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image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao phys stat sol (a)arrow_drop_down
image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao
phys stat sol (a)
Article . 1973 . Peer-reviewed
License: Wiley TDM
Data sources: Crossref
https://doi.org/10.1515/978311...
Part of book or chapter of book . 1973 . Peer-reviewed
Data sources: Crossref
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The elastic constants of MnAs

Authors: M. Dörfler; K. Bärner;

The elastic constants of MnAs

Abstract

The tensor of elastic constants of MnAs in the ferromagnetic and paramagnetic states is evaluated from bending vibrations of straight and helical MnAs whiskers. The isotropic compressibility, predicted by the Bean-Rodbell model to be 4.6 × 10−12 dyn−1 cm2 and the same in both phases, is found experimentally to be (4.3 ± 1.0) × 10−12 dyn−1 cm2 in the paramagnetic state, changing by −0.6 × 10−12 dyn−1 cm2 at the first order phase transition. However, the data in the ferromagnetic state include magnetostrictive effects. Observation of the ΔE-effect shows that the magnetostriction softens the lattice appreciably and tends to minimize the difference in elastic constants between the two states. Die elastischen Konstanten des MnAs werden aus den Eigenfrequenzen der Biegeschwingungen von geraden und schraubenformigen Whiskern ermittelt. Die isotrope Kompressibilitat, die sich aus dem Bean-Rodbell-Modell in beiden Phasen zu 4,6 × X 10−12 dyn−1 cm2 berechnet, ergibt sich experimentell zu (4,3 ± 1,0) × 10−12 dyn−1 cm2 im paramagnetischen Zustand und andert sich um −0,6 × 10−12 dyn−1 cm2 beim Ubergang in den ferromagnetischen Zustand. Die Messungen an der ferromagnetischen Phase enthalten jedoch noch die zusatzlichen magnetostriktiven Dehnungen des Gitters. Aus Beobachtungen des ΔE-Effekts folgt, das die Magnetostriktion das Material gerade um soviel weicher macht, das der Unterschied in den elastischen Konstanten der Phasen nahezu verschwindet.

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selected citations
These citations are derived from selected sources.
This is an alternative to the "Influence" indicator, which also reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Citations provided by BIP!
popularity
This indicator reflects the "current" impact/attention (the "hype") of an article in the research community at large, based on the underlying citation network.
BIP!Popularity provided by BIP!
influence
This indicator reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Influence provided by BIP!
impulse
This indicator reflects the initial momentum of an article directly after its publication, based on the underlying citation network.
BIP!Impulse provided by BIP!
45
Average
Top 10%
Average
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