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 |
|