2,214 research outputs found
Theory of AC Anomalous Hall Conductivity in d-electron systems
To elucidate the intrinsic nature of anomalous Hall effect (AHE) in
-electron systems, we study the AC anomalous Hall conductivity (AHC) in a
tight-binding model with ()-orbitals. We drive a general
expression for the AC AHC , which is valid for finite
quasiparticle damping rate =, and find that the AC AHC is
strongly dependent on . When , the AC AHC shows a spiky peak
at finite energy that originates from the interband particle-hole
excitation, where represents the minimum band-splitting measured from
the Fermi level. In contrast, we find that this spiky peak is quickly
suppressed when is finite. By using a realistic value of
at in -electron systems, the spiky peak
is considerably suppressed. In the present model, the obtained results also
represents the AC spin Hall conductivity in a paramagnetic state.Comment: 13pages, 9 figure
Anisotropic intrinsic anomalous Hall effect in ordered 3dPt alloys
By performing first principles calculations we investigate the intrinsic
anomalous Hall conductivity (AHC) and its anisotropy in ordered L1o FePt, CoPt
and NiPt ferromagnets, and their intermediate alloys. We demonstrate that the
AHC in this family of compounds depends strongly on the direction of the
magnetization in the crystal. We predict that such pronounced orientational
dependence in combination with the general decreasing trend of the AHC when
going from FePt to NiPt leads to a sign change of the AHC upon rotating the
magnetization direction in the crystal of CoPt alloy. We also suggest that for
a range of concentration x in Co(x)Ni(1-x)Pt alloy it is possible to achieve a
complete quenching of the anomalous Hall current for a certain direction of the
magnetization in the crystal. By analyzing the spin-resolved AHC in 3dPt alloys
we endeavor to relate the overall trend of the AHC in these compounds to the
changes in their densities of d-states around the Fermi energy upon varying the
atomic number. Moreover, we show the generality of the phenomenon of
anisotropic anomalous Hall effect by demonstrating its occurrence within the
three-band tight-binding model.Comment: 10 page
Correlation of high energy muons with primary composition in extensive air shower
An experimental investigation of high energy muons above 200 GeV in extensive air showers has been made for studying high energy interaction and primary composition of cosmic rays of energies in the range 10 to the 14th power approx. 10 to the 15th power eV. The muon energies are estimated from the burst sizes initiated by the muons in the rock, which are measured by four layers of proportional counters, each of area 5 x 2.6 sq m, placed at 30 m.w.e. deep, Funasaka tunnel vertically below the air shower array. These results are compared with Monte Carlo simulations based on the scaling model and the fireball model for two primary compositions, all proton and mixed
Proportional drift tubes for large area muon detectors
A proportional drift chamber which consists of eight rectangular drift tubes with cross section of 10 cm x 5 cm, a sense wire of 100 micron phi gold-plated tungsten wire and the length of 6 m, was tested using cosmic ray muons. Spatial resolution (rms) is between 0.5 and 1 mm over drift space of 50 mm, depending on incident angle and distance from sense wire
Chromium at High Pressures: Weak Coupling and Strong Fluctuations in an Itinerant Antiferromagnet
The spin- and charge-density-wave order parameters of the itinerant
antiferromagnet chromium are measured directly with non-resonant x-ray
diffraction as the system is driven towards its quantum critical point with
high pressure using a diamond anvil cell. The exponential decrease of the spin
and charge diffraction intensities with pressure confirms the harmonic scaling
of spin and charge, while the evolution of the incommensurate ordering vector
provides important insight into the difference between pressure and chemical
doping as means of driving quantum phase transitions. Measurement of the charge
density wave over more than two orders of magnitude of diffraction intensity
provides the clearest demonstration to date of a weakly-coupled, BCS-like
ground state. Evidence for the coexistence of this weakly-coupled ground state
with high-energy excitations and pseudogap formation above the ordering
temperature in chromium, the charge-ordered perovskite manganites, and the blue
bronzes, among other such systems, raises fundamental questions about the
distinctions between weak and strong coupling.Comment: 11 pages, 9 figures (8 in color
Effects of non-frozen cold storage on the growth, organogenesis and secondary metabolism of callus cultures
Abstract. Callus tissues derived from chilling-tolerant herbaceous plant, Atractylodes lancea, Atropa belladonna, Bupleurum falcatum, Dioscorea tokoro, Lithospermum erythrorhizon and Phytolacca americana could be cold-stored at 4°C for three months or more, whereas those from chilling-sensitive herbaceous plants such as Datura innoxia and Perilla frutescens vat. crispa and a deciduous tree, Mallotus ]aponicus, could not survive after cold storage for two to three months. Tobacco callus cultures could be stored at 4°C for two or four months depending on a callus strain. The effect of cold storage on secondary metabolite production varied. Nicotine and betalain production suffered from cold storage of tobacco and Phytolacca americana callus cultures, respectively. However, production of anthocyanin in cultures of Mallotus ]aponicus and Bupleurum falcatum and shikonin derivatives in Lithospermum erythrorhizon callus was affected very little. Root-forming ability was retained for more than one year in cold-stored callus tissues of Bupleurum falcatum, while the control callus tissues maintained at 25°C completely lost the organogenetic ability six months after the first subculture
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Precise measurements of the energy losses of heavy ions
Accurate measurements of the energy loss of all charged particles are needed to determine the reliability of the Bethe theory of stopping power. Few measurements have been made for particles with energies greater than 20 MeV/u. A first step to accurate measurements is to establish the precision of an experimental method. The authors report here about the recent energy loss measurements for 290 MeV/u carbon ions from the HIMAC. They have been made with the method used for 70 MeV protons. The ion beam traverses an absorber of thickness t and the residual range of the ions is measured with a water container of adjustable thickness (``range gauge``)
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