Nuclear orientation of156Tb in gadolinium matrix

The anisotropy of the angular distribution of gamma-rays from the decay of¹⁵⁶Tb, oriented in a gadolinium matrix at low temperatures, has been measured at the angles of 0 and π/2 with respect to the applied magnetic field direction in the range of temperatures from 14·6 to 68·4 mK. The temperature dependence of anisotropy was measured for the first time. The parameters of hyperfine magnetic dipole and electric quadrupole splittings have been determined and the values of the magnetic dipole moment ¦Μ¹⁵⁶¦=(9·6±1·3)×10^?27 J/T and the electric quadrupole momentQ ¹⁵⁶=(2·9±0·9)×10^?28 m² of the¹⁵⁶Tb ground state have been calculated. Multipole mixing ratios andB(E2) branching ratios of many gamma-ray transitions occurring in¹⁵⁶Gd have been found and the results have been discussed in terms of the rotational-vibration and pairing-plus-quadrupole models.     

Effects of edge-localized mode-induced neoclassical toroidal viscosity torque on the toroidal intrinsic rotation in the EAST tokamak

Intrinsic rotation has been observed in lower hybrid current-driven (LHCD) H-mode plasmas with type-III edge-localized modes (ELMs) on Experimental Advanced Superconducting Tokamak (EAST), and it is found that the edge toroidal rotation accelerated before the onset of the ELM burst. Magnetic perturbation analysis shows there is a perturbation amplitude growth below 30 kHz corresponding to the edge rotation acceleration. Using the filament model, the neoclassical toroidal viscosity (NTV) code shows there is a co-current NTV torque at the edge, which may be responsible for the edge rotation acceleration. For maximum displacement ～1 cm and toroidal mode number n=15, the calculated torque density is ～0.44 N/m², comparable with the average edge toroidal angular momentum change rate ～1.24 N/m². Here, the 1 cm maximum magnetic surface displacement estimated from the experimental observation corresponds to a maximum magnetic perturbation ～ 10^?3–10^?2 T, in accordance with magnetic perturbation measurements during ELMs. By varying n from 10 to 20, the magnitude of the edge NTV torque density is mainly ～0.1–1 N/m². This significant co-current torque indicates that the NTV theory may be important in rotation problems during ELMs in H-mode plasmas. To better illuminate the problem, magnetic surface deformation obtained from other codes is desired for a more accurate calculation.     

Schnell rotierender Lichtbogen als spektroskopische Lichtquelle

An electric arc quickly moved magnetically forms a closed plasma cone or plasma ring between two concentrically arranged electrodes. Aerosols and suspended matters can be brought into the plasma in an optimum manner with a little carrier gas flow, and can be excited to emission. The dates applied and attained till now are: Arc current 5…?20 A, magnetic field strength 10⁴…?4 · 10⁵ A/m, magnetic induction 0.1…?0.3 T, rotation frequency 8…?15 kc, carrier gas air or argon maximum flow 0.5 1/min, intensity increase for CuI-lines up to factor 100. Further applications are possible for special lamps and electric arc diagnostics.     

Bestimmung von Temperatur und Dichte eines Gleitfunkens aus der Bremsstrahlung im Infrarot

The absolute intensity of a vacuum sliding spark (length 2–10 cm, half cycle 0,8 μsec) has been measured in the spectral region between 0,4 and 3μ. From the long wavelength radiation emitted from an optically thick layer, one gets the temperature, from the short wavelength radiation emitted from an optically thin layer, one obtains the density. Using polyethylene as an insulator we reached a temperature of 4·10⁵ °K at electron densities of 8·10¹⁸ cm^?3 and current densities of 1.2·10⁶ A/cm². The temporal development of temperature and density has been determined. The maximum intensity at λ=0.43 μ was found to be 5·10⁴ (7·10¹⁰ W/cm³ ster) as large as that of the positive crater of a properly driven carbon arc. At λ=3 μ this same parameter turned out to be 300 times as large (5·10⁷ W/cm³ ster).     

