L. Žurauskaitė
, S. Balevičius
, S. Keršulis
, V. Stankevič
Č. Šimkevičius
, J. Novickij
The long-term stability of
electrical
resistance
and magnetoresistance in nanostructured La1-xSrxMnO3
(x = 0.17) manganite
thin
films grown on lucalox (Al2O3 + MgO)
substrate by
the MOCVD
method was investigated. It was found that the storage of up to
3
months
of the free surfaces of these films in normal atmosphere (air)
conditions
increases their resistivity by almost two times, while the
annealing of
the
films in an Ar atmosphere at 450 °C decreases their resistivity
only by
15%.
It was concluded that the final increase of resistivity is
determined
by
a long-term relaxation of the grain boundaries in the
nanostructured
films.
The magnetoresistance of the films does not change
significantly, which
produces
an advantage for magnetic field sensor applications. The passive
protective
coating of the free surfaces of the films stabilizes their
electrical
and
magnetic properties. The results were analysed using various
electron
scattering mechanisms when the films were in a ferromagnetic
state, and
the Mott’s variable
range hopping model when they were in a paramagnetic insulating
state.
Siekiant panaudoti manganitų
sluoksnius
įvairių prietaisų kūrimui, labai svarbu, kad jų parametrai ilgą
laiką
išliktų
stabilūs. Ištirta senėjimo įtaka nanostruktūrizuotų La1-xSrxMnO3
(x = 0,17) sluoksnių,
užaugintų MOCVD metodu ant polikoro (Al2O3
+ MgO)
padėklo, savitajai
varžai ir magnetovaržai. Nustatyta, kad sluoksniui esant (keletą
mėn.)
normalioje
atmosferoje (ore), beveik du kartus padidėja jo varža (kaitinant
420 °C
temperatūroje),
o atmosferoje ji sumažėja 15 %. Padaryta išvada, kad sluoksnio
savitosios
varžos ilgalaikius pokyčius lemia tarpkristalitinių sričių
relaksacija,
todėl
atsiranda papildomi defektai ir vakansijos. Sluoksnių
magnetovarža
mažai
pakinta. Pasyvuojanti paviršių medžiaga stabilizuoja sluoksnių
elektrines
ir magnetines savybes. Gauti rezultatai išanalizuoti panaudojant
įvairius elektronų sklaidos aprašymus, esant sluoksniui
feromagnetinėje
būsenoje bei
Mott’o šuolinio laidumo modeliui paramagnetinėje būsenoje.
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