) IR and Raman spectrum of the (Me4N) salt is assigned by a normal coordinate analysis. The strengthening of the Re–Br′ bond due to the trans influence is indicated by an increase of the valence force constant fd(ReBr′) = 1.43 by 8% as compared with fd(ReBr) = 1.32 mdyn/Å of symmetric axes. 相似文献
12.
Synthesis, Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of cis‐ and trans‐(n‐Bu4N)2[PtF2(ox)2] and (n‐Bu4N)2[PtF4(ox)] By treatment of trans‐(n‐Bu4N)2[PtCl2(ox)2] and (n‐Bu4N)2[PtCl4(ox)] with XeF2 in propylene carbonate cis‐ and trans‐(n‐Bu4N)2[PtF2(ox)2] ( 1 , 2 ) and (n‐Bu4N)2[PtF4(ox)] ( 3 ) are formed which have been isolated by ion exchange chromatography on diethylaminoethyl cellulose. The crystal structure of trans(n‐Bu4N)2[PtF2(ox)2] ( 2 ) (tetragonal, space group P42/n, a = 15.5489(9), b = 15.5489(9), c = 17.835(1)Å, Z = 4) und Cs2[PtF4(ox)] ( 3 ) (monoclinic, space group C2/m, a = 14.5261(7), b = 6.2719(4), c = 9.6966(9)Å, β = 90.216(8)°, Z = 4) reveal complex anions with nearly D2h and C2v point symmetry. The average bond lengths in the symmetrical coordinated axes are Pt—F = 1.93 ( 2 , 3 ) and Pt—O = 1.987 ( 2 ) and in the F•—Pt—O′‐axes Pt—F• = 1.957 and Pt—O′ = 1.977Å ( 3 ). The oxalato ligands are nearly planar with a maximum displacement of the ring atoms of 0.05 ( 2 ) und 0.01Å ( 3 ) to the calculated best planes. In the vibrational spectra the symmetric and antisymmetric PtF stretching vibrations are observed at 583 and 586 ( 2 ) and 576 and 568 cm—1 ( 3 ). The PtF• modes appear at 565 and 562 ( 1 ) and 560 cm—1 ( 3 ). The PtO and PtO′ stretching vibrations are coupled with internal modes of the oxalato ligands and appear in the range of 400—800 cm—1. Based on the molecular parameters of the X‐ray determinations ( 2 , 3 ) and estimated data ( 1 ) the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants are fd(PtF) = 3.55 ( 2 ) and 3.38 ( 3 ), fd(PtF•) = 3.23 ( 1 ) and 3.20 ( 3 ), fd(PtO) = 2.65 ( 1 ) and 2.84 ( 2 ) and fd(PtO′) = 2.97 ( 1 ) and 3.00 mdyn/Å ( 3 ). Taking into account increments of the trans influence a good agreement between observed and calculated frequencies is achieved. The NMR shifts are δ(195Pt) = 8485 ( 1 ), 8597 ( 2 ) and 10048 ppm ( 3 ), δ(19F) = —350 ( 2 ) and —352 ( 3 ) and δ(19F•) = —323 ( 1 ) and —326 ppm ( 3 ) with the coupling constants 1J(PtF) = 1784 ( 2 ) and 1864 ( 3 ) and 1J(PtF•) = 1525 ( 1 ) and 1638 Hz ( 3 ). 相似文献
13.
