Observation of Bs production at the Y(5S) resonance

Using the CLEO detector at the Cornell Electron Storage Ring, we have observed the Bs meson in e+e- annihilation at the Y(5S) resonance. We find 14 candidates consistent with Bs decays into final states with a J/psi or a Ds(*)- . The probability that we have observed a background fluctuation is less than 8 x 10(-10) . We have established that at the energy of the Y(5S) resonance Bs production proceeds predominantly through the creation of Bs*Bs* pairs. We find sigma(e+e- --> Bs*Bs*) = [0.11(-0.03))(+0.04)(stat) +/- 0.02(syst)]nb , and set the following limits: sigma(e+e- --> BsBs)/ sigma(e+ e- --> Bs*Bs*) <0.16 and [sigma(e+e- --> BsBs*) + sigma(e+e- --> Bs*Bs)]/sigma(e+e- -->Bs*Bs*) < 0.16 (90% C.L.). The mass of the Bs* meson is measured to be M(Bs*) = [5.414+/- 0.001(stat) +/- 0.003(syst)] GeV/c2 .     

N2O脉冲高压直流放电的光谱研究

建立了一套产生瞬变物种的脉冲高压放电及其光谱探测的分子束装置,该装置的放电部分可在最高10kV电压条件下长期稳定工作,在数据采集中利用软件实现了取样积分器的功能,并且可以进行多通道数据的同时采集。利用此装置在几Pa压力下对N2O脉冲高压直流放电过程进行了研究,对得到的N2O (A~2Σ —~X2Πi)发射谱进行了标识,由振动光谱的强度得到了N2O ~A态的相对振动布居,和以往的研究结果相比,得到的N2O ~A态更偏离Bolzmann分布,产生的~A态是初生态。     

Cross section and resonance effects in photoemission from Sn-doped In2O3(111)

Photoemission spectra of Sn-doped In₂O₃(111) have been measured using a range of photon energies between 40 and 1300 eV. The intensity of structure at the bottom of the valence band associated with states of mixed Sn 5s/O 2p character increases with increasing photon energy relative to that of states of more dominantly O 2p character at the top of the valence band, as expected from one electron ionisation cross sections. In addition a pronounced resonance in the intensity of a weak conduction band feature is observed around the In 4p core threshold.     

"Hot-atom" O2 dissociation and oxide nucleation on Al(111)

We propose an atomistic model for the nucleation of aluminum oxide on the Al(111) surface derived from first principles molecular dynamics simulations. The process begins with the dissociative adsorption of O2 molecules on the metal surface, which occurs via a "hot-atom" mechanism driven by the partial filling of the sigma* antibonding molecular orbital of O2. During the subsequent hyperthermal motion, O atoms can be spontaneously incorporated underneath the topmost Al surface layer, initiating the nucleation of the oxide far below the saturation coverage of one (1 x 1) O adlayer.     

Spectroscopic study of neutron shell closures via nucleon transfer in the near-dripline nucleus 23O

Neutron single particle energies have been measured in 23O using the 22O(d,p)23O*-->22O+n process. The energies of the resonant states have been deduced to be 4.00(2) MeV and 5.30(4) MeV. The first excited state can be assigned to the nu d3/2 single particle state from a comparison with shell model calculations. The measured 4.0 MeV energy difference between the nu s1/2 and nu d3/2 states gives the size of the N=16 shell gap which is in agreement with the recent USD05 ("universal" sd from 2005) shell model calculation, and is large enough to explain the unbound nature of the oxygen isotopes heavier than A=24. The resonance detected at 5.3 MeV can be assigned to a state out of the sd shell model space. Its energy corresponds to a approximately 1.3 MeV sized N=20 shell gap, therefore, the N=20 shell closure disappears at Z=8 in agreement with Monte Carlo shell model calculations using SDPF-M interaction.     

用SAC-CI方法研究Si(CH3)2O双自由基的基态、激发态、阳离子态和阴离子态

采用Nakatsuji提出的对称匹配耦合簇相互作用(SAC-CI)方法,计算了Si(CH3)2O双自由基分子的基态,单重三重激发态,阳离子二重态和阴离子二重态的激发能,光电子谱,电离能等.结果表明,SAC-CI方法比TDDFT有明显优势.     

Study of the reaction 16O(7Li, 3He)20F

Angular distributions for the ¹⁶O(⁷Li,³He)²⁰F reaction, at a bombarding energy of 24 MeV, have been measured for all states below 6.25 MeV excitation, using a gas target and a multi-angle spectrograph. Low-lying core-excited states are populated much less strongly than known (sd)⁴ states. Cross sections decrease rapidly with excitation energy, but states at 4.20, 4.52, 4.58 and 5.41 MeV are quite strong — suggesting they have high spin and (sd)⁴ configurations. Previously suggested high-spin states at 4.73 and 4.76 MeV are weak, implying they are probably of core-excited character.     

