Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)Ir3Si5

被引:17
|
作者
Sangeetha, N. S. [1 ]
Thamizhavel, A. [2 ]
Tomy, C. V. [3 ]
Basu, Saurabh [1 ]
Awasthi, A. M. [4 ]
Ramakrishnan, S. [2 ]
Pal, D. [1 ]
机构
[1] Indian Inst Technol, Dept Phys, Gauhati 781039, Assam, India
[2] Tata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Bombay 400005, Maharashtra, India
[3] Indian Inst Technol, Dept Phys, Bombay 400076, Maharashtra, India
[4] IUC DAEF, Indore 452017, Madhya Pradesh, India
来源
PHYSICAL REVIEW B | 2012年 / 86卷 / 02期
关键词
EARTH-IRON SILICIDES; PEIERLS TRANSITION; PHASE-TRANSITION; FERMI-SURFACE; R5IR4SI10; R; BLUE BRONZE; K0.3MOO3; NBSE3; ENHANCEMENT; INSTABILITY;
D O I
10.1103/PhysRevB.86.024524
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We explore the interplay and competition between superconductivity (SC) and the charge density wave (CDW) ordering transition on pseudoternary alloys (Lu1-xScx)(2)Ir3Si5, Lu-2(Ir1-xRhx)(3)Si-5, and Lu2Ir3(Si1-xGex)(5) via magnetization, thermal and transport measurements. We track the evolution of the superconducting transition temperature T-SC and the CDW ordering transition temperature T-CDW as a function of doping concentration x to present a temperature-concentration phase diagram for each of the series of compounds. We find that as we increase x, T-CDW and T-SC show a nonmonotonic behavior in Lu2Ir3(Si1-xGex)(5). Here, we observe that both CDW and SC survive till 20% of the Ge substitution. In Lu-2(Ir1-xRhx)(3)Si-5, as Rh concentration increases, T-CDW varies rapidly from 207 to 284 K, whereas the T-SC changes gradually from 5.5 to 2.5 K. In addition, the Sc substitution at the Lu site of Lu2Ir3Si5 displays a slight change in CDW transition temperature, without affecting the SC ordering temperature too much. Our study reveals that the CDW anomalies are broadened and smeared out, probably by substitutional disorder effects. The heat capacity data in the vicinity of the CDW transition for all the substituted alloys are analyzed using a model of critical fluctuations in addition to a mean-field contribution and a smooth lattice background. The critical exponent changes appreciably with increasing disorder, which suggests that the first-order CDW transition in the parent compound Lu2Ir3Si5 changes to a second-order transition via doping.
引用
收藏
页数:16
相关论文
共 50 条
  • [41] Eu2Ru3Si5 and Eu2Ir3Ga5 - first europium compounds with U2Mn3Si5-type structure but different europium valence
    Seidel, Stefan
    Harmening, Thomas
    Koesters, Jutta
    Koldemir, Aylin
    Proebsting, Wilma
    Engelbert, Simon
    Poettgen, Rainer
    ZEITSCHRIFT FUR NATURFORSCHUNG SECTION B-A JOURNAL OF CHEMICAL SCIENCES, 2023, 78 (05): : 293 - 300
  • [42] Two-band superconductivity featuring different anisotropies in the ternary iron silicide Lu2Fe3Si5
    Nakajima, Yasuyuki
    Hidaka, Hikaru
    Nakagawa, Tsuyoshi
    Tamegai, Tsuyoshi
    Nishizaki, Terukazu
    Sasaki, Takahiko
    Kobayashi, Norio
    PHYSICAL REVIEW B, 2012, 85 (17)
  • [43] TRANSITION FROM SUPERCONDUCTIVITY TO HEAVY-FERMION BEHAVIOR IN U-DOPED LU2FE3SI5
    MIELKE, A
    KIM, WW
    RIEGER, JJ
    FRAUNBERGER, G
    SCHEIDT, EW
    STEWART, GR
    PHYSICAL REVIEW B, 1994, 50 (22) : 16522 - 16527
  • [44] Disorder-Sensitive Superconductivity and Bonding Network in the Iron-Silicide Superconductor Lu2Fe3Si5
    Okuyama, H.
    Takase, K.
    Takano, Y.
    Watanabe, T.
    Yoshida, F.
    Moriyoshi, C.
    Kuroiwa, Y.
    SOLID COMPOUNDS OF TRANSITION ELEMENTS, 2011, 170 : 118 - 121
  • [45] Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)
    Watanabe, Tadataka
    Sasame, Hiroki
    Okuyama, Hiroaki
    Takase, Kouichi
    Takano, Yoshiki
    PHYSICAL REVIEW B, 2009, 80 (10):
  • [46] Two-gap superconductivity in Lu2Fe3Si5: A transverse-field muon spin rotation study
    Biswas, P. K.
    Balakrishnan, G.
    Paul, D. McK.
    Lees, M. R.
    Hillier, A. D.
    PHYSICAL REVIEW B, 2011, 83 (05):
  • [47] Two-gap superconductivity seen in penetration-depth measurements of Lu2Fe3Si5 single crystals
    Gordon, R. T.
    Vannette, M. D.
    Martin, C.
    Nakajima, Y.
    Tamegai, T.
    Prozorov, R.
    PHYSICAL REVIEW B, 2008, 78 (02):
  • [48] Non-magnetic and magnetic impurity effects on superconductivity in the ternary iron-suicide Lu2Fe3Si5
    Watanabe, Tadataka
    Okuyama, Hiroaki
    Takase, Kouichi
    Takano, Yoshiki
    PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 2010, 470 : S768 - S769
  • [49] Magnetic structure of the Er3+ moments in the charge-density-wave compound Er5Ir4Si10
    Galli, F
    Feyerherm, R
    Hendrikx, RWA
    Ramakrishnan, S
    Nieuwenhuys, GJ
    Mydosh, JA
    PHYSICAL REVIEW B, 2000, 62 (21): : 13840 - 13843
  • [50] SYNTHESIS AND MOLECULAR-STRUCTURE OF ([1,3-(ME3SI)2C5H3]2LU(MU-CL))2
    VOSKOBOINIKOV, AZ
    CHUKLANOVA, EB
    PARSHINA, IN
    SHESTAKOVA, AK
    GUSEV, AI
    BELETSKAYA, IP
    RUSSIAN CHEMICAL BULLETIN, 1993, 42 (03) : 531 - 533