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991.
B. Singh 《Indian Journal of Physics》2011,85(12):1687-1694
In the present work, measurements are made on the intensity and angular distribution of Compton scattered gamma rays of energy
279 keV from K-shell electrons of tin at scattering angles ranging from 30° to 150° and also determined the K-shell to free electron differential collision, absorption and scattering cross section ratio. For this purpose, two NaI(Tl)
scintillation detectors working in coincidence with 30 nsec resolving time are used to record the events. The experimental
results are compared with the available experimental and theoretical data. 相似文献
992.
Many molecules with an even number of electrons belong to open-shell systems due to π
2 ground state electronic configuration. This configuration gives rise to three low-lying states X
3
Σ
−, a
Δ
1 and b
1
Σ
+. The inclusion of these target states in a trial wave function of the entire scattering system have important implications
in the resonances that may be detected in these open-shell molecules. Various molecules like O2, PX (X = H and halogens), SO, Si2, BF have π
2 ground state configuration. The R-matrix method is a well established ab initio formalism to calculate differential, integral and momentum-transfer cross sections for the elastic scattering of electrons
by molecules. We have calculated these cross sections for PH and SO molecules in the incident electron energy range 0–10 eV.
The results are obtained by using the R-matrix method in which the closecoupling expansion of the wave function of the scattering system includes only the ground
state. This target state is described by configuration interaction wave function that includes correlation effects. The cross
section for electron impact on PH and SO are presented. 相似文献
993.
We study the effect of finite chemical potential for the QGP constituents in the Ramanathan et al. statistical model [Phys. Rev.
C70, 027903, (2004)]. While the earlier computations using this model with vanishing chemical potentials indicated a weakly first
order phase transition for the system in the vicinity of 170 MeV [Pramana
68 757 (2007)], the introduction of finite values for the chemical potentials of the constituents makes the transition a smooth
roll over of the phases, while allowing fireball formation with radius of a few ‘fermi’ to take place. This seems to be in
conformity with the latest consensus on the nature of the QGP-Hadron phase transition. 相似文献
994.
Bipin Singh Koranga Vinod Kumar A. Jha 《International Journal of Theoretical Physics》2011,50(8):2609-2613
We give a phenomenological model of CPT violating neutrino oscillation above the GUT scale. In this paper, we consider the
effect of Planck scale operators on neutrino mixing. We assume that the main part of neutrino masses and mixing arise through
GUT scale operators The dispersion relation for the CPT violating neutrino and anti-neutrino oscillation are discussed. 相似文献
995.
Using the combustion synthesis, CaYAl3O7:Er3+ phosphor powders co-doped with Yb3+ have been prepared at low temperatures (550 °C) in a few minutes. Formation of the compound was confirmed by X-ray powder diffraction. Near-infrared to visible upconversion fluorescence emission in the Er3+ doped CaYAl3O7 phosphor powder has been observed. The effect of co-doping with triply ionized ytterbium in the CaYAl3O7:Er3+ phosphor has been studied and the process involved is discussed. 相似文献
996.
Lithium borate (Li2B4O7) is a low Zeff, tissue equivalent material that is commonly used for medical dosimetry using the thermoluminescence (TL) technique. Nanocrystals of lithium borate were synthesized by the combustion method for the first time in the laboratory. TL characteristics of the synthesized material were studied and compared with those of commercially available microcrystalline Li2B4O7. The optimum pre-irradiation annealing condition was found to be 300 °C for 10 min and that of post-irradiation annealing was 300 °C for 30 min. The synthesized Li2B4O7 nanophosphor has very poor sensitivity for low doses of gamma up to 101 Gy whereas from 101 to 4.5×102 Gy this phosphor exhibits a linear response and then from 4.5×102 to 103 Gy it shows supralinearity. Thermoluminescence properties of Li2B4O7 nanophosphor doped with Cu has also been investigated in this paper. It shows low fading and a linear response over a wide range of gamma radiation from 1×102 to 5×103 Gy. Therefore the synthesized lithium borate nanophosphor doped with Cu may be used for high dose measurements of gamma radiations. 相似文献
997.
Poonam Singh U.P. Verma Per Jensen 《Journal of Physics and Chemistry of Solids》2011,72(12):1414-1418
The structural, electronic and optical properties of HgAl2Se4 are investigated using the full potential linear augmented plane wave method based on density functional theory. The calculated structural parameters using LDA are in excellent agreement with the available experimental result. The obtained energy band gap (2.24 eV) using EV-GGA approximation is in excellent agreement with experimental data (2.20 eV). Variation in the energy band gap as a function of the unit cell lattice parameter has been studied. The optical properties show a considerable anisotropy, which makes this compound very useful for various linear–nonlinear optical devices. 相似文献
998.
Singh N 《Physical review letters》2011,107(24):245003
Despite the widely discussed role of whistler waves in mediating magnetic reconnection (MR), the direct connection between such waves and the MR has not been demonstrated by comparing the characteristic temporal and spatial features of the waves and the MR process. Using the whistler wave dispersion relation, we theoretically predict the experimentally measured rise time (τ(rise)) of a few microseconds for the fast rising MR rate in the Versatile Toroidal Facility at MIT. The rise time is closely given by the inverse of the frequency bandwidth of the whistler waves generated in the evolving current sheet. The wave frequencies lie much above the ion cyclotron frequency, but they are limited to less than 0.1% of the electron cyclotron frequency in the argon plasma. The maximum normalized MR rate R=0.35 measured experimentally is precisely predicted by the angular dispersion of the whistler waves. 相似文献
999.
In this paper, a rigorous theoretical analysis has been made to study the dispersion relation of EM waves in periodic ternary one-dimensional photonic crystal having two different structures. In one case we have chosen glass-plasma and ZnS in one unit cell and in other case we have considered glass-plasma and MgF2 in one unit cell. Using Kronig-Penney model the dispersion relation for proposed structures has been obtained and numerical results are presented in the form of dispersion curves. The dependence of photonic band gap (PBG) characteristics on plasma frequency, plasma width and the width of dielectric media are discussed in the light of frequency gap and cutoffs of binary one-dimensional plasma photonic crystal. An attempt has been made to show how the PBG characteristic of a particular structure changes when the dielectric materials of its unit cell is changed by the other dielectric material. It is found that the structure having glass-plasma-ZnS in unit cell is more useful for broad band filtering and other plasma functioning devices compared to the structure having glass-plasma-MgF2 in one unit cell. 相似文献
1000.
The modal dispersion characteristics of EM waves in a new unconventional plasma loaded doubly clad waveguide having a shape of the lemniscates of Bernoulli-type core cross-section have been studied analytically. The proposed waveguide has three parts namely the core with slighter high index, the inner cladding with plasma and the outer cladding with air. Now using the necessary orthogonal coordinates for the proposed structure and imposing the boundary conditions under the weak guidance condition, the modal characteristics equation has been obtained considering variations in plasma width and plasma frequency, the dispersion curves and cutoff frequencies have been obtained and presented in this paper. It is noted that as the width of plasma layer increases, the cutoff frequency also increases considerably in all considered cases. This shows that using plasma width as a new parameter we can control any particular mode on our wish. 相似文献