Effect of the Λ n interaction on the cross section of the reaction γd → K+Λ n

Taking into account the n interaction, a nonrelativistic graphical technique is used to calculate the differential cross section of the reaction d K⁺ n as a function of photon energy, K⁺-momentum, and angle of emission of the K⁺. The kinematic region in which variation of the n-scattering parameters gives the most noticeable effect is separated out.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 8, pp. 104–106, August, 1978.The author thanks G. M. Radutskii and V. A. Filimonov for many useful discussions.     

Preliminary computation of the gap eigenmode of shear Alfvén waves on the LAPD

Characterizing the gap eigenmode of shear Alfv′en waves(SAWs) and its interaction with energetic ions is important to the success of magnetically confined fusion. Previous studies have reported an experimental observation of the spectral gap of SAW on the on Large Plasma Device(LAPD)(Zhang et al. 2008 Phys. Plasmas 15 012103), a linear large plasma device(Gekelman et al. 1991 Rev. Sci. Instrum. 62 2875) possessing easier diagnostic access and lower cost compared with traditional fusion devices, and analytical theory and numerical gap eigenmode using ideal conditions(Chang 2014 Ph.D Thesis at Australian National University). To guide experimental implementation, the present work models the gap eigenmode of SAWs using exact LAPD parameters. A full picture of the wave field for previous experiment reveals that the previously observed spectral gap is not global but an axially local result. To form a global spectral gap, the number of magnetic mirrors has to be increased and stronger static magnetic field makes it clearer. Such a spectral gap is obtained for the magnetic field of B_0(z) = 1.2 + 0.6 cos[2π(z-33.68)/3.63] with 7.74-m magnetic beach. By introducing two types of local defects(corresponding to E_θ(z_0) = 0 and E'_θ(z_0) = 0 respectively), odd-parity and even-parity discrete eigenmodes are formed clearly inside the gap. The strength of these gap eigenmodes decreases significantly with collision frequency, which is consistent with previous studies. Parameter scans show that these gap eigenmodes can be even formed successfully for the field strength of B_0(z) = 0.2 + 0.1 cos[2π(z-33.68)/3.63] and with only four magnetic mirrors, which are achievable by the LAPD at its present status. This work can serve as a strong motivation and direct reference for the experimental implementation of the gap eigenmode of SAWs on the LAPD and other linear plasma devices.     

Scaling factors associated withM-furcations of the 1−μ∥x∥z map

A numerical study is made of the scaling behavior associated withM-furcations (M=3, 4, 5) in the mapx _t+1 =1–x _t ^z (z>1). The scaling constants and are calculated as functions ofz, as well as the more general scaling functions andf(a).     

On the gap problem for the sequence ∥mβ∥

We discuss the gap problem for the sequence m used in our previous Letter (D. H. Mayer, Lett. Math. Phys. 16, 139–143 (1988)).     

Investigation of the π–π stacking interactions without direct electrostatic effects of substituents: the aromatic∥aromatic and aromatic∥anti-aromatic complexes

Stability of the π–π stacking interactions in the ben∥substituted-ben and ben∥substituted-COT complexes was studied using the computational quantum chemistry methods (where ben and COT are benzene and cyclooctatetraene, ∥ denotes π–π stacking interaction, substituted-ben and substituted-COT are benzene and cyclooctatetraene which substituted with four ethynyl-X groups, respectively, and X = OH, CH₃, H, F, CF₃, CN and NO₂). In these complexes electron-withdrawing substituents lead to larger binding energies and electron-donating ones lead to weaker interactions compared to X = H. There are meaningful correlations between the Hammett constants and binding energies. The atoms in molecules (AIM) analysis shows that formation of these complexes is accompanied by increase in the electron charge densities at the ring critical points of the substituted-ben and substituted-COT rings which leads to increase/decrease of the π–π stacking interactions in the ben∥substituted-ben/ben∥substituted-COT complexes. The charge transfer occurs from benzene to substituted-ben in the ben∥substituted-ben complexes and from substituted-COT to benzene (with the exception of X = CN) in the ben∥substituted-COT ones. Nuclear magnetic resonance calculations demonstrate that interactions of the more aromatic substituted-ben/less anti-aromatic substituted-COT rings with benzene in the ben∥substituted-ben/ben∥substituted-COT complexes can be helpful to enhance strength of the π–π stacking interactions. Thus, regardless of ring size, the π–π stacking interaction is an aromatic–aromatic interaction and π electron cloud properties of interacting rings affect on the strength of this interaction.     

Effect of Cu doping on the magnetic and electrical properties of n=2 Ruddlesden-Popper manganates

A series of polycrystalline Cu-doped n=2 Ruddlesden-Popper manganates La1.2Sr1.8CuzMn（2-x）O7 （x=0, 0.04, 0.13） were synthesized by the solid state reaction method. The effect of Cu doping on the magnetic and transport properties has been studied. It is found that Cu substitution for Mn greatly affects the magnetic and electrical properties of the parent phase La1.2Sr1.8Mn2O7. With the increase of Cu content, the system undergoes a transition from longrange ferromagnetic order to the spin glass state and further to an antiferromagnetic order. A little of Cu dopant can lead to the samples showing semiconductor or insulator behaviour in the whole observed temperature range while the parent phase has a metal-insulator transition. These samples show colossal magnetoresistance at low temperatures and the value of it decreases with increasing Cu content.     

