TY - JOUR
T1 - Electrical transport properties and small polarons in Eu1-xCaxB6
AU - Rhyee, Jong Soo
AU - Cho, B. K.
AU - Ri, H. C.
PY - 2003/3
Y1 - 2003/3
N2 - Temperature- and field-dependent resistivity ρ(T,H) and Hall effect measurements have been carried out for the Eu1-xCaxB6 (x=0.2, 0.4, 0.6, and 0.9) compounds. The replacement of Eu with Ca invoked drastic changes in the ρ(T) although Ca and Eu are isoelectronic. While Eu0.8Ca0.2B6 showed a phase transition similar to that of pure EuB6, the ρ(T) of Eu1-xCaxB6 with x = 0.4 and 0.6 showed a rapid increase at low temperatures (T ≤ 10 K). The upturn of the ρ(T) was suppressed as the magnetic field increased, resulting in negative magnetoresistance (MR). For Eu0.1Ca0.9B6, the MR changed from positive at 10 K ≤ T ≤ 50 K to negative at T≊2 K. It was found that the observed exotic ρ(T) is due to the change of the effective carrier density neff and Hall mobility μH determined from the Hall measurements. Analysis of the Hall mobility based on a small polaronic model showed that the carrier transport is dominated by hopping between the polaron sites in a nonadiabatic regime with four-site hopping for the Eu-rich side and three-site hopping for the Eu-poor side of the compounds. This polaronic scenario of the transport is consistent with the observed ρ(T,H), MR(T), neff(T,H), and μH(T) variation.
AB - Temperature- and field-dependent resistivity ρ(T,H) and Hall effect measurements have been carried out for the Eu1-xCaxB6 (x=0.2, 0.4, 0.6, and 0.9) compounds. The replacement of Eu with Ca invoked drastic changes in the ρ(T) although Ca and Eu are isoelectronic. While Eu0.8Ca0.2B6 showed a phase transition similar to that of pure EuB6, the ρ(T) of Eu1-xCaxB6 with x = 0.4 and 0.6 showed a rapid increase at low temperatures (T ≤ 10 K). The upturn of the ρ(T) was suppressed as the magnetic field increased, resulting in negative magnetoresistance (MR). For Eu0.1Ca0.9B6, the MR changed from positive at 10 K ≤ T ≤ 50 K to negative at T≊2 K. It was found that the observed exotic ρ(T) is due to the change of the effective carrier density neff and Hall mobility μH determined from the Hall measurements. Analysis of the Hall mobility based on a small polaronic model showed that the carrier transport is dominated by hopping between the polaron sites in a nonadiabatic regime with four-site hopping for the Eu-rich side and three-site hopping for the Eu-poor side of the compounds. This polaronic scenario of the transport is consistent with the observed ρ(T,H), MR(T), neff(T,H), and μH(T) variation.
UR - http://www.scopus.com/inward/record.url?scp=0037544311&partnerID=8YFLogxK
M3 - Article
AN - SCOPUS:0037544311
SN - 0163-1829
VL - 67
SP - 1251021
EP - 1251028
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 12
M1 - 125102
ER -