1,891 research outputs found
Muon-spin-relaxation and magnetic-susceptibility studies of effects of the magnetic impurity Ni on the Cu-spin dynamics and superconductivity in La_2-x_Sr_x_Cu_1-y_Ni_y_O_4_ with x = 0.13
Effects of the magnetic impurity Ni on the Cu-spin dynamics and
superconductivity have been studied in La_2-x_Sr_x_Cu_1-y_Ni_y_O_4_ with x =
0.13 changing y finely up to 0.10. Compared with the case of the nonmagnetic
impurity Zn, it has been found from the muon-spin-relaxation measurements that
a large amount of Ni is required to stabilize a magnetic order of Cu spins.
However, the evolution toward the stabilization of the magnetic order with
increasing impurity concentration is qualitatively similar to each other. The
area of the non-superconducting and slowly fluctuating or static region of Cu
spins around Ni has been found to be smaller than that around Zn, suggesting
that the pinning of rather long-ranged dynamical spin correlation such as the
so-called dynamical stripe by Ni is weaker than that by Zn. This may be the
reason why Zn destroys the superconductivity in the hole-doped high-T_c_
cuprates more markedly than Ni.Comment: 4 pages, 4 figures, accepted for publication in Phys. Rev.
ADAP Pesticide Applicator Training: Instructor's Manual
A survey course which covers the pests and diseases of crop plants with specific reference to Pacific Island conditions. The fields of Entomology, Plant Pathology, and Weed Science are each presented within the context of an integrated pest management system. Each topic includes objectives, vocabulary, lecture outlines, and review questions. Regionally important pests and disease cycles are thoroughly illustratedFunded through the U.S. Department of Agriculture Cooperative State Research, Education, and Extension Service. Grant 194-38826-0l79
Scalability of spin FPGA: A Reconfigurable Architecture based on spin MOSFET
Scalability of Field Programmable Gate Array (FPGA) using spin MOSFET (spin
FPGA) with magnetocurrent (MC) ratio in the range of 100% to 1000% is discussed
for the first time. Area and speed of million-gate spin FPGA are numerically
benchmarked with CMOS FPGA for 22nm, 32nm and 45nm technologies including 20%
transistor size variation. We show that area is reduced and speed is increased
in spin FPGA owing to the nonvolatile memory function of spin MOSFET.Comment: 3 pages, 7 figure
Massive galaxies in cosmological simulations: UV-selected sample at redshift z=2
We study the properties of galaxies at z=2 in a Lambda CDM universe, using
two different types of hydrodynamic simulation methods (Eulerian TVD and SPH)
and a spectrophotometric analysis in the Un, G, R filter set. The simulated
galaxies at z=2 satisfy the color-selection criteria proposed by Adelberger et
al. (2004) when we assume Calzetti extinction with E(B-V)=0.15. We find that
the number density of simulated galaxies brighter than R<25.5 at z=2 is about
2e-2 h^3/Mpc^3, roughly one order of magnitude larger than that of Lyman break
galaxies at z=3. The most massive galaxies at z=2 have stellar masses >~1e11
Msun, and their observed-frame G-R colors lie in the range 0.0<G-R<1.0. They
typically have been continuously forming stars with a rate exceeding 30 Msun/yr
over a few Gyrs from z=10 to z=2, although the TVD simulation indicates a more
sporadic star formation history than the SPH simulations. Of order half of
their stellar mass was already assembled by z~4. The reddest massive galaxies
at z=2 with G-R >= 1.0 and Mstar>1e10 Msun/h finished the build-up of their
stellar mass by z~3. Interestingly, our study suggests that the majority of the
most massive galaxies at z=2 should be detectable at rest-frame UV wavelengths,
contrary to some recent claims made on the basis of near-IR studies of galaxies
at the same epoch, provided the median extinction is less than E(B-V)<0.3.
However, our results also suggest that the fraction of stellar mass contained
in galaxies that pass the color-selection criteria could be as low as 50% of
the total stellar mass in the Universe at z=2. Our simulations suggest that the
missing stellar mass is contained in fainter (R>25.5) and intrinsically redder
galaxies. Our results do not suggest that hierarchical galaxy formation fails
to account for the massive galaxies at z>=1. (abridged)Comment: 35 pages, 11 figures. Submitted to ApJ. Error in AB magnitude
calculation corrected. Higher resolution version available at
http://cfa-www.harvard.edu/~knagamine/redgal.ps.g
The effect of beam inclination on the performance of a passive vibration isolator using buckled beams
Passive vibration isolators are desired to have both high static stiffness to support large static load and low local stiffness to reduce the displacement transmissibility at frequencies greater than resonance. Utilization of a vertical buckled beam as a spring component is one way to realize such a stiffness characteristic since it exhibits a smaller ratio of local stiffness to static stiffness than that of a linear spring. This paper investigates the behaviour of a vibration isolator using inclined beams as well as vertical ones and examines the effect of beam inclination for the purpose of improving the isolation performance. The experimental system investigated has anisolated mass which is supported by a combination of two types of beams: buckled beams and constraining beams. The buckled beams can be inclined from the vertical by attachment devices, and the constraining beams are employed to prevent off-axis motion of the isolated mass. The results demonstrate that the inclination of the buckled beams reduces the resonance frequency and improves the displacement transmissibility at frequencies greater than resonance
Absence of the impurity-induced magnetic order in the electron-doped high-T_c_ cuprates Pr_0.86_LaCe_0.14_Cu_1-y_(Zn, Ni)_y_O_4_
Zero-field muon-spin-relaxation measurements have been carried out in order
to investigate the Zn- and Ni-substitution effects on the Cu-spin dynamics in
the electron-doped Pr_0.86_LaCe_0.14_Cu_1-y_(Zn, Ni)_y_O_4+\alpa-\delta_ with y
= 0, 0.01, 0.02, 0.05 and different values of the reduced oxygen content
\delta(\delta \le 0.09). For the samples with y = 0 and very small \delta
values of \delta < 0.01, a muon-spin precession due to the formation of a
long-range antiferromagnetic order has been observed at low temperatures below
\~ 5 K. For the moderately oxygen-reduced samples of 0.01 \le \delta \le 0.09,
on the contrary, no muon-spin precession has been observed and the temperature
dependence of the spectra is similar to one another regardless of the y value.
That is, no impurity-induced slowing down of the Cu-spin fluctuations has been
detected, which is very different from the results of the hole-doped high-T_c_
cuprates. The reason is discussed.Comment: 13 pages, 2 figures, Proceedings of ISS2004 (to be published in
Physica C
Astrophysics: Most distant cosmic blast seen
The most distant -ray burst yet sighted is the earliest astronomical object
ever observed in cosmic history. This ancient beacon offers a glimpse of the
little-known cosmic dark ages.Comment: Published in Nature News & View
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