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      SiCl2 | 
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      Chlorine | 
       
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      Nuclear
Quadrupole Coupling Constants | 
       
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      in
Silicon Dichloride | 
       
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      Calculation of the Cl nqcc's in
silicon dichloride was amde of the ro [1] and re
[2] molecular structures.  These are compared with the
experimental [1] nqcc's in Tables 1 and 2.  Structure parameters
are given in Table 3. | 
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      In Tables 1 and 2, RMS is the root
mean square difference between calculated and experimental diagonal
nqcc's (percentage of the average of the magnitudes of the experimental
nqcc's).  RSD is the calibration residual standard deviation for
the B1LYP/TZV(3df,2p) model for calculation of the chlorine
nqcc's.  | 
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      Subscripts a,b,c refer to the
principal axes of the inertia tensor; x,y,z to the principal axes
of the nqcc tensor.  The nqcc y-axis is chosen coincident with the
inertia c-axis, these are perpendicular to the molecular plane. 
Ø (degrees) is the angle between its subscripted
parameters.  ETA = (Xxx - Xyy)/Xzz. | 
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            Table 1. Chlorine
nqcc's in SiCl2 (MHz).  Calculation was made on the
effective ro molecular structure of Tanimoto et al. [1]. | 
             
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            Calc. | 
             
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            Expt. [1] | 
             
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            35Cl | 
            Xaa | 
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            - 7.37 | 
            - | 
            8.061(80) | 
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            Xbb | 
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              5.82 | 
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            5.520 | 
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            Xcc | 
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              1.56 | 
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            2.540 | 
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            Xab | 
            ± | 
            23.83 | 
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            RMS | 
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            0.71 (13 %) | 
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            RSD | 
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            0.49 (1.1 %) | 
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            Xxx | 
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            23.95 | 
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            Xyy | 
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              1.56 | 
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            Xzz | 
            - | 
            25.50 | 
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            ETA | 
            - | 
            0.878 | 
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            Øz,a | 
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            37.26 | 
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            Øa,SiCl | 
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            39.37 | 
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            Øz,SiCl | 
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              2.11 | 
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            37Cl | 
            Xaa | 
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            - 5.81 | 
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            Xbb | 
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              4.58 | 
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            Xcc | 
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              1.23 | 
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            Xab | 
            ± | 
            18.78 | 
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      The angle between the two z-axes is
4.22o larger than
the ClSiCl angle.  This is typical of  the XCl2
dichloride moiety. | 
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            Table 2. Chlorine
nqcc's in SiCl2 (MHz).  Calculation was made on the
equilibrium re molecular structure of Fujitake and
Hirota [2]. | 
             
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            Calc. | 
             
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            Expt. [1] | 
             
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            35Cl | 
            Xaa | 
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            - 7.32 | 
            - | 
            8.061(80) | 
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            Xbb | 
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              5.91 | 
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            5.520 | 
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            Xcc | 
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              1.41 | 
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            2.540 | 
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            Xab | 
            ± | 
            23.68 | 
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            RMS | 
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            0.81 (15 %) | 
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            RSD | 
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            0.49 (1.1 %) | 
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            Xxx | 
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            23.88 | 
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            Xyy | 
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              1.41 | 
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            Xzz | 
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            25.29 | 
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            ETA | 
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            0.889 | 
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            Øz,a | 
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            37.20 | 
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            Øa,SiCl | 
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            39.34 | 
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            Øz,SiCl | 
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              2.14 | 
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            37Cl | 
            Xaa | 
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            - 5.77 | 
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            Xbb | 
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              4.66 | 
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            Xcc | 
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              1.11 | 
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            Xab | 
            ± | 
            18.66 | 
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      The angle between the two z-axes is
4.28o larger than
the ClSiCl angle.  This is typical of  the XCl2
dichloride moiety. | 
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            | Table 3.  Molecular
structure parameters, ro and re (Å and
degrees). | 
           
          
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            ro [1] | 
            re [2] | 
           
          
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            SiCl | 
            2.0700 | 
            2.065310(26) | 
           
          
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            ClSiCl | 
            101.25 | 
            101.3240(16) | 
           
        
       
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      [1] M.Tanimoto, H.Takeo,
C.Matsumura, M.Fujitake, and E.Hirota, J.Chem.Phys. 91,2102(1989). | 
       
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      [2] M.Fujitake and E.Hirota,
Spectrochim.Acta A, 59,1345(1994). | 
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      A.Rizzo, C.Puzzarini, S.Coriani, and
J.Gauss, J.Chem.Phys.
124,064302(2006).  CCSD(T) caculation of the nuclear quadrupole
coupling constants. | 
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      B.P.Prascher, R.M.Lucente-Schultz,
and A.K.Wilson, Chem.Phys. 359,1(2009).  CCSD(T) optimization of
the molecular structure. | 
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       SiH3Cl | 
       SiHCl3 | 
       GeH3Cl | 
       CH3SiCl2CH3 | 
       
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      CCl2 | 
      SiCl | 
      (CH3)3SiCl | 
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      Table of Contents | 
       
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      Molecules/Chlorine | 
       
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      SiCl2.html | 
    
    
       
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      Last
Modified 30 March 2006 | 
    
    
       
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