Elastocaloric evidence for a multicomponent superconductor stabilized within the nematic state in Ba(Fe <sub> 1− <i>x</i> </sub> Co <sub> <i>x</i> </sub> ) <sub>2</sub> As <sub>2</sub>

S Sayak Ghosh (Geballe Laboratory for Advanced Materials) M Matthias S. Ikeda (Geballe Laboratory for Advanced Materials) A Anzumaan R. Chakraborty (School of Physics and Astronomy) T Thanapat Worasaran (Geballe Laboratory for Advanced Materials) F Florian Theuss (Stanford Institute for Materials and Energy Sciences) L Luciano B. Peralta (Laboratory of Atomic and Solid State Physics) P P. M. Lozano (Advanced Photon Source) J Jong-Woo Kim (Advanced Photon Source) P P. J. Thompson (Department of Physics) P Philip J. Ryan (Advanced Photon Source) L Linda Ye (Geballe Laboratory for Advanced Materials) A Aharon Kapitulnik (Geballe Laboratory for Advanced Materials) S Steven A. Kivelson (Geballe Laboratory for Advanced Materials) B B. J. Ramshaw R Rafael M. Fernandes I Ian R. Fisher (Department of Applied Physics)

Abstract

The iron-based high- T c superconductors (SCs) exhibit rich phase diagrams with intertwined phases, including magnetism, nematicity, and superconductivity. The superconducting T c in many of these materials is maximized in the regime of strong nematic fluctuations, making the role of nematicity in influencing the superconductivity a topic of intense research. Here, we use the AC elastocaloric effect (ECE) to map out the phase diagram of Ba(Fe 1− x Co x ) 2 As 2 near optimal doping. The ECE signature at T c on the overdoped side, where superconductivity condenses without any nematic order, is quantitatively consistent with other thermodynamic probes that indicate a single-component superconducting state. In contrast, on the slightly underdoped side, where superconductivity condenses within the nematic phase, ECE reveals a second thermodynamic transition proximate to and below T c . We rule out magnetism and reentrant tetragonality as the origin of this transition and find that our observations strongly suggest a phase transition into a multicomponent superconducting state. This implies the existence of a subdominant pairing instability that competes strongly with the dominant s ± instability. Our results highlight the significant role of nematic order in determining the pairing symmetry close to optimal doping in this extensively studied iron-based SC, while also demonstrating the power of ECE in uncovering strain-tuned phase diagrams of quantum materials.

Article Details

Volume / Issue Vol. 122, Issue 37
Published September 16, 2025
ISSN 0027-8424
Publisher National Academy of Sciences

Authors (16)

S

Sayak Ghosh

Geballe Laboratory for Advanced Materials

M

Matthias S. Ikeda

Geballe Laboratory for Advanced Materials

A

Anzumaan R. Chakraborty

School of Physics and Astronomy

T

Thanapat Worasaran

Geballe Laboratory for Advanced Materials

F

Florian Theuss

Stanford Institute for Materials and Energy Sciences

L

Luciano B. Peralta

Laboratory of Atomic and Solid State Physics

P

P. M. Lozano

Advanced Photon Source

J

Jong-Woo Kim

Advanced Photon Source

P

P. J. Thompson

Department of Physics

P

Philip J. Ryan

Advanced Photon Source

L

Linda Ye

Geballe Laboratory for Advanced Materials

A

Aharon Kapitulnik

Geballe Laboratory for Advanced Materials

S

Steven A. Kivelson

Geballe Laboratory for Advanced Materials

B

B. J. Ramshaw

R

Rafael M. Fernandes

I

Ian R. Fisher

Department of Applied Physics