Isotope effect in hydrogen peroxide formation during H2O and D2O sonication

The kinetics of hydrogen peroxide formation have been studied during H2O and D2O sonication in the presence of argon and oxygen (f = 22 kHz, I = 3.0 W cm-2, Pac = 0.52 W ml-1, V = 20 ml, T = 20 degrees C). It was found that the sonochemical reaction rate W has a zero order with respect to hydrogen peroxide (H2O, D2O or DHO2) concentration. In argon atmosphere the kinetic isotope effect was found to be equal to alpha = WH2O/WD2O = 2.2 +/- 0.3. The alpha value decreases in H2O-D2O mixtures with increasing H2O concentration. In oxygen atmosphere the isotope effect is not observed (alpha = 1.05 +/- 0.10). It is assumed that the revealed isotope effect is related to the mechanism of water sonolysis including the H2O-Ar* and D2O-Ar* energy transition, where Ar* is an argon atom in an excited state, in nonequilibrium plasma generated by the shock-wave.     

First-principles calculation of the electronic structure and energy loss near edge spectra of chiral carbon nanotubes

We present first principles calculations of the electronic structure of small carbon nanotubes with different chiral angles theta and different diameters (d<1 nm). Results are obtained with a full potential method based on the density functional theory (DFT), with the local density approximation (LDA). We compare the band structure and density of states (DOS) of chiral nanotubes with those of zigzag and armchair tubes with similar diameters. The carbon K-edge energy loss near edge structures (ELNES) have been studied and pi* and sigma* contributions have been evaluated. These contributions give information on the degree of hybridization for the small chiral nanotubes.     

掺杂铽(Ⅲ)离子的邻苯二甲酸锶发光材料的晶体结构和发光机理

合成了掺杂三价铽离子的邻苯二甲酸锶发光材料。测定了材料的热稳定性、晶体结构及紫外吸收光谱、激发光谱和发射光谱。研究了晶体中邻苯二甲酸根单线态Sл、л1*、Sn、л1*跃迁吸收和由三线态Tл、л1*、Tn、л1*到铽(Ⅲ)离子5D4能级的能量传递机理。     

H,O,N,He原子掺杂Al原子的第一性原理研究

采用密度泛函理论框架下的第一性原理平面波赝势方法,对Al中分别加入H,O,N和He原子后的晶体状态进行了研究.通过晶体结构和形成能分析比较了杂质原子占据不同位置的难易程度及对晶体稳定性的影响,并从态密度、电荷密度和电荷布居的角度,分析了其电子结构.结果表明:H、O和N原子占据金属Al的四面体间隙最稳定,而He原子主要占据金属Al的八面体间隙. O和N原子与Al原子具有强烈的共价作用,H原子与Al原子存在共价作用但相对较弱,而He原子与Al原子的相互作用以范德华力为主.进一步揭示了四种原子在金属Al中不同行为的电子机制.     

Nanocrystalline versus microcrystalline Li(2)O:B(2)O3 composites: anomalous ionic conductivities and percolation theory

We study ionic transport in nano- and microcrystalline (1-x)Li(2)O:xB(2)O3 composites using standard impedance spectroscopy. In the nanocrystalline samples (average grain size of about 20 nm), the ionic conductivity sigma(dc) increases with increasing content x of B2O3 up to a maximum at x approximately 0.5. Above x approximately 0.92, sigma(dc) vanishes. By contrast, in the microcrystalline samples (grain size about 10 &mgr;m), sigma(dc) decreases monotonically with x and vanishes above x approximately 0. 55. We can explain this strikingly different behavior by a percolation model that assumes an enhanced conductivity at the interfaces between insulating and conducting phases in both materials and explicitly takes into account the different grain sizes.     

Electron spectroscopy of autoionizing states of oxygen,chlorine and bromine atoms

The autoionizing atomic states are obtained in dissociation Of O₂, Cl₂ and Br₂ molecules excited by either fast neutral He atoms (O₂) or by photons with 21.217 eV energy (Cl₂, and Br₂). Tentative assignment of the autoionizing levels is given for Cl* and for Br* atoms, and a more detailed one for O* atoms.     

Measurement of the Raman cross section of O(2)(a(1)D(g))

Two different measurement methods are described that indicate that the Raman cross section of O(2)(a(1)D(g)), sigma(a)= (0.45+/-0.02) sigma(X), where sigma(X) is the Raman cross section of O(2)(X(3)?(g)(-)). Spontaneous Raman scattering is a potentially useful technique for measuring the singlet O(2)yield in high-power oxygen iodine lasers. For the full potential of this method to be realized, one must determine sigma(O)(2(a)) to measure the yield directly.     

