4091 - 4098 |
The influence of high-frequency modes on two pulse spectroscopy Kobrak MN, Rice SA |
4099 - 4111 |
Dimensional perturbation theory for vibration-rotation spectra of linear triatomic molecules Suvernev AA, Goodson DZ |
4112 - 4117 |
Raman intensities of C=C stretching vibrational frequencies of polyenes: Nodal mode analysis Lee JY, Lee SJ, Kim KS |
4118 - 4132 |
Temperature, pressure, and perturber dependencies of line-mixing effects in CO2 infrared spectra .1. Sigma<-Pi branches Rodrigues R, Khalil B, LeDoucen R, Bonamy L, Hartmann JM |
4133 - 4153 |
Nonadditive three-body dipoles of inert gas trimers and H-2 center dot center dot center dot H-2 center dot center dot center dot H-2: Long-range effects in far infrared absorption and triple vibrational transitions Li X, Hunt KLC |
4154 - 4164 |
Pump-probe spectroscopy of dissipative energy transfer dynamics in photosynthetic antenna complexes: A density matrix approach Kuhn O, Sundstrom V |
4165 - 4171 |
Wigner spectrogram representations of heterodyne-detected four-wave-mixing and fluorescence up-conversion Mukamel S |
4172 - 4178 |
Manipulation of rovibrational wave packet composition in the Li-2 E((1)Sigma(+)(g)) shelf state using intermediate state selection and shaped femtosecond laser pulses Papanikolas JM, Williams RM, Leone SR |
4179 - 4188 |
Sideband optical-optical double resonance zeeman spectroscopy .2. Studies of NIH, PdD, and PtH McCarthy MC, Kanamori H, Steimle TC, Li MG, Field RW |
4189 - 4193 |
Sideband optical-optical double resonance Zeeman spectroscopy .3. Analysis of composite lines and selective detection McCarthy MC, Field RW |
4194 - 4206 |
Cluster isolated chemical reactions: Reactivity of Ba atoms and small Ba clusters with SF6 and CO2 molecules on large argon clusters Gee C, Gaveau MA, Sublemontier O, Mestdagh JM, Visticot JP |
4207 - 4218 |
Pair potential for water from symmetry-adapted perturbation theory Mas EM, Szalewicz K, Bukowski R, Jeziorski B |
4219 - 4224 |
One-electron versus multielectron effects in the near-threshold C 1s photoionization of acetylene Kempgens B, Kivimaki A, Koppe HM, Neeb M, Bradshaw AM |
4225 - 4232 |
Transitions through fluctuating barrier: Role of asymmetry and memory Fulinski A |
4233 - 4243 |
Quasiclassical trajectory simulations of collisional deactivation of vibrationally excited HgBr(B (2)Sigma) .1. Dependence on vibrational energy Bollati RA, Ferrero JC |
4244 - 4252 |
State-specific reaction and product energy disposal of electronically excited potassium with hydrogen molecule Liu DK, Lin KC |
4253 - 4270 |
The Xe-129 nuclear shielding surfaces for Xe interacting with linear molecules CO2, N-2, and CO deDios AC, Jameson CJ |
4271 - 4285 |
Properties of atoms in molecules: Atoms under pressure Bader RFW, Austen MA |
4286 - 4294 |
Quantum corrections to the classical path equations: Multitrajectory and Hermite corrections Billing GD |
4295 - 4306 |
Correlation states of propene Bawagan ADO, Desjardins SJ, Dailey R, Davidson ER |
4307 - 4317 |
Violation of the weak noncrossing rule between totally symmetric closed-shell states in the valence-isoelectronic series O-3, S-3, SO2, and S2O Ivanic J, Atchity GJ, Ruedenberg K |
4318 - 4328 |
The C-H activation reaction of methane for all transition metal atoms from the three transition rows Wittborn AMC, Costas M, Blomberg MRA, Siegbahn PEM |
4329 - 4336 |
Lithium bonding interaction in H2CY center dot center dot center dot LiF (Y=O,S) complexes: A theoretical probe Ammal SSC, Venuvanalingam P, Pal S |
4337 - 4344 |
Ionic solids at elevated temperatures and high pressures: MgF2 Barrera GD, Taylor MB, Allan NL, Barron THK, Kantorovich LN, Mackrodt WC |
4345 - 4349 |
Crystal structures of symmetric Lennard-Jones mixtures Vlot MJ, Huitema HEA, deVooys A, vanderEerden JP |
4350 - 4357 |
Effect of pressure on hydrogen bonding in glycerol: A molecular dynamics investigation Root LJ, Berne BJ |
4358 - 4363 |
On the gas-gas equilibria of second kind of nonpolar fluid binary mixtures from a hard-sphere EXP-6 molecular model Zarragoicoechea GJ, Scalise OH |
4364 - 4372 |
Competitive adsorption of xenon and krypton in zeolite NaA: Xe-129 nuclear magnetic resonance studies and grand canonical Monte Carlo simulations Jameson CJ, Jameson AK, Lim HM |
4373 - 4383 |
Distribution and Xe-129 NMR chemical shifts of Xe-n clusters in the alpha cages of zeolite AgA Jameson CJ, Lim HM |
4384 - 4389 |
Normal, single-file, and dual-mode diffusion of binary adsorbate mixtures in AlPO4-5 Sholl DS, Fichthorn KA |
4390 - 4395 |
Adsorption of fluid vesicles Baumgartner A, Bhattacharjee SM |
4396 - 4407 |
Extended ensemble molecular dynamics method for constant strain rate uniaxial deformation of polymer systems Yang L, Srolovitz DJ, Yee AF |
4408 - 4415 |
Compaction and folding in model proteins Chiu TL, Goldstein RA |
4416 - 4422 |
Layer-by-layer homoepitaxial growth process of MgO(001) as investigated by molecular dynamics, density functional theory, and computer graphics Kubo M, Oumi Y, Miura R, Fahmi A, Stirling A, Miyamoto A |
4423 - 4435 |
Dissipative particle dynamics: Bridging the gap between atomistic and mesoscopic simulation Groot RD, Warren PB |
4436 - 4438 |
The excitation energy dependence of the Raman-Stokes shift: The resonance Raman spectra of phenol blue in methanol Yamaguchi T, Kimura Y, Hirota N |
4439 - 4442 |
The identification of In2O in the gas phase by high resolution electronic spectroscopy Lakin NM, vandenHoek G, Beattie IR, Brown JM |
4443 - 4444 |
Experimental determination of a longitudinal phonon dispersion curve in a quasi-two-dimensional system - Comment Bruch LW |
4445 - 4445 |
Experimental determination of a longitudinal phonon dispersion curve in a quasi-two-dimensional system - Response Graham AP, Bertino MF, Hofmann F, Toennies JP, Woll C |