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Horowitz

S.Horowitz and T.Pavlidis, Picture Segmentation by a tree Traversal Algorithm, Journal of the Association for Computing Machinery, vol 23, N°2, April 1976, pp, 368- 388. [Pg.531]

Figure B3.4.1. The potential surfaee for the eollinear D + H2 DH + H reaetion (this potential is the same as for H + H2 — H2 + H, but to make the produets and reaetants identifieation elearer the isotopieally substituted reaetion is used). The D + H2 reaetant arrangement and the DH + H produet arrangement are denoted. The eoordinates are r, the H2 distanee, and R, the distanee between the D and the H2 eentre of mass. Distanees are measured in angstroms the potential eontours shown are 4.7 eV-4.55 eV,.. ., -3.8 eV. (The potential energy is zero when the partieles are far from eaeh other. Only the first few eontours are shown.) For referenee, the zero-point energy for H2 is -4.47 eV, i.e. 0.27 eV above the H2 potential minimum (-4.74 eV) the room-temperature thennal kinetie energy is approximately 0.03 eV. The graph uses the aeeiirate Liu-Seigbalm-Triihlar-Horowitz (LSTH) potential surfaee [195]. Figure B3.4.1. The potential surfaee for the eollinear D + H2 DH + H reaetion (this potential is the same as for H + H2 — H2 + H, but to make the produets and reaetants identifieation elearer the isotopieally substituted reaetion is used). The D + H2 reaetant arrangement and the DH + H produet arrangement are denoted. The eoordinates are r, the H2 distanee, and R, the distanee between the D and the H2 eentre of mass. Distanees are measured in angstroms the potential eontours shown are 4.7 eV-4.55 eV,.. ., -3.8 eV. (The potential energy is zero when the partieles are far from eaeh other. Only the first few eontours are shown.) For referenee, the zero-point energy for H2 is -4.47 eV, i.e. 0.27 eV above the H2 potential minimum (-4.74 eV) the room-temperature thennal kinetie energy is approximately 0.03 eV. The graph uses the aeeiirate Liu-Seigbalm-Triihlar-Horowitz (LSTH) potential surfaee [195].
Neuhauser D, Baer M, Judson R S and Kouri D J 1989 Time-dependent three-dimensional body frame quantal wavepacket treatment of the atomic hydrogen + molecular hydrogen exchange reaction on the Liu-Siegbahn-Truhlar-Horowitz (LSTH) surfaced. Chem. Phys. 90 5882... [Pg.2325]

Truhlar D G and Horowitz C J 1978 Functional representation of Liu and Siegbahn s accurate ab initio potential energy calculations for H + H2 J. Chem. Phys. 68 2466... [Pg.2331]

L. Horowitz, Patent Office Rules and Practice, Matthew Bender and Co., 1992. [Pg.41]

P. Horowitz and W. Hill, TheArtofE/ectronics, 2nd ed., Cambridge University Press, Cambridge, U.K., 1989. [Pg.355]

LCAO with best exponent of 1.238 Finkelstein and Horowitz (1928) 2.354 106.8... [Pg.81]

Blackburn, J. L. (1952) Ground Relay Polarization. AIEE Trails., Part III, PAS, Vol. 71, December, pp. 1088-1093. Horowitz, S. H., and Phadke, A. G. (1996). Power System Relaying. New York John Wiley Sons, Inc. [Pg.422]

IEEE Power Engineering Society. (1980). Protective Relaying for Power Systems, ed. Stanley H. Horowitz. New York IEEE Press. [Pg.422]

R. Danieli, W. Gebauer, O. Greco, E. Lunedei, R. Mahrt, R. N. Marks, R. Michel, P. Moretti, M. Murgia, P. Ostoja, G. Ruani, P. Samori, T. Virgili, R. Zamboni, D. Beljonne, J. Comil, P. Viville, R. Lazzaroni, J.-L. Bredas, H. Biissler, F. Gamier, G. Horowitz, and A. Bree have participated to the work which is reviewed here. [Pg.106]


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