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1.
The X-band EPR spectrum of SrCl2:V has been measured at liquid nitrogen temperature. A signal associated with V2+ in a site of trigonal symmetry is observed. The EPR data have been explained using the spin hamiltonian , with D ? hv, g∥ = 1.957 ± 0.004, g6 = 1.954 ± 0.004, A∥ = 230 ± 5 MHz, A6 = 235 ± 5 MHz. This V2+ defect is similar to those previously reported in fluoride crystals with the fluorite structure. 相似文献
2.
The X-ray structure (293 K) of UO2(H2PO4)2·3H2O has been refined (R = 0.062): Mr = 518g, space group: P21/c (Z = 4); , , , β = 105.65(1)°, ; Dc = 3.17 Mg m?3. The structure consists of infinite chains along the (101) axis with U atoms bridged by two H2PO4 groups. The U atom is surrounded by a pentagonal bipyramid of oxygen atoms, one of them being an equatorial water molecule. The cohesion between the chains is ensured by hydrogen bonds involving the two last water molecules. An assignment of IR and Raman bands with isotopic substitution spectra is proposed. A phase transition at 128 K was made evident by DSC and spectroscopy. The room-temperature phase is characterized by a high disorder of the OH bond orientation while in the low-temperature phase H2O and POH species appear well oriented. The conductivity seems to occur by proton transfer and protonic-species rotation at the POH-water molecular interface between the chains. ac conductivity has been determined by means of the complex-impedance method (; E ~ 0.20 eV). 相似文献
3.
A. Baldacci S. Ghersetti S.C. Hurlock K. Narahari Rao 《Journal of Molecular Spectroscopy》1976,59(1):116-125
The rotational structure of about 40 bands of 12C2HD observed in the region 6000?600 cm?1 has been measured and interpreted with the purpose of determining a comprehensive set of molecular constants for this isotopic variety of acetylene. Combining these data with the results for 12C2H2 and 12C2D2, a reevaluation of the equilibrium internuclear distances for the acetylene molecule has been made: and were obtained. This paper presents all the molecular constants derived in this study. 相似文献
4.
V.K. Birulev V. Genchev N.N. Govorun T.S. Grigalashvili B.N. Guskov J. Hladky I.M. Ivanchenko V.D. Kekelidze D. Kiss V.G. Krivokhizhin V.V. Kukhtin M.F. Likhachev E. Nagy M. Novak A. Prokes Yu.I. Salomatin I.A. Savin L.V. Silvestrov J. Votruba 《Nuclear Physics B》1976,115(2):249-268
The energy dependence of the modulus and phase of the KL0-KS0 regeneration amplitude on hydrogen in the range of 14–50 GeV has been investigated at the Serpukhov 70 GeV accelerator.It has been established that the modulus of the modified regeneration amplitude decreases with increasing momentum as . The amplitude phase is energy-independent and its mean value is ?210 = ?132° ± 5°. The results obtained are compared with other experiments and with predictions of different theoretical models. 相似文献
5.
J.C.D. Brand U.D. Deshpande A.R. Hoy S.M. Jaywant 《Journal of Molecular Spectroscopy》1983,100(1):143-150
The E-B (0g+-0u+) band system of Br2 has been investigated at Doppler-limited resolution using polarization labeling spectroscopy. Merged E state data for the three naturally occurring isotopes in the range vE = 0–16, expressed in terms of the constants for 79Br2, are (in cm?1) Y0,0 = 49 777.962(54), Y1,0 = 150.834(22), Y2,0 = ?0.4182(28), Y3,0 = 6.6(11) × 10?4, Y0,1 = 4.1876(28) × 10?2, Y1,1 = ?1.607(16) × 10?4, and Y0,2 = 1.39(39) × 10?8. The bond distance is , and the diabatic dissociation energy to . 相似文献
6.
The half-lives of the states at 522.6 and 393.9 keV in 113Cd and 115Cd have been determined to be 0.322±0.012 and 0.75± 0.03 ns, respectively. Values of the ) and the energy difference in odd Cd (A = 113–119) are compared with those in neighbouring even Cd. The level properties are interpreted in the framework of the triaxial rotor model. 相似文献
7.
G. Carboni G. Gorini E. Iacopini L. Palffy F. Palmonari G. Torelli E. Zavattini 《Physics letters. [Part B]》1978,73(2):229-231
The measurement of the energy transition in muonic helium is presented. The energy difference S1 is found to be Sexp1 = 1381.3±0.5 meV. This result agrees with the expected value obtained assuming the previously measured value for the energy difference. 相似文献
8.
