A re-examination of the induction (crystal field) energy contribution to the relative stabilities of the f.c.c. and h.c.p. rare-gas crystal structures

A new calculation of the induction (crystal field) energy of the f.c.c. and h.c.p. structures of the rare-gas crystals of neon and argon gives an energy in favour of f.c.c. which is more than sufficient to counter the summed pair-potential which favours h.c.p. Predicted values of (E _f.c.c. - E _h.c.p.)/E _f.c.c. for neon and argon are 0·9 × 10^-3 and 1·3 × 10^-3 respectively. These values are similar to those that have been obtained for a modified dispersion energy and it is concluded that they should be added to these dispersion energies. Calculations on solid helium show a negligible difference in the induction energy for the two close-packed structures.     

The density of states of b.c.c. Nb3Au: A comparison with A-15 Nb3Au

When Nb₃Au is converted from the A-15 structure to the b.c.c. allotrope, a sharp decrease in the superconducting transition temperature, T_c, occurs (11.1 to 1.5 K). To study possible causes for this sharp decrease, specific heat measurements have been made on the b.c.c. form of Nb₃Au yielding values of γ=19.2 mJ/mole-K², β=0.274 mJ/mole-K⁴ and θ_D=305 K. These parameters compared with published values for the A-15 Nb₃Au indicate that a sharp drop in the density of states at the Fermi level, N(0), occurs when the A-15 structure is converted to the b.c.c. form.     

Hall effect studies in ytterbium through the f.c.c.-h.c.p. transformation

The Hall coefficient (R_H) of polycrystalline Yb showing the f.c.c.-h.c.p. transformation has been determined at 20 koe in the range 1.8–420°K. Both the structural and the associated magnetic transformation would separately be expected to modify R_H, but the evidence suggests that the observed behaviour through the transition arises primarily from the effects of the change in structure. A more detailed interpretation is presently not possible, however, because of the lack of knowledge of the band structure of h.c.p. Yb.     

A.c. conductivity in AsF5 doped polyphenylacetylene (PPA)

The a.c. conductivity of semiconducting cis-cisoid polyphenylacetylene (PPA) pellets has been studied at temperatures between 230 and 290 K and frequencies, ?, from 37 to 10⁵ Hz. The a.c. conductivity (σ_a.c.) is found to be strongly temperature dependent. σ_a.c. is proportional to ?^s with s varying from 0.45 to 0.75 as temperature is raised from 230 to 290 K. Both frequency dispersion and strong temperature dependence of σ_a.c. are best explained by the mechanism of hopping conduction in the band-tails.     

A.C. loss and related effects in type II superconductors

This review gathers together information important to the understanding of superconducting materials under a.c. conditions, and points out some features which are at present not too well understood. The idea is to try to build a consistent picture of the performance of superconductors rather than to present a historical account of the subject.

The basic behaviour of fluxons in the bulk of type II superconductors can be explained by the critical state model, but some of the details of flux pinning and the method of flux motion are in doubt. Flux instabilities under d.c. conditions have received a lot of attention and so have the methods of stabilization, but instabilities under a.c. conditions have not been studied in so much detail, and the problem of stabilization is more difficult than for f.c.

Generally surface effects are less well understood than bulk effects, partly because there are a number of possible phenomena to contend with. A.C. loss in the Meissner state can be explained by field enhancement and flux penetration at peaks in the surface. For fields between H _c3 and H _c2 present solutions of the Ginzburg-Landau equations for the currents in the surface sheath do not give sufficient agreement with experiment and some alternative explanation, such as flux pinning, may be necessary. There are a number of effects between H _c2 and H _c1, but the most important are Meissner currents and flux pinning.     

Ordering behaviors of the F.C.C. and B.C.C. phase alloys in the InMg,LiMg and AlZn systems

Expressions of the band-structure energy and the electrostatic energy characterized by the usual long-range and short-range order parameters are given to a binary alloy of simple metals with the f.c.c.-type or b.c.c.-type structure.The ordering energy and the local ordering energy are calculated for the InMg, LiMg and AlZn systems. The numerical results explain successfully the facts that the InMg system has the Ll₀-type and Ll₂-type ordered phases, each of which exists over a wide range of concentration and that the LiMg system has a local order with a negative short-range order parameter, while the AlZn system has that with the positive one. A lattice distortion in the Ll₀-type ordered structure of InMg is also discussed.     

