58 research outputs found
力量調整を伴うタイミング動作の分析
本研究は, 力量調整を伴うタイミング動作について検討を加えた。被験者は男女各8名の計16名であった。課題は移動指標がタイミング点に到達する時点に合わせて, 三本の指で指圧力盤のボタンに瞬間的に力を加えるというものである。反応する力量は, 移動指標がタイミング点到達前に probe として呈示され, 2kgか5kgのいずれかであった。また probe 呈示時期は, タイミング点前480, 400, 320, 280, 240msの5条件であった。40試行の力量記銘試行につづき, 20試行のタイミング練習試行が行われ, その後30試行のテスト試行が行われた。力量再生におけるPCEの分析から, 2kgの方が5kgより有意に undershooting する傾向が認められた。これはタイミング動作ではより小さな力の方が再生が困難で, undershooting する傾向を示していると考えられた。また, タイミング誤差の分析から, probe 呈示時期が遅くなるにつれ, 遅延反応が見られることが明らかになった。このことから, 力量情報の処理を伴う選択反応時間が500ms程度ではないかと考えられた。The present study investigated the effect of the selective force reproduction on coincident timing task. The task assigned to the sixteen subjects was to synchronize the peak force of pressing the key by their three fingers with the arrival of moving target at the timing point. The criterion forces which were consisted of 2kg and 5kg were determined by the probe that was presented at predetermined five different times, which were 480, 400, 320, 280, and 240 msec before the timing point respectively. Before the 30 test trials without KR, 20 trials on each criterion force as the original learning, and as timing training trial 10 trials on each criterion force were completed with KR. The result of percent constant error (PCE) on the force reproduction showed that the PCE on 2kg tended to undershoot rather than the PCE on 5kg significantly. This result suggested the movements required a fine force recall could be difficult to control exactly, and the subjects required 2 kg for force reproduction in the present study experienced more difficulty processing the probe that was presented just prior to, or simultaneously with timing response. The result of timing constant error showed that the tendency toward time delay increased as a function of the probe presentation time on both criterion forces. It appears that these timing delay due to processing force information, therefore the choice reaction time on force reproductin would be necessary to about 500 msec
CO(=1-0) mapping survey of 64 galaxies in the Fornax cluster with the ALMA Morita array
We conduct a CO(=1-0) (hereafter CO) mapping survey of 64
galaxies in the Fornax cluster using the ALMA Morita array in cycle 5. CO
emission is detected from 23 out of the 64 galaxies. Our sample includes dwarf,
spiral and elliptical galaxies with stellar masses of ~M. The achieved beam size and sensitivity are
and ~mJy~beam at the velocity resolution of
~km~s, respectively. We study the cold-gas (molecular- and
atomic-gas) properties of 38 subsamples with ~M
combined with literature HI data. We find that: (1) the low star-formation (SF)
activity in the Fornax galaxies is caused by the decrease in the cold-gas mass
fraction with respect to stellar mass (hereafter, gas fraction) rather than the
decrease of the SF efficiency from the cold gas; (2) the atomic-gas fraction is
more heavily reduced than the molecular-gas fraction of such galaxies with low
SF activity. A comparison between the cold-gas properties of the Fornax
galaxies and their environmental properties suggests that the atomic gas is
stripped tidally and by the ram pressure, which leads to the molecular gas
depletion with an aid of the strangulation and consequently SF quenching.
Pre-processes in the group environment would also play a role in reducing
cold-gas reservoirs in some Fornax galaxies.Comment: 53 pages, 41 figures, accepted for publication in ApJ
EMPRESS. IX. Extremely Metal-Poor Galaxies are Very Gas-Rich Dispersion-Dominated Systems: Will JWST Witness Gaseous Turbulent High-z Primordial Galaxies?
We present kinematics of 6 local extremely metal-poor galaxies (EMPGs) with
low metallicities () and low stellar masses
(). Taking deep medium-high resolution
() integral-field spectra with 8.2-m Subaru, we resolve the small
inner velocity gradients and dispersions of the EMPGs with H emission.
