940 research outputs found
Universal behavior of spin-mediated energy transport in S=1/2 chain cuprates: BaCu2Si2O7 as an example
The thermal conductivity of the spin-1/2 chain cuprate BaCu2Si2O7 was
measured along different crystallographic directions in the temperature region
between 0.5 and 300 K. The thermal conductivity along the chain direction
considerably exceeds that along perpendicular directions. Near the
antiferromagnetic transition at T_N = 9.2 K the data indicates enhanced
scattering of phonons by critical fluctuations in the spin system. A comparison
of the data above T_N with available results on similar materials reveals
similarities in the main features of the temperature dependence of the mean
free path of itinerant spin excitations. This universal behavior is most likely
caused by the spin-lattice interaction.Comment: 7 pages, 3 figure
Effect of Pt doping on the critical temperature and upper critical field in YNi2-xPtxB2C (x=0-0.2)
We investigate the evolution of superconducting properties by doping
non-magnetic impurity in single crystals of YNi2-xPtxB2C (x=0-0.2). With
increasing Pt doping the critical temperature (Tc) monotonically decreases from
15.85K and saturates to a value ~13K for x>0.14. However, unlike conventional
s-wave superconductors, the upper critical field (HC2) along both
crystallographic directions a and c decreases with increasing Pt doping.
Specific heat measurements show that the density of states (N(EF)) at the Fermi
level (EF) and the Debye temperatures (Theta_D) in this series remains constant
within the error bars of our measurement. We explain our results based on the
increase in intraband scattering in the multiband superconductor YNi2B2C.Comment: ps file with figure
Thermo-magnetic history effects in the vortex state of YNi_2B_2C superconductor
The nature of five-quadrant magnetic isotherms for is different from that for
in a single crystal of YNi2B2C, pointing towards an anisotropic behaviour of
the flux line lattice (FLL). For, a well defined peak effect (PE) and second
magnetization peak (SMP) can be observed and the loop is open prior to the PE.
However, for, the loop is closed and one can observe only the PE. We have
investigated the history dependence of magnetization hysteresis data for by
recording minor hysteresis loops. The observed history dependence in across
different anomalous regions are rationalized on the basis of
su-perheating/supercooling of the vortex matter across the first-order-like
phase transition and possible additional effects due to annealing of the
disordered vortex bundles to the underlying equilibrium state.Comment: 4 pages, 4 figure
Lanthanide Al-Ni base Ericsson cycle magnetic refrigerants
A magnetic refrigerant for a magnetic refrigerator using the Ericsson thermodynamic cycle comprises DyAlNi and (Gd.sub.0.54 Er.sub.0.46)AlNi alloys having a relatively constant ΔTmc over a wide temperature range
Field-induced charge transport at the surface of pentacene single crystals: a method to study charge dynamics of 2D electron systems in organic crystals
A method has been developed to inject mobile charges at the surface of
organic molecular crystals, and the DC transport of field-induced holes has
been measured at the surface of pentacene single crystals. To minimize damage
to the soft and fragile surface, the crystals are attached to a pre-fabricated
substrate which incorporates a gate dielectric (SiO_2) and four probe pads. The
surface mobility of the pentacene crystals ranges from 0.1 to 0.5 cm^2/Vs and
is nearly temperature-independent above ~150 K, while it becomes thermally
activated at lower temperatures when the induced charges become localized.
Ruling out the influence of electric contacts and crystal grain boundaries, the
results contribute to the microscopic understanding of trapping and detrapping
mechanisms in organic molecular crystals.Comment: 14 pages, 4 figures. Submitted to J. Appl. Phy
Tuning in magnetic modes in Tb(Co_{x}Ni_{1-x})_{2}B_{2}C: from longitudinal spin-density waves to simple ferromagnetism
Neutron diffraction and thermodynamics techniques were used to probe the
evolution of the magnetic properties of Tb(Co_{x}Ni_{1-x})_{2}B_{2}C. A
succession of magnetic modes was observed as x is varied: the longitudinal
modulated k=(0.55,0,0) state at x=0 is transformed into a collinear
k=([nicefrac]\nicefrac{1}{2},0,[nicefrac]\nicefrac{1}{2})
antiferromagnetic state at x= 0.2, 0.4; then into a transverse c-axis modulated
k=(0,0,[nicefrac]\nicefrac{1}{3}) mode at x= 0.6, and finally
into a simple ferromagnetic structure at x= 0.8 and 1. Concomitantly, the
low-temperature orthorhombic distortion of the tetragonal unit cell at x=0 is
reduced smoothly such that for x >= 0.4 only a tetragonal unit cell is
manifested. Though predicted theoretically earlier, this is the first
observation of the k=(0,0,[nicefrac]\nicefrac{1}{3}) mode in
borocarbides; our findings of a succession of magnetic modes upon increasing x
also find support from a recently proposed theoretical model. The implication
of these findings and their interpretation on the magnetic structure of the
RM_{2}B_{2}C series are also discussed
Intersubband electronic Raman scattering in narrow GaAs single quantum wells dominated by single-particle excitations
We measured resonant Raman scattering by intersubband electronic excitations
in GaAs/AlAs single quantum wells (QWs) with well widths ranging from 8.5 to 18
nm. In narrow (less than 10 nm) QWs with sufficiently high electron
concentrations, only single-particle excitations (SPEs) were observed in
intersubband Raman scattering, which was confirmed by the well-width dependence
of Raman spectra. We found characteristic variations in Raman shift and line
shape for SPEs with incident photon energy in the narrow QWs.Comment: 5 pages including 4 figure
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