Inhomogeneous Superconductivity in the Heavy Fermion CeRhIn5 Tuson Park Department of Physics, Sungkyunkwan University, Suwon 440-746, South Korea 成 均 館 (since 1398) IOP Workshop, Nov. 10-12, 2012 Collaborators E. Park, S. Seo, S. Lee, D. Shin, S. Shin : Sungkyunkwan Univ. X. Lu, H. Lee, F. Ronning, E. D. Bauer, R. Movshovich, J. L. Sarrao, I. Martin, Z. Zhu, J. D. Thompson: Los Alamos National Lab. H. Q. Yuan: Zhejiang University, China V. Sidorov: HPPI, Russia Z. Fisk: Univ. California - Irvine I. Vekhter: Louisiana State Univ. N. Curro: Univ. California - Davis. R. R. Urbano: UNICAMP. SKKU Outline Quantum criticality and superconductivity Inhomogeneous SC state in the quantum critical superconductor CeRhIn5 - Phys. Rev. Lett. 108, 077003 (2012) Disorder, magnetism, and superconductivity: Cd-doped CeMIn5 (M=Co, Rh, Ir) (unpublished) Phase diagram of unconventional SCs cuprate organics Fe-based pnictides heavy fermion CeRhIn5 Non-Fermi liquid at optimal Tc cuprate Fe pnictides Common threads heavy fermion 100 Universial Class of SCs 0.6 CeRhIn T 5 10 c (-cm) organics CeRhIn5 1 2 T 0.1 1 1 bar 22.7 kbar 52.6 kbar 10 100 Temperature (K) temperature Emergent phases near a quantum critical point Quantum critical matter (NFL) Ordered Ordered state state SC Fermi liquid δc temperature –control parameter (δ) phase diagram δ P. Coleman & A. J. Schofield, Nature 433 ('05) Quantum phase transition is a transition between ordered and disordered states driven by quantum fluctuations at T = 0 K Breakdown of Fermi liquid: Δρ Tn (n <2), C/T log T0/T Continuous source of new emergent states: unconventional superconductivity, metamagnetism (Sr3Ru2O7), stripes in the cuprates, nematic states in URu2Si2 & Fe-based SCs Quantum critical superconductivity in CeRhIn5 100 I // ab-plane 2.3 K 20 K 50 K 280 K ab (P) (P) // abab (5.2 (5.2 GPa) GPa) ab 80 60 40 20 0 0 1 2 3 4 5 P (GPa) [100] [010] [100] 905 SC 900 C / T (a. u.) Isothermal measurements of CeRhIn5 as a fn of pressure: (P) / (5.2 GPa) Nature 456, 366 (2008) 1.8 K & 0.5 T 895 330 328 326 Quantum fluctuations are the origin of the unconventional superconductivity 0.3 K & 0.5 T 324 0 90 180 angle () 4-fold modulation in field-angle specific heat PRL 101, 177002 (2008) Outline Quantum criticality and superconductivity Inhomogeneous SC state in the quantum critical superconductor CeRhIn5 - Phys. Rev. Lett. 108, 077003 (2012) Disorder, magnetism, and superconductivity: Cd-doped CeMIn5 (M=Co, Rh, Ir) (unpublished) ab (m cm) Textured SC in high-Tc cuprates 10 -1 10 -2 10 -3 10 -4 La1.875Ba.125CuO4 bulk Tc 0 10 20 30 40 50 T (K) Q. Li et al., PRL 99, 067001 (2007) resistive transition far above bulk Tc Broad tail below the Tc onset temperature for transition in c < ab I. Martin & C. Panagopoulos, EPL 92, 67001 (2010) Y. Ando et al., PRL 92, 247004 (2004) Filamentary superconductivity in CeRhIn5 Filamentary superconductivity due to bad sample quality? Manifestation of a new state of matter in the vicinity of a QCP? Tc difference below 1.9 Gpa (Knebel et al., JPCM 16, 8905 (2004)) Experiments: simultaneous measurements of heat capacity and resistivity under pressure Hybrid clamp-type pressure cell (up to 3 GPa) with silicone as transmitting medium Plug with samples mounted Pb Tc as a meausre of pressure CeRhIn5 in the coexisting phase TN 12.0 TN bulk Tc 6000 Tc onset T (K) C/T (arb. units) 4 2 AFM 10.0 P = 15.8 kbar Ton 8.0 4000 6.0 4.0 2000 SC 2.0 AFM+ SC 0 0.0 0.5 1.0 1.5 2.0 2.5 P (GPa) Phase diagram for better sample with RRR ~ 1000 0 0.0 0 1 2 3 4 T (K) Tc Tc onset in the resistivity is different from the bulk Tc determined by the heat capacity ab ( cm) 6 Pressure effects on the Tc difference a a Tc onset C/T (arb. units) 6000 bulk Tc c b T (K) 4 0 0.0 1.0 2.0 3.0 0.0 4.0 1.5 2.0 2.5 P (GPa) Tc difference between resistivity and specific heat only in the coexisting phase Tc difference is not from disorder, but from competing orders 10.0 P = 1.7 GPa GPa 2000 5.0 0 0.0 1.0 2.0 3.0 ab ( cm) 1.0 4000 0.0 4.0 c 6000 10.0 P = 2.2 GPa 4000 5.0 2000 0 0.0 1.0 2.0 3.0 ab ( cm) AFM+ SC 0.5 5.0 2000 b SC 0 0.0 4000 AFM C/T (arb. units) 2 10.0 P = 1.58 GPa GPa ab ( cm) TN C/T (arb. units) 6 0.0 4.0 T (K) TP et al., Phys. Rev. Lett. 108, 077003 (2012) Resistivity anisotropy in the SC transition regioin 6 TN bulk Tc Tc onset 10.00 10.00 T (K) ,, ab cc (( -cm) -cm) ab 4 1.00 1.00 (ab) ab) bar(J(J ////ab) 11bar 1.61 GPa (ab) // ab) 1 bar (J // c)(J 2.42 (J GPa // c)(ab) 1bar 1bar GPa (c) (J // c) 1.65 1.65 GPa (c) 2.43 GPa (c) 0.10 0.10 cm cm 90nn (0)==90 c(0) cc 2 AFM SC AFM+ SC 0 0.0 0.5 1.0 1.5 2.0 2.5 P (GPa) cm cm 7.9nn (0) (0)==7.9 ab ab ab 0.01 0.01 1.0 1.0 2.0 2.0 3.0 3.0 4.0 4.0 5.0 5.0 T(K) T(K) At 1bar, residual resistivity for J//c is larger than J // ab by a factor of 10 Contradicting conventional expectation, however, resistivity drops to zero immediately for J // c, while it has a long tail for J // ab Resistivity anisotropy only in the coexisting phase Textured SC state Broad tail of SC transition in ρab is not from heating effects. Additional in-plane anisotropy 1.00 ( cm) 1.00 P = 1.58 GPa @ 0.1 mA @ 10.0 mA 0.10 0.01 0.10 1.6 1.8 2.0 2.2 2.4 1.6 1.7 T (K) 2.2 I//100 I//110 3.0 2.0 1.0 T (K) Tc, mid (K) ab (-cm) 10.00 I//100 I//110 2.0 c 1.8 AF SC AF SC b AF a 1.3 1.4 1.5 P (GPa) Recent neutron scattering in the coexisting phase of CeRhIn5 4 Tc TN T (K) 3 AFM 2 SC 1 AFM+ SC 0 0.0 0.5 1.0 1.5 2.0 2.5 P (GPa) T*Tcorresponds to resistive T c corresponds to the bulk Tc, cwhere => & Q2 coexists, while Q1 QSC 2 completely replaces Q1 and disappears below bulk Tc coexists with SC state c Q1 Neutron scattering of CeRhIn5 at 1.48 GPa - Aso et al., JPSJ 78, 073703 (2009). SC & Q1 SC & Q1 Q2 Q2 b a Q1 = (0.5, 0.5, 0.326), Q2 = (0.5, 0.5, 0.391) Summary & Discussion I Discovery of a textured SC phase in the heavy fermion compound CeRhIn5: - Tc difference - Resistivity anisotropy among different crystalline axes - Coincidence of Q2 onset with Tc onset Presence of competing phase & proximity to a QCP are keys to the textured SC phase Is textuerd SC unique in CeRhIn5? c Q1 SC & Q1 SC & Q1 Q2 Q2 b a Q1 = (0.5, 0.5, 0.326), Q2 = (0.5, 0.5, 0.391) ab (m cm) Textured SC in high-Tc cuprates 10 -1 10 -2 10 -3 10 -4 La1.875Ba.125CuO4 bulk Tc 0 10 20 30 40 50 T (K) Q. Li et al., PRL 99, 067001 (2007) resistive transition far above bulk Tc Broad tail below the Tc onset temperature for transition in c < ab I. Martin & C. Panagopoulos, EPL 92, 67001 (2010) Textured SC in organics (TMTSF)2PF6 Pasquier et al., Physica B 407, 1806 (2012) pressure Textured SC in Fe pnictides Fernandes et al., Phys. Rev. B 81, 140501 (2010) Chu et al., Science 329, 824 (2010) (arXiv:1112.2243v1) Perspective on textured state Quantum critical SCs seem susceptible to new electronic states Electrons spontaneously adjust themselves to minimize the stress coming from frustration among competing phases Is textured SC state universal? Most likely Add one more common thread to the unconventional SCs Is it beneficial to superconductivity? Probably not in CeRhIn5 Thank you ! 감사합니다!