Abstract

The $J_1$-$J_2$ quantum spin sawtooth chain is a paradigmatic one-dimensional frustrated quantum spin system exhibiting unconventional ground-state and finite-temperature properties. In particular, it exhibits a flat energy band of one-magnon excitations accompanied by an enhanced magnetocaloric effect for two singular ratios of the basal interactions $J_1$ and the zigzag interactions $J_2$. In our paper, we demonstrate that one can drive the spin system into a flat-band scenario by applying an appropriate electric field, thus overcoming the restriction of fine-tuned exchange couplings $J_1$ and $J_2$ and allowing one to tune more materials towards flat-band physics, that is to show a macroscopic magnetization jump when crossing the magnetic saturation field, a residual entropy at zero temperature as well as an enhanced magnetocaloric effect. While the magnetic field acts on the spin system via the ordinary Zeeman term, the coupling of an applied electric field with the spins is given by the sophisticated Katsura-Nagaosa-Balatsky (KNB) mechanism, where the electric field effectively acts as a Dzyaloshinskii-Moriya spin-spin interaction. The resulting novel features are corresponding reciprocal effects: We find a magnetization jump driven by the electric field as well as a jump of the electric polarization driven by the magnetic field, i.e.\ the system exhibits an extraordinarily strong magnetoelectric effect. Moreover, in analogy to the enhanced magnetocaloric effect the system shows an enhanced electrocaloric effect.

Highlights

  • The magnetoelectric effect (MEE) allows to manipulate magnetic materials by electric fields [1]

  • The key target of the present paper is the study of the interplay of the KNB mechanism and magnetic frustration at and in the vicinity of a flat-band point

  • (a) A crucial finding of our work is that just the electric field via the KNB mechanism may dissolve the fine tuning of J1 and J2 and can lead to a large variety of J1-J2 ratios, where for appropriate direction and magnitude of E the lowest one-magnon band is flat

Read more

Summary

INTRODUCTION

The magnetoelectric effect (MEE) allows to manipulate magnetic materials by electric fields [1]. Quantum systems hosting flat bands in their energy spectrum, on the other hand, constitute realizations of materials that already exhibit enhanced magnetocaloric effects thanks to the special frustrated nature of their interactions. In the case of zero electric field, for this model two flat-band scenarios are known: For the AFM sawtooth chain, J1, J2 > 0, the lowest band of one-magnon excitations above the fully polarized FM state |FM = | ↑↑↑ · · · is dispersionless for J2 = 2J1 (flat-band point) [27,36,75,77,79,83,84]. Further examples for magnetic compounds with sawtooth chain geometry of exchange bonds are the atacamite Cu2Cl(OH)3 [110], the fluoride Cs2LiTi3F12 [111], the euchroite Cu2(AsO4)(OH) · 3H2O [112], the sawtooth spin ring Mo75V20 [113], the frustrated [Mn18] magnetic wheel-ofwheels molecule [114], and the iron compound Fe2Se2O7 [115]

Summary of results
KNB MECHANISM FOR THE SAWTOOTH CHAIN
ELECTRIC FIELD INDUCED FLAT BANDS
Flat-band case I
Flat-band case II
NUMERICAL RESULTS
Ground-state properties
Finite-temperature properties
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call