The 0-0, 1-1, 2-2, and 3-3 bands of the A2Π-X2Σ+ transition of the tritiated beryllium monohydride molecule have been observed at 5000 Å in emission using a beryllium hollow-cathode discharge in a He + T2 mixture. The rotational analysis of these bands yields the following principal molecular constants. From the pure electronic energy difference (EΠ - EΣ)BeT = 20 037.91 ± 1.5 cm?1 and the corresponding previously known values for BeH and BeD, the following electronic isotope shifts are derived and related to the theoretical approach given by Bunker to the problem of the breakdown of the Born-Oppenheimer approximation. 相似文献
9.
Laser-induced fluorescence excitation has been used to measure Stark splittings of selected lines in the and band systems of H2CS in electric fields up to 13 kV/cm. The derived excited state a-axis dipole moments are 0.820 ± 0.007 D for the 41 level of the 1A2 state; 0.838 ± 0.008 D for the zeroth vibrational level of 1A2; and 0.534 ± 0.015 D for the zeroth vibrational level of the 3A2 state. These results are compared with the corresponding values of H2CO, and interpreted in terms of the changing localization of the π and orbitals accompanying electronic excitation. 相似文献
10.
EPR of 61Ni+ doped CuGaS2 at 4.2 K leads to the following experimental data: . High axial field splitting of 2T2 state stabilizes the center against Jahn-Teller interaction. Covalency reduction factor k is 0.76. 相似文献
11.
Marek Danielewski Jaeosław Da̧bek Stanisł;aw Mrowec Grażyna Siemińska 《Solid State Ionics》1985,17(4):331-335
Using the re-equilibration kinetic method the chemical diffusion coefficient in nonstoichiometric chromium sesquisulfide, Cr2+yS3, has been determined as a function of temperature (1073–1373 K) and sulphur vapour pressure (10?104 Pa). It has been found that this coefficient is independent of sulphur pressure and can be described by the following empirical equation: . It has been shown that the mobility of the point defects inCr2+yS3 is independent of their concentration and that the self-diffusion coefficient of chromium in this sulfide has the following function of temperature and sulphur pressure: . (cm2s?1). 相似文献
12.
The electron paramagnetic resonance spectrum of Gd3+ in YCl3·6H20 with dilution of Gd/Y ions, has been studied with an X-band spectrometer at 295, 77 and 1.77°K and with a K-band spectrometer at 295 and 77°K. The individual values of all the parameters are evaluated from the data at the three temperatures. In particular, the following values for the g-tensor and the zero-field splitting parameters b20 and b22 are obtained from X-band data: at 295°K, gzz = 1.994±0.005, gxx = 1.992±0.005, gyy = 1.997±0.005, b20 = 1.898 ±0.015 GHz, b22 = ?2.247 ± 0.015GHz; at 77°K, gzz = 1.999±0.008, gxx = 2.000±0.008, b20= 1.978 ±0.022 GHz, b22 = ?1.574±0.022GHz; at 1.77°K, gzz = 2.002±0.010, gxx = 1.990 ±0.010, b20 = 2.011 ± 0.025 GHz, b22 = ?1.650 ±0.025 GHz. (The K-band values are found to be consistent with the X-band values). From the angular dependence of the data in the ZX plane (i) the angle X0 which the Z axis makes with the a vector of the unit cell, is determined to be 58.00 ±0.25° and (ii) the existence of pseudo-symmetry axes at ±5° from the Z axis in the ZX plane as found by heat capacity and specific heat data has been confirmed. An estimate is also made of the extent of admixture of the excited state with the ground state . 相似文献
13.
A. Valentin A. Henry Ph. Cardinet M.F. Le Moal Da-Wun Chen K. Narahari Rao 《Journal of Molecular Spectroscopy》1978,70(1):9-17
The wavenumbers of the vibration rotation band lines of 14N16O are reported for the , and subbands of the 1-0 transition in the infrared. The full set of spectroscopic constants for this band has been determined by direct approach using the analysis of Zare, Schmeltekopf, Harrop, and Albritton. In addition to the band origin ν0 and the B, D, H constants for the lower and upper vibrational levels, the following spin-orbit coupling constants have been derived: and (in cm?1). Apparent centrifugal corrections to these constants have been determined and the values obtained for them are and . Λ-Type doubling constants evaluated by using both grating and tunable laser data are also reported. 相似文献
14.
