177 - 180 |
Diffusion of Xe on Ni(111) Nabighian E, Zhu XD |
181 - 185 |
Observation of size oscillations in poly(ethylene) glycol/electrolyte composite microparticles Ford JV, Sumpter BG, Noid DW, Barnes MD |
186 - 190 |
Resonant Raman study of the structure and electronic properties of single-wall carbon nanotubes Alvarez L, Righi A, Guillard T, Rols S, Anglaret E, Laplaze D, Sauvajol JL |
191 - 198 |
The size distribution, imaging and obstructing properties of C-60 and higher fullerenes formed within arc-grown single walled carbon nanotubes Sloan J, Dunin-Borkowski RE, Hutchison JL, Coleman KS, Williams VC, Claridge JB, York APE, Xu CG, Bailey SR, Brown G, Friedrichs S, Green MLH |
199 - 204 |
The superhard crystalline three-dimensional polymerized C-60 phase Chernozatonskii LA, Serebryanaya NR, Mavrin BN |
205 - 210 |
Macroscopic synthesis and characterization of giant fullerenes Selvan R, Unnikrishnan R, Ganapathy S, Pradeep T |
211 - 216 |
Mass-production of boron nitride double-wall nanotubes and nanococoons Cumings J, Zettl A |
217 - 221 |
Fine structure of the low-frequency Raman phonon bands of single-wall carbon nanotubes Iliev MN, Litvinchuk AP, Arepalli S, Nikolaev P, Scott CD |
222 - 228 |
Novel double resonance pulse sequence for low sensitivity nuclei selection Capuani S, Mancini L, Maraviglia B, Sette M, Paci M |
229 - 237 |
MATI and PIRI studies of the (X)over-tilde and (A)over-tilde state of trans-1,3-butadiene cation Hofstein JD, Johnson PM |
238 - 242 |
Inhomogeneity of molecular distribution in supercritical fluids Nishikawa K, Morita T |
243 - 247 |
SiNCO+ and SiNCS+ and their neutral counterparts Srinivas R, Vivekananda S, Schroder D, Schwarz H |
248 - 256 |
On the behavior of single-surface nuclear wavefunctions in the vicinity of the conical intersection for an X-3 system Varandas AJC, Xu ZR |
257 - 265 |
Valence photoionization and autoionizing states of acetylene studied by the complex basis function method in the random phase approximation Yasuike T, Yabushita S |
266 - 270 |
Forbidden electric dipole rotation and rotation-vibration transitions in H-2(+) Bunker PR, Moss RE |
271 - 279 |
Variational EKE-calculations of rovibrational energies of the ozone molecule from an empirical potential function Tyuterev VG, Tashkun SA, Schwenke DW, Jensen P, Cours T, Barbe A, Jacon M |
280 - 284 |
Spin-lattice relaxation in metal-organic platinum(II) complexes Homeier HHH, Strasser J, Yersin H |
285 - 296 |
Time-averaged normal coordinate analysis of polymer particles and crystals Noid DW, Fukui K, Sumpter BG, Yang C, Tuzun RE |
297 - 302 |
Density functional calculations of the structure of crystalline urea under high pressure Miao MS, Van Doren VE, Keuleers R, Desseyn HO, Van Alsenoy C, Martins JL |
303 - 310 |
Wavepacket dynamics in the ground electronic state of a diatomic molecule Eryomin VV, Umanskii IM, Kuz'menko NE |
311 - 317 |
A Monte Carlo model for the non-equilibrium coherent kinetics of ensembles of two level systems Longo S, Bruno D, Capitelli M, Minelli P |
318 - 323 |
A simplified scheme for relativistic density functional computation in the zeroth-order regular approximation Wang F, Hong GY, Li LM |
324 - 329 |
General atom-bond electronegativity equalization method and its application in prediction of charge distributions in polypeptide Cong Y, Yang ZZ |