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 |
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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. |
doi_str_mv | 10.1134/S1063783413110024 |
format | Article |
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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.</description><identifier>ISSN: 1063-7834</identifier><identifier>EISSN: 1090-6460</identifier><identifier>DOI: 10.1134/S1063783413110024</identifier><language>eng</language><publisher>Boston: Springer US</publisher><subject>Magnetic fields ; Mechanical Properties ; Physics ; Physics and Astronomy ; Physics of Strength ; Plasticity ; Solid State Physics</subject><ispartof>Physics of the solid state, 2013-11, Vol.55 (11), p.2289-2296</ispartof><rights>Pleiades Publishing, Ltd. 2013</rights><rights>COPYRIGHT 2013 Springer</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c409t-57d2444401367ac66b3de60e19f91e86f4034b3d2ecbacc83a27718fc2fe2df03</citedby><cites>FETCH-LOGICAL-c409t-57d2444401367ac66b3de60e19f91e86f4034b3d2ecbacc83a27718fc2fe2df03</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1134/S1063783413110024$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1134/S1063783413110024$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27915,27916,41479,42548,51310</link.rule.ids></links><search><creatorcontrib>Alshits, V. I.</creatorcontrib><creatorcontrib>Darinskaya, E. V.</creatorcontrib><creatorcontrib>Morozov, V. A.</creatorcontrib><creatorcontrib>Kats, V. M.</creatorcontrib><creatorcontrib>Lukin, A. A.</creatorcontrib><title>Resonant dislocation motion in NaCl crystals in the EPR scheme in the Earth’s magnetic field with pulsed pumping</title><title>Physics of the solid state</title><addtitle>Phys. Solid State</addtitle><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.</description><subject>Magnetic fields</subject><subject>Mechanical Properties</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Physics of Strength</subject><subject>Plasticity</subject><subject>Solid State Physics</subject><issn>1063-7834</issn><issn>1090-6460</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNp9kU1OwzAQhSMEEuXnAOy8ZRHwxK6TLKuq_EgIUIF15Drj1FXiVLYr6I5rcD1OgksRUoWEZ_FGz--bxUySnAG9AGD88gmoYHnBODAASjO-lwyAljQVXND9TS9Yuvk_TI68X1AKAMNykLgp-t5KG0htfNsrGUxvSdd_i7HkXo5botzaB9n6jRHmSCaPU-LVHDv8daQL88_3D0862VgMRhFtsK3Jqwlzsly1Huso3dLY5iQ50HEYnv7ocfJyNXke36R3D9e349FdqjgtQzrM64zHR4GJXCohZqxGQRFKXQIWQnPKePQyVDOpVMFkludQaJVpzGpN2XFysZ3byBYrY3UfnFSxauyM6i1qE_0RG2a8KMqcR-B8B4iZgG-hkSvvq9un6W4Wtlnleu8d6mrpTCfdugJabS5S_blIZLIt42PWNuiqRb9yNu7gH-gLL5eN4w</recordid><startdate>20131101</startdate><enddate>20131101</enddate><creator>Alshits, V. I.</creator><creator>Darinskaya, E. V.</creator><creator>Morozov, V. A.</creator><creator>Kats, V. M.</creator><creator>Lukin, A. A.</creator><general>Springer US</general><general>Springer</general><scope>AAYXX</scope><scope>CITATION</scope><scope>ISR</scope></search><sort><creationdate>20131101</creationdate><title>Resonant dislocation motion in NaCl crystals in the EPR scheme in the Earth’s magnetic field with pulsed pumping</title><author>Alshits, V. I. ; Darinskaya, E. V. ; Morozov, V. A. ; Kats, V. M. ; Lukin, A. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c409t-57d2444401367ac66b3de60e19f91e86f4034b3d2ecbacc83a27718fc2fe2df03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Magnetic fields</topic><topic>Mechanical Properties</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Physics of Strength</topic><topic>Plasticity</topic><topic>Solid State Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Alshits, V. I.</creatorcontrib><creatorcontrib>Darinskaya, E. V.</creatorcontrib><creatorcontrib>Morozov, V. A.</creatorcontrib><creatorcontrib>Kats, V. M.</creatorcontrib><creatorcontrib>Lukin, A. A.</creatorcontrib><collection>CrossRef</collection><collection>Gale In Context: Science</collection><jtitle>Physics of the solid state</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Alshits, V. I.</au><au>Darinskaya, E. V.</au><au>Morozov, V. A.</au><au>Kats, V. M.</au><au>Lukin, A. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Resonant dislocation motion in NaCl crystals in the EPR scheme in the Earth’s magnetic field with pulsed pumping</atitle><jtitle>Physics of the solid state</jtitle><stitle>Phys. Solid State</stitle><date>2013-11-01</date><risdate>2013</risdate><volume>55</volume><issue>11</issue><spage>2289</spage><epage>2296</epage><pages>2289-2296</pages><issn>1063-7834</issn><eissn>1090-6460</eissn><abstract>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.</abstract><cop>Boston</cop><pub>Springer US</pub><doi>10.1134/S1063783413110024</doi><tpages>8</tpages></addata></record> |
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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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