Synthesis and Spectroscopic Characterization of [Rh(SeCN)6]3– and trans ‐[Rh(CN)2(SeCN)4]3–, Crystal Structure of (Me4N)3[Rh(SeCN)6] Treatment of RhCl3 with KSeCN in acetone yields a mixture of selenocyanato‐rhodates(III), from which [Rh(SeCN)6]3– and trans‐[Rh(CN)2(SeCN)4]3– have been isolated by ion exchange chromatography on diethylaminoethyl cellulose. The X‐ray structure determination on a single crystal of (Me4N)3[Rh(SeCN)6] (trigonal, space group R3, a = 14.997(2), c = 24.437(3) Å, Z = 6) reveals, that the compound crystallizes isotypically to (Me4N)3[Ir(SCN)6]. The exclusively via Se coordinated selenocyanato ligands are bonded with the average Rh–Se distance of 2.490 Å and the Rh–Se–C angle of 104.6°. In the low temperature IR and Raman spectra the metal ligand stretching modes ν(RhSe) of (n‐Bu4N)3[Rh(SeCN)6] ( 1 ) and trans‐(n‐Bu4N)3[Rh(CN)2(SeCN)4] ( 2 ) are in the range of 170–250 cm–1. In 2 νas(CRhC) is observed at 479 cm–1. The vibrational spectra are assigned by normal coordinate analysis based on the molecular parameters of the X‐ray determination. The valence force constants are fd(RhSe) = 1.08 ( 1 ), 1.10 ( 2 ) and fd(RhC) = 3.14 mdyn/Å ( 2 ). fd(RhS) = 1.32 mdyn/Å is determined for [Rh(SCN)6]3–, which has not been calculated so far. The 103Rh NMR resonances are 2287 ( 1 ), 1680 ppm ( 2 ) and the 77Se NMR resonances are –32.7 ( 1 ) and –110.7 ppm ( 2 ). The Rh–C bonding of the cyano ligand in 2 is confirmed by a dublett in the 13C NMR spectrum at 136.3 ppm. 相似文献
14.
Synthesis, Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of cis‐(n‐Bu4N)2[Pt(ECN)2(ox)2], E = S, Se By exposure of trans‐(n‐Bu4N)2[Pt(ECN)2(ox)2], E = S and Se, in dichloromethane cis‐(n‐Bu4N)2[Pt(SCN)2(ox)2] ( 1 ) and cis‐(n‐Bu4N)2[Pt(SeCN)2(ox)2] ( 2 ) are formed. The crystal structure of 1 (triclinic, space group P1¯, a = 10.789(1), b = 11.906(1), c = 18.580(1)Å, α = 85.619(10), β = 85.272(10), γ = 75.173(10)°, Z = 2) reveals, that the compound crystallizes as a racemic mixture with C2 point symmetrical complex anions. The bond lengths in both S′‐Pt‐O˙ axes are Pt‐S′ = 2.321 and Pt‐O˙ = 2.048 and in the O‐Pt‐O axis Pt‐O = 2.007Å. The oxalato ligands are nearly plane with O‐C‐C‐O torsion angles of 1.4 — 3.9°. The via S′ bound linear thiocyanate groups are coordinated with Pt‐S′‐C angles of 102.6°. In the vibrational spectra the PtE′ stretching vibrations are observed at 327 — 330 ( 1 ) and 217 — 231 cm—1 ( 2 ). The PtO˙ and PtO stretching vibrations are coupled with internal vibrations of the oxalato ligands and appear in the range of 400 — 800 cm—1. Based on the molecular parameters of the X‐ray determination ( 1 ) and estimated data ( 2 ) the IR and Raman spectra are assigned by normal coordinate analysis. The valence force constants are fd(PtS′) = 2.08, fd(PtSe′) = 1.78, fd(PtO˙) = 2.45 ( 1 ) and 2.27 ( 2 ) and fd(PtO) = 2.65 ( 1 ) and 2.60 mdyn/Å ( 2 ). Taking into account increments of the trans influence a good agreement between observed and calculated frequencies is achieved. The NMR shifts are δ(195Pt) = 4925.9 ( 1 ), 4783.0 ( 2 ) and δ(77Se) = 161.7 ppm with the coupling constant 1J(SePt) = 366.2 Hz. 相似文献
15.
Syntheses, Vibrational Spectra, and Normal Coordinate Analysis of Halogenonitrosylruthenates [Ru(NO)ClnBr5–n]2–, n = 0–5, and the Crystal Structure of (CH2py2)[Ru(NO)ClBr4] By treatment of [Ru(NO)Cl5]2– with anhydrous HBr in dichloromethane a mixture of [Ru(NO)ClnBr5–n]2–, n = 0–5, is formed, from which individual complexes can be separated by ion exchange chromatography on diethylaminoethyl cellulose. The X-Ray structure determination on a single crystal of (CH2py2)[Ru(NO)ClBr4] (monoclinic, space group P21/c, a = 11.480(2), b = 10.175(4), c = 16.025(6) Å, β = 107.40(1)°, Z = 4) reveals, that the chlorine atom is trans positioned to the nitrosyl group. The low temperature IR and Raman spectra have been recorded of six complexes of the series (n-Bu4N)2[Ru(NO)ClnBr5–n], n = 0–5, and are assigned by normal coordinate analysis. A good agreement between observed and calculated frequencies is achieved. The valence force constants are fd(NO) = 13.86–13.93 und fd(RuN) = 5.43–5.49 mdyn/Å. 相似文献
16.
