Magnetic Molecular Materials 1991
DOI: 10.1007/978-94-011-3254-1_24
|View full text |Cite
|
Sign up to set email alerts
|

Frequency Dependent Susceptibilities of Magnetic Materials

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2001
2001
2001
2001

Publication Types

Select...
1

Relationship

0
1

Authors

Journals

citations
Cited by 1 publication
(1 citation statement)
references
References 7 publications
0
1
0
Order By: Relevance
“…21 Thus, the M ′′ versus T plots at different frequencies provide 1/τ versus T data, and a kinetic analysis can be performed using the Arrhenius relationship (eq 5). This is the characteristic behavior of a thermally activated Orbach process, 23 where U eff is the effective anisotropy energy barrier, k is the Boltzmann constant, and 1/τ 0 is the pre-exponential term. Plots of ln(1/τ) versus 1/T for 5 and 6 using M ′′ versus T data are shown in Figures 8 and 9, respectively, with the least-squares fit to eq 4 shown as a solid line.…”
Section: Description Of Structuresmentioning
confidence: 99%
“…21 Thus, the M ′′ versus T plots at different frequencies provide 1/τ versus T data, and a kinetic analysis can be performed using the Arrhenius relationship (eq 5). This is the characteristic behavior of a thermally activated Orbach process, 23 where U eff is the effective anisotropy energy barrier, k is the Boltzmann constant, and 1/τ 0 is the pre-exponential term. Plots of ln(1/τ) versus 1/T for 5 and 6 using M ′′ versus T data are shown in Figures 8 and 9, respectively, with the least-squares fit to eq 4 shown as a solid line.…”
Section: Description Of Structuresmentioning
confidence: 99%