Nematic fluctuations in an orbital selective superconductor Fe1+yTe1−xSex

Abstract

Fe1+yTe1−xSex is characterized by its complex magnetic phase diagram and highly orbital-dependent band renormalization. Despite this, the behavior of nematicity and nematic fluctuations, especially for high tellurium concentrations, remains largely unknown. Here we present a study of both B1g and B2g nematic fluctuations in Fe1+yTe1−xSex (0 ≤ x ≤ 0.53) using the technique of elastoresistivity measurement. We discovered that the nematic fluctuations in two symmetry channels are closely linked to the corresponding spin fluctuations, confirming the intertwined nature of these two degrees of freedom. We also revealed an unusual temperature dependence of the nematic susceptibility, which we attributed to a loss of coherence of the dxy orbital. Our results highlight the importance of orbital differentiation on the nematic properties of iron-based materials.

Transfer learning from Hermitian to non-Hermitian quantum many-body physics

“…The interplay between various degrees of freedom in manybody systems results in the emergence of novel phases of matter, including superconducting [1][2][3][4][5][6], Mott insulating [7][8][9][10][11], nematic [12][13][14][15][16] and topological [17][18][19][20][21][22] phases. Due to their inherent complexity, these systems are often studied computationally, using, e.g.…”