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dc.contributor.author | Muratov A. | |
dc.contributor.author | Sadakov A. | |
dc.contributor.author | Gavrilkin S. | |
dc.contributor.author | Prishchepa A. | |
dc.contributor.author | Epifanova G. | |
dc.contributor.author | Chareev D. | |
dc.contributor.author | Pudalov V. | |
dc.date.accessioned | 2018-04-05T07:09:25Z | |
dc.date.available | 2018-04-05T07:09:25Z | |
dc.date.issued | 2017 | |
dc.identifier.issn | 0921-4526 | |
dc.identifier.uri | http://dspace.kpfu.ru/xmlui/handle/net/129725 | |
dc.description.abstract | © 2017 Elsevier B.V. We present detailed study of specific heat of FeSe single crystals with critical temperature Tc=8.45 K at 0.4-200 K in magnetic fields 0-9 T. Analysis of the electronic specific heat at low temperatures shows the coexistence of isotropic s-wave gap and strongly anisotropic extended s-wave gap without nodes. It was found two possibilities of superconducting gap parameters which give equally description of experimental data: (i) two gaps with approximately equal amplitudes and weight contribution to specific heat: isotropic δ1=1.7 meV (2δ1/kBTc=4.7) and anisotropic gap with the amplitude δ2max=1.8 meV (2δ2max/kBTc=4.9 and anisotropy parameter m=0.85); (ii) two gaps with substantially different values: isotropic large gap δ1=1.65 meV (2δ1/kBTc=4.52) and anisotropic small gap δ2max=0.75 meV (2δ2max/kBTc=2) with anisotropy parameter m=0.71. These results are confirmed by the field behavior of the residual electronic specific heat γr. | |
dc.relation.ispartofseries | Physica B: Condensed Matter | |
dc.subject | Fe-based superconductors | |
dc.subject | FeSe | |
dc.subject | Specific heat | |
dc.subject | Superconductors | |
dc.subject | Two-gap superconductivity | |
dc.title | Specific heat of FeSe: Two gaps with different anisotropy in superconducting state | |
dc.type | Article in Press | |
dc.collection | Публикации сотрудников КФУ | |
dc.source.id | SCOPUS09214526-2017-SID85032787134 |