A calculation of surface diffusion coefficients of adsorbates on the (110) plane of tungsten

An attempt to calculate the prefactors of the diffusion coefficients of tungsten, xenon and oxygen atoms on the W(110) plane in the zero-coverage limit was made, using a Fokker-Planck formalism. Pairwise substrate-substrate and adsorbate-substrate atom interactions were assumed and expressed by appropriate Morse potentials. The vibrations of the substrate were approximated by an Einstein model of independent oscillators. When Morse potentials were so adjusted as to give good agreement between experimental and calculated activation energies, a prefactor in excellent agreement with experiment was calculated for W/W(110). For Xe/W(110) and O/W(110) the calculated values were ～10^?4 cm²/s, i.e. essentially “normal”, while the experimental values are much lower. Possible reasons for the discrepancies are discussed.     

Analyzing the transition rates of the ionization of atoms by strong fields of a CO<Subscript>2</Subscript> laser including nonzero initial momenta

Here, the method of including nonzero initial momenta for ejected electrons in strong infrared laser fields is further developed [8]. It has been shown that, apart from being natural, including the nonzero initial momenta enables one to go into a deeper analysis of the process of tunnel ionization of atoms in strong laser fields (intensity up to 10¹⁶ W/cm²). This is due to looking closely at Fig. 2, which indicates that all electrons that could be ejected, under the circumstances, are ejected at a field intensity ～10¹³ W/cm², and that the effect of ionization after that is strongly diminished, which can be seen from the slope of the plates on Figs. 2 and 4. This also explains the saturation effect for fields up to 10¹⁶ W/cm² [1, 4, 5, 7], and probably this saturation goes on until the fields raising relativistic effects ～10¹⁸ W/cm² [7]. Opposite to what was believed earlier [7], the atomic field intensities could be increased to values over 10¹⁷ W/cm² only when more than 10 electrons are ejected from the atom, it is shown that the properly calculated ionization of 9 electrons increases the atomic field intensity to ～10¹⁸ W/cm².     

Levels in179W studied in the181Ta(p, 3n) reaction by on-line electron and gamma ray spectroscopy

Levels in¹⁷⁹W have been deduced from in-beam gamma and conversion electron studies of the¹⁸¹Ta(p, 3n)¹⁷⁹W reaction. The gamma-ray spectrum was studied with Ge(Li) detectors and a crystal diffraction spectrometer; the conversion electrons were measured with a broad range transport solenoid Si(Li) spectrometer. The multipolarities of some 50 transitions could be determined. Coriolis mixing of the Nilsson orbits withN=6 was calculated.     

强激光场中离子HD+光解离几率的相干控制

对含时薛定谔方程用短时传播子的对称分割法求得了非微扰的数值解,计算了强超短脉冲基频激光(波长306.7nm)与其三倍频激光作用下的离子HD⁺光解离的相干控制参量大小设该离子的初态为电子振动.基态其中的相干激发是共振的.二束光之间的相对相位变化从0到360°在基频和倍频激光强度各为5×10¹³W/cm²和5.09×10⁸W/cm²情形下,发现相对相位为π时,光解离几率达到最大。     

Intensitätsmessung von Röntgen- und Kerngammastrahlung an einigen schweren Myonenatomen

Absolute intensities of the 5–4 muonic X-ray transition in muonic W, Os, and Bi, and relative intensities of other X-ray transitions have been measured and compared with cascade calculations. The excitation of several levels in W, Os, Ir, Tl, and Bi nuclei resulting from the muonic cascade process has been observed and absolute excitation probabilities have been determined. For the first 2⁺ level of¹⁸⁸Os and the first 3/2⁺-levels of^203,205Tl the excitation probabilities are larger than calculated. The results are discussed.     

Decay of the new isotope167W

Theα- and β-decay of the new isotope¹⁶⁷W were observed in the reaction of 191 MeV³⁶Ar with¹³⁶Ba using a helium-jet and a fast tape-transport system. The identification is based on coincidences with tantalum X-rays and excitation function measurements. The measured half-life is 19.9(5) s. A decay scheme comprising 12 levels was constructed from γγ-coincidences. The β-decay is discussed within experimental and calculated level systematics. Alpha-rays with energy 4.55(2) MeV were assigned to¹⁶⁷W.     

