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1.
Based on the meson-meson mixing and Regge trajectory, this paper establishes the mass relations which can describe the mass spectrum of 1^1 P1 meson state. Using these mass relations, it obtains the mass of K1B, hi (1380) and hc(1P) to be 1358.5MeV, 1468 MeV and 3543.9 MeV, respectively. The results are compared with other theoretical results and should be tested by experiments in the future. 相似文献
2.
<正>This paper discusses the masses and possible members of 21S0 and 23S1 meson multiplets in the framework of meson-meson mixing and Regge phenomenology.For the 21S0 meson nonet,K*(1460) may be the observed state of the 21S0 isodoublet with a mass of 1400 MeV and the mass ofω(1420) is 1412 MeV.For the 23S1 meson nonet,K*(1410) seems too light to be the 23S1 ns member.The fact that the agreement between the present findings and those given by experiments and other different approaches is satisfactory implies that the assignments in this paper may be reasonable. 相似文献
3.
E.J. Sacharidis W. Blum H. Dietl G. Grayer G. Hentschel W. Koch E. Lorenz G. Lütjens G. Lutz W. Männer J. Meissburger R. Richter U. Stierlin V. Chabaud C. Jones P. Weilhammer W. Hoogland 《Nuclear Physics B》1981,179(1):9-32
We have measured 618 K+p → π+KS0p events at 12.7 GeV/c incident lab momentum, mass range 790 ? mπ+Ks0 ? 990 MeV and t range 0.01 ? ?t ? 0.60 (GeV/c)2. The π+KS0 mass spectrum is dominated by the K1+ (892) resonance and a Breit-Wigner fit yields a mass m = 893.5 ± 1.1 MeV and a width Γ = 33.2 ± 4.1 MeV which is much narrower than measured hitherto. The t distribution of K1+ (892) events shows a dip in the forward direction and an exponential fall off thereafter, consistent with dominance of helicity flip amplitudes. The spin density matrix is almost saturated by ρ11 and ρ1?1 which are very close to their maximum allowed value of throughout the measured t range except in the very forward direction where ρ00 and Re ρ10 deviate from zero. Natural parity exchanges, therefore, dominate with unnatural parity exchanges being restricted to a small region in the forward direction. A Regge pole analysis of the differential cross sections of the present measurement in conjunction with previously measured total cross sections supports the f-coupled-pomeron hypothesis. 相似文献
4.
M. Kamimura 《Nuclear Physics A》1981,351(3):456-480
All the multipole transition densities between the seven T = 0 states in 12C are calculated with the use of the microscopic 3α resonating-group wave functions which are obtained by dynamically solving the 3α relative motion with the total antisymmetrization taken into account exactly. The observed elastic and inelastic electron scattering form factors for the transition to the 21+, 41+, 02+, 11?and 31? states are well reproduced with no additional effective charge. The existence of a deformed intrinsic state for the 01+, 21+and 41+states is deduced by the analysis of the transition densities between them which are derived by the weak-coupling-type 3α wave functions; the intrinsic density distribution is illustrated. The monopole density distribution of the 02+, 22+ and 11?, states is found to be much longer ranged than that of the 01+, 21+ and 41+ states; the 31? state case is intermediate. On the basis of the transition densities between the 01+, 21+, 02+ and 22+ states, analysis is made of the transition between the shell-like states and the molecule-like states with a large spatial-structure change. Specific, effective nucleon-nucleon interactions are folded into the transition densities here obtained. The evident dependence of the radial shape of the folded nucleon-12C form factors on the choice of the interactions and the multi-step form factors for the excitation of the 02+, 11? and 31? states are discussed. 相似文献
5.
6.
L.J.S. Halloran 《Optics Communications》2009,282(4):554-557
We have measured the isotope shift between 41K and 39K in the 4s1/2 → 5p1/2 transition at 405 nm using saturation spectroscopy. Our measured isotope shift is 456.1 ± 0.8 MHz, implying a residual isotope shift (sum of specific mass shift and field shift) of −52.7 ± 0.8 MHz. We deduce a specific mass shift of −40 ± 5 MHz, which would imply that the 5p1/2 state has a considerably larger specific mass shift than the 4p1/2 state. We have in addition measured the 5p1/2 hyperfine splitting for 41K. 相似文献
7.
8.
