967 research outputs found
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
An Efficient Algorithm for Enumerating Chordless Cycles and Chordless Paths
A chordless cycle (induced cycle) of a graph is a cycle without any
chord, meaning that there is no edge outside the cycle connecting two vertices
of the cycle. A chordless path is defined similarly. In this paper, we consider
the problems of enumerating chordless cycles/paths of a given graph
and propose algorithms taking time for each chordless cycle/path. In
the existing studies, the problems had not been deeply studied in the
theoretical computer science area, and no output polynomial time algorithm has
been proposed. Our experiments showed that the computation time of our
algorithms is constant per chordless cycle/path for non-dense random graphs and
real-world graphs. They also show that the number of chordless cycles is much
smaller than the number of cycles. We applied the algorithm to prediction of
NMR (Nuclear Magnetic Resonance) spectra, and increased the accuracy of the
prediction
Cu- and Cl-NMR Studies of Triplet Localization in the Quantum Spin System NHCuCl
Cu- and Cl-NMR experiments were performed to investigate
triplet localization in the dimer compound NHCuCl, which shows
magnetization plateaus at one-quarter and three-quarters of the saturation
magnetization. In Cu-NMR experiments, signal from only the singlet Cu
site was observed, because that from the triplet Cu site was invisible due to
the strong spin fluctuation of onsite 3-spins. We found that the temperature
dependence of the shift of Cu-NMR spectra at the singlet Cu site
deviated from that of macroscopic magnetization below T=6 K. This deviation is
interpreted as the triplet localization in this system. From the
Cl-NMR experiments at the 1/4-plateau phase, we found the two
different temperature dependences of Cl-shift, namely the temperature
dependence of one deviates below T=6 K from that of the macroscopic
magnetization as observed in the Cu-NMR experiments, whereas the
other corresponds well with that of the macroscopic magnetization in the entire
experimental temperature region. We interpreted these dependences as reflecting
the transferred hyperfine field at the Cl site located at a singlet site and at
a triplet site, respectively. This result also indicates that the triplets are
localized at low temperatures. Cu-NMR experiments performed at high
magnetic fields between the one-quarter and three-quarters magnetization
plateaus have revealed that the two differently oriented dimers in the unit
cell are equally occupied by triplets, the fact of which limits the theoretical
model on the periodic structure of the localized triplets.Comment: 19 pages, 9 figures, submitted to PRB (in press
Kernels for graphs
This chapter contains sections titled: Introduction, Label Sequence Kernel between Labeled Graphs, Experiments, Related Works, Conclusion
Space-Time Structure of Loop Quantum Black Hole
In this paper we have improved the semiclassical analysis of loop quantum
black hole (LQBH) in the conservative approach of constant polymeric parameter.
In particular we have focused our attention on the space-time structure. We
have introduced a very simple modification of the spherically symmetric
Hamiltonian constraint in its holonomic version. The new quantum constraint
reduces to the classical constraint when the polymeric parameter goes to
zero.Using this modification we have obtained a large class of semiclassical
solutions parametrized by a generic function of the polymeric parameter. We
have found that only a particular choice of this function reproduces the black
hole solution with the correct asymptotic flat limit. In r=0 the semiclassical
metric is regular and the Kretschmann invariant has a maximum peaked in
L-Planck. The radial position of the pick does not depend on the black hole
mass and the polymeric parameter. The semiclassical solution is very similar to
the Reissner-Nordstrom metric. We have constructed the Carter-Penrose diagrams
explicitly, giving a causal description of the space-time and its maximal
extension. The LQBH metric interpolates between two asymptotically flat
regions, the r to infinity region and the r to 0 region. We have studied the
thermodynamics of the semiclassical solution. The temperature, entropy and the
evaporation process are regular and could be defined independently from the
polymeric parameter. We have studied the particular metric when the polymeric
parameter goes towards to zero. This metric is regular in r=0 and has only one
event horizon in r = 2m. The Kretschmann invariant maximum depends only on
L-Planck. The polymeric parameter does not play any role in the black hole
singularity resolution. The thermodynamics is the same.Comment: 17 pages, 19 figure
Infrared Photodissociation Spectroscopy of H+(CH3OH)n-Ar (n=1-3)
第19回化学反応討論会, 2003年6月11日-6月13日, 仙台市戦災復興記念館(仙台
Intermolecular interaction in the benzene-benzyl alcohol hetero-dimer ion
第16回化学反応討論会, 2000年6月1日-3日, サタケ講堂(東広島
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