N.Gorinchoy et al./Chem.J.Mold. 2008, 3 (1), 105-111It is seen from the Table 2, that the values <strong>of</strong> K = K 0-2V 2/ (the curvature <strong>of</strong> the adiabatic potential) in allthese geometries are negative. This confirms that all symmetrical forms (D h, C 2hand C 2v) <strong>of</strong> the hydrogen peroxidemolecule H 2O 2are energetically unstable due to the PJT effect. Both transition paths from the D hto C 2(D hC 2hC 2and D hC 2vC 2) have the same energetic effect: ~ 6.47 eV.Note, that the energy gaps between the mixing ground and excited electronic states are rather large in all thecases. However, the vibronic coupling is much larger producing at first one <strong>of</strong> the planar bent configurations and thenthe stable “skewed” anticline shape <strong>of</strong> the hydrogen peroxide. Note also that more sophisticated methods <strong>of</strong> calculationscan give more precise values <strong>of</strong> the total energies, but they do not change the qualitative details <strong>of</strong> the rearrangement <strong>of</strong>molecular orbitals and the formation <strong>of</strong> new covalent bonds in the system by distortion.ConclusionOn the base <strong>of</strong> the ab initio calculations <strong>of</strong> the electronic structure and the potential energy surfaces it was shownthat the H 2O 2molecule is unstable in both the linear nuclear configuration <strong>of</strong> the D hsymmetry and planar bent cis-(C 2v) or trans- (C 2h) shapes. By fitting <strong>of</strong> the equation (1) obtained from the vibronic theory to the ab initio calculatedhydrogen peroxide APES it is shown that the origin <strong>of</strong> the instability <strong>of</strong> these configurations is the pseudo Jahn-Tellereffect. The equilibrium “skewed” anticline shape <strong>of</strong> the C 2symmetry can be realized in two ways: D h C 2vC 2orD h C 2h C 2with decreasing adiabatic potential energy at every step.References[1] Koput J., J. Mol. Spectrosc., 1986, 115, 438-441.[2] I. B. Bersuker, The Jahn-Teller Effect, Cambridge University Press, Cambridge, England, 2006.[3] I. B. Bersuker, N.N.Gorinchoi, V.Z.Polinger, Theor. Chim. Acta, 1984, 66, 161.[4] V.Z.Polinger, N.N.Gorinchoi and I.B.Bersuker, Chem. Phys., 1992, 159, 75-87.[5] N.N.Gorinchoi, F.Cimpoesu, I.B.Bersuker, J. Mol. Struct. (Theochem), 2001, 530, 281–290.[6] I.Ogurtsov, N.Gorinchoy, I.Balan, J. Mol. Struct., 2007, 838, 107–111.[7] I. B. Bersuker, N. B. Balabanov, D. M. Pekker, J. E. Boggs, J. Chem. Phys., 2002, 117, 10478-86.[8] J.E.Carpenter and F.Weinhold, J. Phys. Chem., 1988, 92, 4295-4306.[9] R.Block and L.Jansen, J. Chem. Phys., 1985, 82, 3322-3328.[10] T.H.Dunning, Jr., N.W.Winter, J. Chem. Phys., 1975, 63, 1847-1855.[11] Alex A. Granovsky, www http://classic.chem.msu.su/gran/gamess/index.html.[12] M.W.Schmidt, K.K.Baldridge, J.A.Boatz, S.T.Elbert, M.S.Gordon, J.H.Jensen, S.Koseki, N.Matsunaga,K.A.Nguyen, S.Su, T.L.Windus, M.Dupuis, J.A.Montgomery, J.Comput.Chem., 1993, 14, 1347-1363.111
