TY - JOUR
T1 - Thermoelectric power anomaly of PrTi2Al20 and PrV2Al20 with non-kramers Γ3 ground state
AU - Kuwai, Tomohiko
AU - Funane, Mayumi
AU - Tada, Kouhei
AU - Mizushima, Toshio
AU - Isikawa, Yosikazu
PY - 2013/7
Y1 - 2013/7
N2 - We investigated thermoelectric properties for PrTi2Al20 and PrV 2Al20 below room temperature down to 0.13 K. A clear positive peak has been observed at 75K in the thermoelectric power S for PrTi2Al20. Also for PrV2Al20, the similar S peak has been detected at 40 K. These peaks arise from the Kondo effect in the magnetic excited levels of the 4f -electronic state under a cubic crystalline electric field (CEF). In addition, for PrTi2Al20, S takes a minimum with a negative sign at 10K owing to the CEF effect, and shows an additional tiny negative hump below 2K as a signature of quadrupole ordering. On the other hand, S for PrV 2Al20 manifests a large negative peak at 3K with the magnitude of 3 μV/K. This gives a large enhancement in absolute S divided by temperature T, jSj=T , approximately below 10K on cooling. jSj=T reaches 4 μV/K2 at 0.2 K, which is larger than that in the zero-T limit for a heavy-electron compound CeRu2Si2. This observation strongly indicates that the heavy-electron state brought by the quadrupolar Kondo effect is realized in the non-Kramers Γ3 ground state of PrV2Al20.
AB - We investigated thermoelectric properties for PrTi2Al20 and PrV 2Al20 below room temperature down to 0.13 K. A clear positive peak has been observed at 75K in the thermoelectric power S for PrTi2Al20. Also for PrV2Al20, the similar S peak has been detected at 40 K. These peaks arise from the Kondo effect in the magnetic excited levels of the 4f -electronic state under a cubic crystalline electric field (CEF). In addition, for PrTi2Al20, S takes a minimum with a negative sign at 10K owing to the CEF effect, and shows an additional tiny negative hump below 2K as a signature of quadrupole ordering. On the other hand, S for PrV 2Al20 manifests a large negative peak at 3K with the magnitude of 3 μV/K. This gives a large enhancement in absolute S divided by temperature T, jSj=T , approximately below 10K on cooling. jSj=T reaches 4 μV/K2 at 0.2 K, which is larger than that in the zero-T limit for a heavy-electron compound CeRu2Si2. This observation strongly indicates that the heavy-electron state brought by the quadrupolar Kondo effect is realized in the non-Kramers Γ3 ground state of PrV2Al20.
KW - Kondo effect
KW - Non-Kramers Γ doublet
KW - PrTiAl
KW - PrVAl
KW - Quadrupolar Kondo effect
KW - Thermoelectric power
UR - http://www.scopus.com/inward/record.url?scp=84879834035&partnerID=8YFLogxK
U2 - 10.7566/JPSJ.82.074705
DO - 10.7566/JPSJ.82.074705
M3 - 学術論文
AN - SCOPUS:84879834035
SN - 0031-9015
VL - 82
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 7
M1 - 074705
ER -