scholarly journals Time evolution of spin singlet in static homogeneous exchange and magnetic fields

2021 ◽  
Vol 47 (10) ◽  
pp. 823-829
Author(s):  
S. V. Kuplevakhsky ◽  
S. V. Bengus
1990 ◽  
Vol 04 (02) ◽  
pp. 129-135 ◽  
Author(s):  
A. S. SHERBAKOV ◽  
V. E. STARTSEV ◽  
E. G. VALIULIN ◽  
V. L. KOZHEVNIKOV

The results of temperature and time (at T = 4.2 K ) dependent magnetization (M) measurements on polycrystalline high T c superconductor EuBa 2 Cu 3O7−δ are reported for different magnetic fields from 2.2 kOe to 35 kOe. The measurements were performed in the field-cooled regime (measuring the Meissner effect). A new phenomenon is found: the magnetization sign inversion from negative to positive during the time at which the external conditions (T, H) remains unchanged. The differential susceptibility in a new mixed state with M > 0 is diamagnetic. It is shown that origin of this state is not connected with a flux trapping, but rather caused by the unusual nature of the vortex themselves in FC mixed state of high T c superconductors.


2015 ◽  
Vol 55 (3) ◽  
pp. 780-786 ◽  
Author(s):  
E.V. Miletsky ◽  
V.G. Ivanov ◽  
Yu.A. Nagovitsyn

2018 ◽  
Vol 392 ◽  
pp. 242-259 ◽  
Author(s):  
R. Grimaudo ◽  
Yu. Belousov ◽  
H. Nakazato ◽  
A. Messina

1990 ◽  
Vol 138 ◽  
pp. 191-211
Author(s):  
Å. Nordlund ◽  
R. F. Stein

As a prelude to discussing the interaction of magnetic fields with convection, we first review some general properties of convection in a stratified medium. Granulation, which is the surface manifestation of the major energy carrying convection scales, is a shallow phenomenon. Below the surface, the topology changes to one of filamentary cool downdrafts, immersed in a gently ascending isentropic background. The granular downflows merge into more widely separated downdrafts, on scales of mesogranulation and super-granulation.The local topology and time evolution of the small scale, kilo Gauss, network and facular magnetic field elements are controlled by convection on the scale of granulation. The topology and time evolution of larger scale magnetic field concentrations are controlled by the hierarchical structure of the horizontal components of the large scale velocity field. In sunspots, the small scale magnetic field structure determines the energy balance, the systematic flows and the waves. Below the surface, the small scale structure of the magnetic field may change drastically, with little observable effect at the surface. We discuss results of some recent numerical simulations of sunspot magnetic fields, and some mechanisms that may be relevant in determining the topology of the sub-surface magnetic field. Finally, we discuss the role of active region magnetic fields in the global solar dynamo.


1990 ◽  
Vol 142 ◽  
pp. 101-105
Author(s):  
K.R. Sivaraman

It is now well established (McIntosh 1979; Makarov and Sivaraman 1983) that the filament and filament channels seen in the H-alpha spectroheliograms (or filtergrams) can be used as reliable tracers for studying the time evolution of large-scale magnetic fields on the Sun. These features represent the neutral lines between the unipolar regions of opposite polarity. Comparison of the synoptic charts compiled from H-alpha pictures with those from full-disc magnetograms for the same period shows very good agreement and hence the former can be used with confidence for time evolution studies of large-scale unipolar regions for those periods when the magnetographs did not even exist. In this paper we shall present one of the results of our study (Makarov and Sivaraman 1983, 1989) on the migration of H-alpha filaments, namely, the existence of the meridional flow on the Sun. We shall extend it further to show the participation of this meridional flow in the solar cycle variation.


1999 ◽  
Vol 191 ◽  
pp. 195-200 ◽  
Author(s):  
P. J. Diamond ◽  
A. J. Kemball

We have produced a movie of the time evolution of the v=1, J=1−0 43 GHz SiO masers in the inner circumstellar envelope of the isolated Mira variable TX Cam. Our observations, taken every two weeks with the VLBA, currently cover about 60% of the stellar cycle from ϕ ∼ 0.6 → ϕ ∼ 1.2. They show that, in contrast to previous observations and theoretical models, the gas in which the masers are embedded is undergoing expansion during this period with a typical velocity of 3.65 ± 0.15 km/s. Some isolated features are seen to start falling back towards the star at around ϕ ∼ 1.0. We suggest that the 5 → 10 G magnetic fields we have previously detected at the position of the SiO masers may explain the departure from the expected behaviour.


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