High resolution (0.001 cm−1) coherent anti-Stokes Raman spectroscopy (CARS) was used to directly examine the ν1 symmetric stretching mode of the planar symmetric D3h molecules 10BF3 and 11BF3. Simulations of the spectra were done using ν1 rovibrational parameters deduced from published infrared hot-band and difference-band studies and the close similarity to the observed CARS spectra confirms the validity of the infrared constants. No significant perturbations by Fermi resonance or Coriolis interactions with nearby states are observed, in marked contrast to the case of sulfur trioxide, a similar D3h molecule recently studied. In the harmonic approximation, the 10BF3 and 11BF3ν1 Q-branches would be identical since the isotopic substitution is at the center of mass but, interestingly, the ν1 stretching frequency for 11BF3 is found to be 0.198 cm−1higher than for the lighter 10BF3 isotopomer. This counterintuitive result is reproduced almost exactly (0.200 cm−1) by ab initio calculations (B3LYP/cc-pVTZ) that included evaluation of cubic and quartic force constants and xij anharmonicity constants. The ab initio computations also predict to within 1% the ΔB, ΔC changes in the rotational constants in going from the ground state to the v1 = 1 vibrational level. The results illustrate nicely the complementary interplay of modern infrared, Raman, and ab initio methods in obtaining and analyzing rovibrational spectra. 相似文献
9.
10.
Analytical potential energy function for the electronic states 2^∏1/2 and 2^∏3/2 of O^x2 (x=+1, -1) 下载免费PDF全文
The splitting of potential energy levels for ground state X^2∏g of O^x2 (x = +1,-1) under spin-orbit coupling (SOC) has been calculated by using the spin-orbit (SO) multi-configuration quasi-degenerate perturbation theory (SO-MCQDPT). Their Murrell-Sorbie (M S) potential functions are gained, and then the spectroscopic constants for electronic states 2^∏1/2 and 2^∏3/2 are derived from the M S function. The vertical excitation energies for O^x2 (x = +1,-1) are v[O2+1^(2∏3/2→X^2∏1/2)] =195.652cm^-1, and v[O2^-1(2^∏1/2 →X^2∏3/2)] =182.568cm^-1, respectively. All the spectroscopic data for electronic states 2^∏1/2 and 2^∏3/2 are given for the first time. 相似文献
11.
Atomic krypton was excited in presence of SF6 by an intense electron beam. The radiation emitted by the Kr2F1(2B2→ A1) transition was studied at 430 nm using time resolved spectroscopic techniques. The radiative lifetimes of Kr2F1 and of Kr12 were found to be 200 ns and 270 ns respectively. 相似文献
12.
The high-resolution spectrum of the ν1=5 stretching overtone of gaseous H70GeD3 has been recorded by an intracavity laser absorption spectrometer based on a vertical external cavity surface emitting laser (VECSEL). The rotational structure of the excited state at 9874.605 cm−1 was found weakly perturbed by unidentified interaction with dark states. Finally, of the 313 lines rotationally assigned, 239 lines were found unperturbed and could be reproduced with a root-mean-square (rms) deviation of 0.012 cm−1. The retrieved set of rotational parameters agrees with the values extrapolated from the previously studied ν1=6-8 stretching overtones. High-resolution FTIR spectra of the ν1 and 2ν1 bands have also been recorded and analyzed. The ν1=1 level, (νeff=2114.15 cm−1) is in anharmonic interaction with a further A1 symmetry level (νeff=2102.39 cm−1). The potential coupling term could be estimated (Wanh=5.6(3) cm−1) and the most probable assignment of the perturber is ν2+ν3. Moreover both levels are rotationally perturbed in an irregular fashion. Only a coarse analysis up to J=6 could be performed. The 2ν1 band reveals irregular perturbations of medium intensity by unknown dark states for almost all K values. Nevertheless the obtained leading rovibrational parameters of the 2ν1 band for J?6 are in agreement with those of the ν1=5-8 states. 相似文献
13.
Yu.S. Kalashnikova I.M. Narodetskii Yu.A. Simonov A.I. Veselov 《Physics letters. [Part B]》1985,155(4):217-222
For nucleons interacting via formation of the quark compound bag the resulting potential is written in a general form. Explicit examples of potentials are constructed in the 1S0, 3S1 and 3S1-3D1 states fitted to the experimental data at TL ? 1 GeV. As an outcome the QCB energy levels (dibaryons) and NN admixture in QCB are obtained in good agreement with theoretical predictions. 相似文献
14.
We have generated thep-cyanobenzyl radical in supersonic free expansion, and measured the vibrationally and rotationally resolved laser induced fluorescence (LIF) excitation spectra and the LIF dispersed spectra from the single vibronic levels (SVL) in the green-blue region. The lowest energy band at 20 738 cm−1with the strongest intensity in the excitation spectrum has been assigned to the 000band of the visible spectrum, on the basis of the vibronic structures in the SVL dispersed spectra. Based on the band type of the 000band,a-type, determined from the rotationally resolved LIF excitation spectrum, we have definitely assigned the visible band to theD122B1–D012B1electronic transition. We have found, on the grounds of the vibrational analysis of the dispersed spectra, that the vibronic structure of the 22B1–12B1electronic transition of the benzyl type is characterized by totally symmetric fundamental modes, 1, 8a, and 9a. 相似文献
15.
