Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference

Street, R. ; Brown, S. D.

[S.l.] : American Institute of Physics (AIP)
Published 1994
ISSN:
1089-7550
Source:
AIP Digital Archive
Topics:
Physics
Notes:
Time dependence of magnetization in ferromagnetic materials was first described towards the end of the 19th century. Subsequently, two types of mechanisms responsible for time dependent behavior were identified and became known as "diffusion'' and "fluctuation'' after-effect or viscosity. The former depends on thermally induced motion of impurity atoms. The latter is a consequence of thermal activation of irreversible domain processes such as domain-wall motion and the nucleation of domains of reverse magnetization. Fluctuation viscosity affects, to a greater or smaller extent, all magnetic materials subject to hysteresis. In the late 1940s descriptions of magnetic viscosity in terms of fluctuation fields (Néel) and activation energy distributions (Street and Woolley) were developed. The two approaches will be described. An analysis of the time dependent phenomena exhibited by magneto-optical films will be presented as a simple example of the application of activation energy modeling.
Type of Medium:
Electronic Resource
URL:
_version_ 1798289652109541376
autor Street, R.
Brown, S. D.
autorsonst Street, R.
Brown, S. D.
book_url http://dx.doi.org/10.1063/1.358275
datenlieferant nat_lic_papers
hauptsatz hsatz_simple
identnr NLZ218556985
iqvoc_descriptor_title iqvoc_00000092:materials
issn 1089-7550
journal_name Journal of Applied Physics
materialart 1
notes Time dependence of magnetization in ferromagnetic materials was first described towards the end of the 19th century. Subsequently, two types of mechanisms responsible for time dependent behavior were identified and became known as "diffusion'' and "fluctuation'' after-effect or viscosity. The former depends on thermally induced motion of impurity atoms. The latter is a consequence of thermal activation of irreversible domain processes such as domain-wall motion and the nucleation of domains of reverse magnetization. Fluctuation viscosity affects, to a greater or smaller extent, all magnetic materials subject to hysteresis. In the late 1940s descriptions of magnetic viscosity in terms of fluctuation fields (Néel) and activation energy distributions (Street and Woolley) were developed. The two approaches will be described. An analysis of the time dependent phenomena exhibited by magneto-optical films will be presented as a simple example of the application of activation energy modeling.
package_name American Institute of Physics (AIP)
publikationsjahr_anzeige 1994
publikationsjahr_facette 1994
publikationsjahr_intervall 8009:1990-1994
publikationsjahr_sort 1994
publikationsort [S.l.]
publisher American Institute of Physics (AIP)
reference 76 (1994), S. 6386-6390
search_space articles
shingle_author_1 Street, R.
Brown, S. D.
shingle_author_2 Street, R.
Brown, S. D.
shingle_author_3 Street, R.
Brown, S. D.
shingle_author_4 Street, R.
Brown, S. D.
shingle_catch_all_1 Street, R.
Brown, S. D.
Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
Time dependence of magnetization in ferromagnetic materials was first described towards the end of the 19th century. Subsequently, two types of mechanisms responsible for time dependent behavior were identified and became known as "diffusion'' and "fluctuation'' after-effect or viscosity. The former depends on thermally induced motion of impurity atoms. The latter is a consequence of thermal activation of irreversible domain processes such as domain-wall motion and the nucleation of domains of reverse magnetization. Fluctuation viscosity affects, to a greater or smaller extent, all magnetic materials subject to hysteresis. In the late 1940s descriptions of magnetic viscosity in terms of fluctuation fields (Néel) and activation energy distributions (Street and Woolley) were developed. The two approaches will be described. An analysis of the time dependent phenomena exhibited by magneto-optical films will be presented as a simple example of the application of activation energy modeling.
1089-7550
10897550
American Institute of Physics (AIP)
shingle_catch_all_2 Street, R.
Brown, S. D.
Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
Time dependence of magnetization in ferromagnetic materials was first described towards the end of the 19th century. Subsequently, two types of mechanisms responsible for time dependent behavior were identified and became known as "diffusion'' and "fluctuation'' after-effect or viscosity. The former depends on thermally induced motion of impurity atoms. The latter is a consequence of thermal activation of irreversible domain processes such as domain-wall motion and the nucleation of domains of reverse magnetization. Fluctuation viscosity affects, to a greater or smaller extent, all magnetic materials subject to hysteresis. In the late 1940s descriptions of magnetic viscosity in terms of fluctuation fields (Néel) and activation energy distributions (Street and Woolley) were developed. The two approaches will be described. An analysis of the time dependent phenomena exhibited by magneto-optical films will be presented as a simple example of the application of activation energy modeling.
1089-7550
10897550
American Institute of Physics (AIP)
shingle_catch_all_3 Street, R.
Brown, S. D.
Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
Time dependence of magnetization in ferromagnetic materials was first described towards the end of the 19th century. Subsequently, two types of mechanisms responsible for time dependent behavior were identified and became known as "diffusion'' and "fluctuation'' after-effect or viscosity. The former depends on thermally induced motion of impurity atoms. The latter is a consequence of thermal activation of irreversible domain processes such as domain-wall motion and the nucleation of domains of reverse magnetization. Fluctuation viscosity affects, to a greater or smaller extent, all magnetic materials subject to hysteresis. In the late 1940s descriptions of magnetic viscosity in terms of fluctuation fields (Néel) and activation energy distributions (Street and Woolley) were developed. The two approaches will be described. An analysis of the time dependent phenomena exhibited by magneto-optical films will be presented as a simple example of the application of activation energy modeling.
1089-7550
10897550
American Institute of Physics (AIP)
shingle_catch_all_4 Street, R.
Brown, S. D.
Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
Time dependence of magnetization in ferromagnetic materials was first described towards the end of the 19th century. Subsequently, two types of mechanisms responsible for time dependent behavior were identified and became known as "diffusion'' and "fluctuation'' after-effect or viscosity. The former depends on thermally induced motion of impurity atoms. The latter is a consequence of thermal activation of irreversible domain processes such as domain-wall motion and the nucleation of domains of reverse magnetization. Fluctuation viscosity affects, to a greater or smaller extent, all magnetic materials subject to hysteresis. In the late 1940s descriptions of magnetic viscosity in terms of fluctuation fields (Néel) and activation energy distributions (Street and Woolley) were developed. The two approaches will be described. An analysis of the time dependent phenomena exhibited by magneto-optical films will be presented as a simple example of the application of activation energy modeling.
1089-7550
10897550
American Institute of Physics (AIP)
shingle_title_1 Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
shingle_title_2 Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
shingle_title_3 Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
shingle_title_4 Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
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source_archive AIP Digital Archive
timestamp 2024-05-06T08:04:14.201Z
titel Magnetic viscosity, fluctuation fields, and activation energies (invited) : The 6th joint magnetism and magnetic materials (MMM)−intermag conference
titel_suche Magnetic viscosity, fluctuation fields, and activation energies (invited)
The 6th joint magnetism and magnetic materials (MMM)−intermag conference
topic U
uid nat_lic_papers_NLZ218556985