Large-scale distribution of magnetic fields,green corona and prominences during an extended activity cycle

The interrelations of the latitudinal distribution of the coronal green emission maxima, maximal numbers and areas of prominences, magnetic fields, sunspots, and polar faculae in the 20th and 21st sunspot cycles have been investigated. It is again demonstrated how the behaviour of all studied data depends on their heliographic latitude. In the polar zone, well separated from the equatorial we observe following polarity magnetic fields transported only polewards, while the equatorial zone is occupied mostly by leading polarity fields, developed there, moving equatorwards, and crossing the equator to the other hemisphere with the new cycle during the minimum of sunspot activity.This magnetic field distribution is well emphasized by the places of maximal occurrence of prominences and by the distribution of coronal green emission maxima which also differ in dependence on latitude.The question of identifying the first and last evolutionary stages of an extended cycle of activity is discussed and the existence of a magnetic activity cycle lasting 15–17 years is suggested.     

Structural and metamorphic evolution of the Sierras Australes (Buenos Aires Province/Argentina)

The Precambrian Basement Complex rocks as well as the Early to Late Palaeozoic cover sediments of the Sierras Australes were affected by one dominant folding and shearing event verging northeastward during Middle to Late Permian times. Strain estimates point to a minimal flattening and lateral shortening of the sedimentary cover sequence of c.20% and c.24% respectively. Continuing rotational deformation within first and second shear and thrust zones is documented by second and third folding and shearing. To the SW the fold belt changes into a fold and thrust belt where imbrication involves the basement. The deformational events were accompanied and outlasted by anchizonal to greenschist facies metamorphism proven by illite crystallinity and quartz deformation and recrystallization data. A temperature increase from ENE to WSW and also from N to S allowed a more ductile deformation of the rock sequence due to different deformation mechanisms operating. The folding and thrusting events were followed by strike-slip shearing on subvertical shear planes and shear zones under an overall sinistral transpressive regime. A model for the tectonic evolution of the Sierras Australes is proposed and some implications for its setting in the Gondwana reconstruction are given.

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Zusammenfassung Das präkambrische Basement sowie die alt- und jungpaläozoischen Deckschichten der Sierras Australes wurden während des Mittl. bis Ob. Perm von einer NE vergenten Faltung und Scherung erfaßt. Strain-Abschätzungen deuten auf eine minimale Plättung und laterale Verkürzung der Sedimentfolge von ca. 20% bzw. 24%. Die fortlaufende relationale Deformation in den ersten und zweiten Scher- und Überschiebungszonen ist durch zweite und dritte Faltung mit Scherung dokumentiert. Der Sierras Australes-Faltengürtel geht nach SW in einen Falten-Überschiebungsgürtel über, dessen nach NE gerichtete Imbrikationen das Basement einbeziehen. Daten der Illit-Kristallinität und Quarz-Deformation/-Rekristallisation zeigen, daß die Deformationen von anchizonaler bis seicht-grünschieferfazieller Metamorphose begleitet und überdauert wurden. Mit der von ENE nach WSW bzw. N nach S zunehmenden Temperierung setzten verschiedene Deformationsmechanismen ein. Sie ermöglichten eine zunehmend duktile Verformung der Gesteinsfolgen. Auf die Faltungen und Auf-/Überschiebungen folgten Lateralverschiebungen an subvertikalen Scherflächen und -zonen unter einem sinistralen transpressiven Regime. Für die tektonische Entwicklung der Sierras Australes wird ein Modell vorgeschlagen, und die Folgerungen für die Stellung in der Gondwana-Rekonstruktion werden angeführt.

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Résumé Les roches du socle précambrien ainsi que la couverture sédimentaire éo- à tardi-paléozoïque des Sierras Australes ont été affectées, au cours du Permien moyen à supérieur, d'un plissement et d'un cisaillement à vergence nord-est. Les déformations sont estimées à au moins 20% d'aplatissement et 24% de raccourcissement latéral. Dans la première et la deuxième zone de cisaillement et de charriage, la déformation rotationnelle continue s'exprime par les deuxième et troisième plissements. Vers le SW la ceinture plissée passe à une ceinture plissée et charriée qui comporte des imbrications du socle. Les déformations ont été accompagnées et suivies d'un métamorphisme de faciès d'anchizone à «schistes verts», ainsi qu'en attestent la cristallinité de l'illite et la déformation et recristallisation du quartz. L'accroissement de la température de l'ENE vers l'WSW ainsi que du N vers le S a donné lieu à des mécanismes de déformation de caractère de plus en plus ductile. La phase de plissement et de charriage a été suivie par un régime de cisaillements décrochants sénestres le long de plans et de shear-zones subverticaux. Les auteurs proposent un modèle de l'évolution tectonique des Sierras Australes et discutent de son insertion dans la reconstruction du Gondwana.

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The highly magnetic (B∼500 mg) white dwarf PG 1031+234: Discovery of wavelength dependent polarization and intensity variations

Our simultaneous five-colour (UBVRI) linear and circular polarimetry of PG 1031+234 have revealed a strong rotationally modulated circular polarization, peaking in the ultraviolet (P _max(U)–17%)Based on observations made at the European Southern Observatory, La Silla, Chile.Paper presented at the 11th European Regional Astronomical Meetings of the IAU on New Windows to the Universe, held 3–8 July, 1989, Tenerife, Canary Islands, Spain.     