The reorientation effect in Coulomb excitation has been used to measure the following static quadrupole moments: . Interference effects from higher excited states have been included in the analysis, with the signs of the E2 matrix elements taken from an anharmonic model. The value obtained for is in disagreement with two previous measurements. We attribute the discrepancy to the smaller internucleon separation distances involved in the previous experiments, which can cause deviations from Coulomb excitation cross sections. The other quadrupole moments have not been measured previously. The B (E2: 0+ → 2+) measured were: . From the angular distribution of the de-excitation γ-rays of the Pb nuclei following recoil into vacuum, we have determined the following (two standard deviations), . Our value of is in agreement with a previous measurement. 相似文献
15.
The charge density wave transition in 2H-TaS2near 75 K has been observed to be incommensurate, using electron diffraction, with along the 〈10.0〉 directions which, within the experimental uncertainty, remains temperature independent to about 14 K. Incommensurate charge density formation is also observed in AgxTaS2 samples for with an increase in q1 to when x?0.26. Within the experimental error q1 appears to be temperature independent to 25 K. 相似文献
16.
Takashi Tonegawa 《Solid State Communications》1981,40(11):983-986
The transverse spin pair correlation function pxn=<SxmSxm+n>=<SxmSxm+n> is calculated exactly in the thermodynamic limit of the system described by the one-dimensional, isotropic, spin-, XY Hamiltonian . It is found that at absolute zero temperature (T = 0), the correlation function ρxn for n ≥ 0 is given by , , where the plus sign applies when J is positive and the minus sign applies when J is negative. From these the asymptotic behavior as n → ∞ of |?xn| at T = 0 is derived to be with a = 0.147088?. For finite temperatures, ρxn is calculated numerically. By using the results for ?xn, the transverse inverse correlation length and the wavenumber dependent transverse spin pair correlation function are also calculated exactly. 相似文献
17.
O. Häusser T.K. Alexander T. Faestermann D. Horn D. Ward H.R. Andrews I.S. Towner 《Physics letters. [Part B]》1978,73(2):127-130
The time-differential perturbed angular distribution method was used to determine the g-factors of the states in 43Ti and 43Sc. The results for the mass 43 mirror pair are: , . Considering in addition the magnetic moments in A = 41 and 42, it is suggested that the deformed states considered by Johnstone and Castel and by Erikson are responsible for the observed large deviations from the Schmidt values. 相似文献
18.
The heat capacity of synthetic α-Fe2O3 has been measured in the range 300–1050K by adiabatic shield calorimetry with intermittent energy inputs and temperature equilibration in between. A λ-type transition, related to the change from antiferro- to paramagnetism in the compound, is delineated and a maximum heat capacity of about 195 JK?1 mole?1 is observed over a 3 K interval around 955 K. Values of thermodynamic functions have been derived and CP (1000K), [H0(1000K)-H0(0)], and [S0(1000K)-S0(0)] are 149.0JK?1 mole?1, 115.72 kJ mole?1, and 252.27 JK?1 mole?1, respectively, after inclusion of earlier low-temperature results [X0 (298.15K)-X0(0)]. The non-magnetic heat capacity is estimated and the thermodynamic properties of the magnetic transition evaluated. The results are compared with spin-wave calculations in the random phase approximation below the Néel temperature and the Oguchi pair model above. An upper estimate of the total magnetic entropy gives 32.4JK?1 mole?1, which compares favorably with that calculated for randomization of five unpaired electron spins on each iron, ΔS = 2R ln 6 = 29.79 JK?1 mole?1 for α-Fe2O3. The critical exponent α in the equation is ?(0.50±0.10) below the maximum and 0.15±0.10 above, for Tn = 955.0K. The high temperature tail is discussed in terms of short range order. 相似文献
19.
The radiative lifetimes of the and states of CO2+ were measured by means of the delayed coincidence method. Excitation was performed by a pulsed electron beam incident on CO2. The results of these measurements are 115 ± 5 nsec for the state and 126 ± 3 nsec for the state. 相似文献
20.
The nature of mesons in the 0++ nonet is studied. In particular we discuss the parameterization of the I = 0 S wave in terms of the S1 and possible ? mesons. The S1 parameters are determined by fitting to π?π+ and K?K+ production data. In particular we find . 相似文献