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1.
《Nuclear Physics A》1987,462(1):150-162
Energy and angular distributions of protons and α-particles in coincidence with fusion residues produced in the reaction of 150 MeV 16O with 27Al were measured. Experimental results are reproduced by a statistical model calculation except a forward component of α-particle yield. About 20% of the total α-particle yield is considered to originate from incomplete fusion process.  相似文献   

2.
The four 5v 3 bands of 18O enriched ozone have been observed and analysed for the first time. Two species (16O18O16O and 18O16O18O) belong to the C2v symmetry group and two other (18O18O16O and 16O16O18O) to the Cs symmetry group. They have been recorded at a resolution of 0.008 cm?1 with a pathlength of 32.16 m. Despite the very weak absorptions observed, almost 250 energy levels have been derived for each of the 4 species, with J ? 35 and K a ? 13, and suitable sets of Hamiltonian parameters have been determined. For 3 species it has been necessary to account for the resonance between the (005) and (311) states to correctly reproduce the spectra observed. These resonances, anharmonic for C2v, and hybrid (both anhar-monic and Coriolis) for Cs symmetry confirm the accidentally extremely strong coupling between the (005) and (311) states for 16O3, due in that case to the very close distance between unperturbed energy levels. This work also confirms the excellent prediction of band centres of these four species derived from the recently determined isotopically invariant molecular potential function.  相似文献   

3.
采用乘积近似法计算了臭氧分子16O3及其同位素16O18O16O在20-6000 K温度范围内的总配分函数。其中转动配分函数用Watson的刚性转子模型,振动配分函数用谐振子模型.总的温度范围被划分为五个温度段。计算的配分函数在这五个温度段分别被拟合到一个温度T的五阶多项式,从而在每个温度段均得到六个拟合系数。由这些拟合系数就可以快速、准确的获得分子在所研究温度范围内任意温度的总配分函数。研究结果为目标特性识别、气动物理的高超声速技术等领域的研究提供了重要的参考信息。  相似文献   

4.
《Nuclear Physics A》1999,660(1):57-68
Generalized nucleon polarizabilities for virtual photons can be defined in terms of electroproduction cross sections as function of the 4-momentum transfer Q2. In particular, the sum of the generalized electric and magnetic polarizabilities Σ=α+β and the spin polarizability γ can be expressed by virtual photon absorption cross sections integrated over the excitation energy. These quantities have been calculated within the framework of the recently developed unitary isobar model for pion photo- and electroproduction on the proton, which describes the available experimental data up to an excitation energy of about 1 GeV. Our results have been compared to the predictions of chiral perturbation theory.  相似文献   

5.
6.
The α-particle structure for 16O nucleus is examined by means of the 16O + 16O scattering. The theoretical results well reproduce the experimental data.  相似文献   

7.
Head-on collisions between 16O nuclei are treated in the Time-Dependent Hartree-Fock (TDHF) approximation. Reactions at center-of-mass bombarding energies of 2 and 8 MeV per nucleon result in fusion-fission processes with strong internal excitation of the fragments.  相似文献   

8.
臭氧分子同位素16O18O16O的高温光谱研究   总被引:1,自引:3,他引:1  
在直接计算分子配分函数的基础上,将无转动跃迁偶极矩平方近似为一常数,计算了非对称陀螺臭氧分子同位素16O18O16O 001-000跃迁在中等温度和高温下的线强度.计算结果在1000 K时与HITRAN数据库的结果吻合相当好.在温度高达3000 K时与HITRAN数据库的结果仍符合较好(最大百分误差为5.48%),表明分子配分函数和线强度的高温计算是可靠的.在此基础上,进一步计算了非对称陀螺分子16O18O16O 001-000跃迁带在极端高温4000和5000 K的线强度并报道其模拟光谱.计算结果对大气分子高温光谱的实验测量和理论研究均有一定的参考价值.  相似文献   

9.
10.
Using the Landau-Zener approximation, we have calculated probabilities for inelastic processes and fusion for head-on collisions of 16O + 16O. For fusion the results show the importance of reaching a critical distance between the two ions.  相似文献   

11.
The molecular structure with the 16O+16O configuration in 32S and the superdeformed structure in 32S are discussed from the viewpoint of the cluster model.  相似文献   

