Ferroelectricity in a one-dimensional organic quantum magnet

In magnetically controllable ferroelectrics, electric polarization is induced by charge redistribution or lattice distortions that occur to minimize the energy associated with both the magnetic order and interaction of spins with an applied magnetic field. Conventional approaches to designing materi...

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Published inNature physics Vol. 6; no. 3; pp. 169 - 172
Main Authors Kagawa, Fumitaka, Horiuchi, Sachio, Tokunaga, Masashi, Fujioka, Jun, Tokura, Yoshinori
Format Journal Article
LanguageEnglish
Published London Nature Publishing Group UK 01.03.2010
Nature Publishing Group
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Abstract In magnetically controllable ferroelectrics, electric polarization is induced by charge redistribution or lattice distortions that occur to minimize the energy associated with both the magnetic order and interaction of spins with an applied magnetic field. Conventional approaches to designing materials that exploit such spin-mediated behaviour have focused mainly on developing the cycloidal spin order, and thereby producing ferroelectric behaviour through the so-called antisymmetric Dzyaloshinskii-Moriya interaction. However, engineering such spin structures is challenging. Here we suggest a different approach. Direct measurements of magnetic-field-dependent variations in the polarization of the one-dimensional organic quantum magnet, tetrathiafulvalene-p-bromanil, suggest a spin-Peierls instability has an important role in its response. Our results imply that one-dimensional quantum magnets, such as organic charge-transfer complexes, could be promising candidates in the development of magnetically controllable ferroelectric materials.
AbstractList Measurements of the magnetic-field-dependent polarization of a one-dimensional organic quantum magnet suggest its ferroelectric behaviour is mediated by a spin–Peierls instability. Such behaviour could provide a promising new approach to the design of spin-driven ferroelectrics. In magnetically controllable ferroelectrics 1 , 2 , 3 , electric polarization is induced by charge redistribution or lattice distortions that occur to minimize the energy associated with both the magnetic order and interaction of spins with an applied magnetic field. Conventional approaches to designing materials that exploit such spin-mediated behaviour have focused mainly on developing the cycloidal spin order 4 , 5 , and thereby producing ferroelectric behaviour through the so-called antisymmetric Dzyaloshinskii–Moriya interaction 6 , 7 , 8 . However, engineering such spin structures is challenging. Here we suggest a different approach. Direct measurements of magnetic-field-dependent variations in the polarization of the one-dimensional organic quantum magnet, tetrathiafulvalene- p -bromanil, suggest a spin–Peierls instability has an important role in its response. Our results imply that one-dimensional quantum magnets, such as organic charge-transfer complexes, could be promising candidates in the development of magnetically controllable ferroelectric materials.
In magnetically controllable ferroelectrics, electric polarization is induced by charge redistribution or lattice distortions that occur to minimize the energy associated with both the magnetic order and interaction of spins with an applied magnetic field. Conventional approaches to designing materials that exploit such spin-mediated behaviour have focused mainly on developing the cycloidal spin order, and thereby producing ferroelectric behaviour through the so-called antisymmetric Dzyaloshinskii-Moriya interaction. However, engineering such spin structures is challenging. Here we suggest a different approach. Direct measurements of magnetic-field-dependent variations in the polarization of the one-dimensional organic quantum magnet, tetrathiafulvalene-p-bromanil, suggest a spin-Peierls instability has an important role in its response. Our results imply that one-dimensional quantum magnets, such as organic charge-transfer complexes, could be promising candidates in the development of magnetically controllable ferroelectric materials.
In magnetically controllable ferroelectrics1-3, electric polarization is induced by charge redistribution or lattice distortions that occur to minimize the energy associated with both the magnetic order and interaction of spins with an applied magnetic field. Conventional approaches to designing materials that exploit such spin-mediated behaviour have focused mainly on developing the cycloidal spin order4,5, and thereby producing ferroelectric behaviour through the so-called antisymmetric Dzyaloshinskii-Moriya interaction6-8. However, engineering such spin structures is challenging. Here we suggest a different approach. Direct measurements of magnetic-field-dependent variations in the polarization of the one-dimensional organic quantum magnet, tetrathiafulvalene-p-bromanil, suggest a spin-Peierls instability has an important role in its response. Our results imply that one-dimensional quantum magnets, such as organic charge-transfer complexes, could be promising candidates in the development of magnetically controllable ferroelectric materials. [PUBLICATION ABSTRACT]
Author Fujioka, Jun
Horiuchi, Sachio
Kagawa, Fumitaka
Tokunaga, Masashi
Tokura, Yoshinori
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Snippet In magnetically controllable ferroelectrics, electric polarization is induced by charge redistribution or lattice distortions that occur to minimize the energy...
Measurements of the magnetic-field-dependent polarization of a one-dimensional organic quantum magnet suggest its ferroelectric behaviour is mediated by a...
In magnetically controllable ferroelectrics1-3, electric polarization is induced by charge redistribution or lattice distortions that occur to minimize the...
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SubjectTerms Atomic
Classical and Continuum Physics
Complex Systems
Condensed Matter Physics
Ferroelectrics
letter
Magnetic fields
Mathematical and Computational Physics
Molecular
Optical and Plasma Physics
Physics
Physics and Astronomy
Polarization
Quantum physics
Theoretical
Title Ferroelectricity in a one-dimensional organic quantum magnet
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