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Magnetic phase diagram of Li<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow /><mml:mn>2</mml:mn></mml:msub></mml:math>(Pd<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow /><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math>Pt<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow /><mml:mi>x</mml:mi></mml:msub></mml:math…
The $H$-$T$ phase diagram and several superconducting parameters for the noncentrosymmetric system Li${}_{\text{2}}$(Pd${}_{\text{1}\ensuremath{-}x}$Pt${}_{x}$)${}_{\text{3}}$B 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 …