Spin dependence of the shape of even-even nuclei within the Davydov-Chaban model

Within a model of a nonaxial even-even nucleus soft in β vibrations, the shape parameters of the ¹⁵⁴Gd, ^156,158,160Dy, ^164,168Er, ¹⁶⁸Yb, ¹⁷⁶Hf, and ¹⁸⁰W nuclei are calculated in the quadrupole approximation as functions of the excited-state spin.     

Calculation of thermal parameters of SiGe microbolometers

The thermal parameters of a SiGe microbolometer were calculated using numerical modeling. The calculated thermal conduction and thermal response time are in good agreement with the values found experimentally and range between 2·10⁻⁷ and 7·10⁻⁸ W/K and 1.5 and 4.5 ms, respectively. High sensitivity of microbolometer is achieved due to optimization of the thermal response time and thermal conduction by fitting the geometry of supporting heat-removing legs or by selection of a suitable material providing boundary thermal resistance higher than 8·10⁻³ cm²·K/W at the SiGe interface. __________ Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 12, pp. 44–50, December, 2007.     

High-spin states and rotation-particle coupling in 179W

The ¹⁷⁸Hf(α, 3n)¹⁷⁹W and ¹⁸¹Ta(p, 3n)¹⁷⁹W reactions are used to populate rotational states in ¹⁷⁹W. Particular attention is paid to the strongly perturbed positive-parity bands. The rotational energies within these bands are successfully explained within the unified model with pairing and Coriolis interactions included if the theoretical Coriolis matrix elements are reduced. The wave functions are calculated from a fit to the experimental energies and the theoretical and experimental transition probabilities are compared. Rotational bands built on the $\text{7}\text{2}$^?[514], $\text{1}\text{2}$^?[521] and $\text{5}\text{2}$^?[512] intrinsic states are also observed.     

Excitation function for high-energy (p, 2p) reactions

The excitation functions of the (p, 2p) reaction cross sections for the elements ²⁵Mg, ³⁰Si, ⁵⁷Fe, ⁶⁸Zn, ¹¹⁸Sn, ¹⁴²Ce and ¹⁸⁶W have been calculated in the energy region above 100 MeV. The calculated values are compared with the available experimental results and the agreement between the two is found to be fairly good. The dependence of σ(p,2p) on the target mass number has been explained in terms of the expression derived.     

Comparison of simulated X-ray conversion efficiency of laser produced iron plasma with experimental results

X-ray resonance lines between 11 Å and 17 Å emitted from iron plasmas created by a modest KrF laser have been simulated by modifying the atomic and hydrodynamic code EHYBRID. Free–free and free–bound emission from the Si-, Al-, Mg-, Na-, Ne- and F-like ions is calculated in the simulation. In the original experiments, a KrF laser (249 nm wavelength) with focused irradiances between 1×10¹² W/cm² and 1×10¹⁵ W/cm² was focused on iron targets. The laser pulse duration was varied between 10 ps and 20 ns. We have calculated X-ray conversion efficiencies to be, for example, 0.5% over 2 sr for 2×10¹³ W/cm² and 20 ns pulse duration, in good agreement with experimental measurements. The simulation of X-ray emission is also presented for an experiment where a train of eight 7 ps KrF laser pulses is incident onto an iron target. PACS 52.50.Jm; 52.38.Ph; 52.65.Kj; 52.30.Ex; 32.30.Rj     

Measurements of activation cross-sections for 165Ho(n,2n)164gHo and 180W(n,2n)179gW reactions induced by neutrons around 14 MeV

The cross-sections of ¹⁶⁵Ho(n,2n)^164gHo and ¹⁸⁰W(n,2n)^179gW reactions induced by neutrons around 14 MeV were measured using activation technique and calculated by a previously developed formulas, in which the neutron flux was determined using the monitor reaction ⁹³Nb(n,2n)^92mNb. Because both of the excited and ground states were produced in each of the two reactions, one formula was introduced to take out the effect from excited state. Comparison between this work and old data were given.     

The effect of an external electric field on the survival of surface-produced negative ions

Resonant charge exchange between slow atomic particles and a partially coated metal surface, in the presence of a homogeneous electric field, is considered. The survival probabilities are calculated for H^- ions, emerging from Cs-coated W and K-coated Ni(110) in fields of strengths 10^-4, 10^-5 and 0 au.     

Parity violating effects in Σ→Λγ and Σ→Λe t>+ e − decays

Parity violating effects in Σ→Λγ are calculated in non relativistic quark model usingW, Z and gluon exchanges. These effects are found to give dominant contribution to the parity violating effects in Σ→Λe ⁺⁺ e ^? decay as compared to the neutral current effects.     

