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Bases del tipo Orbitales Naturales

                      Atomic Natural Orbital Basis                             
                      ----------------------------                             
Elements          Contraction                        References                
 H     : (8s,6p,4d,3f)      -> [4s,3p,2d,1f]     J. Almlof and P.R. Taylor,    
 B - Ne: (13s,8p,6d,4f,2g)  -> [5s,4p,3d,2f,1g]  J.C.P. 86, 4070 (1987).       
Al - P : (18s,13p,6d,4f,2g) -> [6s,5p,3d,2f,1g]  (unpublished)                 
Ti     : (21s,16p,10d,6f)   -> [7s,6p,4d,2f]     C.W. Bauschlicher, Jr.        
Fe     : (21s,15p,10d,6f,4g)-> [7s,6p,4d,3f,2g]  S. R. Langhoff and            
Ni     : (20s,15p,10d,6f)   -> [7s,6p,4d,2f]     Kormornicki, Theor. Chim. Acta
                                                                               
                                                 77, 263 (1990).               
                                                 C.W. Bauschlicher, Jr. and    
                                                 P.R. Taylor, Theor. Chim. Acta
                                                                               
                                                 86, 13 (1993).                
**                                                                             
The atomic natural orbital basis sets of Almlof, Taylor and coworkers are      
based on atomic valence SD-CI densities or densities derived from state-       
averaged MR SD-CI calculations.  The aim was to derive generally contracted    
sets with large numbers of Gaussian primitives without significant loss in     
the SCF or correlation energy. Choices of what mixture of s,p,d,f,g            
functions to group together were based on the natural orbital occupation       
numbers.


HYDROGEN     ! (8s,6p,4d,3f) -> [4s,3p,2d,1f]                    
 S   8
  1        402.0099000        -0.2420000000E-03
  2        60.24196000        -0.1776000000E-02
  3        13.73217000        -0.9897000000E-02
  4        3.904505000        -0.3476500000E-01
  5        1.282709000        -0.1213760000    
  6       0.4655440000        -0.2207770000    
  7       0.1811200000        -0.1901840000    
  8       0.7279100000E-01    -0.5065700000E-01
 S   8
  1        402.0099000        -0.3560000000E-03
  2        60.24196000        -0.1274000000E-02
  3        13.73217000        -0.1849300000E-01
  4        3.904505000        -0.1751900000E-01
  5        1.282709000        -0.4574310000    
  6       0.4655440000        -0.3222800000    
  7       0.1811200000         0.5788380000    
  8       0.7279100000E-01     0.1181480000    
 S   8
  1        402.0099000        -0.4190000000E-03
  2        60.24196000        -0.3615000000E-02
  3        13.73217000        -0.1750700000E-01
  4        3.904505000        -0.1636840000    
  5        1.282709000         -1.177592000    
  6       0.4655440000          1.845239000    
  7       0.1811200000        -0.7117840000    
  8       0.7279100000E-01    -0.1712490000    
 S   8
  1        402.0099000         0.3410000000E-03
  2        60.24196000        -0.1953800000E-01
  3        13.73217000         0.5137700000E-01
  4        3.904505000         -1.320052000    
  5        1.282709000          1.740413000    
  6       0.4655440000        -0.6684020000    
  7       0.1811200000        -0.4990350000    
  8       0.7279100000E-01     0.5429700000    
 P   6
  1        9.880000000         0.3085000000E-02
  2        3.950000000         0.2969000000E-02
  3        1.580000000         0.8387600000E-01
  4       0.6300000000         0.3251330000    
  5       0.2500000000         0.1896030000    
  6       0.1000000000         0.1770800000E-01
 P   6
  1        9.880000000        -0.1735100000E-01
  2        3.950000000         0.2125300000E-01
  3        1.580000000        -0.5528160000    
  4       0.6300000000        -0.1528990000    
  5       0.2500000000         0.5248460000    
  6       0.1000000000         0.1411100000E-01
 P   6
  1        9.880000000         0.3736000000E-02
  2        3.950000000        -0.2742180000    
  3        1.580000000        -0.7744190000    
  4       0.6300000000          1.369931000    
  5       0.2500000000        -0.7356830000    
  6       0.1000000000        -0.2270400000E-01
 D   4
  1        4.000000000         0.1265000000E-02
  2        1.600000000        -0.1599150000    
  3       0.6400000000        -0.3822080000    
  4       0.2600000000        -0.1004870000    
 D   4
  1        4.000000000        -0.3379900000E-01
  2        1.600000000        -0.6592290000    
  3       0.6400000000         0.2157450000    
  4       0.2600000000         0.3213840000    
 F   3
  1        2.500000000        -0.4089700000E-01
  2        1.000000000        -0.2615790000    
  3       0.4000000000        -0.1040000000
Basis Set Library Information on: Roos Augmented Double Zeta 

                      Atomic Natural Orbital Basis                             
                      ----------------------------                             
Elements          Contraction                        Reference                 
      H:  (8s,4p)     -> [3s,2p]     P. O. Widmark, P. A. Malmqvist, B. Roos,  
     He:  (9s,4p)     -> [3s,2p]     Theoret. Chim. Acta, 77, 291 (1990).      
Li - Ne:  (14s,9p,4d) -> [4s,3p,2d]                                            
Na - Ar:  (17s,12p,5d)-> [5s,4p,2d]  P. O. Widmark, B. J. Persson and B. Roos, 
                                     Theoret. Chim. Acta, 79, 419 (1991).      
**                                                                             
The ANO basis sets of Widmark, Malmqvist, Persson and Roos are based on        
atomic valence SD-CI's. However, in contrast to the ANO contractions of        
Almlof and Taylor, these contractions were based not just on the atomic        
ground states, but on the positive and negative ions and electric field        
polarized atom as well.                                                        
**                                                                             
Additional low-lying electronic states were included for some atoms.  For      
example, the singlet D state of oxygen was included in the averaging process.  
**                                                                             
The Gaussian primitive set for first row elemets is based on the van           
Duijneveldt (13s,8p) set augmented with a extra shell of diffuse functions. 
The second row sets were derived in an analogous fashion from a (16s,11p) set.



Emilio San Fabian 2008-04-08