Preparation, Crystal Structures, Vibrational Spectra, and Normal Coordinate Analysis of the Linkage Isomeric Chlororhodanoiridates(III) trans-[IrCl2(SCN)4]3? and trans-[IrCl2(NCS)(SCN)3]3? By treatment of Na2[IrCl6] with NaSCN in 2N HCl the linkage isomers trans-[IrCl2(SCN)4]3? and trans-[IrCl2(NCS)(SCN)3]3? are formed which have been separated by ion exchange chromatography on diethylaminoethyl cellulose. X-ray structure determinations on single crystals of trans-(n-Bu4N)3[IrCl2(SCN)4] ( 1 ) (monoclinic, space group P21/a, a = 18.009(4), b = 15.176(3), c = 23.451(4) Å, β = 93.97(2)°, Z = 4) and trans-(Me4N)3[IrCl2(NCS)(SCN)3] ( 2 ) (monoclinic, space group P21/a, a = 17.146(5), b = 9.583(5), c = 18.516(5) Å, β = 109.227(5)°, Z = 4) reveal the complete ordering of the complex anions. The via S or N coordinated thiocyanate groups are bonded with Ir? S? C angles of 105.7–109.7° and the Ir? N? C angle of 171.4°. The torsion angles Cl? Ir? S? C and N? Ir? S? C are 3.6–53.0°. The IR and Raman spectra of ( 1 ) are assigned by normal coordinate analysis using the molecular parameters of the X-ray determination. The valence force constants are fd(IrS) = 1.52 and fd(IrCl) = 1.72 mdyn/Å. 相似文献
17.
Synthesis, Crystal Structures, Vibrational Spectra, and Normal Coordinate Analyses of the mer ‐Trihalogeno‐tris‐Pyridine‐Osmium(III) Complexes mer‐[OsX3Py3], X = Cl, Br, I By reaction of the hexahalogenoosmates(IV) with pyridine and iso‐amylalcohol mer‐trihalogeno‐tris‐pyridine‐osmium(III) complexes are formed and purified by chromatography. X‐ray structure determinations on single crystals have been performed of mer‐[OsBr3Py3] (monoclinic, space group P21/n, a = 9.098(5), b = 12.864(5), c = 15.632(5) Å, β = 90.216(5)°, Z = 4) and mer‐[OsI3Py3] (monoclinic, space group P21/n, a = 9.0952(17), b = 13.461(4), c = 15.891(10), β = 91.569(5)°, Z = 4). The pyridine rings are twisted propeller‐like against the N3 meridional plane with mean angles of 49° (Cl), 46° (Br), 44° (I). Based on the molecular parameters of the X‐ray structure determinations and assuming C2 point symmetry, the IR and Raman spectra are assigned by normal coordinate analysis. Due to the stronger trans influence of pyridine as compared with the halide ligands for N'–Os–X · axes significantly different valence force constants are observed in comparison with symmetrically coordinated octahedron axes: fd(OsCl) = 1.74, fd(OsCl·) = 1.49, fd(OsBr) = 1.43, fd(OsBr · ) = 1.18, fd(OsI) = 0.99, fd(OsI · ) = 0.96, fd(OsN) between 1.96 and 2.07 and fd(OsN') between 2.13 and 2.32 mdyn/Å. 相似文献
18.
Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of ( n ‐Bu4N)2[{Ru(NO)ClI2}2(μ‐I2)] · 2 I2 By treatment of (n‐Bu4N)2[Ru(NO)I5] with (n‐Bu4N)Cl in dichloromethane (n‐Bu4N)2[{Ru(NO)ClI2}2(μ‐I2)] is formed. The X‐Ray structure determination on a single crystal of (n‐Bu4N)2[{Ru(NO)ClI2}2(μ‐I2)] · 2 I2 (monoclinic, space group I 2/a, a = 20.446(6), b = 11.482(8), c = 27.225(3) Å, β = 107.51(4)°, Z = 4) reveals a dinuclear iodine bridged structure, in which the chlorine atoms are trans positioned to the nitrosyl groups. The low temperature IR and Raman spectra have been recorded of (n‐Bu4N)2[{Ru(NO)ClI2}2(μ‐I2)] · 2 I2 and are assigned by normal coordinate analysis. A good agreement between observed and calculated frequencies is achieved. The valence force constants are fd(NO) = 14.08, fd(RuN) = 5.58, fd(RuCl) = 1.52, fd(RuIt) = 0.90 and fd(RuIb) = 0.76 mdyn/Å. 相似文献
19.
