1983
DOI: 10.1002/pssa.2210760112
|View full text |Cite
|
Sign up to set email alerts
|

The magnetic contribution to specific heat in thin ferromagnetic films

Abstract: The magnetic contribution to the specific heat of thin ferromagnetic films is discussed. The numerical calculations made for the special case of S.C. crystallographic lattice and 8 = 112 reveal that the specific heat is larger in thin films than in bulk materials in contrary to the behaviour of another properties, e.g. magnetization or electrical resistivity.Der magnetische Beitrag zur spezifischen Wlrme dunner ferromagnetischer Schichten wird diskutiert. Numerische Rechnungen fiir den Spezialfall des simplen … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
5
0

Year Published

1989
1989
2012
2012

Publication Types

Select...
5

Relationship

1
4

Authors

Journals

citations
Cited by 5 publications
(5 citation statements)
references
References 3 publications
0
5
0
Order By: Relevance
“…We now introduce the k-space which is usually considered in the case of the thin film geometry [22]. We assume the usual notation, k for 3D systems and h for 2D subsystems so that k = (τ, h) where τ labels the subsystems.…”
Section: The Basic Concept Of the Reaction Field Approachmentioning
confidence: 99%
See 3 more Smart Citations
“…We now introduce the k-space which is usually considered in the case of the thin film geometry [22]. We assume the usual notation, k for 3D systems and h for 2D subsystems so that k = (τ, h) where τ labels the subsystems.…”
Section: The Basic Concept Of the Reaction Field Approachmentioning
confidence: 99%
“…The details of T α ν j τ h transformation are discussed in [22]. Now, we present the detailed calculations leading to the expressions for λ and other quantities which are necessary to describe our system.…”
Section: The Basic Concept Of the Reaction Field Approachmentioning
confidence: 99%
See 2 more Smart Citations
“…It can be noted that in the case of S = 112 (6) can be written in the simple form [15] tgh[ (3/P)1/2 sin a ] ' -2 for T < T,(n, c ) and G = 112 for T > T,(n, c ) .…”
Section: Spin Autocorrelation Timementioning
confidence: 98%