68 research outputs found
Tuning the spin dynamics of kagome systems
Despite the conceptional importance of realizing spin liquids in solid states
only few compounds are known. On the other side the effect of lattice
distortions and anisotropies on the magnetic exchange topology and the
fluctuation spectrum are an interesting problem. We compare the excitation
spectra of the two s=1/2 kagome lattice compounds volborthite and vesignieite
using Raman scattering. We demonstrate that even small modifications of the
crystal structure may have a huge effect on the phonon spectrum and low
temperature properties.Comment: 3 pages, 2 figure
Dynamical Dzyaloshinsky-Moriya interaction in KCuF3: Raman evidence for an antiferrodistortive lattice instability
In the orbitally ordered, quasi-one dimensional Heisenberg antiferromagnet
KCuF3 the low-energy Eg and B1g phonon modes show an anomalous softening (25%
and 13%) between room temperature and the characteristic temperature T_S = 50
K. In this temperature range a freezing-in of F ion dynamic displacements is
proposed to occur. In addition, the Eg mode at about 260 cm-1 clearly splits
below T_S. The width of the phonon lines above T_S follows an activated
behavior with an activation energy of about 50 K. Our observations clearly
evidence a reduction of the structural symmetry below T_S and indicate a strong
coupling of lattice and spin fluctuations for T>T_S.Comment: 7 pages, 9 figure
Dynamical lattice instability versus spin liquid state in a frustrated spin chain system
The low-dimensional s=1/2 compound (NO)[Cu(NO3)3] has recently been suggested
to follow the Nersesyan-Tsvelik model of coupled spin chains. Such a system
shows unbound spinon excitations and a resonating valence bond ground state due
spin frustration. Our Raman scattering study demonstrates phonon anomalies as
well as the suppression of a broad magnetic scattering continuum for
temperatures below a characteristic temperature, T<T*=100K. We interpret these
effects as evidence for a dynamical interplay of spin and lattice degrees of
freedom that might lead to a further transition into a dimerized or
structurally distorted phase at lower temperatures.Comment: 5 pages, 6 figure
Optical phonons, spin correlations, and spin-phonon coupling in the frustrated pyrochlore magnets CdCr2O4 and ZnCr2O4
We report on infrared, Raman, magnetic susceptibility, and specific heat
measurements on CdCr2O4 and ZnCr2O4 single crystals. We estimate the
nearest-neighbor and next-nearest neighbor exchange constants from the magnetic
susceptibility and extract the spin-spin correlation functions obtained from
the magnetic susceptibility and the magnetic contribution to the specific heat.
By comparing with the frequency shift of the infrared optical phonons above TN
, we derive estimates for the spin-phonon coupling constants in these systems.
The observation of phonon modes which are both Raman and infrared active
suggest the loss of inversion symmetry below the Neel temperature in CdCr2O4 in
agreement with theoretical predictions by Chern and coworkers [Phys. Rev. B 74,
060405 (2006)]. In ZnCr2O4 several new modes appear below TN, but no phonon
modes could be detected which are both Raman and infrared active indicating the
conservation of inversion symmetry in the low temperature phase.Comment: 11 pages, 13 figure
Evidence for Dimer Crystal Melting in the Frustrated Spin-Ladder BiCu2PO6
In the spin ladder compound BiCuPO there exists a decisive dynamics
of spin excitations that we classify and characterize using inelastic light
scattering. We observe low-energy singlets and a broad triplon continuum
extending from 36 cm to 700 cm in (), (), and ()
light scattering polarizations. Though isolated spin ladder physics can roughly
account for the observed excitations at high energies, frustration and
interladder interactions need to be considered to fully describe the spectral
distribution and scattering selection rules at low and intermediate energies.
More significantly, an interladder singlet bound mode at 24 cm, lying
below the continuum, shows its largest scattering intensity in interladder
() polarization. In contrast, two intraladder bound states at 62 cm
and 108 cm with energies comparable to the continuum are observed with
light polarization along the leg () and the rung (). We attribute the
rich spectrum of singlet bound modes to a melting of a dimer crystal. Our study
provides evidence for a Z quantum phase transition from a dimer to a
resonating valence bond state driven by singlet fluctuations.Comment: 14 pages, 4 figures, Accepted for publication in PR
Enhanced quasiparticle dynamics of quantum well states: the giant Rashba system BiTeI and topological insulators
In the giant Rashba semiconductor BiTeI electronic surface scattering with
Lorentzian linewidth is observed that shows a strong dependence on surface
termination and surface potential shifts. A comparison with the topological
insulator Bi2Se3 evidences that surface confined quantum well states are the
origin of these processes. We notice an enhanced quasiparticle dynamics of
these states with scattering rates that are comparable to polaronic systems in
the collision dominated regime. The Eg symmetry of the Lorentzian scattering
contribution is different from the chiral (RL) symmetry of the corresponding
signal in the topological insulator although both systems have spin-split
surface states.Comment: 6 pages, 5 figure
Magnetic domain tuning and the emergence of bubble domains in the bilayer manganite La 2−2x Sr 1+2x Mn 2 O 7 (x=0.32)
We report a magnetic force microscopy study of the magnetic domain evolution in the layered manganite La2-2x Sr1+2x Mn2O7 (with x = 0.32). This strongly correlated electron compound is known to exhibit a wide range of magnetic phases, including a recently uncovered biskyrmion phase. We observe a continuous transition from dendritic to stripelike domains, followed by the formation of magnetic bubbles due to a field-and temperaturedependent competition between in-plane and out-of-plane spin alignments. The magnetic bubble phase appears at comparable field and temperature ranges as the biskyrmion phase, suggesting a close relation between both phases. Based on our real-space images we construct a temperature-field phase diagram for this composition.open115Ysciescopu
Lattice and electronic anomalies of CaFe_2As_2 studied by Raman spectroscopy
We report inelastic light scattering experiments on CaFe_2As_2 in the
temperature range of 4 to 290 K. In in-plane polarizations two Raman-active
phonon modes are observed at 189 and 211 cm-1, displaying A_1g and B_1g
symmetries, respectively. Upon heating through the tetragonal-to-orthorhombic
transition at about T_S=173 K, the B_1g phonon undergoes a discontinuous drop
of the frequency by 4 cm-1 whereas the A_1g phonon shows a suppression of the
integrated intensity. Their linewidth increases strongly with increasing
temperature and saturates above T_S. This suggests (i) a first-order structural
phase transition and (ii) a drastic change of charge distribution within the
FeAs plane through T_S.Comment: 4 pages, 4 figure
Soft tilt and rotational modes in the hybrid improper ferroelectric CaMnO
Raman spectroscopy is employed to probe directly the soft rotation and
tilting modes, which are two primary order parameters predicted in the hybrid
improper ferroelectric material CaMnO. We observe a giant softening
of the 107-cm octahedron tilting mode by 26~cm, on heating
through the structural transition from a ferroelectric to paraelectric
orthorhombic phase. This is contrasted by a small softening of the
150-cm rotational mode by 6~cm. In the intermediate phase, the
competing soft modes with different symmetries coexist, bringing about
many-faceted anomalies in spin excitations and lattice vibrations. Our work
demonstrates that the soft rotation and tilt patterns, relying on a
phase-transition path, are a key factor in determining ferroelectric, magnetic,
and lattice properties of CaMnO.Comment: accepted for publication in PR
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