Low-dimensional magnetism
Electronic transport in low-dimensional copper oxides has been the focus
of much activity during the past decade. In particular, unusual
superconducting states have been observed in layered cuprates, and more
recently also in cuprates with quasi-one-dimensional structures.
One-dimensional systems are more amenable to analytical and numerical
calculations and may well hold lessons for the two-dimensional systems
as well. Unfortunately, quasi-one-dimensional cuprates that can be
doped, such as (Sr, Ca)14Cu24O41, are structurally very complicated,
with several electronically active units. Structurally simple
quasi-one-dimensional copper oxides such as CuGeO3, SrCuO2, and Sr2CuO3
have also been widely studied, but attempts to introduce mobile charge
carriers into the copper oxide chains have thus far been unsuccessful.
The discovery of a new class of copper oxides with quasi-one-dimensional
electronic structure in Jansen's
department [1] opens up a new
perspective for a detailed description of the interplay between
magnetism and charge order in the cuprates. These compounds are free of
chemical disorder and can be highly doped. We have established the
presence of helical order due to long-range competing exchange
interactions in NaCu2O2, the insulating parent compound of this family
(Fig. 1a) [2,3]. We also characterized its magnetic and dielectric
properties [3] as well as the magnetic and lattice dynamical excitations
[4] of NaCu2O2. An investigation of the optical properties of a related
copper-oxide chain compound has led to the discovery of novel excitonic
modes whose spectral weight is controlled by one-dimensional spin
correlations [5]. These results are an excellent basis for ongoing
experiments on doped analogs. Initial experiments on Na8Cu5O10, a
compound exhibiting an intricate charge-ordering pattern (Fig. 1b), have
already revealed an unusual spin-density modulation [6]. These projects
are carried out in close cooperation with chemists in Jansen's
department, and with theorists in Metzner's department.
In another line of research, we are using the newly developed TRISP
spectrometer to probe the lifetimes of collective excitations in
low-dimensional quantum magnets, following successful experiments on a
three-dimensional classical magnet [7]. These experiments allow detailed
tests of long-standing theoretical predictions.
References
- M. Sofin, E.-M. Peters, M. Jansen. J. Solid State Chem. 178 (2005), 3708
- L. Capogna, M. Mayr, P. Horsch, M. Raichle, R. K. Kremer, M. Sofin, A. Maljuk, M. Jansen, B. Keimer. Phys. Rev. B 71 (2005), 140402(R)
- Ph. Leininger, M. Rahlenbeck, M. Raichle, B. Bohnenbuck, A. Maljuk, C. T. Lin, B. Keimer, E. Weschke, E. Schierle, S. Seki, Y. Tokura, J. W. Freeland.
Phys. Rev. B 81 (2010), 085111
- K.-Y. Choi, V. P. Gnezdilov, P. Lemmens, L. Capogna, M. R. Johnson, M. Sofin, A. Maljuk, M. Jansen, B. Keimer. Phys. Rev. B 73 (2006), 094409
- Y. Matiks, P. Horsch, R. K. Kremer, B. Keimer, A. V. Boris.
Phys. Rev. Lett. 103 (2009), 187401
- M. Raichle, M. Reehuis, G. André, L. Capogna, M. Sofin, M. Jansen, B. Keimer. Phys. Rev. Lett. 101 (2008), 047202
- S. P. Bayrakci, T. Keller, K. Habicht, B. Keimer. Science 312 (2006), 1926
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Figures
a) NaCu2O2, the progenitor of a new family of charge-ordered spin chain compounds. Neutron diffraction measurements revealed that the ground state has helicoidal magnetic order due to competing interactions [2].
b) Charge order and magnetic structure of the doped copper oxide spin-chain compound Na8Cu5O10
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