Resonant dislocation motion in NaCl crystals in the EPR scheme in the Earth’s magnetic field with pulsed pumping

Resonant dislocation motions in NaCl(Ca) crystals under the simultaneous action of the Earth’s magnetic field B Earth (∼66 μT) and a pulsed pump field of sufficient amplitude and certain duration τ have been detected and studied. The measured dislocation path peaks l (τ) have a maximum at τ = τ r ≈...

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Veröffentlicht in:Physics of the solid state 2013-11, Vol.55 (11), p.2289-2296
Hauptverfasser: Alshits, V. I., Darinskaya, E. V., Morozov, V. A., Kats, V. M., Lukin, A. A.
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container_issue 11
container_start_page 2289
container_title Physics of the solid state
container_volume 55
creator Alshits, V. I.
Darinskaya, E. V.
Morozov, V. A.
Kats, V. M.
Lukin, A. A.
description Resonant dislocation motions in NaCl(Ca) crystals under the simultaneous action of the Earth’s magnetic field B Earth (∼66 μT) and a pulsed pump field of sufficient amplitude and certain duration τ have been detected and studied. The measured dislocation path peaks l (τ) have a maximum at τ = τ r ≈ 0.53 μs. The resonance criterion has been found to be the ordinary EPR condition in which the g -factor is close to 2 and the optimum inverse pulse duration τ r −1 is used instead of the harmonic pump field frequency ν r . The largest peak l (τ) height is reached at mutually orthogonal dislocation ( L ) and magnetic field ( B Earth and ) orientations. Pulsed field rotation to the position ‖ B Earth significantly decreases but does not “kill” the effect. For dislocations parallel to the Earth’s field ( L ‖ B Earth ), the resonance almost disappears even at ⊥ B Earth . In the optimum geometry of experiments, as the pump field amplitude decreases from 17.6 to 10 μT, the path peak height l r = l (τ r ) decreases only by 7.5%, remaining at the level of l r ∼ 10 2 μm, and at a further fall-off to 4 μT, it rapidly decreases to background values. In this case, the relative density of mobile dislocations similarly decreases from ∼90 to 40%. Possible physical mechanisms of the observed effect have been discussed.
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For dislocations parallel to the Earth’s field ( L ‖ B Earth ), the resonance almost disappears even at ⊥ B Earth . In the optimum geometry of experiments, as the pump field amplitude decreases from 17.6 to 10 μT, the path peak height l r = l (τ r ) decreases only by 7.5%, remaining at the level of l r ∼ 10 2 μm, and at a further fall-off to 4 μT, it rapidly decreases to background values. In this case, the relative density of mobile dislocations similarly decreases from ∼90 to 40%. 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subjects Magnetic fields
Mechanical Properties
Physics
Physics and Astronomy
Physics of Strength
Plasticity
Solid State Physics
title Resonant dislocation motion in NaCl crystals in the EPR scheme in the Earth’s magnetic field with pulsed pumping
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