1981
DOI: 10.1063/1.328899
|View full text |Cite
|
Sign up to set email alerts
|

Enhancement of uniaxial anisotropy constant by introducing oxygen vacancies in Ca-doped YIG

Abstract: Ca-doped YIG films having composition Y3−x3+ Cax2+ Fe3+5−x Fex4+ O1 2 have been grown with a value of x = 0.25 and thickness 1.15 μm. Upon annealing in saturated FeCl2 solution, oxygen vacancies are introduced, which compensate for Ca2+ ions and reduce Fe4+ ions to Fe3+ ions. The uniaxial anisotropy constant changed from −5.89×103 erg/cm3 to −17.0×103 erg/cm3, which is consistent with a change in the crystal field effects reduction as proposed by Stacy and Rooymans. The exchange stiffness coefficient changed f… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

1982
1982
2013
2013

Publication Types

Select...
4
3

Relationship

0
7

Authors

Journals

citations
Cited by 14 publications
(2 citation statements)
references
References 8 publications
0
2
0
Order By: Relevance
“…The FMR measurements were performed in single crystals of silicon-iron, nickel-iron, nickel and hcp cobalt , thin films (Knorr, 1959;Davis, 1965;Hsia, 1981;Krebs, 1982;Maksymowich, 1983Maksymowich, , 1985Maksymowich, , 1992Platow, 1998;Durusoy, 2000;Baek, 2002;Kuanr, 2004), CoCr magnetic thin films (Cofield, 1987), NiFe/FeMn thin films (Layadi, 1988), single-crystal Fe/Cr/Fe(100) sandwiches (Krebs, 1989), polycrystalline single films (Hathaway, 1981;Rezende, 1993) and ultrathin multilayers of the system Au/Fe/Au/Pd/Fe (001) prepared on GaAs(001) (Woltersdorf, 2004). The FMR techniques have been succesfully applied peak-topeak linewidth (Yeh, 2009;, superconducting and ferromagnetic coupled structures (Richard, 2012) and thin Co films of 50 nm thick (Maklakov, 2012).…”
Section: Introductionmentioning
confidence: 99%
“…The FMR measurements were performed in single crystals of silicon-iron, nickel-iron, nickel and hcp cobalt , thin films (Knorr, 1959;Davis, 1965;Hsia, 1981;Krebs, 1982;Maksymowich, 1983Maksymowich, , 1985Maksymowich, , 1992Platow, 1998;Durusoy, 2000;Baek, 2002;Kuanr, 2004), CoCr magnetic thin films (Cofield, 1987), NiFe/FeMn thin films (Layadi, 1988), single-crystal Fe/Cr/Fe(100) sandwiches (Krebs, 1989), polycrystalline single films (Hathaway, 1981;Rezende, 1993) and ultrathin multilayers of the system Au/Fe/Au/Pd/Fe (001) prepared on GaAs(001) (Woltersdorf, 2004). The FMR techniques have been succesfully applied peak-topeak linewidth (Yeh, 2009;, superconducting and ferromagnetic coupled structures (Richard, 2012) and thin Co films of 50 nm thick (Maklakov, 2012).…”
Section: Introductionmentioning
confidence: 99%
“…The FMR measurements were performed in single crystals of silicon-iron, nickel-iron, nickel and hcp cobalt (Frait, 1965), thin films (Knorr, 1959;Davis, 1965;Hsia, 1981;Krebs, 1982;Maksymowich, 1983Maksymowich, , 1985Maksymowich, , 1992Platow, 1998;Durusoy, 2000;Baek, 2002;Kuanr, 2004), CoCr magnetic thin films (Cofield, 1987), NiFe/FeMn thin films (Layadi, 1988), single-crystal Fe/Cr/Fe(100) sandwiches (Krebs, 1989), polycrystalline single films (Hathaway, 1981;Rezende, 1993) and ultrathin multilayers of the system Au/Fe/Au/Pd/Fe (001) prepared on GaAs(001) (Woltersdorf, 2004). The FMR techniques have been succesfully applied peak-topeak linewidth (Yeh, 2009;, superconducting and ferromagnetic coupled structures (Richard, 2012) and thin Co films of 50 nm thick (Maklakov, 2012).…”
Section: Introductionmentioning
confidence: 99%