Elastische und unelastische Streuung von Elektronen an Gasen

The theoretical differential cross section for the elastic scattering and for the excitation of optical transitions in helium by electron impact has been refined in Born approximation by use of the two parameter Eckart eigenfunction for the ground state and for the excited states. The angular distributions of 25 kev electrons scattered elastically and inelastically by helium were measured in the angular range 2·3·10^?4≦?≦4·10^?2. The intensity distribution of the elastically scattered electrons is in accordance with the theoretical curve for?>7·10^?3 and is disturbed at smaller angles by the primary beam. Normalization of the experimental values to the theoretical elastic differential cross section leads to agreement between the experimental differential cross section for the excitation of the 2¹ P and 3¹ P state and the scattering formulae given in this paper. There are small systematic deviations (<20%) for the 2¹ P differential cross section in the angular range 3·10^?3<?<1·10^?2 only. The oscillator strength of these two transitions has been determined from the scattering measurements:f ₂₁=0·312±0·04 andf ₃₁=0·0898±0·006.     

Diagnostics of the solar corona structure by the refraction effects on radio emission

The solar disc radio brightness distribution observed at RATAN-600 can be interpreted as the angular directivity of the disk center emission at viewing anglesΘ=arcsin(R/R₀) over an angular range of R<0.9R ₀ at several wavelengths in the 2.0–32 cm region. These spectra can be treated as an emission enhancement due to refraction effects in free-free corona emission. The model simulations show good agreement with the observations and lead to estimation of the electron density N_e=1·10 ⁹ cm^?3 and emission measureEM=6·10 ²⁶ cm^?5 for the quiet Sun.     

Spin lattice relaxation of F+ centers in neutron irradiated cao crystals

Abstract

We have measured the electron spin-lattice relaxation rates of F⁺ centers in CaO crystals at different F⁺ centers concentrations (from 5.8·10¹⁵ to 1.4·10¹⁷ cm^?3) in magnetic fields from 10^?3 to 4.8 T and temperatures from 0.4 to 4.2 K. At temperatures above 1 K the relaxation rate is nearly proportional to the F⁺ centers concentration. Spin diffusion to fast relaxing centers is essential in determining the F⁺ centers spin polarization decay.     

Untersuchungen über die thermische Belastbarkeit und die Form von Düsen zur Führung von Hochstromplasmen

The electrical and thermal limitings of nozzle are calculated from electrical dates of argon arcs for guiding and constricting high current plasmas. The electrical field strength in nozzles resulted from the arc characteristics. Hence it follows the maximum nozzle length as a function of nozzle diameter and amperage. From the arc power converted in the nozzle the power density resulted at the nozzle wall. By use of known material functions of nozzle material the needed wall thicknes of nozzle and quantities and velocities of cooling water are calculable. The experimental verification of the results gives the following relation between the minimum nozzle diameter and amperage for argon arcs using the best nozzle cooling d [cm] = 10^?3 I [A]. With superposed gas flow values are riched up to d [cm] = 0,5 · 10^?3 I [A]. The attainable current density is 6 · 10³ A cm^?2 without superposed gas flow and 6 · 10⁴ A cm^?2 with superposed gas flow. New nozzle typs for plasma technological uses ensue from the results of investigations.     

Spurenanalyse von Cu in ZnS-Phosphoren mittels Neutronenaktivierung

The half life of the 206 kev state of Re¹⁸⁷ was determined with delayed coincidence technic to be:T _1/2=(5·70±0·05)·10^?7 s. The rotation of the spin of the 206 kev state in a magnetic field has been observed in a differential angular correlation measurement with the 480 kev?72 kevγ?γ cascade. From the observed Larmor frequency a magnetic moment ofμ=(5·02±0·06)μ _K for the 206 kev level has been derived. The 480 kev?72 kevγ?γ angular correlation was found to be undisturbed in an aqueous solution of ammoniumtungstate.     

Influence of the axial magnetic field on the current instability and on the collective acceleration of ions in plasma diodes

It is shown that, while suppressing transverse electron motion, the axial magnetic field with an induction of up to 6.8 × 10⁻² T in the gap of a plasma diode has no significant effect on the current instability and on the acceleration of ions at electron beam currents of ≤40 A. The increase in both the critical current and the period of current oscillations is related to an increase in the plasma density after applying the magnetic field. The maximum energy of the accelerated magnesium ions decreases by ≈25% at an induction of 1.7 × 10⁻² T and does not depend on the magnetic field in the range (1.7–6.8) × 10⁻² T.     