The electrochemical behavior of Dy(III) in eutectic LiF-DyF<Subscript>3</Subscript> at W electrode

The electrochemical reduction process of Dy ion on tungsten electrode at 1103 K in Dy₂O₃-LiF-DyF₃ molten system was studied by cyclic voltammetry, chronoamperometry, and chronopotentiometry methods with a three-electrode system on the electrochemical workstation AUTOLAB. The results showed that Dy³⁺ could be deposited at around ?0.75 V on inert W electrode compared with platinum electrode. The reduction process of Dy ion on W electrode occurred in a single step with the exchange of three electrons because one reduction peak was observed, and the calculated transfer electron number was three. Chronoamperograms indicated that the nucleation process of dysprosium ions was instantaneous three-dimensional nucleation on a tungsten electrode. The cathode electrochemical process on the tungsten electrode was controlled by the diffusion of ions, and the diffusion coefficient was 1.159 × 10^?4 cm²/s, which was calculated from a chronopotentiogram.     

W doped SnO2 growth via sol–gel routes and characterization: Nanocubes

The effects of W doping on the characteristical properties of SnO₂ thin films prepared by sol–gel spin coating method were investigated. The SnO₂ thin films were deposited at various W doping ratios and characterized by various measurements. XRD studies indicated that the undoped and W doped SnO₂ films had cubic and tetragonal phases. The SEM images of WTO thin films showed cubic shaped nanocubes corresponding to cubic phase and the smaller particles corresponding to tetragonal phase were formed on the film surfaces, and their distributions and sizes were dependent on the W doping ratio. EDX spectroscopy analyses showed that the calculated and participated atomic ratios of W/(W + Sn) (at.%) in the starting solution and in the WTO thin films were almost close. It was found that the sheet resistance depended on W doping ratio and 2.0 at.% W doped SnO₂ (WTO) exhibited lowest value of sheet resistance (7.11 × 10³ Ω/cm²).     

First-principles investigation of diffusion behaviours of H isotopes:From W(110) surface into bulk and in bulk W

<正>The diffusion behaviours of hydrogen（H）,deuterium（D）,and tritium（T） from W（110） surface into bulk and in bulk W are investigated using first-principles calculations combined with simplified models.The diffusion energy barrier is shown to be 1.87 eV from W（110） surface to the subsurface,along with a much reduced barrier of 0.06 eV for the reverse diffusion process.After H enters into the bulk,its diffusion energy barrier with quantum correction is 0.19 eV. In terms of the diffusion theory presented by Wert and Zener,the diffusion pre-exponential factor of H is calculated to be 1.57×10^-7 m²·s^-1,and it is quantitatively in agreement with the experimental value of 4.1×10^-7 m²·s^-1. Subsequently,according to mass dependence(（1/m）^1/2) of H isotope effect,the diffusion pre-exponential factors of D and T are estimated to be 1.11×10^-7 m²·s^-1 and 0.91×10^-7 m²·s^-1,respectively.     

Semiclassical formula for the alpha-decay rate in an electromagnetic field

A semiclassical correction to the alpha-decay rate in an alternating electromagnetic field is obtained. Single-particle Gamow theory is used to describe the alpha-decay process. The relative change in the alpha-decay rate is calculated as a function of the charge of the alpha-active nucleus being considered, the alpha-particle energy, and the laser-radiation intensity. It is shown that the lower the alpha-particle energy and the larger the charge-number value, the greater the increase in the alpha-decay rate. It is found that, even at the liming values of the laser-radiation intensity (10²⁶–10²⁸ W/cm²), the relative enhancement of alpha decay does exceed a few percent—in particular, it is as small as 2% for ²³⁸U at the radiation intensity of 10²⁸ W/cm².     

Direct measurement of the electron-phonon interaction in Pd,Mo and W by point-contact spectroscopy

The point-contact electron-phonon interaction function α²F has been obtained for the three transition metals Pd, Mo and W. The measured^Pα²F_p-spectra show clear structures which are in agreement with characteristic features in the phonon densities of states and calculated α²(ω)F(ω)-spectra.     

Third-harmonic generation in a vacuum at the focus of a high-intensity laser beam

A new physical effect lying in the harmonic generation by a focused high-intensity (I ～ 10²⁷ W/cm²) laser beam in a vacuum is predicted. The probability for the third-harmonic generation is calculated for a specific model of a monochromatic laser beam (symmetric beam) with the optical frequency.