A Green's function formalism is used to calculate the spectrum of
localized states associated with an interstitial magnetic impurity in a
semi-infinite ferromagnet described by the transverse Ising model. The
nonresonant and resonant excitations of the system due to the impurity
(i.e. the defect modes outside and inside, respectively, the region of
the bulk and surface spin waves (SW)) are calculated numerically for the
high-temperature phase. Two situations are analyzed, depending on the
position of the interstitial impurity: the impurity is in the surface (N = 1) and the impurity is in the bulk region (N > 2).
%0 Journal Article
%1 WOS:000400271700007
%A Freire, M M
%A Filho, Raimundo N Costa
%A Leite, R V
%C 5 TOH TUCK LINK, SINGAPORE 596224, SINGAPORE
%D 2017
%I WORLD SCIENTIFIC PUBL CO PTE LTD
%J INTERNATIONAL JOURNAL OF MODERN PHYSICS C
%K Ising ferromagnets; function; impurity magnets; model-transverse; nodes} spin {Green's
%N 4
%R 10.1142/S0129183117500498
%T Green's functions theory for an interstitial magnetic impurity in a
transverse Ising ferromagnet
%V 28
%X A Green's function formalism is used to calculate the spectrum of
localized states associated with an interstitial magnetic impurity in a
semi-infinite ferromagnet described by the transverse Ising model. The
nonresonant and resonant excitations of the system due to the impurity
(i.e. the defect modes outside and inside, respectively, the region of
the bulk and surface spin waves (SW)) are calculated numerically for the
high-temperature phase. Two situations are analyzed, depending on the
position of the interstitial impurity: the impurity is in the surface (N = 1) and the impurity is in the bulk region (N > 2).
@article{WOS:000400271700007,
abstract = {A Green's function formalism is used to calculate the spectrum of
localized states associated with an interstitial magnetic impurity in a
semi-infinite ferromagnet described by the transverse Ising model. The
nonresonant and resonant excitations of the system due to the impurity
(i.e. the defect modes outside and inside, respectively, the region of
the bulk and surface spin waves (SW)) are calculated numerically for the
high-temperature phase. Two situations are analyzed, depending on the
position of the interstitial impurity: the impurity is in the surface (N = 1) and the impurity is in the bulk region (N > 2).},
added-at = {2022-05-23T20:00:14.000+0200},
address = {5 TOH TUCK LINK, SINGAPORE 596224, SINGAPORE},
author = {Freire, M M and Filho, Raimundo N Costa and Leite, R V},
biburl = {https://www.bibsonomy.org/bibtex/28b6591c242c24d1f935ec6b8edc8f2c8/ppgfis_ufc_br},
doi = {10.1142/S0129183117500498},
interhash = {3d3e8b41fc2f36bb6931938ee9db5eac},
intrahash = {8b6591c242c24d1f935ec6b8edc8f2c8},
issn = {0129-1831},
journal = {INTERNATIONAL JOURNAL OF MODERN PHYSICS C},
keywords = {Ising ferromagnets; function; impurity magnets; model-transverse; nodes} spin {Green's},
number = 4,
publisher = {WORLD SCIENTIFIC PUBL CO PTE LTD},
pubstate = {published},
timestamp = {2022-05-23T20:00:14.000+0200},
title = {Green's functions theory for an interstitial magnetic impurity in a
transverse Ising ferromagnet},
tppubtype = {article},
volume = 28,
year = 2017
}