Time-dependent hyperfine interactions in moderately diluted Ni(Hf)

The magnetic hyperfine interaction of¹⁸¹Ta in Ni(Hf) has been measured as a function of temperature by means of the time differential γγ angular correlation technique. While for very low concentrations of less than 10^?4 a pure static interaction is observed, which follows the bulk magnetization apart from small deviations, spectra obtained from a source with 1·10^?3 Hf content show a more complex behaviour. From the comparison of the experimental data with theoretical spectra, which result from various dynamical models, we conclude that for a Hf concentration of 1·10^?3 the impurity-impurity interaction causes a local breakdown of the ferromagnetic ordering near the Curie point. The arising paramagnetic domains may change their geometrical form and position so that a probe nucleus is subject to a time-dependent hyperfine interaction.     

Magnetic and electric hyperfine interactions of181Ta implanted in thulium

The magnetic and electric hyperfine interaction at the site of dilute¹⁸¹Ta impurities in the rare earth metal Tm has been investigated as a function of temperature by TDPAC measurements. The samples were prepared by ion implantation of radioactive¹⁸¹Hf. In the paramagnetic phase between 100 K and 700 K the electric fieldgradient is a linear function of temperature: V_zz(T)=V_zz(O)·(1-A·T) with A=4.6·10^?4K^?1 and V_zz(293K)=6.4 (4)·10¹⁷v/cm². The TDPAC spectrum observed at 4.2 K reflects the 4 magnetically non-equivalent sites for an impurity in magnetically ordered Tm. The relative values and amplitudes of the corresponding 4 magnetic hyperfine fields are consistent with the predictions of the RKKY theory.     

Properties of straight and curved neutron guide tubes

The properties of straight and curved neutron guides for neutrons of the energy region 4·10^?7 eV≦E≦2·10^?6 eV (very cold neutrons) are investigated. Experimental data for the angular distribution of neutrons emerging from a straight neutron guide are presented and it is shown that they can be theoretically verified using Steyerl's approximation. In the second part we consider a strongly curved neutron guide. The effect of laminating such a guide is investigated experimentally and theoretically and the conditions for optimum transmission are discussed.     

Quantitative Lorentz transmission electron microscopy of structured thin permalloy films

The defocusing of images of ferromagnetic particles in the transmission electron microscope gives rise to magnetic contrast (Lorentz microscopy). We have developed a theory which allows from this contrast to determine quantitatively the distribution of the magnetic fields of the specimen. The measurements were performed on permalloy particles of disc (diameter 50 nm), and rectangular (25×50 nm² and 50×50 nm²) shapes, thickness of 21 nm. These particles had a vortex and Landau–Lifshitz structure, respectively. The determined value of the magnetic induction in the material amounted to 1.1±0.1 T. The stray fields in angular sectors of the rectangular particles reached 0.35±0.05 T. The width of the 90° Néel wall between domains turned out to be equal to 4.5±0.5 nm.     

Magnetic field effects on the hydrogen abstraction reaction of triplet 4-methoxybenzophenone with thiophenol as studied by a picosecond laser flash photolysis technique

The hydrogen abstraction reaction of triplet 4-methoxybenzophenone with thiophenol at 265 K has been studied with a newly developed picosecond laser flash photolysis apparatus under magnetic fields of 0–1.7 T. The decay rate constant of the radical pair generated was found to increase from 3.42 × 10⁹ s^?1 to 4.15 × 10⁹ s^?1 with increasing the magnetic field from 0 to 1.7 T. The observed magnetic field effects can be explained by the Δg mechanism. Using the simple kinetics model with the Δg mechanism, the rate constant of the escape process from the pair (k _esc) and two rate constants for the T-S spin conversion process (k _T-S) at 0 and 1.7 T were found to be 1.97 × 10⁹ s^?1, 1.45 × 10⁹ s^?1, and 2.12 × 10⁹ s^?1, respectively. From the magnetic field dependence on k _T-S, the difference in the g values of the 4-methoxybenzophenone ketyl and phenylthiyl radicals was estimated to be 0.0087.     

