Rolf Walter Lortz

Specific heat of Nb 3 Sn: The case for a second energy gap

We present specific-heat data for

Superconductivity mediated by a soft phonon mode: Specific heat, resistivity, thermal expansion, and magnetization of YB6

{mathrm{Nb}}_{3}mathrm{Sn}

Specific heat, magnetic susceptibility, resistivity and thermal expansion of the superconductor ZrB12

, a well-known technically applied superconductor with a critical temperature

Specific heat and magnetization of a Zr B 12 single crystal: Characterization of a type-II/1 superconductor

{T}_{c}ensuremath{cong}18phantom{rule{0.3em}{0ex}}mathrm{K}

Effect of electron-phonon coupling on the superconducting transition temperature in dodecaboride superconductors: A comparison of LuB 12 with ZrB 12

, in the temperature range from

On the origin of the double superconducting transition in overdoped YBa2Cu3Ox

1.2phantom{rule{0.5em}{0ex}}text{to}phantom{rule{0.5em}{0ex}}200phantom{rule{0.3em}{0ex}}mathrm{K}

Origin of the magnetization peak effect in the Nb 3 Sn superconductor

in zero magnetic field, and from

Phonon mode spectroscopy, electron-phonon coupling, and the metal-insulator transition in quasi-one-dimensional M 2 Mo 6 Se 6

1.5phantom{rule{0.5em}{0ex}}text{to}phantom{rule{0.5em}{0ex}}22phantom{rule{0.3em}{0ex}}mathrm{K}

Phonon density of states, anharmonicity, electron-phonon coupling, and possible multigap superconductivity in the clathrate superconductors Ba 8 Si 46 and Ba 24 Si 100 : Factors behind large difference in T c

in fields

Evolution of the specific-heat anomaly of the high-temperature superconductor YBa2Cu3O7 under the influence of doping through application of pressure up to 10 GPa

Hensuremath{leqslant}16phantom{rule{0.3em}{0ex}}mathrm{T}