Sally Chapman - Publications
Affiliations: | Chemistry | Barnard College, New York, NY, United States |
Website:
http://www.chemheritage.org/discover/collections/oral-histories/details/chapman-sally.aspxYear | Citation | Score | |||
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1976 | Chapman S, Garrett BC, Miller WH. Semiclassical eigenvalues for nonseparable systems: Nonperturbative solution of the Hamilton–Jacobi equation in action‐angle variables The Journal of Chemical Physics. 64: 502-509. DOI: 10.1063/1.432266 | 0.545 | |||
1975 | Chapman S, Garrett BC, Miller WH. Semiclassical transition state theory for nonseparable systems: Application to the collinear H+H2 reaction The Journal of Chemical Physics. 63: 2710-2716. DOI: 10.1063/1.431620 | 0.595 | |||
1975 | Chapman S, Hornstein SM, Miller WH. Accuracy of transition state theory for the threshold of chemical reactions with activation energy. Collinear and three-dimensional atomic hydrogen + molecular hydrogen Journal of the American Chemical Society. 97: 892-894. DOI: 10.1021/Ja00837A035 | 0.496 | |||
1975 | Chapman S, Bunker DL. An exploratory study of reactant vibrational effects in CH 3+H2 and its isotopic variants The Journal of Chemical Physics. 62: 2890-2899. DOI: 10.1002/Chin.197527162 | 0.593 | |||
1975 | CHAPMAN S, HORNSTEIN SM, MILLER WH. ChemInform Abstract: ACCURACY OF TRANSITION STATE THEORY FOR THE THRESHOLD OF CHEMICAL REACTIONS WITH ACTIVATION ENERGY, COLLINEAR AND THREE-DIMENSIONAL H+H2 Chemischer Informationsdienst. 6: no-no. DOI: 10.1002/Chin.197519034 | 0.511 | |||
1974 | Chapman S, Preston RK. Nonadiabatic molecular collisions: Charge exchange and chemical reaction in the Ar+ + H2 system Journal of Chemical Physics. 60: 650-659. DOI: 10.1063/1.1681088 | 0.619 | |||
1974 | Chapman S, Valencich T, Bunker DL. Origin of bond energy effects in hot atom chemistry The Journal of Chemical Physics. 60: 329-330. DOI: 10.1063/1.1680794 | 0.627 | |||
1974 | Chapman S, Suplinskas RJ. Classical trajectory study of bond energy effects Journal of Chemical Physics. 60: 248-257. DOI: 10.1063/1.1680776 | 0.643 | |||
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