T. Adachi, T. Ogawa, Y. Komiyama, T. Sumura, Y. Saito-Tsuboi, T. Takeuchi, K. Mano, K. Manabe, K. Kawabata, T. Imazu, A. Koda, W. Higemoto, H. Okabe, J. G. Nakamura, T. U. Ito, R. Kadono, C. Baines, I. Watanabe, Y. Imai, J. Goryo, M. Nohara, K. Kudo
{"title":"Spontaneous magnetic field and disorder effects in BaPtAs_1-x_Sb_x_ with honeycomb network","authors":"T. Adachi, T. Ogawa, Y. Komiyama, T. Sumura, Y. Saito-Tsuboi, T. Takeuchi, K. Mano, K. Manabe, K. Kawabata, T. Imazu, A. Koda, W. Higemoto, H. Okabe, J. G. Nakamura, T. U. Ito, R. Kadono, C. Baines, I. Watanabe, Y. Imai, J. Goryo, M. Nohara, K. Kudo","doi":"arxiv-2409.05266","DOIUrl":null,"url":null,"abstract":"Chiral superconductivity exhibits the formation of novel electron pairs that\nbreaks the time-reversal symmetry and has been actively studied in various\nquantum materials in recent years. However, despite its potential to provide\ndefinitive information, effects of disorder in the crystal structure on the\nchiral superconductivity has not yet been clarified, and therefore the\ninvestigation using a solid-solution system is desirable. We report\nmuon-spin-relaxation (muSR) results of layered pnictide BaPtAs_1-x_Sb_x_ with a\nhoneycomb network composed of Pt and (As, Sb). We observed an increase of the\nzero-field muon-spin relaxation rate in the superconducting (SC) state at the\nSb end of x=1.0, suggesting the occurrence of spontaneous magnetic field due to\nthe time-reversal symmetry breaking in the SC state. On the other hand,\nspontaneous magnetic field was almost and completely suppressed for the As-Sb\nmixed samples of x=0.9 and 0.2, respectively, suggesting that the time-reversal\nsymmetry breaking SC state in x=1.0 is sensitive to disorder. The magnetic\npenetration depth estimated from transverse-field muSR measurements at x=1.0\nand 0.2 behaved like weak-coupling s-wave superconductivity. These seemingly\nincompatible zero-field and transverse-field muSR results of BaPtAs_1-x_Sb_x_\nwith x=1.0 could be understood in terms of chiral d-wave superconductivity with\npoint nodes on the three-dimensional Fermi surface.","PeriodicalId":501069,"journal":{"name":"arXiv - PHYS - Superconductivity","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Superconductivity","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.05266","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Chiral superconductivity exhibits the formation of novel electron pairs that
breaks the time-reversal symmetry and has been actively studied in various
quantum materials in recent years. However, despite its potential to provide
definitive information, effects of disorder in the crystal structure on the
chiral superconductivity has not yet been clarified, and therefore the
investigation using a solid-solution system is desirable. We report
muon-spin-relaxation (muSR) results of layered pnictide BaPtAs_1-x_Sb_x_ with a
honeycomb network composed of Pt and (As, Sb). We observed an increase of the
zero-field muon-spin relaxation rate in the superconducting (SC) state at the
Sb end of x=1.0, suggesting the occurrence of spontaneous magnetic field due to
the time-reversal symmetry breaking in the SC state. On the other hand,
spontaneous magnetic field was almost and completely suppressed for the As-Sb
mixed samples of x=0.9 and 0.2, respectively, suggesting that the time-reversal
symmetry breaking SC state in x=1.0 is sensitive to disorder. The magnetic
penetration depth estimated from transverse-field muSR measurements at x=1.0
and 0.2 behaved like weak-coupling s-wave superconductivity. These seemingly
incompatible zero-field and transverse-field muSR results of BaPtAs_1-x_Sb_x_
with x=1.0 could be understood in terms of chiral d-wave superconductivity with
point nodes on the three-dimensional Fermi surface.