Concentration and temperature dependence of asphericity of 3d-electrons in f.c.c. Co-Ni and Co-Fe alloys

The asphericity of 3d-electrons was measured as a function of temperature in some f.c.c. ferromagnetic Co alloys by means of the polarized neutron technique. The asphericity, as measured by the population of the e_g and t_2g sub-levels, was found to be almost independent of temperature. Simple models failed to explain the data.     

The effect of hydrogen on the superconducting and structural properties of b.c.c. Nb-Ru alloys

The superconducting transition temperature (T_c) has been measured before and after the introduction of hydrogen into Nb_(1?x)Ru_x$\text{(0.20?x?0.33)}$. In all cases, the presence of appreciable amounts of this interstitial component led to a sharp increase in the T_c. All the evidence suggests that conversion of the host metal lattice to f.c.c. is necessary for the appearance of the elevated T_c.     

Monte-Carlo calculation for the classical F.C.C. Heisenberg ferromagnet

The equilibrium properties of the classical f.c.c. Heisenberg ferromagnet are studied by Monte- Carlo techniques for small finite systems. Using the asymptotic dependence on the system size the results are extrapolated to the infinite system. The critical temperature is found to be T_c = 3.18 ± 0.02 and the critical exponents obtained are β = 0.33 ± 0.02, γ = 1.37 ± 0.04. The specific heat appears to have a cusp with α′_s = 0.1 ± 0.03 and α_s = 0.1 ± 0.1. Remarkable agreement is found with the finite-scaling theory.     

Pressure dependence of the Néel temperature of f.c.c. stainless steel

The Néel temperature T_N of f.c.c. stainless steel has been measured as a function of pressure using the Mössbauer effect. A sample with approximately 74 wt.% Fe, doped with ^57Co, and having T_N = 58.4 ± 0.1 K at zero pressure, shows T_N rising with pressure with increasing slope. Our results indicate that T_N is raised to room temperature by a pressure of 175 ± 5 kbar.     

A.C. susceptibility measurements in the presence of D.C. magnetic fields in CoGa alloys — A cluster spin glass system

Low field a.c. susceptibility measurements in the presence of large d.c. magnetic fields are reported on Co_xGa_1?x alloys (x = 0.585, 0.60 and 0.63), a cluster spin glass system, in the temperature range of 77 to 500 K. A peak in the a.c. susceptibility is observed in each case. The peak position shifts towards lower temperatures with increasing d.c. magnetic fields. In conjunction with the zero field NMR measurements reported earlier, these results may be taken to imply the existence of a continuous spectrum of freezing temperatures — cluster with highest anisotropy field having the lowest freezing temperature.     

有机固体薄膜的交流电导

本文讨论了有机固体薄膜交流电导的频率依赖性,指出在较高频率下,电导正比于频率两次方的依赖性,是由于电极接触电阻和薄膜电容所引致的假象。作者建议了一种外加串联电阻法来求取电极接触电阻值,从而使电导和电容的频率依赖性实验数据得到改正。提出了表征有机固体薄膜交流电导特性的三个参数,即在极低频下的直流电导率σ_d.c.值、在较高频区σ(f)∝fⁿ中的n值和在lgσ-lgf图上高频区直线与σ_d.c.水平线的交点f_x。对聚乙烯咔唑( 关键词：     

Resonances in at rest

Data on at rest show two resonant processes: (a) f₀(1370)η,f₀(1370)→σσ and ρρ, (b) η(1440)σ, η(1440)→ηπ⁺π⁻. The branching ratio BR[f₀(1370)→ρρ]/BR[f₀(1370)→σσ]=0.98±0.25 in the mass range available here. Using data on , the ratio Γ_4π/Γ_2π5 for f₀(1370). The effects of the strongly s-dependent width of f₀(1370) are discussed in some detail.The η(1440) is observed decaying to ησ and a₀(980)π, with strong destructive interference between them. In its decay to a₀(980)π, a narrow peak appears in the ηπ mass spectrum, but 30–50 MeV above that usually attributed to a₀(980) and significantly above the KK threshold. This effect is explained naturally by a two-step process: η(1440)→K^*(890)K followed by rescattering of the two kaons through a₀(980) to ηπ above the KK threshold.     