Precision electromagnet for a mass spectrometer

A precision electromagnet generating a magnetic field with an induction ranging from 0.05 to 0.50 T is designed, manufactured, and studied. It is intended for a magnetic resonance mass spectrometer with a rated resolution of about 10⁶. The magnetic field inhomogeneity on a circular orbit with a diameter of 400 mm along which the ion beam moves is no more than ±1 × 10^?5 of induction B ₀ at the center of the magnetic gap. At any point of the orbit, the magnetic field is kept constant with an accuracy of higher than 10^?6 for several minutes, which is sufficient to record mass spectra.     

Ion-molecule collisions in gaseous111InCl and111InI systems

Using gaseous sources of¹¹¹InCl and¹¹¹InI with densities between 1.0·10¹⁷ cm^?3 and 4.4·10¹⁹ cm^?3 the perturbation of the 171.3–245.4 keVγ-γ cascade was measured as a function of time and density by the time-differential perturbed angular correlation (TDPAC) method. The anisotropy shows a strong dependence on the density. By means of an extended model based on a stochastic model of Bosch and Spehl collision cross sections for charge transfer and deorientation could be determined. The cross sections for charge transfer collisions were within the region from 2·10^?15 cm² to 26·10^?15 cm² and for deorientation collisions between 1·10^?15 cm² and 100·10^?15 cm².     

Features of low-temperature thermal expansion of n-type Bi<Subscript>2</Subscript>Se<Subscript>3</Subscript> single crystals in magnetic field

Tensometric study of n-type Bi₂Se₃ single crystals in dc magnetic fields to 6 T in a temperature range of 7–23 K detected a weak negative thermal expansion (NTE) in the basal plane. The NTE increases with the field strength and depends on its orientation with respect to the trigonal c axis. In a magnetic field of 6 T, parallel to the c axis, the linear NTE coefficient reaches ?7 · 10^?7 K^?1, and a minimum sample length is reached at a temperature of 13 K, where a Hall carrier concentration maximum is also detected. The found magnetoelastic anomaly can be associated with the topological insulator state.     

Measurement of the hyperfine interaction of free75As ions In H2, He,Ne, Kr and Xe buffer environments and estimate of clolision cross sections in the eV and meV energy region

With the time-integral perturbed angular correlation (TIPAC) method the pressure dependence of the perturbation of the 121.1–279.5 keV γ-γ cascade in⁷⁵As has been investigated using gaseous H₂ ⁷⁵Se sources in different buffer environments. The obtained attenuation coefficients G₂₂ (∞) in the range of 0.55 to 1.0 were fitted with a theoretical stochastic model. In the region of low density, where the correlation time τ_C is large compared to the lifetime τ of the intermediate level of the nucleus, charge transfer collision cross sections have been evaluated between 8.1·10^?16 cm² for He, 1.3·10^?14 cm² for Xe and 1.8·10^?14 cm² for the molecular H₂ buffer gas. For increasing densities of the buffer gases the correlation time τ_C became small compared to the intermediate lifetime τ. The main effect in this region is the depolarization, and we found cross sections between 5.2·10^?15 cm² for He, 8.7·10^?14 cm² for Xe and 1.2·10^?13 cm² for the H₂ buffer gas.     

Saturation of the acoustic waves produced by pulsed arcs

Rapid simultaneous measurements of the arc current and voltage and the emitted acoustic wave were made on a small 20 A DC arc in open air, which was subjected to current pulses ranging in amplitude from 0·4 kA to 40 kA and in rise time from 10^?4 s to 10^?7 s. The results show that for a rise time Δt < 10^?5s, the amplitude of the pressure wave generated by the arc no longer varies with Δt but remains constant for a given amplitude of the current pulse. An additional study shows that this saturation is accompanied by a modification in the electrical behaviour of the arc, which suggests that the observed saturation is due to the arc itself and not to absorption of the pressure wave in the surrounding air.