Chemistry Journal I. <strong>of</strong> Ogurtsov, Moldova. A. General, Tihonovschi Industrial / Chem.J.Mold. and Ecological 2008, Chemistry. 3 (1), 112-117 2008, 3 (1), 112-117AB INITIO ANALYSIS OF EXCHANGE INTERACTIONS IN[V 2O(bipy) 4Cl 2] 2+ COMPLEXIvan Ogurtsov*, Andrei TihonovschiInstitute <strong>of</strong> Chemistry, Academy <strong>of</strong> Sciences <strong>of</strong> Moldova, Republic <strong>of</strong> Moldova, Chisinau, Academiei str., 3.* io_quant@yahoo.com, +373 22 739675Abstract: In this work an ab initio analysis <strong>of</strong> the binuclear vanadium complex [V 2O(bipy) 4Cl 2] 2+ electronic structureis performed. The ground state was calculated to be a quintet, which means a ferromagnetic interaction betweencenters. The orbitals participating in exchange interaction according to ROHF+CI calculations are two molecularorbitals consisting <strong>of</strong> vanadium d-orbitals and two molecular orbitals with main contributions from p-orbitals <strong>of</strong>bipyridine ligands perpendicular to V-V axis, vanadium d- and p-orbitals and -oxygen p-orbital. Calculated energyvalues <strong>of</strong> the multielectronic states are placed in accordance with Lande rule. The value <strong>of</strong> magnetic moment at 293Kcalculated for the complex in vacuum taking into consideration the Boltzmann distribution and the energies <strong>of</strong> theexcited states is 3.95BM which is in accordance with experimental value <strong>of</strong> 3.99BM (for complex in acetone).Keywords: binuclear vanadium complex, binuclear -oxo-bridged complex, exchange interactions, magneticproperties, theoretical ab initio study.IntroductionPolynuclear compounds <strong>of</strong> vanadium as well as <strong>of</strong> other transitional metals are <strong>of</strong> great interest not only fromthe theoretical point <strong>of</strong> view. They can be used as models <strong>of</strong> metalloproteins <strong>of</strong> natural enzymatic systems (especiallyiron complexes) [1]. Moreover they can serve as model systems in studies and development <strong>of</strong> new molecular magneticmaterials [2]. Natural enzymatic systems containing paramagnetic ions have been characterized by their magneticproperties [3] too.Numerous magneto-structural correlations have been established for the polynuclear complexes (see, forinstance [4-8] and references therein). In order to describe these correlations the Heisenberg-Dirac-Van Vleck model<strong>of</strong> the exchange interactions between metal centers is usually used. Detailed studies <strong>of</strong> the electronic structure andrelated properties are not performed. Meanwhile the knowledge <strong>of</strong> the interactions origin is needed to work out thewell-founded theoretical models <strong>of</strong> the polynuclear magnetic materials and to predict new systems with the wantedproperties.The relatively simple binuclear oxygen bridged compounds can be useful for the elaboration <strong>of</strong> the magneticinteractions models based on their electronic structure. There are known some theoretical attempts to give theinterpretation <strong>of</strong> the exchange parameters dependence from the Metal-Oxygen-Metal angle values in these compounds[9]. However the suggested in [9] interpretation is based on the crystal-field theory or on the Angular Overlap Modelwhich both are only approximate models <strong>of</strong> the compounds electronic structure and do not give the base for the adequateexchange interaction theory.N 4Cl*N 4N Cl *3V OV **N 3N 1 *N 2N 1*N 2C 1 C *2 C* 1C 2Fig. 1. The system [V 2O(bipy) 4Cl 2] 2+ and atom numbering112
- Page 7:
Chemistry Journal of Moldova. Gener