Crystal Structures, Vibrational Spectra, and Normal Coordinate Analyses of the Chloro-Iodo-Rhenates(IV) (CH2Py2)[ReCl5I], cis -(CH2Py2)[ReCl4I2] · 2 DMSO, trans -(CH2Py2)[ReCl4I2] · 2 DMSO, and fac -(EtPh3P)2[ReCl3I3] [ReCl5I]2–, cis-[ReCl4I2]2–, trans-[ReCl4I2]2–, and fac-[ReCl3I3]2– have been synthesized by ligand exchange reactions of [ReI6]2– with HCl and are separated by ion exchange chromatography on diethylaminoethyl cellulose. X-ray structure determinations have been performed on single crystals of (CH2Py2)[ReCl5I] ( 1 ) (triclinic, space group P1 with a = 7.685(2), b = 9.253(2), c = 12.090(4) Å, α = 90.06(2), β = 101.11(2), γ = 95.07(2)°, Z = 2), cis-(CH2Py2)[ReCl4I2] · 2 DMSO ( 2 ) (triclinic, space group P1 with a = 8.662(2), b = 12.109(2), c = 12.9510(12) Å, a = 97.533(11), β = 96.82(2), γ = 89.90(2)°, Z = 2) , trans-(CH2Py2)[ReCl4I2] · 2 DMSO ( 3 ) (triclinic, space group P1 with a = 9.315(7), b = 9.663(3), c = 15.232(3) Å, α = 80.09(2), β = 81.79(4), γ = 83.99(5)°, Z = 2) and fac-(EtPh3P)2[ReCl3I3] ( 4 ) (monoclinic, space group P21/a with a = 17.453(2), b = 13.366(1), c = 19.420(1) Å, β = 112.132(8)°, Z = 4). The crystal structure of ( 1 ) reveals a positional disorder of the anion sublattice along the asymmetric axis. Due to the stronger trans influence of I compared with Cl on asymmetric axes Cl˙–Re–I′ is caused a mean lenghthening of the Re–Cl˙ distances of 0.020 Å (0.8%) and a shortening of the Re–I′ distances of 0.035 Å (1.3%) with regard to symmetrically coordinated axes Cl–Re–Cl and I–Re–I, respectively. Using the molecular parameters of the X-Ray determinations the low temperature (10 K) IR and Raman spectra of the (n-Bu4N) salts of all four chloro-iodo-rhenates(IV) are assigned by normal coordinate analyses. The weakening of the Re–Cl˙ bonds and the strengthening of the Re–I′ bonds is indicated by a decrease or increase of the valence force constants each by 9%. 相似文献
20.
Crystal Structure, Vibrational Spectra, and Normal Coordinate Analysis of (CH2py2)[Ru(NO)FCl4] By treatment of [Ru(NO)Cl5]2– with a BrF3 saturated frigen solution in dichloromethane the complex [Ru(NO)FCl4]2– is formed, which can be separated from hydrolysis products by ion exchange chromatography on diethylaminoethyl cellulose. The X‐Ray structure determination on a single crystal of (CH2py2)[Ru(NO)FCl4] · 1/2 (CH3)2CO (triclinic, space group P1, a = 9.416(2), b = 14.919(6), c = 15.127(3) Å, α = 61.86(3), β = 80.31(2), γ = 72.49(3)°, Z = 4) reveals, that the fluorine atom is trans positioned to the nitrosyl group. The low temperature IR and Raman spectra have been recorded of (n‐Bu4N)2[Ru(NO)FCl4] and are assigned by normal coordinate analysis. A good agreement between observed and calculated frequencies is achieved. The valence force constants are fd(NO) = 13.92, fd(RuN) = 5.16, fd(RuF) = 3.19 and fd(RuCl) = 1.45 mdyn/Å. The 19F NMR spectra exhibits one singlet at –144.6 ppm. 相似文献