12.
用于符合测量的多通道符合计数器   总被引:2,自引:0,他引:2  
符合测量在量子光学实验中有着重要的应用,它可以用于测量纠缠光子对和单光子干涉等实验。在使用过程中,经常用到三通道或更多通道的符合测量,这种情况下简单的门电路无法满足使用要求,而现场可编程门阵列(FPGA)为实现低成本、小体积的多通道符合计数系统提供了解决方案。同时,基于FPGA的多通道符合计数系统还可以提供ns精度的符合分辨时间,避免本底光噪声对探测器的影响,从而有效抑制偶然符合,进一步提高了多通道符合计数系统的性能。本文介绍了基于FPGA的多通道符合计数器,并实验测量了单光子探测器信号的符合计数。  相似文献   

13.
We examine the two-photon exchange contribution to the eN --> edelta(1232) --> epiN process with the aim of a precision study of the ratios of electric quadrupole (E2) and Coulomb quadrupole (C2) to the magnetic dipole (M1) gamma*Ndelta transitions. We relate the two-photon exchange amplitude to the N --> delta generalized parton distributions and obtain a quantitative estimate of the two-photon effects. The two-photon exchange corrections to the C2/M1 ratio depend strongly on whether this quantity is obtained from an interference cross section or from the Rosenbluth-type cross sections, in similarity with the elastic, eN --> eN, process.  相似文献   

14.
15.
Taking 16O+16O elastic scattering at 124 MeV as an example, we show that a barrier-wave-internal-wave decomposition of the elastic scattering amplitude provides valuable information on the light heavy-ion interaction and complements the more conventional nearside-farside decomposition. In particular, we show that the Airy minima present in the angular distributions are due to a barrier-wave-internal-wave interference mechanism, which sheds additional light on the exceptional transparency displayed by some light heavy-ion scattering systems. Extension of these ideas to other fields, like atomic and molecular collision physics, could prove rewarding.  相似文献   

16.
The muonic 2p-1s transitions in16O and18O have been measured with a Ge detector, with the 3d-2p transitions of Cl as reference line. Therms radii of18O and16O differ by 3.5±0.8 per cent as compared with 4.0 per cent according to the A1/3 law.  相似文献   

17.
Using 0.002 cm(-1) resolution Fourier transform absorption spectra of an (17)O enriched ozone sample, an extensive analysis of the v(1)+v(3) bands of the (16)O(17)O(16)O and (16)O(16)O(17)O isotopomers of ozone has been performed for the first time. The experimental rotational levels of the (101) vibrational states were satisfactorily reproduced using a Hamiltonian matrix that takes into account the observed rovibrational resonances. More precisely, for (16)O(17)O(16)O, as for the other C(2v)-type ozone isotopomers, it was necessary to account for the Coriolis type resonances linking the (101) rotational levels with the levels of the (200) and (002) vibrational states and the Darling-Dennison interaction coupling the levels of (200) with those of (002). For the C(s)-type isotopomer, namely (16)O(16)O(17)O, as for (16)O(16)O(18)O and (16)O(18)O(18)O, it proved necessary to also account for an additional DeltaK(a)&equals+/-2 resonance involving the rotational levels from (101) and (002) (J.-M. Flaud and R. Bacis, Spectrochimica Acta Part A 54, 3-16 (1998)). Using a Hamiltonian matrix which takes these resonances explicitly into account, precise vibrational energies and rotational and coupling constants were deduced, leading to the following band centers: v(0)(v(1)+v(3))=2078.3496 cm(-1) for (16)O(17)O(16)O and v(0)(v(1)+v(3))=2098.8631 cm(-1) for (16)O(16)O(17)O. Copyright 2001 Academic Press.  相似文献   

18.
19.
The combination of a new high-resolution grating spectrometer and a spontaneous emission source has made it possible to measure precisely the 1 → 0, 2 → 1, and 2 → 0 transitions of 12C16O relative to the accurately known 12C16O laser lines which have been referred to pure frequency standards by Eng et al. The 1 → 0 and 2 → 0 band centers agree to within 0.0002 cm?1 with those measured relative to wavelength standards by Fourier transform spectroscopy (FTS). From a weighted simultaneous fit to the FTS-absorption, FTS-flame, our grating-emission, and microwave results, a set of calculated line positions was obtained for the 1 → 0, 2 → 1, and 2 → 0 transitions of 12C16O. The absolute accuracy of these line positions is believed to be ±0.0005 cm?1 and we propose that the lines can be used as secondary wavenumber standards in the infrared.The spontaneous emission sequences v′ → (v′ ? 1) were measured for 12C16O up to v′ = 20, for 13C16O up to v′ = 11 (using a 13C-enriched sample), and for 12C18O up to v′ = 4 (in natural abundance). Internally consistent sets of Dunham coefficients were calculated from the best available data for the molecules of 12C16O, 13C16O, and 12C18O.  相似文献   

20.
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