# Magnetic and thermodynamic properties of Cu$_x$TiSe$_2$ single crystals

**Authors:** Z. Pribulov\'a, Z. Medveck\'a, J. Ka\v{c}mar\v{c}\'ik, V. Komanick\'y,, T. Klein, P. Rodi\`ere, F. Levy-Bertrand, B. Michon, C. Marcenat, P., Husan\'ikov\'a, V. Cambel, J. \v{S}olt\'ys, G. Karapetrov, S. Borisenko, D., Evtushinsky, H. Berger, and P. Samuely

arXiv: 1704.08463 · 2017-06-07

## TL;DR

This study investigates the magnetic and thermodynamic properties of Cu$_x$TiSe$_2$ single crystals, revealing a small energy gap and complex doping dependence of the condensation energy through combined experimental techniques.

## Contribution

It provides a comprehensive analysis of the phase diagram and superconducting gaps in Cu$_x$TiSe$_2$, highlighting discrepancies between magnetic and specific heat measurements.

## Key findings

- Superfluid density indicates a small energy gap with strong coupling.
- Specific heat suggests a larger single gap, contradicting magnetic data.
- Doping affects the condensation energy in a non-trivial way.

## Abstract

We present a detailed study of the phase diagram of copper intercalated TiSe$_2$ single crystals, combining local Hall-probe magnetometry, tunnel diode oscillator technique (TDO), specific-heat, and angle-resolved photoemission spectroscopy measurements. A series of the Cu$_x$TiSe$_2$ samples from three different sources with various copper content $x$ and superconducting critical temperatures $T_c$ have been investigated. We first show that the vortex penetration mechanism is dominated by geometrical barriers enabling a precise determination of the lower critical field, $H_{c1}$. We then show that the temperature dependence of the superfluid density deduced from magnetic measurements (both $H_{c1}$ and TDO techniques) clearly suggests the existence of a small energy gap in the system, with a coupling strength $2\Delta_s \sim [2.4-2.8]k_BT_c$, regardless of the copper content, in puzzling contradiction with specific heat measurements which can be well described by one single large gap $2\Delta_l \sim [3.7-3.9]k_BT_c$. Finally, our measurements reveal a non-trivial doping dependence of the condensation energy, which remains to be understood.

## Full text

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## Figures

9 figures with captions in the complete paper: https://tomesphere.com/paper/1704.08463/full.md

## References

35 references — full list in the complete paper: https://tomesphere.com/paper/1704.08463/full.md

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Source: https://tomesphere.com/paper/1704.08463