194 research outputs found
Gaps and excitations in fullerides with partially filled bands : NMR study of Na2C60 and K4C60
We present an NMR study of Na2C60 and K4C60, two compounds that are related
by electron-hole symmetry in the C60 triply degenerate conduction band. In both
systems, it is known that NMR spin-lattice relaxation rate (1/T1) measurements
detect a gap in the electronic structure, most likely related to
singlet-triplet excitations of the Jahn-Teller distorted (JTD) C60^{2-} or
C60^{4-}. However, the extended temperature range of the measurements presented
here (10 K to 700 K) allows to reveal deviations with respect to this general
trend, both at high and low temperatures. Above room temperature, 1/T1 deviates
from the activated law that one would expect from the presence of the gap and
saturates. In the same temperature range, a lowering of symmetry is detected in
Na2C60 by the appearance of quadrupole effects on the 23Na spectra. In K4C60,
modifications of the 13C spectra lineshapes also indicate a structural
modification. We discuss this high temperature deviation in terms of a coupling
between JTD and local symmetry. At low temperatures, 1/TT tends to a
constant value for Na2C60, both for 13C and 23Na NMR. This indicates a residual
metallic character, which emphasizes the proximity of metallic and insulting
behaviors in alkali fullerides.Comment: 12 pages, 13 figure
Surface charging of thick porous water ice layers relevant for ion sputtering experiments
We use a laboratory facility to study the sputtering properties of
centimeter-thick porous water ice subjected to the bombardment of ions and
electrons to better understand the formation of exospheres of the icy moons of
Jupiter. Our ice samples are as similar as possible to the expected moon
surfaces but surface charging of the samples during ion irradiation may distort
the experimental results. We therefore monitor the time scales for charging and
dis- charging of the samples when subjected to a beam of ions. These
experiments allow us to derive an electric conductivity of deep porous ice
layers. The results imply that electron irradiation and sputtering play a
non-negligible role for certain plasma conditions at the icy moons of Jupiter.
The observed ion sputtering yields from our ice samples are similar to previous
experiments where compact ice films were sputtered off a micro-balance.Comment: arXiv admin note: text overlap with arXiv:1509.0400
Role of dynamic Jahn-Teller distortions in Na2C60 and Na2CsC60 studied by NMR
Through 13C NMR spin lattice relaxation (T1) measurements in cubic Na2C60, we
detect a gap in its electronic excitations, similar to that observed in
tetragonal A4C60. This establishes that Jahn-Teller distortions (JTD) and
strong electronic correlations must be considered to understand the behaviour
of even electron systems, regardless of the structure. Furthermore, in metallic
Na2CsC60, a similar contribution to T1 is also detected for 13C and 133Cs NMR,
implying the occurence of excitations typical of JT distorted C60^{2-} (or
equivalently C60^{4-}). This supports the idea that dynamic JTD can induce
attractive electronic interactions in odd electron systems.Comment: 3 figure
Mn local moments prevent superconductivity in iron-pnictides Ba(Fe 1-x Mn x)2As2
75As nuclear magnetic resonance (NMR) experiments were performed on
Ba(Fe1-xMnx)2As2 (xMn = 2.5%, 5% and 12%) single crystals. The Fe layer
magnetic susceptibility far from Mn atoms is probed by the75As NMR line shift
and is found similar to that of BaFe2As2, implying that Mn does not induce
charge doping. A satellite line associated with the Mn nearest neighbours
(n.n.) of 75As displays a Curie-Weiss shift which demonstrates that Mn carries
a local magnetic moment. This is confirmed by the main line broadening typical
of a RKKY-like Mn-induced staggered spin polarization. The Mn moment is due to
the localization of the additional Mn hole. These findings explain why Mn does
not induce superconductivity in the pnictides contrary to other dopants such as
Co, Ni, Ru or K.Comment: 6 pages, 7 figure
Comment on "Isoelectronic Ru substitution at Fe-site in Sm(FeRu)AsOF compound and its effects on structural, superconducting and normal state properties" (arXiv:1004.1978)
Based on the five-orbital model, we derive the reduced impurity scattering
rate in Sm(FeRu)AsOF
from the residual resistivity. At , the transition temperature is
K. For ) the obtained value
of ranges from 1.5 to 2.9, which suggests that the -wave state
cannot survive. We point out that the magnetoresistance frequently gives an
underestimated value of in correlated electron systems.Comment: 2 page
Fermi Surface reconstruction in the CDW state of CeTe3 observed by photoemission
CeTe3 is a layered compound where an incommensurate Charge Density Wave (CDW)
opens a large gap (400 meV) in optimally nested regions of the Fermi Surface
(FS), whereas other sections with poorer nesting remain ungapped. Through