Influence of sample geometry on the magnetic-field induced metal-insulator transition in nHgCdTe

We report on measurements of the Hall-resistivity as a function of sample geometry in n-Hg_0.8Cd_0.2Te. The results demonstrate that the data measured with an nHgCdTe sample by Shayegan et al.¹ quite recently are a mere consequence of the sample geometry and do not represent the Hall resistivity. The magneto-transport properties of pure n-HgCdTe are not identical with those of n-InSb in strong magnetic fields and at low temperatures.     

Photoabsorption Spectra of （SiO2）n （n ≤ 5） Clusters on the Basis of Time-Dependent Density Functional Theory

The photoabsorption spectra of （SiO2）n （n = 2-5） clusters [including isomers （D3h, D2d） structures of （SiO2）3 and （C2v, D2h, D4h） structures of （SiO2）4] are calculated by using time-dependent density-function theory. The equilibrium geometries, the binding energy, the gap between the highest occupied and lowest unoccupied molecular orbitals and vertical ionization potential for corresponding structures are computed using several methods with different types of the basis functions. It is found that the polarizability functions are necessary for the basis functions when optimize the structures of silicon oxide clusters. For different geometries of various clusters and the related isomers, their spectra are very different. Meanwhile, the comparison between using local-density generalized-gradient approximations for exchange-correlation potentials shows that both the calculated spectra present the same spectral feature. We suggest that the calculated photoabsorption spectra could be taken as a tool to elucidate the isomers and dusters structure.     

Observation and Simulation of n=1 Reversed Shear Alfvén Eigenmode on the HL-2A Tokamak

A branch of high-frequency Alfvénic modes is observed on the HL-2 A tokamak. The electromagnetic mode can be driven unstably in the plasma with an off-axis neutral beam heating. Its mode frequency keeps almost unchanged or presents a slow-sweeping behavior, depending on the detail current evolution. The poloidal and toroidal mode numbers are m/n = 1/1. The mode has a quite short duration(≤20 ms) and usually appears 5–10 ms after the neutral beam being injected into the plasma. Hybrid simulations...     

Excitation of isomeric states in the (γ,n), (n, 2n), and (γ, 2n) reactions on the 113In nucleus

The induced-activity method was used to measure the isomeric ratio of the yields of the (γ, n), (n, 2n), and (γ, 2n) reactions on the ¹¹³In nucleus. The energy dependence of the isomeric ratios of the yields of the photonuclear reactions ¹¹³In(γ, n)^112m,g In and ¹¹³In(γ, 2n)^111m,g In is studied in the energy range of 12–35 MeV.     

Photoluminescence of the n+‐n‐i Submicron Structures of Gallium Arsenide

The special features of the photoluminescence of the n ⁺ni submicron structures of gallium arsenide are investigated. It is found that the character of the dependence of the fluorescence intensity on the thickness of the structure is determined by the relationship between three characteristic lengths: diffusional length, thickness of the n ⁺ layer, and depth of absorption of exciting radiation, whereas the decrease in the mobility of charge carriers in epitaxial layers leads to an increase in the fluorescence intensity of the structure, with exciting radiation being strongly absorbed.     

Investigation of the (n, γf) process on a235U nucleus

The fluctuations of uranium X-rays yield in coincidence with fission of the²³⁵U nucleus were observed at several neutron resonances. The results show the dependence ofK ₁ yield on fission width _f. This dependence is explained by the (n, f) process which is the result of competition between fission and -decay during the deexcitation of the²³⁶U compound nucleus. The mean width _f was determined to be equal to (2·1 _–1·7 ^+1·5 ) meV. The mean energy of prefission-rays was found to be (750 _–130 ⁺⁴⁰⁰ ) keV. It seems that the -transitions taking place before fission of the²³⁶U compound nucleus are mostly of the magnetic dipole.It is a great pleasure to express our gratitude to Yu. I. Kolgin for considerable help in all the experimental work, to L. B. Pikelner and Yu. P. Popov for many useful discussions, I. M. Salamatin, A. Mateeva for the programme supply of the experiment, to A. A. Bogdzel and V. G. Tishin for taking part in different steps of the work.     

Application of Doppler Backscattering for Alfvén Mode Study on the Globus-M Spherical Tokamak

Physics of Atomic Nuclei - The Alfvén oscillations were studied using the multifrequency Doppler backscattering (DBS) method on the Globus-M spherical tokamak during the neutral deuterium...     

Distributions of products of the quasifree knocking-out reaction (p,p′n) on halo nuclei in the intermediate-energy region

Expressions for the distribution functions of products of the reaction (p, p′n) of valence neutron knocking-out from halo nuclei were derived using space-time correlation functions. The possibility of using this reaction to study the neutron halo structure was analyzed.     

On the hall resistivity of nHgCdTe

We discuss the measurements of the Hall resistivity of nHgCdTe and InSb which have demonstrated the similarity of the electronic properties of these two materials. Gebhardt and Nimitz [1] dispute the validity of our results. We cite the evidence that confirms the correctness of our original observations.     

Parameterization of the nuclear Hulthén potentials

Within the formalism of supersymmetry-inspired factorization method, a two-term nuclear Hulthén potential has been developed and parameterized to reproduce the nucleon–nucleon scattering phase shifts for P and D partial wave states.