Towards the assignment of the REMPI spectrum of Ph2O using CIS and TD-DFT methods

Tentative assignment of the low-lying vibrational features of the first electronic excited singlet-state S₁ of diphenyl ether (Ph₂O), obtained from resonance-enhanced multiphoton ionisation (REMPI) spectroscopy, is performed using CIS and time-dependent density functional theory (TD-DFT) methods. The potential energy surfaces, regarding the rotation of the phenyl rings relatively to the C–O–C plane, are obtained at the B3LYP/6-31G(d) level of theory, for the ground-state of neutral and cationic Ph₂O and for its first excited singlet state. The torsional barriers of the ground state of diphenyl ether were studied by means of quantum-chemical perturbations of increasing accuracy and an extrapolation to the complete basis set limit and full configuration interaction (FCI) was performed through the use of correlation consistent basis sets and the continued fraction method. The first adiabatic ionisation energy (AIE) of the twist conformer is computed at 8.60 eV in the FCI limit, much higher than the experimental results of Terlouw et al. (8.09±0.03 eV) and Paiva et al. (7.8±0.1 eV). The B3LYP result of 7.82 eV is, however, in reasonable agreement with the result of Paiva et al. The first singlet excitation energy for the twist conformation is found to be 5.5 eV at the CIS/6-311++G(d,p) level of theory. Some features of the experimental REMPI spectrum, previously obtained by one of the authors, are explained and a new insight on the ionisation energy of diphenyl ether is presented.     

Theoretical study on the influence of ancillary ligand on the energy and optical properties of heteroleptic phosphorescent Ir(III) complexes

The geometries, energies, and electronic properties of a series of phosphorescent Ir(III) complexes including FIrpic, FIrmpic, FIrpca, and FIrprza have been characterized within density functional theory DFT calculations, which can reproduce and rationalize experimental results. The properties of excited states of the Ir(III) complexes were characterized by the configuration interaction with single-excitation (CIS) method. The ground- and excited-state geometries were optimized at the B3LYP/LANL2DZ and CIS/LANL2DZ levels, respectively. The absorption and phosphorescence wavelengths were computed based on the optimized ground- and excited-state geometries, respectively, by the time-dependent density functional theory (TD-DFT) methods. All the energies have been calculated by B3LYP method. The predictions revealed that the nature of the ancillary ligands can influence the distributions of frontier molecular orbitals and their energies, resulting in impact on the transition character and change in the emission color. In addition, the charge of transport quality has been estimated approximately by the predicted reorganization energy (λ). Our result also indicates that the substituent groups and different auxiliary ligand not only change the character of transition but also affect the rate and balance of charge transfer.     

Correlation-driven heavy-fermion formation in LiV2O4

Optical reflectivity measurements were performed on a single crystal of the d-electron heavy-fermion (HF) metal LiV2O4. Our results evidence the highly incoherent charge dynamics above T* approximately 20 K and the redistribution of the spectral weight of the optical conductivity over broad energy scales ( approximately 5 eV) as the quantum coherence of the charge carriers is recovered. This reveals that LiV2O4 is close to a correlation-driven insulating state and indicates that, in sharp contrast to f-electron HF Kondo-lattice systems, strong electronic correlation effects dominate the heavy quasiparticle formation in LiV2O4.     

Electron impact ionization of sodium Rydberg atoms below 2 eV

We have observed electron impact ionization of highly excited sodium Rydberg atoms in ns and nd states, n=35-51, below E=2 eV electron kinetic energy with energy resolution 0.25 eV. Measured absolute cross sections near 0 eV range from sigma(35d) approximately 7 x 10(-10) to sigma(50d) approximately 4 x 10(-9) cm(2). The energy dependence is consistent with that of widely used binary encounter approximation cross sections, and sigma(n) follows a power law in n. The measured cross sections are 14 to 24 times larger than theoretically predicted values. This enhancement may signal the effect of large polarizabilities of high Rydberg states not yet accounted for in ionization theories.     

Topologically Stable Lumps in SO(d) Gauged O((d+1) Sigma Models in d Dimensions: d =2,3,4

The gauge-invariant topological charge is defined for, and the inequalities supplying the lower bound on the action of an SO(4) gauged O(5) sigma model in four dimensions are established. The consistency of the solution with finiteness of the action and with topological stability is briefly verified for a particular dynamical example. Against the background of the topologically stable finite energy solitons of SO(d) gauged O(d+1) sigma models in d dimensions already known for d=2 and for d=3, the present example can be viewed as a demonstration by induction for the existence of such solitons in the case of arbitrary k.     

Chemisorption and dissociation of O2, on Ag(110)

Using an Ag₂₄ cluster, we have calculated the potential energy surface of an O₂ molecule chemisorbing and dissociating on the Ag(110) surface, with its molecular axis parallel to the grooves in the [1&#x0304;10] direction. For molecular chemisorption, we find equilibrium positions and vibrational frequencies in good agreement with experiment and with earlier calculations; the chemisorption energy, ∼ 0.1 eV, may be somewhat too low. Although both our calculated and the experimental vibrational frequencies suggest a chemisorbed O²⁻₂ ion, our calculated charge transfer to the O₂ molecule is a little less than one electron. We can explain the calculated low OO strength frequency by changing occupations of OO bonding and antibonding states with changing OO separation. These results show that one has to be cautious in directly relating observed vibrational frequency lowerings of chemisorbed molecules to their charge states. The dissociation path is completely along the direction of the OO stretch; we find a barrier height of ∼ 0.2 eV. The atomic equilibrium distance, vibrational frequency, and binding energy are in reasonable agreement with experiment. At large OO separation, the energy still decreases with increasing OO distance, indicative of OO Coulomb repulsion.