Optical variability of NGC 7469 in 1967–1987

Within the framework of a five-year campaign of coordinated multifrequency observations of the 3 Tauri star RU Lupi, we present results obtained in X-ray, UV, optical, and IR spectral regions. In five cases, simultaneous data from UV to IR were collected. Data analysis shows a large variability at different wavelengths both in the continuum and lines, stronger in the UV and weaker in the IR. Correlations among variations in the UV and optical continua have been found. Moreover flare-like events (FLEs), probably due to strong activity in the surface layers of the star and burst phenomena on large scale, were detected. No forbidden coronal lines were detected in UV and optical regions with IUE and ESO 1.4m CAT telescope, respectively. This means either the used instruments have not enough sensitivity to detect the predicted forbidden lines, or the low X-ray detected intensity — with ASTRON satellite (2–25 keV) — is due to the absorption of the X-rays in the circumstellar envelope. In this paper we will discuss these results within the framework of the current models.Based on observations with IUE satellite (VILSPA) and ESO telescopes.Paper presented at the 11th European Regional Astronomical Meetings of the IAU on New Windows to the Universe, held 3–8 July, 1989, Tenerife, Canary Islands, Spain     

Astron observations of the Rapid Burster MXB 1730-335 and constraints on burster parameters from spectra of trailing bursts

We report on eight X-ray bursts detected by ASTRON from the Rapid Burster (RB) on 13 and 28 April and 16 August, 1983. Six of them (trailing bursts), with durations of 1.5–2 min, rise times of 5–10 s and intervals of 1–1.5 hours, exhibit spectral softening during the burst decay and may be related to the type I bursts. Two of the bursts (triangle bursts) observed on 28 April at interval of 28 min with much longer rise times (30–50 s) and longer durations (3 min), do not show distinct spectral softening. Persistent flux from RB on 16 August was estimated asF _p(2.0–2.4)×10^–9 erg cm^–2 s^–1. Spectral evolution of two trailing bursts was investigated by fitting their spectra in consecutive time intervals with the blackbody (BB), isothermal scattering photosphere (SP) and thermal bremsstrahlung (TB) models. Around the burst maxima the SP model fits the data best whereas in the burst tails the TB model is generally better. The BB model is worse than at least one of the two others. Interpretation of the burst spectra in terms of the BB radiation leads to improbably small neutron star mass and radius (M<0.86M ,R _NS<5 km) if the peak luminosity does not exceed the Eddington limit. Interpretation of the spectra around the burst maxima (3–15 s from the burst onset) in terms of an isothermal SP yields reasonable constraints onM,R _NS, and distanceD. For instance, for the hydrogen photosphere we obtainedM=(1.0–2.1)M R _NS=(7.1–16.4) km ifD=11 kpc. If one postulatesM=1.4M , thenD=(8.5–13) kpc for hydrogen photosphere; if, besides,D=11 kpc, thenR _NS=(8.1–13.3) km. It follows also from the SP-interpretation that the photosphere radius may increase up to 20–30 km in maxima of the trailing bursts when the luminosity becomes close to the Eddington luminosity.     

Diffuse extragalactic gamma-radiation above ‘black-body cutoff’

The possible contribution of gamma-rays predicted within the universal cosmic-ray (CR) hypothesis to the energy range of CR spectrum above black-body cutoff is calculated. These gamma-rays arise from the relativistic electromagnetic cascade generated in the field of microwave background radiation (MBR). The ultra-high energy photons and electrons that initiate the cascade are produced at the decay of -mesons created in interactions of photons with the MBR. Simple analytic expression for cascade gamma-ray spectrum is obtained from the solution of kinetic equations for electrons and photons as well as for protons propagating in the MBR field. It is shown that at certain values of magnetic field and radio-wave density in the intergalactic space te flux of cascade gamma-rays may at least partly mask the black-body cutoff in the CR spectrum.Deceased, August 13, 1989.     

Models of white dwarfs distorted by magnetic field and differential rotation: Numerical approach

In this paper we construct a generalized classical model of a white dwarf distorted by magnetic field and differential rotation. The numerical method, to be presented, will be implemented in a subsequent quantitative treatment of the model.     

Transmission and reflection of Rayleigh waves at a thin low velocity vertical layer: A laboratory and theoretical study

A three-dimensional ultrasonic modelling was used to study the Rayleigh waves reflected from a thin low velocity vertical layer and those transmitted through the same zone. The reflection and transmission coefficients of the Rayleigh waves have been calculated by an approximate method based on the Green function technique. Nonrigid contact boundary conditions were used for the low velocity layer modelling. A rather good correspondence between the theoretical and experimental absolute values of the reflection and the transmission coefficients was obtained. Some discrepancies between experimental and theoretical results, in particular with regard to phase shifts, may be explained by a certain inadequacy of the theoretical model to the low velocity layer investigated by the ultrasonic modelling.     

M computed from strong motion accelerograms recorded in Yugoslavia

It is shown that the new definition¹ of strong motion local magnitude M leads to stable estimates of magnitudes for earthquakes in Yugoslavia, with epicentral distances R <100 km and for 2.5 < M < 6.5. Tables with magnitudes computed using this new procedure are presented for all earthquakes contributing to the strong motion accelerogram files in EQINFOS for Yugoslavia.² The similarity of our findings with the analogous analyses for California suggests new possibilities for relative calibration between various local magnitude scales, which are used in southeastern Europe, and M_L in California.     

Intercomparison of measurements of stratospheric hydrogen fluoride

Observations of the vertical profile of hydrogen fluoride (HF) vapor in the stratosphere and of the vertical column amounts of HF above certain altitudes were made using a variety of spectroscopic instruments in the 1982 and 1983 Balloon Intercomparison Campaigns. Both emission instruments working in the far infrared spectral region and absorption instruments using solar occultation in the 2.5m region were employed. No systematic differences were seen in results from the two spectral regions. A mean profile from 20–45 km is presented, with uncertainties ranging from 20% to 50%. Total columns measured from ground and from 12 km are consistent with the profile if the mixing ratio for HF is small in the tropophere and low stratosphere.