2011
DOI: 10.1143/jpsj.80.074605
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Fermi Surface Property and Characteristic Crystalline Electric Field Effect in PrIr2Zn20

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Cited by 25 publications
(20 citation statements)
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“…3 energy is approximately below 100 K, and this is consistent with the results of high-field magnetization. It is noted that the splitting energy is estimated to be 106 K in YbIr 2 Zn 20 [4] and 103 K in PrIr 2 Zn 20 [5].…”
Section: Experimental Results and Analysesmentioning
confidence: 99%
“…3 energy is approximately below 100 K, and this is consistent with the results of high-field magnetization. It is noted that the splitting energy is estimated to be 106 K in YbIr 2 Zn 20 [4] and 103 K in PrIr 2 Zn 20 [5].…”
Section: Experimental Results and Analysesmentioning
confidence: 99%
“…The entropy released at T Q is only 0.2R ln 2, indicating that quadrupolar fluctuations could play an important role in the formation of Cooper pairs [382]. However, extremely low upper critical field values with upper limit H c2 (0) < 20 Oe are observed and cyclotron effective masses of order m 0 are obtained in quantum oscillation measurements [384], indicating that Cooper pairs are not formed from heavy quasiparticles in PrIr 2 Zn 20 . Though it is probably not a heavy-fermion compound, uncovering superconductivity in PrIr 2 Zn 20 (and in the related compound PrRh 2 Zn 20 at T c 0.06 K [385]) set the stage for the discovery of heavy-fermion superconductivity in other Pr-based 1-2-20 compounds with Γ 3 ground states.…”
Section: Superconductivity In Prt 2 X 20 Compoundsmentioning
confidence: 95%
“…7,8) In PrIr 2 Zn 20 , the SC emerges at 50 mK in the antiferroquadrupolar phase whose ordering temperature is T Q ¼ 0:11 K. The critical field has not been precisely determined, but is known to be <20 Oe. 35) In contrast with the strong hybridization effects in PrTi 2 Al 20 , 4f electrons are so localized in PrIr 2 Zn 20 that do not exhibit the Kondo effect in ðT Þ, show nearly Curie behavior of ðT Þ with a vanishingly small  W , and have the cyclotron effective mass of m à cyc =m 0 $ 1. 8,35) Thus, the origin of the higher T c of the superconductivity in PrTi 2 Al 20 than in PrIr 2 Zn 20 may partly come from the larger effective mass or density of states of itinerant electrons coming from the stronger hybridization.…”
Section: à6mentioning
confidence: 99%
“…35) In contrast with the strong hybridization effects in PrTi 2 Al 20 , 4f electrons are so localized in PrIr 2 Zn 20 that do not exhibit the Kondo effect in ðT Þ, show nearly Curie behavior of ðT Þ with a vanishingly small  W , and have the cyclotron effective mass of m à cyc =m 0 $ 1. 8,35) Thus, the origin of the higher T c of the superconductivity in PrTi 2 Al 20 than in PrIr 2 Zn 20 may partly come from the larger effective mass or density of states of itinerant electrons coming from the stronger hybridization. In this case, the superconducting T c and its associated effective mass would increase under pressure as pressure enhances the hybridization and suppresses the quadrupolar ordering temperature.…”
Section: à6mentioning
confidence: 99%