Magnetic form factor of pure cobalt in the high temperature f.c.c. phase

The magnetic form factor of pure cobalt has been studied in the high temperature f.c.c. phase by means of the polarized neutron technique. The amount of aspericity of the 3d-electron has been determined; the e_g sub-level population has been found to be p = 0.43 ± 0.01. A comparison of this result with other experimental data on f.c.c. ferfomagnetic Co alloys and with existing theoretical evaluations is discussed.     

A.C. specific heat of terbium and dysprosium

The dependence of a.c. specific heat measurements upon the temperature modulation amplitude ΔT has confirmed the first-order nature of the antiferromagnetic-ferromagnetic transition in single crystal terbium (T_C～221K) and polycrystalline dysprosium (T_C～85K). No peak in a.c. specific heat is obtained for 2ΔT less than the temperature hysteresis at the transition. By comparison, the peaks expected in a.c. specific heat were observed at the higher-order antiferromagnetic-paramagnetic transition in both materials for ΔT amplitudes as low as～40 mK.     

On stage V recovery in VIa b.c.c. metals

Abstract

A resistometric study at 4.2 °K of the high-temperature recovery spectrum of neutron-irradiated molybdenum as a function of fast fluence and of cold-worked molybdenum as a function of the heating program, yields evidence against vacancy migration in the 0.31 T_m stage for VIa b.c.c. metals.     

Temperature dependence of the soft acoustic shear modes in h.c.p. zirconium

Neutron measurements of the dispersion curve v(q) for [10·0] phonons polarized in [11·0] are presented for hexagonal close-packed Zr at 300°, 773°, and 1073°K. Given that the crystal transforms to b.c.c. at 1135°K and demonstrates a pronounced softening in the C₆₆ elastic constant, v(q) shows only a uniform lowering of the entire branch, consistent with the behavior of C₆₆(T) but fractionally smaller for large wave vectors. No anomalous phonon linewidths are observed.     

Evidence for tunnelling relaxation in the a.c. conductivity of chalcogenide glasses

The a.c. conductivity of chalcogenide glasses is well fitted at low temperature by the expression Σ_a.c.=Aω^sTⁿ where s=1 and n≤0.5. This expression is consistent with correlated barrier hopping (CBH) of bipolarons between both random and paired defects. However, a study of the temperature and frequency dependence of the capacitance shows that in a-SiO₂ and a-GeSe₂ the capacitance obeys the scaling relation: C=A ln (Tω^?1). This result would suggest that the a.c. conduction mechanism in chalcogenide glasses may be better described by tunneling relaxation than by CBH.     

Superconductivity and the b.c.c. to A-15 transformation in Nb-Au alloys2

Nb-Au alloys near the composition Nb₃Au can be quenched from the high temperature α solid solution phase field, retaining the b.c.c. structure. We report results on their superconducting, mechanical and physical properties as a function of composition. Short low temperature anneals transform these materials to the equilibrium A-15 structure with T_c up to 11K. We report results on the superconducting and physical properties of the transformed A-15 structure materials and describe how the properties of the transformed materials are affected by annealing temperature and time.     

The D.C. voltage-dependent resistivity of CuCl powder compacts under pressure

The CuCl powder compacts are found to exhibit d.c. voltage dependent resistivity. The resistivity drops by six orders of magnitudes when the applied voltage exceeds a critical value V_c.V_c is found to decrease with the increase in pressure. The high conducting phase shows a positive temperature coefficient of resistance at 1 atm of 0.004°C^-1 which increases with pressure at a rate 0.0004°C^?1 GPa^?1. It is suggested that the pressure induced transition reported at 4 GPa could arise from the application of d.c. voltage.