| 
 
 
 
 |  |  
 
 
 
        
          | Mattar's Computational Laboratory |  
          |  |  A variety of ab initio computations are carried out in my laboratory. They are performed using clusters   of parallel personal computers running 64 bit LINUX.  
	    They communicate with   one another via the message passing interface (MIPCH) protocol.
A super computer consisting of five rack mounted PCs running LINUX  -     Multireference Configuration Interaction (MRD-CI) Computaions. These   are the most accurate computations that can be performed. However, they are time   consuming and require a large amount of disk space and memory. MRD-CI computations are   used to accurately compute the hyperfine and g tensors for small gas phase   molecules containing transition metals.  Programs used are ORCA and MELD. 
 -     Complete Active Space  Self Consistent   Field and Moller-Plesset Post Hartree-Fock Computations. These are used to optimize the geometry of small   molecules and determine their infrared and Raman intensities and frequencies.   These are relatively extensive computations and use programs such as ORCA,   DALTON and Gaussian03.
 
 -                   Density Functional   LCAO Self Consistent Field Computations. These computations scale as N^3 instead of   N^5 for configuration interaction computations, where N is the number   of primitives in the basis set. They are fast and accurate methods. We mainly   use them for determination of the electronic structure .   Although we have been using density functional methods for over 20 years, they   have finally gained recognition after they were implemented in various programs   such Gaussian, DeMON, DEMOL etc.
-     Hybrid-Density Functional LCAO Self   Consistent Field Computations. They are our preferred methods for fast and accurate   calculations of the geometries, vibrational frequencies electronic and magnetic   properties (hyperfine interactions) of radicals (spin labels), large   paramagnetic molecules and half sandwich organometallic transients.
 |         | 
 
 |  |