- Page 10:
Chemistry Journal of Moldova. Gener
- Page 14 and 15:
Gh. Duca et al./Chem.J. Mold.. 2008
- Page 16 and 17:
Gh. Duca et al./Chem.J. Mold.. 2008
- Page 20 and 21:
Gh. Duca et al./Chem.J. Mold.. 2008
- Page 22 and 23:
Gh. Duca et al./Chem.J. Mold.. 2008
- Page 24 and 25:
Gh. Duca et al./Chem.J. Mold.. 2008
- Page 26 and 27:
Gh. Duca et al./Chem.J. Mold.. 2008
- Page 28 and 29:
Gh. Duca et al./Chem.J. Mold.. 2008
- Page 30 and 31:
Gh. Duca et al./Chem.J. Mold.. 2008
- Page 32 and 33:
Chemistry Journal of Moldova. Ion D
- Page 34 and 35:
Ion Dranca/Chem.J. Mold. 2008, 3 (1
- Page 36 and 37:
Ion Dranca/Chem.J. Mold. 2008, 3 (1
- Page 38 and 39:
Ion Dranca/Chem.J. Mold. 2008, 3 (1
- Page 40 and 41:
Ion Dranca/Chem.J. Mold. 2008, 3 (1
- Page 42 and 43:
Ion Dranca/Chem.J. Mold. 2008, 3 (1
- Page 44 and 45:
Ion Dranca/Chem.J. Mold. 2008, 3 (1
- Page 46 and 47:
M. Revenco et al./Chem.J. Mold. 200
- Page 48 and 49:
M. Revenco et al./Chem.J. Mold. 200
- Page 50 and 51:
Gh. Zgherea/Chem.J. Mold. 2008, 3 (
- Page 52 and 53:
Gh. Zgherea/Chem.J. Mold. 2008, 3 (
- Page 54 and 55:
Gh. Zgherea/Chem.J. Mold. 2008, 3 (
- Page 56 and 57:
Gh. Zgherea/Chem.J. Mold. 2008, 3 (
- Page 58 and 59:
G. Vasile et al./Chem.J. Mold. 2008
- Page 60 and 61:
G. Vasile et al./Chem.J. Mold. 2008
- Page 62 and 63: G. Vasile et al./Chem.J. Mold. 2008
- Page 64 and 65: V. Mukhin et al./Chem.J.Mold. 2008,
- Page 66 and 67: V. Mukhin et al./Chem.J.Mold. 2008,
- Page 68 and 69: Chemistry Journal of Moldova. N. Ku
- Page 70 and 71: N. Kulikov et al./Chem.J.Mold. 2008
- Page 72 and 73: V. Gladchi et al./Chem.J.Mold. 2008
- Page 74 and 75: V. Gladchi et al./Chem.J.Mold. 2008
- Page 76 and 77: V. Gladchi et al./Chem.J.Mold. 2008
- Page 78 and 79: Chemistry Journal of Moldova. R. St
- Page 80 and 81: R. Sturza et al./Chem.J.Mold. 2008,
- Page 82 and 83: R. Sturza et al./Chem.J.Mold. 2008,
- Page 84 and 85: R. Sturza et al./Chem.J.Mold. 2008,
- Page 86 and 87: Chemistry Journal of Moldova. V. Bo
- Page 88 and 89: V. Boldescu et al./Chem.J.Mold. 200
- Page 90 and 91: Chemistry Journal of Moldova. I. Lu
- Page 92 and 93: I. Lunga et al./Chem.J.Mold. 2008,
- Page 94 and 95: I. Lunga et al./Chem.J.Mold. 2008,
- Page 96 and 97: N.Gorinchoy et al./Chem.J.Mold. 200
- Page 98 and 99: N.Gorinchoy et al./Chem.J.Mold. 200
- Page 100 and 101: N.Gorinchoy et al./Chem.J.Mold. 200
- Page 102 and 103: N.Gorinchoy et al./Chem.J.Mold. 200
- Page 104 and 105: N.Gorinchoy et al./Chem.J.Mold. 200
- Page 106 and 107: Chemistry Journal of Moldova. N.Gor
- Page 108 and 109: N.Gorinchoy et al./Chem.J.Mold. 200
- Page 110 and 111: N.Gorinchoy et al./Chem.J.Mold. 200
- Page 114 and 115: I. Ogurtsov, A. Tihonovschi / Chem.
- Page 116 and 117: I. Ogurtsov, A. Tihonovschi / Chem.
- Page 118 and 119: I. Ogurtsov, A. Tihonovschi / Chem.
- Page 120 and 121: M. Gonta et al./Chem.J.Mold. 2008,
- Page 122 and 123: M. Gonta et al./Chem.J.Mold. 2008,
- Page 124 and 125: M. Gonta et al./Chem.J.Mold. 2008,
- Page 126 and 127: M. Gonta et al./Chem.J.Mold. 2008,
- Page 128 and 129: Chemistry Journal of Moldova. N. Se
- Page 130 and 131: Chemistry Journal of Moldova. D. Ba
- Page 132 and 133: D. Batîr/Chem.J.Mold. 2008, 3 (1),
- Page 134 and 135: CHEMISTRY JOURNAL OF MOLDOVA.Genera
- Page 136 and 137: CHEMISTRY JOURNAL OF MOLDOVA.Genera
- Page 138: CHEMISTRY JOURNAL OF MOLDOVA.Genera