Picosecond Fresnel transmission electron microscopy
We report the demonstration of picosecond Fresnel imaging with an ultrafast transmission electron microscope (UEM). By operating with a low instrument repetition rate (5 kHz) and without objective-lens excitation, the picosecond demagnetization of an FePt film, via in situ, femtosecond laser excitat...
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Veröffentlicht in: | Applied physics letters 2017-05, Vol.110 (22) |
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creator | Schliep, Karl B. Quarterman, P. Wang, Jian-Ping Flannigan, David J. |
description | We report the demonstration of picosecond Fresnel imaging with an ultrafast transmission electron microscope (UEM). By operating with a low instrument repetition rate (5 kHz) and without objective-lens excitation, the picosecond demagnetization of an FePt film, via in situ, femtosecond laser excitation, is directly imaged. The dynamics are quantified and monitored as a time-dependent change in the degree of electron coherence within the magnetic domain walls. The relative coherence of conventional (thermionic) Fresnel transmission electron microscopy is also directly compared to that of Fresnel UEM through the domain-wall size. Further, the robustness and reversibility of the domain-wall dynamics are illustrated by repeating the picosecond image scans at defocus values having the same magnitude but different signs (e.g., +25 mm vs. −25 mm). Control experiments and approaches to identifying and isolating systematic errors and sources of artifacts are also described. This work, and continued future developments also described here, opens the way to direct correlation of transient structure, morphology, and magnetic dynamics in magnetic thin films and spintronic devices. |
doi_str_mv | 10.1063/1.4984586 |
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By operating with a low instrument repetition rate (5 kHz) and without objective-lens excitation, the picosecond demagnetization of an FePt film, via in situ, femtosecond laser excitation, is directly imaged. The dynamics are quantified and monitored as a time-dependent change in the degree of electron coherence within the magnetic domain walls. The relative coherence of conventional (thermionic) Fresnel transmission electron microscopy is also directly compared to that of Fresnel UEM through the domain-wall size. Further, the robustness and reversibility of the domain-wall dynamics are illustrated by repeating the picosecond image scans at defocus values having the same magnitude but different signs (e.g., +25 mm vs. −25 mm). Control experiments and approaches to identifying and isolating systematic errors and sources of artifacts are also described. This work, and continued future developments also described here, opens the way to direct correlation of transient structure, morphology, and magnetic dynamics in magnetic thin films and spintronic devices.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.4984586</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Coherence ; Demagnetization ; Domain walls ; Electrons ; Excitation ; Magnetic domains ; Morphology ; Systematic errors ; Thin films ; Time dependence ; Transmission electron microscopy</subject><ispartof>Applied physics letters, 2017-05, Vol.110 (22)</ispartof><rights>Author(s)</rights><rights>2017 Author(s). 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By operating with a low instrument repetition rate (5 kHz) and without objective-lens excitation, the picosecond demagnetization of an FePt film, via in situ, femtosecond laser excitation, is directly imaged. The dynamics are quantified and monitored as a time-dependent change in the degree of electron coherence within the magnetic domain walls. The relative coherence of conventional (thermionic) Fresnel transmission electron microscopy is also directly compared to that of Fresnel UEM through the domain-wall size. Further, the robustness and reversibility of the domain-wall dynamics are illustrated by repeating the picosecond image scans at defocus values having the same magnitude but different signs (e.g., +25 mm vs. −25 mm). Control experiments and approaches to identifying and isolating systematic errors and sources of artifacts are also described. This work, and continued future developments also described here, opens the way to direct correlation of transient structure, morphology, and magnetic dynamics in magnetic thin films and spintronic devices.</description><subject>Applied physics</subject><subject>Coherence</subject><subject>Demagnetization</subject><subject>Domain walls</subject><subject>Electrons</subject><subject>Excitation</subject><subject>Magnetic domains</subject><subject>Morphology</subject><subject>Systematic errors</subject><subject>Thin films</subject><subject>Time dependence</subject><subject>Transmission electron microscopy</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNqd0E9LwzAUAPAgCtbpwW9Q8KTQmZfXrMlRhlNhoAc9h_Q1hY6tqUkn7Nub0YF3T-89-PH-MXYLfA58gY8wL7UqpVqcsQx4VRUIoM5ZxjnHYqElXLKrGDeplAIxY_jRkY-OfN_kq-Bi77b5GGwfd12Mne9zt3U0hpTsOgo-kh8O1-yitdvobk5xxr5Wz5_L12L9_vK2fFoXhBrHQgGgbuq6UUhSagQibRtsBdRoK8ubUjtZC05SVCQBSECluJKlTYlsOc7Y3dR3CP577-JoNn4f-jTSCBBlqWXiSd1P6rheDK41Q-h2NhwMcHP8iQFz-kmyD5ON1I12TPf9D__48AfN0LT4C0Ewbn8</recordid><startdate>20170529</startdate><enddate>20170529</enddate><creator>Schliep, Karl B.</creator><creator>Quarterman, P.</creator><creator>Wang, Jian-Ping</creator><creator>Flannigan, David J.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20170529</creationdate><title>Picosecond Fresnel transmission electron microscopy</title><author>Schliep, Karl B. ; Quarterman, P. ; Wang, Jian-Ping ; Flannigan, David J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c393t-81139dbbd83c55931cc9ad3f21b3a7a0d49e5b20c527c511c21780854a2175f03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Applied physics</topic><topic>Coherence</topic><topic>Demagnetization</topic><topic>Domain walls</topic><topic>Electrons</topic><topic>Excitation</topic><topic>Magnetic domains</topic><topic>Morphology</topic><topic>Systematic errors</topic><topic>Thin films</topic><topic>Time dependence</topic><topic>Transmission electron microscopy</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Schliep, Karl B.</creatorcontrib><creatorcontrib>Quarterman, P.</creatorcontrib><creatorcontrib>Wang, Jian-Ping</creatorcontrib><creatorcontrib>Flannigan, David J.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schliep, Karl B.</au><au>Quarterman, P.</au><au>Wang, Jian-Ping</au><au>Flannigan, David J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Picosecond Fresnel transmission electron microscopy</atitle><jtitle>Applied physics letters</jtitle><date>2017-05-29</date><risdate>2017</risdate><volume>110</volume><issue>22</issue><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>We report the demonstration of picosecond Fresnel imaging with an ultrafast transmission electron microscope (UEM). By operating with a low instrument repetition rate (5 kHz) and without objective-lens excitation, the picosecond demagnetization of an FePt film, via in situ, femtosecond laser excitation, is directly imaged. The dynamics are quantified and monitored as a time-dependent change in the degree of electron coherence within the magnetic domain walls. The relative coherence of conventional (thermionic) Fresnel transmission electron microscopy is also directly compared to that of Fresnel UEM through the domain-wall size. Further, the robustness and reversibility of the domain-wall dynamics are illustrated by repeating the picosecond image scans at defocus values having the same magnitude but different signs (e.g., +25 mm vs. −25 mm). Control experiments and approaches to identifying and isolating systematic errors and sources of artifacts are also described. This work, and continued future developments also described here, opens the way to direct correlation of transient structure, morphology, and magnetic dynamics in magnetic thin films and spintronic devices.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4984586</doi><tpages>5</tpages></addata></record> |
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subjects | Applied physics Coherence Demagnetization Domain walls Electrons Excitation Magnetic domains Morphology Systematic errors Thin films Time dependence Transmission electron microscopy |
title | Picosecond Fresnel transmission electron microscopy |
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