Abstract

We report on a comprehensive de Haas--van Alphen (dHvA) study of the iron pnictide LaFe$_2$P$_2$. Our extensive density-functional band-structure calculations can well explain the measured angular-dependent dHvA frequencies. As salient feature, we observe only one quasi-two-dimensional Fermi-surface sheet, i.e., a hole-like Fermi-surface cylinder around $\Gamma$, essential for $s_\pm$ pairing, is missing. In spite of considerable mass enhancements due to many-body effects, LaFe$_2$P$_2$ shows no superconductivity. This is likely caused by the absence of any nesting between electron and hole bands.

Highlights

  • We report on a comprehensive de Haas–van Alphen study of the iron pnictide LaFe2P2

  • Important results on the topology of the Fermi surfaces and many-body mass enhancements have been obtained already, but more information is needed for gaining a coherent picture on the band-structure properties relevant for superconductivity in these materials

  • We report on a detailed de Haas–van Alphen study combined with band-structure calculations of the 122 iron phosphide LaFe2P2

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Summary

Introduction

We report on a comprehensive de Haas–van Alphen (dHvA) study of the iron pnictide LaFe2P2. Fermi-surface topology of the iron pnictide LaFe2P2 Our extensive density-functional band-structure calculations can well explain the measured angular-dependent dHvA frequencies.

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