125 - 134 |
Adsorbates on graphene: Impurity states and electron scattering Wehling TO, Katsnelson MI, Lichtenstein AI |
135 - 137 |
Temperature dependence of rotational excitation rate coefficients of SH(X-2 Pi) in collision with He Klos J, Lique F, Alexander MH |
138 - 142 |
Kinetic study of the reaction of chlorine atoms with chloromethane in the gas phase Sarzynski D, Gola AA, Drys A, Jodkowski JT |
143 - 146 |
Combination bands of the N2O trimer involving the intermolecular modes in the 2260 cm(-1) region Dehghany M, Afshari M, Moazzen-Ahmadi N, McKellar ARW |
147 - 150 |
Origin of fine structures on the dissociative 1s ->sigma* resonance in X-ray absorption spectra of O-2 Velkov Y, Kimberg V, Kosugi N, Salek P, Gel'mukhanov F |
151 - 156 |
Rydberg, valence and mixed states in the vertical spectrum of HF Pitarch-Ruiz J, Sanchez-Marin J, Lavin C, Velasco AM, Martin I |
157 - 162 |
Electron momentum spectroscopy study on valence electronic structures of pyrimidine Ning CG, Liu K, Luo ZH, Zhang SF, Deng JK |
163 - 167 |
Non-adiabatic molecular dynamics of excited Na-2(+) solvated in Ar-17 clusters Douady J, Jacquet E, Giglio E, Zanuttini D, Gervais B |
168 - 173 |
Quantum chemical study of the O-3-HONO complex Roohi H, Ashuri M |
174 - 177 |
Stability of protonated and ionized hydroxylamine in the interstellar medium Largo L, Rayon VM, Barrientos C, Largo A, Redondo P |
178 - 181 |
Electron impact ionization of formaldehyde Vacher JR, Jorand F, Blin-Simiand N, Pasquiers S |
182 - 185 |
Scattering of electrons by gaseous CS((1)Sigma): The role of short-range forces on the very-low energy (2)Pi resonance Sebastianelli F, Gianturco FA, Stoecklin T, Baccarelli I |
186 - 190 |
Optical absorption of silver clusters: A study of the effective potential core size Harb M, Rabilloud F, Simon D |
191 - 195 |
Substituent effect on geometry of the NO and N(CH3)(2) groups in para substituted derivatives of nitrosobenzene and N,N-dimethylaniline Sadlej-Sosnowska N, Krygowski TM |
196 - 200 |
A density functional study of N-15 chemical shielding tensors in quinolines Behzadi H, Esrafili MD, Beheshtian J, Hadipour NL, van der Spoel D |
201 - 204 |
Surface effects in the crystallization process of elastic flexible polymers Schnabel S, Vogel T, Bachmann M, Janke W |
205 - 208 |
Attenuated total reflectance-far ultraviolet (ATR-FUV) spectra of CH3OH, CH3OD, CD3OH and CD3OD in a liquid phase similar to Rydberg states similar to Morisawa Y, Ikehata A, Higashi N, Ozaki Y |
209 - 212 |
Eu-151 Mossbauer studies on La0.46Eu0.21Ca0.33MnO3 CMR system Reddy TG, Gupta A, Reddy KR |
213 - 217 |
Electronic structure and lattice anisotropy of Cd(UO2)O-2 Matar SF |
218 - 222 |
Vibrational features of phospho-silicate glasses: Periodic B3LYP simulations Corno M, Pedone A |
223 - 226 |
Proton distribution in KHCO3 from ab initio molecular dynamics simulation Dopieralski PD, Latajka Z, Olovsson I |
227 - 231 |
Possible effect of carbon nanotube diameter on gas-surface interactions - The case of benzene, water, and n-pentane adsorption on SWCNTs at ultra-high vacuum conditions Komarneni M, Sand A, Goering J, Burghaus U, Lu M, Veca LM, Sun YP |
232 - 235 |
On the compressibility of C-60 individual molecules Amer MS, Maguire JF |
236 - 239 |
Electronic structure of the mixed aluminum and sodium cluster Al2Na Lin L, Kita Y, Udagawa T, Sakai S, Nguyen MT |
240 - 243 |
Narrowed bandgaps and stronger excitonic effects from small boron nitride nanotubes Yu J, Yu DH, Chen Y, Chen H, Lin MY, Cheng BM, Li J, Duan WH |
244 - 248 |
Brij-micelle and polyacrylic acid interaction investigated by Cu2+-induced pyrene fluorescence: Effect of brij-micelle structure Bandyopadhyay P, Ghosh AK, Bandyopadhyay S |
249 - 252 |
Negatively charged GaAs clusters Gutsev GL, Mochena MD, O'Neal RH, Saha BC |
253 - 257 |
On the difference in electronic properties between fullerene C-60 and C60X2 Tokunaga K |
258 - 261 |
Characterization of acid-treated carbon nanotube thin films by means of Raman spectroscopy and field-effect response Zhang ZB, Li JT, Cabezas AL, Zhang SL |
262 - 266 |
Correlation between the microstructure and the origin of the green luminescence in ZnO: A case study on the thin films and nanowires Bera A, Basak D |
267 - 270 |
Thermal transport through a fluid-solid interface Murad S, Puri IK |
271 - 276 |
Hydrogen-bond enhanced thermal energy transport at functionalized, hydrophobic and hydrophilic silica-water interfaces Schoen PAE, Michel B, Curioni A, Poulikakos D |
277 - 280 |
Novel spectral representation of RNA secondary structure without loss of information Randic M, Plavsic D |
281 - 286 |
A 2D graphical representation of protein sequence and its numerical characterization Wen J, Zhang YY |
287 - 292 |
Conformational behavior of the simplest dipeptide: Formylglycine. Quantum chemical and matrix isolation FTIR study Wierzejewska M, Olbert-Majkut A |
293 - 302 |
Electron density distribution in cladribine (2-chloro-2'-deoxyadenosine) - A drug against leukemia and multiple sclerosis -Studied by multinuclear NQR spectroscopy and DFT calculations Latosinska JN, Latosinska M, Seliger J, Zagar V, Kazimierczuk Z |
303 - 307 |
Optimized complementary auxiliary basis sets for explicitly correlated methods: aug-cc-pVnZ orbital basis sets Yousaf KE, Peterson KA |
308 - 316 |
Using the Source Function descriptor to dampen the multipole model bias in charge density studies from X-ray structure factors refinements Lo Presti L, Gatti C |
317 - 322 |
Revised model core potentials for third-row transition-metal atoms from Lu to Hg Mori H, Ueno-Noto K, Osanai Y, Noro T, Fujiwara T, Klobukowski M, Miyoshi E |
323 - 328 |
Extended continuous-flow stirred-tank reactor (ECSTR) as a simple model of life under thermodynamically open conditions Takinoue M, Ma Y, Mori Y, Yoshikawa K |