Role of interface coupling inhomogeneity in domain evolution in exchange bias
Models of exchange-bias in thin films have been able to describe various aspects of this technologically relevant effect. Through appropriate choices of free parameters the modelled hysteresis loops adequately match experiment, and typical domain structures can be simulated. However, the use of thes...
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creator | Benassi, Andrea Marioni, Miguel A Passerone, Daniele Hug, Hans J |
description | Models of exchange-bias in thin films have been able to describe various aspects of this technologically relevant effect. Through appropriate choices of free parameters the modelled hysteresis loops adequately match experiment, and typical domain structures can be simulated. However, the use of these parameters, notably the coupling strength between the systems' ferromagnetic (F) and antiferromagnetic (AF) layers, obscures conclusions about their influence on the magnetization reversal processes. Here we develop a 2D phase-field model of the magnetization process in exchange-biased CoO/(Co/Pt)xn that incorporates the 10 nm-resolved measured local biasing characteristics of the antiferromagnet. Just three interrelated parameters set to measured physical quantities of the ferromagnet and the measured density of uncompensated spins thus suffice to match the experiment in microscopic and macroscopic detail. We use the model to study changes in bias and coercivity caused by different distributions of pinned uncompensated spins of the antiferromagnet, in application-relevant situations where domain wall motion dominates the ferromagnetic reversal. We show the excess coercivity can arise solely from inhomogeneity in the density of biasing- and anti-biasing pinned uncompensated spins in the antiferromagnet. Counter to conventional wisdom, irreversible processes in the latter are not essential. |
doi_str_mv | 10.48550/arxiv.1404.0317 |
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Through appropriate choices of free parameters the modelled hysteresis loops adequately match experiment, and typical domain structures can be simulated. However, the use of these parameters, notably the coupling strength between the systems' ferromagnetic (F) and antiferromagnetic (AF) layers, obscures conclusions about their influence on the magnetization reversal processes. Here we develop a 2D phase-field model of the magnetization process in exchange-biased CoO/(Co/Pt)xn that incorporates the 10 nm-resolved measured local biasing characteristics of the antiferromagnet. Just three interrelated parameters set to measured physical quantities of the ferromagnet and the measured density of uncompensated spins thus suffice to match the experiment in microscopic and macroscopic detail. We use the model to study changes in bias and coercivity caused by different distributions of pinned uncompensated spins of the antiferromagnet, in application-relevant situations where domain wall motion dominates the ferromagnetic reversal. We show the excess coercivity can arise solely from inhomogeneity in the density of biasing- and anti-biasing pinned uncompensated spins in the antiferromagnet. 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Through appropriate choices of free parameters the modelled hysteresis loops adequately match experiment, and typical domain structures can be simulated. However, the use of these parameters, notably the coupling strength between the systems' ferromagnetic (F) and antiferromagnetic (AF) layers, obscures conclusions about their influence on the magnetization reversal processes. Here we develop a 2D phase-field model of the magnetization process in exchange-biased CoO/(Co/Pt)xn that incorporates the 10 nm-resolved measured local biasing characteristics of the antiferromagnet. Just three interrelated parameters set to measured physical quantities of the ferromagnet and the measured density of uncompensated spins thus suffice to match the experiment in microscopic and macroscopic detail. We use the model to study changes in bias and coercivity caused by different distributions of pinned uncompensated spins of the antiferromagnet, in application-relevant situations where domain wall motion dominates the ferromagnetic reversal. We show the excess coercivity can arise solely from inhomogeneity in the density of biasing- and anti-biasing pinned uncompensated spins in the antiferromagnet. Counter to conventional wisdom, irreversible processes in the latter are not essential.</description><subject>Antiferromagnetism</subject><subject>Bias</subject><subject>Cobalt</subject><subject>Coercivity</subject><subject>Computer simulation</subject><subject>Coupling</subject><subject>Density</subject><subject>Domain walls</subject><subject>Exchanging</subject><subject>Ferromagnetism</subject><subject>Hysteresis loops</subject><subject>Inhomogeneity</subject><subject>Irreversible processes</subject><subject>Magnetization reversal</subject><subject>Mathematical models</subject><subject>Parameters</subject><subject>Physics - Materials Science</subject><subject>Physics - Mesoscale and Nanoscale Physics</subject><subject>Physics - Statistical Mechanics</subject><subject>Platinum</subject><subject>Thin films</subject><subject>Two dimensional models</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj8tqwzAQRUWh0JBm31UxdG1Xj5FlL0voI5BSKNkbWRo5CraV-hGSv6_ddHWZy-Eyh5AHRhPIpKTPujv7U8KAQkIFUzdkwYVgcQac35FV3x8opTxVXEqxIJ_focYouMi3A3ZOG4xMGI-1b6up2ocmVNiiHy7TFdnQ6CnwFOpx8KGdOzybvW4rjEqv-3ty63Td4-o_l2T39rpbf8Tbr_fN-mUba8kgLhUVEnIjHeM0Ta3m2vJSyVKDRJsZziw4m2JpmOUcqABwzjilAHM2QWJJHq-zf6rFsfON7i7FrFzMyhPwdAWOXfgZsR-KQxi7dnqp4DQDykDmIH4B_d1Z1w</recordid><startdate>20140329</startdate><enddate>20140329</enddate><creator>Benassi, Andrea</creator><creator>Marioni, Miguel A</creator><creator>Passerone, Daniele</creator><creator>Hug, Hans J</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20140329</creationdate><title>Role of interface coupling inhomogeneity in domain evolution in exchange bias</title><author>Benassi, Andrea ; 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Through appropriate choices of free parameters the modelled hysteresis loops adequately match experiment, and typical domain structures can be simulated. However, the use of these parameters, notably the coupling strength between the systems' ferromagnetic (F) and antiferromagnetic (AF) layers, obscures conclusions about their influence on the magnetization reversal processes. Here we develop a 2D phase-field model of the magnetization process in exchange-biased CoO/(Co/Pt)xn that incorporates the 10 nm-resolved measured local biasing characteristics of the antiferromagnet. Just three interrelated parameters set to measured physical quantities of the ferromagnet and the measured density of uncompensated spins thus suffice to match the experiment in microscopic and macroscopic detail. We use the model to study changes in bias and coercivity caused by different distributions of pinned uncompensated spins of the antiferromagnet, in application-relevant situations where domain wall motion dominates the ferromagnetic reversal. We show the excess coercivity can arise solely from inhomogeneity in the density of biasing- and anti-biasing pinned uncompensated spins in the antiferromagnet. Counter to conventional wisdom, irreversible processes in the latter are not essential.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1404.0317</doi><oa>free_for_read</oa></addata></record> |
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subjects | Antiferromagnetism Bias Cobalt Coercivity Computer simulation Coupling Density Domain walls Exchanging Ferromagnetism Hysteresis loops Inhomogeneity Irreversible processes Magnetization reversal Mathematical models Parameters Physics - Materials Science Physics - Mesoscale and Nanoscale Physics Physics - Statistical Mechanics Platinum Thin films Two dimensional models |
title | Role of interface coupling inhomogeneity in domain evolution in exchange bias |
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