J.Michael Hollas Barry J Langham Hamdan Musa Trevor Ridley 《Journal of Molecular Spectroscopy》1983,97(2):405-419
The two-photon fluorescence excitation spectrum of 1,2-difluorobenzene was obtained with a tunable dye laser calibrated using a combination of the neon optogalvanic spectrum and etalon fringes. The spectrum consists only of A1-A1 bands but the use of linear and circular polarization divides the bands into two types. The 000 type retains its intensity in circular polarization and, rotationally, shows little or no zero-rank contribution. The 510 (or 1410) type loses much of its intensity in circular polarization and, rotationally, shows a large zero-rank contribution. These observations all accord with the trace of the two-photon transition tensor being close to zero for the 000 type and large for the 510 type, the latter type being involved in vibronic interaction which mixes the and states. There is strong evidence for Fermi resonance between the 51 and 61101 levels. Parts of the one-photon absorption spectrum have been photographed to aid sequence identification and also to look for the 510, A1-A1 transition. This transition is not observed: nor is there any evidence for intensity stealing by b2 vibrations. 相似文献
16.
The two photon coincidence technique yields an absolute measurement of a cascade decay rate without knowing the detection efficiency of each detector. This method is applied to calcium atoms in an atomic beam excited to the 4p21S0 state, and decaying via the resonant 1P1 state; it yields the excitation rate of the upper 4p21S0 level. Since the excitation process (two photon absorption) is controlled, one can compute the excitation rate of the upper level as a function of the transition probabilities in the cascade. The lower transition is well known and we can therefore deduce the transition probability for the 4p21S0 -4s4p 1P1, transition which previously had not been accurately determined. The preliminary measurements yield a line strength s = 0.98 ± 0.3 au in good agreement with a recent measurement of the lifetime of the 4p21S0 state. 相似文献
17.
G. N. Isachenko V. K. Za?tsev M. I. Fedorov A. T. Burkov E. A. Gurieva P. P. Konstantinov M. V. Vedernikov 《Physics of the Solid State》2009,51(9):1796-1799
The results of a study of Mg2Si
x
Sn1 − x
solid solutions (x = 0.25, 0.3, 0.35, 0.4) are reported. The measurements performed cover the Seebeck coefficient, electrical conductivity and
the Hall coefficient over broad ranges of temperatures (80–700 K) and carrier concentrations (1018 to 6 × 1020 cm−3). These measurements were used to derive the band structure parameters (band gap, hole mobility, hole effective mass). The
effective mass of holes was found to grow strongly with an increase in their concentration. 相似文献
18.
J.J. Brehm 《Physics letters. [Part B]》1981,100(5):428-432
A model is outlined for isolating the effects of final state interactions in an amplitude leading to three final pions. The method accounts for rearrangements among ?π and ?π states, producing a factor-of-2 fluctuation in the 1+ intensity below the A1 mass. It follows that this effect should cause a modulation of the A1 resonance. 相似文献
19.
The investigation of the manganites La2/3−xPrxSr1/3MnO3, La2/3Sr1/3−xCaxMnO3 and La2/3+xCa1/3−2xAgxMnO3, which all exhibit Mn3+:Mn4+=2, shows that it is possible to reach high magnetoresistance at room temperature, up to 21% under 1.2 T. These materials are compared to La5/6Ag1/6MnO3 which corresponds to the same Mn3+:Mn4+ ratio and exhibits a magnetoresistance of 25% in this field. An interesting feature deals with the value of the insulator-metal transition temperature TIM, often higher than TC, especially for Ag-based compounds. It is suggested that the latter results either from a better oxygenation of the surface of the grains or from a migration of silver toward the surface. 相似文献
20.
A comprehensive high resolution spectroscopic analysis has been made on the XeO green bands photographed in emission from an RF discharge source. Rotation-vibration constants derived from the analysis of the spectrum of the isotopically enriched species 129Xe16O and 129Xe18O were used to give RKR potential curves for the d1Σ+ and b1Π states. The bond distances and dissociation energies of the d1Σ+ and b1Π states were respectively found to be , De = 693 ± 10 cm?1 and , De = 461 ± 10 cm?1. For the a1Σ+ state it was not possible to establish a unique vibrational numbering or to construct an RKR potential curve, since observed bands of the d1Σ+→a1Σ+ system involve only high vibrational levels of the a1Σ+ state, which are severely predissociated. The observations are consistent with a fairly deep well, in agreement with the latest ab initio calculations which give a well depth of 0.7 eV. 相似文献