THESIS
2016
xiv, 83 pages : illustrations ; 30 cm
Abstract
In this thesis, two kinds of superconductors Ca
3(Ir
0.91Co
0.09)
4Sn
13 and Ba
1-xK
xFe
2As
2 were investigated
through various experiments including magnetization, specific heat, thermal expansion,
thermal conductivity, resistivity and point contact Andreev reflection spectroscopy.
The specific heat and resistivity data of Ca
3(Ir
0.91Co
0.09)
4Sn
13 are presented, together with further analysis to study the electron-phonon interaction. We demonstrated the important role of the low-lying phonon modes in the pairing mechanism of this superconductor which points to a conventional
phonon-mediated origin of superconductivity in Ca
3Ir
4Sn
13 and rules out a magnetic spin fluctuation mediated pairing scenario.
The critical fluctuation in the iron based superconductor Ba
1-xK
xFe
2As
2 was studied by apply...[
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In this thesis, two kinds of superconductors Ca
3(Ir
0.91Co
0.09)
4Sn
13 and Ba
1-xK
xFe
2As
2 were investigated
through various experiments including magnetization, specific heat, thermal expansion,
thermal conductivity, resistivity and point contact Andreev reflection spectroscopy.
The specific heat and resistivity data of Ca
3(Ir
0.91Co
0.09)
4Sn
13 are presented, together with further analysis to study the electron-phonon interaction. We demonstrated the important role of the low-lying phonon modes in the pairing mechanism of this superconductor which points to a conventional
phonon-mediated origin of superconductivity in Ca
3Ir
4Sn
13 and rules out a magnetic spin fluctuation mediated pairing scenario.
The critical fluctuation in the iron based superconductor Ba
1-xK
xFe
2As
2 was studied by applying the 3D XY and the 3D LLL scaling models to our specific heat and thermal expansion data. Our results indicate the weakest critical fluctuations at optimal doping and demonstrate that a strong increase of the critical fluctuations regime is responsible for the transition broadening in magnetic fields, which is a direct consequence of a magnetic-field-induced finite size effect and the confinement of quasiparticles in low Landau levels.
The re-entrant tetragonal phase of Ba
0.76K
0.24Fe
2As
2 was investigated with various experimental
probes. With high precision magnetization measurements, we for the first time proved the spin
reorientation in the re-entrant tetragonal phase transition in Ba
0.76K
0.24Fe
2As
2. Together with earlier
investigations in Na-doped Ba122, our result reveals that the spin reorientation is a universal
property in the hole doped Ba122 system.
The superconducting pairing symmetry of Ba
0.7K
0.3Fe
2As
2 was studied by field-angle resolved
thermal conductivity experiment. A six-fold oscillation in the thermal conductivity was observed,
which is inconsistent with the tetragonal crystal lattice structure, indicating a novel highly complex
superconducting nodal order parameter symmetry rather than ±s-wave or d-wave symmetry.
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