details of animation |
Don Rogers, ( drogers@liu.edu ) -- Computational Thermochemistry: G2 and related calculation of ground-state energies and enthalpies of formation of hydrocarbons, aldehydes, ketones and alcohols. Experimental determination of enthalpies of hydrogenation. | |
Andreas Zavitsas, ( zavitsas@liu.edu ) -- Organic Free Radicals and Physical Organic Chemistry | |
Nikita Matsunaga, ( nmatsuna@liu.edu ) -- Molecular Electronics, Electronically Nonadiabatic Effects and Anharmonic and Mode Coupled Molecular Vibration | |
Eric Posmentier (Physics Department), ( eposment@liu.edu ) -- Climate Model and Deterministic, yet Chaotic Classical Approach to Quantized Systems | |
Frank McLafferty, ( fmclaffe@liu.edu ) -- Theoretical chemical kinetics, path integral techniques, Bohm theory and hidden variables applications to kinetics, ab initio calculations of interaction between classical and quantum systems | |
We want you! Progress of science is in your hand! What are you waiting for? You can make a difference! Come join us.
Tony Li,
System Administrator of Science Division Computer Facility, (
zli@liu.edu )
-- G2(MP2) Study of Hydrocarbons and Their Hydrogenation Products
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No picture yet! | Camille McLean, (st777@hotmail.com
)
|
No picture yet! | Katarina Bromgren, (
, currently at University of Oslo )
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No picture yet! | Shawn Hosein Singh, (mscn1125@aol.com
) Edward Murrow High School, Brooklyn, NY
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No picture, yet! | William C. Howard, (
AMWHOWARD.aol.com
) -- M.S. 2001 -- currently employed at General Building Contractors
of New York, Inc., Albany, NY.
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Nathan Burlak, ( nburlak@earthlink.net ) -- M.S. 1999 -- currently working for Merril Lynch. | |
James
Pan, (
jpan@stevens-tech.edu )
-- currently a graduate student at University of Wisconsin, Milwaukee
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Explanation of the animation: This is a pictorial representation of the square of a 2D Gaussian wave packet colliding with a barrier. The box is 128 x 128 Bohr2 in size and the barrier is 3 Bohr in width and 0.46 Hartree in height. Notice that the much of the wave packet is reflected, but a small portion of the wave packet has tunnelled through to the other side of the barrier. One can also see the development of an interference pattern in the reflected wave packet. More details of the calculation are found this way.