Magnetic Field Concentrator Based on the Superconducting Films with Nanosize Cuts

The flow, energy distribution and concentrations profiles of Ti ions in cathodic arc are studied by test particle Monte Carlo simulations with considering the mass transfer through the macro-particles filters with inhomogeneous magnetic field. The loss of ions due to their deposition on filter walls was calculated as a function of electric current and number of turns in the coil. The magnetic field concentrator that arises in the bending region of the filters leads to increase the loss of the ions component of cathodic arc. The ions loss up to 80 % of their energy resulted by the paired elastic collisions which correspond to the experimental results. The ion fluxes arriving at the surface of the substrates during planetary rotating of them opposite the evaporators mounted to each other at an angle of 120° characterized by the wide range of mutual overlapping.

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Superconductors with spin–orbit interactions

International Journal of Modern Physics B ◽

10.1142/s0217979216501836 ◽

2016 ◽

Vol 30 (25) ◽

pp. 1650183 ◽

Cited By ~ 4

Author(s):

Yu. N. Ovchinnikov

Keyword(s):

Magnetic Field ◽

Superconducting Films ◽

Critical Magnetic Field ◽

Spin Orbit ◽

Zero Temperature ◽

Interband Pairing ◽

Two Parameters ◽

Spin Orbit Interactions ◽

Parameter Values ◽

Thin Superconducting Films

The effect of spin-orbit (SO) interaction on the formation of the critical states in thin superconducting films in magnetic field oriented along the film is investigated. Hereby, the case of interband pairing is considered. It was found that eight branches exist in the plane of two parameters [Formula: see text] determined by the value of magnetic field and SO interaction. Six modes leads to inhomogeneous states with different values of the impulse [Formula: see text]. Each state is doubly degenerate over direction of impulse [Formula: see text]. The parameter values at critical point are found for all eight branches in explicit form for zero temperature. The optimal two branches are estimated, corresponding to largest critical magnetic field value for given SO interaction.

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Increase of Magnetic Sensitivity of Magnetically Controlled MEMS Switches

MRS Advances ◽

10.1557/adv.2016.395 ◽

2016 ◽

Vol 1 (34) ◽

pp. 2393-2399

Author(s):

Sergey M. Karabanov ◽

Dmitry V. Suvorov ◽

Gennady P. Gololobov ◽

Dmitry Y. Tarabrin ◽

Evgeny V. Slivkin

Keyword(s):

Magnetic Field ◽

Research Results ◽

Mems Switches ◽

Field Concentrator ◽

Magnetic Sensitivity ◽

Sensitivity Increase

ABSTRACTThe paper presents the research results of influence of various parameters of magnetic field concentrator geometry on sensitivity of magnetically controlled MEMS switches. It is shown that magnetic sensitivity increases with the growth of the magnetic concentrator width and practically does not depend on its length. It is established that dependence of magnetic sensitivity on the overlap length of the ferromagnetic flexible contact-concentrator has a minimum corresponding to 2-3 lengths of the contact gap. Recommendations on sensitivity increase of magnetically controlled MEMS switches are provided.

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Effect of magnetic field during deposition on growth of Bi2Sr2Can−1CunOy superconducting films

Physica C Superconductivity ◽

10.1016/j.physc.2005.03.057 ◽

2005 ◽

Vol 426-431 ◽

pp. 1439-1443 ◽

Cited By ~ 3

Author(s):

T. Onishi ◽

N. Fujiwara ◽

S. Kishida

Keyword(s):

Magnetic Field ◽

Superconducting Films

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Bifurcation to vortex solutions in superconducting films

European Journal of Applied Mathematics ◽

10.1017/s0956792596002951 ◽

1997 ◽

Vol 8 (2) ◽

pp. 125-148 ◽

Cited By ~ 4

Author(s):

T. BOECK ◽

S. J. CHAPMAN

Keyword(s):

Magnetic Field ◽

Superconducting Films ◽

Leading Order ◽

Nonlinear Stability Analysis ◽

Slab Geometry ◽

Weakly Nonlinear ◽

Double Eigenvalue ◽

Wide Range ◽

Vortex Solutions ◽

Parameter Values

The bifurcation from a normally conducting state to a superconducting state in a decreasing magnetic field is studied for a slab geometry. The leading eigenvalue is a double eigenvalue, leading to a rich structure of possible behaviours. A weakly-nonlinear stability analysis is performed, and the possible responses of the material are classified. Finally, the leading-order equations are solved numerically for a wide range of parameter values to determine which of these behaviours will occur in practice.

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