281 research outputs found
Quasiparticle relaxation dynamics in spin-density-wave and superconducting SmFeAsO_{1-x}F_{x} single crystals
We investigate the quasiparticle relaxation and low-energy electronic
structure in undoped SmFeAsO and near-optimally doped SmFeAsO_{0.8}F_{0.2}
single crystals - exhibiting spin-density wave (SDW) ordering and
superconductivity respectively - using pump-probe femtosecond spectroscopy. In
the undoped single crystals a single relaxation process is observed, showing a
remarkable critical slowing down of the QP relaxation dynamics at the SDW
transition temperature T_{SDW}\simeq125{K}. In the superconducting (SC)
crystals multiple relaxation processes are present, with distinct SC state
quasiparticle recombination dynamics exhibiting a BCS-like T-dependent
superconducting gap, and a pseudogap (PG)-like feature with an onset above 180K
indicating the existence of a pseudogap of magnitude
2\Delta_{\mathrm{PG}}\simeq120 meV above T_{\mathrm{c}}. From the pump-photon
energy dependence we conclude that the SC state and PG relaxation channels are
independent, implying the presence of two separate electronic subsystems. We
discuss the data in terms of spatial inhomogeneity and multi-band scenarios,
finding that the latter is more consistent with the present data.Comment: Replaced by the correct versio
Ultrafast switching to a stable hidden topologically protected quantum state in an electronic crystal
Hidden states of matter with novel and unusual properties may be created if a
system out of equilibrium can be induced to follow a trajectory to a state
which is inaccessible or does not even exist under normal equilibrium
conditions. Here we report on the discovery of a hidden (H) topologically
protected electronic state in a layered dichalcogenide 1T-TaS2 crystal reached
as a result of a quench caused by a single 35 fs laser pulse. The properties of
the H state are markedly different from any other state of the system: it
exhibits a large drop of electrical resistance, strongly modified single
particle and collective mode spectra and a marked change of optical
reflectivity. Particularly important and unusual, the H state is stable for an
arbitrarily long time until a laser pulse, electrical current or thermal erase
procedure is applied, causing it to revert to the thermodynamic ground state.
Major observed events can be reproduced by a kinetic model describing the
conversion of photo excited electrons and holes into an electronically ordered
crystal, thus converting a Mott insulator to a conducting H state. Its
long-time stability follows from the topological protection of the number of
periods in the electronic crystal.Comment: 21 pages and 5 figures, separate supplementary materia
Controlled vaporization of the superconducting condensate in cuprate superconductors sheds light on the pairing boson
We use ultrashort intense laser pulses to study superconducting state
vaporization dynamics in La(2-x)Sr(x)CuO4 (x=0.1 and 0.15) on the femtosecond
timescale. We find that the energy density required to vaporize the
superconducting state is 2+- 0.8 K/Cu and 2.6 +- 1 K/Cu for x=0.1 and 0.15
respectively. This is significantly greater than the condensation energy
density, indicating that the quasiparticles share a large amount of energy with
the boson glue bath on this timescale. Considering in detail both spin and
lattice energy relaxation pathways which take place on the relevant timescale
of picoseconds, we rule out purely spin-mediated pair-breaking in favor of
phonon-mediated mechanisms, effectively ruling out spin-mediated pairing in
cuprates as a consequence.Comment: 5 pages of article plus 4 pages of supplementary materia
Effect of Mineral Nutrition on Red Clover Leaf Area Index
The legume red clover (Trifolium pratense) fixes its own nitrogen (N), but requires P and K fertilisation. There are no recent reliable data in the domestic literature, on the amounts of P and K recommended to farmers; present recommendations are often either inadequate or excessive. Red clover mineral nutrition is significantly affected by soil and weather conditions (Taylor & Quesenberry, 1996). The objective of our twoyear study was to enable rational fertiliser application in accordance with soil type and agro ecological conditions
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