Angle-Resolved Photoemission, we identify bands backfolded according to the CDW
periodicity. They define FS pockets formed by the intersection of the original
FS and its CDW replica. Such pockets illustrate very directly the role of
nesting in the CDW formation but they could not be detected so far in a CDW
system. We address the reasons for the weak intensity of the folded bands, by
comparing different foldings coexisting in CeTe3
The degenerate 3-band Hubbard model with "anti-Hund's rule" interactions; a model for AxC60
We consider the orbitally degenerate 3-band Hubbard model with on-site
interactions which favor low spin and low orbital angular momentum using
standard second order perturbation theory in the large Hubbard-U limit. At even
integer filling this model is a Mott insulator with a non-degenerate ground
state that allows for a simple description of particle-hole excitations as well
as gapped spin and orbital modes. We find that the Mott gap is generally
indirect and that the single particle spectrum at low doping reappears close to
even filling but rescaled by a factor 2/3 or 1/3. The model captures the basic
phenomenology of the Mott insulating and metallic fullerides AxC60. This
includes the existence of a smaller spin gap and larger charge gap at even
integer filling, the fact that odd integer stoichiometries are generally
metallic while even are insulating, as well as the rapid suppression of the
density of states and superconducting transition temperatures with doping away
from x=3.Comment: Revised with additional reference
Influence of local fullerene orientation on the electronic properties of A3C60 compounds
We have investigated sodium containing fullerene superconductors Na2AC60, A =
Cs, Rb, and K, by Na-23 nuclear magnetic resonance (NMR) spectroscopy at 7.5 T
in the temperature range of 10 to 400 K. Despite the structural differences
from the Rb3C60 class of fullerene superconductors, in these compounds the NMR
line of the tetrahedrally coordinated alkali nuclei also splits into two lines
(T and T') at low temperature. In Na2CsC60 the splitting occurs at 170 K; in
the quenched cubic phase of Na2RbC60 and Na2KC60 we observe split lines at 80
K. Detailed investigations of the spectrum, spin-spin and spin-lattice
relaxation as well as spin-echo double resonance (SEDOR) in Na2CsC60 we show
that these two different tetrahedral sites are mixed on a microscopic scale.
The T and T' sites differ in the orientation of first-neighbor C60 molecules.
We present evidence that the orientations of neighboring molecules are
uncorrelated. Thermally activated molecular reorientations cause an exchange
between the T and T' sites and motional narrowing at high temperature. We infer
the same activation energy, 3300 K, in the temperature range 125 to 300 K. The
spin lattice relaxation rate is the same for T and T' down to 125 K but
different below. Both the spin-lattice relaxation rate and Knight shift are
strongly temperature dependent in the whole range investigated. We interpret
this temperature variation by the effect of phonon excitations involving the
rigid librational motion of the C60 molecules. By extending the understanding
of the structure and molecular dynamics of C60 superconductors, these results
may help in clarifying the effects of the structure on the superconducting
properties.Comment: 13 pages, 10 figures, submitted to PR
Nature of the bad metallic behavior of Fe_{1.06}Te inferred from its evolution in the magnetic state
We investigate with angle resolved photoelectron spectroscopy the change of
the Fermi Surface (FS) and the main bands from the paramagnetic (PM) state to
the antiferromagnetic (AFM) occurring below 72 K in Fe_{1.06}Te. The evolution
is completely different from that observed in iron-pnictides as nesting is
absent. The AFM state is a rather good metal, in agreement with our magnetic
band structure calculation. On the other hand, the PM state is very anomalous
with a large pseudogap on the electron pocket that closes in the AFM state. We
discuss this behavior in connection with spin fluctuations existing above the
magnetic transition and the correlations predicted in the spin-freezing regime
of the incoherent metallic state
Evidence for distinct polymer chain orientations in KC60 and RbC60
The KC60 and RbC60 polymer phases exhibit contrasting electronic properties
while powder diffraction studies have revealed no definite structural
difference. We have performed single crystal X-ray diffraction and diffuse
scattering studies of these compounds. It is found that KC60 and RbC60 possess
different chain orientations about their axes, which are described by distinct
space groups Pmnn and I2/m, respectively. Such a structural difference will be
of great importance to a complete understanding of the physical properties.Comment: To be published in Phys. Rev. Let
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