Magnetic Phase Diagram of Li_2(Pd_{1-x}Pt_x)_3B by AC Susceptometry
D. C. Peets, G. Eguchi, M. Kriener, S. Harada, Sk. Md. Shamsuzzamen,, Y. Inada, G.-Q. Zheng, and Y. Maeno

TL;DR
This study maps the magnetic phase diagram and superconducting parameters of Li_2(Pd_{1-x}Pt_x)_3B across different platinum concentrations, revealing that the phase diagram remains stable despite changes in pairing and band structure.
Contribution
It provides the first detailed H-T phase diagram for Li_2(Pd_{1-x}Pt_x)_3B and discusses the impact of cation substitution on superconducting properties.
Findings
Coherence length may vary linearly with platinum concentration
H-T phase diagram remains essentially unchanged despite fundamental changes in pairing state
Upper critical field H_c2(0) is not anomalously high across Pt content
Abstract
The H-T phase diagram and several superconducting parameters for Li_2(Pd_{1-x}Pt_x)_3B have been determined as a function of cation substitution x. Notably, the coherence length may be linear in platinum concentration. Despite the superconducting pairing state and band structure apparently changing fundamentally, the H-T phase diagram is essentially unchanged. Unusual aspects of the shape of the H-T phase diagram are discussed. The upper critical field H_c2(0) is not anomalously high for any Pt content, likely due to an absence of high carrier masses - in such a case, the value of H_c2(0) would not serve as a probe for novel physics.
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