Carefully masking out sub-structures originated by inflow and/or outflow, we
fit 3-dimensional disk models to the observed H flux, velocity, and
velocity-dispersion maps. All the EMPGs show rotational velocities () of 5--23 km s smaller than the velocity dispersions
() of 17--31 km s, indicating dispersion-dominated () systems affected by inflow and/or outflow. Except
for two EMPGs with large uncertainties, we find that the EMPGs have very large
gas-mass fractions of . Comparing our results with
other H kinematics studies, we find that
decreases and increases with decreasing metallicity, decreasing
stellar mass, and increasing specific star-formation rate. We also find that
simulated high- () forming galaxies have gas fractions and dynamics
similar to the observed EMPGs. Our EMPG observations and the simulations
suggest that primordial galaxies are gas-rich dispersion-dominated systems,
which would be identified by the forthcoming James Webb Space Telescope (JWST)
observations at .Comment: Submitted to ApJ; After revisio
Conserved Charged Amino Acids within Sendai Virus C Protein Play Multiple Roles in the Evasion of Innate Immune Responses
One of the accessory proteins of Sendai virus (SeV), C, translated from an alternate reading frame of P/V mRNA has been shown to function at multiple stages of infection in cell cultures as well as in mice. C protein has been reported to counteract signal transduction by interferon (IFN), inhibit apoptosis induced by the infection, enhance the efficiency of budding of viral particles, and regulate the polarity of viral genome-length RNA synthesis to maximize production of infectious particles. In this study, we have generated a series of SeV recombinants containing substitutions of highly conserved, charged residues within the C protein, and characterized them together with previously-reported C′/C(−), 4C(−), and F170S recombinant viruses in infected cell cultures in terms of viral replication, cytopathogenicity, and antagonizing effects on host innate immunity. Unexpectedly, the amino acid substitutions had no or minimal effect on viral growth and viral RNA synthesis. However, all the substitutions of charged amino acids resulted in the loss of a counteracting effect against the establishment of an IFN-α-mediated anti-viral state. Infection by the virus (Cm2′) containing mutations at K77 and D80 induced significant IFN-β production, severe cytopathic effects, and detectable amounts of viral dsRNA production. In addition to the Cm2′ virus, the virus containing mutations at E114 and E115 did not inhibit the poly(I:C)-triggered translocation of cellular IRF-3 to the nucleus. These results suggest that the C protein play important roles in viral escape from induction of IFN-β and cell death triggered by infection by means of counteracting the pathway leading to activation of IRF-3 as well as of minimizing viral dsRNA production
Power-Law Inter-Spike Interval Distributions Infer a Conditional Maximization of Entropy in Cortical Neurons
The brain is considered to use a relatively small amount of energy for its efficient information processing. Under a severe restriction on the energy consumption, the maximization of mutual information (MMI), which is adequate for designing artificial processing machines, may not suit for the brain. The MMI attempts to send information as accurate as possible and this usually requires a sufficient energy supply for establishing clearly discretized communication bands. Here, we derive an alternative hypothesis for neural code from the neuronal activities recorded juxtacellularly in the sensorimotor cortex of behaving rats. Our hypothesis states that in vivo cortical neurons maximize the entropy of neuronal firing under two constraints, one limiting the energy consumption (as assumed previously) and one restricting the uncertainty in output spike sequences at given firing rate. Thus, the conditional maximization of firing-rate entropy (CMFE) solves a tradeoff between the energy cost and noise in neuronal response. In short, the CMFE sends a rich variety of information through broader communication bands (i.e., widely distributed firing rates) at the cost of accuracy. We demonstrate that the CMFE is reflected in the long-tailed, typically power law, distributions of inter-spike intervals obtained for the majority of recorded neurons. In other words, the power-law tails are more consistent with the CMFE rather than the MMI. Thus, we propose the mathematical principle by which cortical neurons may represent information about synaptic input into their output spike trains
The Hyper Suprime-Cam SSP survey: Overview and survey design
Hyper Suprime-Cam (HSC) is a wide-field imaging camera on the prime focus of the 8.2-m Subaru telescope on the summit of Mauna Kea in Hawaii. A team of scientists from Japan, Taiwan, and Princeton University is using HSC to carry out a 300-night multi-band imaging survey of the high-latitude sky. The survey includes three layers: the Wide layer will cover 1400 deg2 in five broad bands (grizy), with a 5 σ point-source depth of r ≈ 26. The Deep layer covers a total of 26 deg2 in four fields, going roughly a magnitude fainter, while the UltraDeep layer goes almost a magnitude fainter still in two pointings of HSC (a total of 3.5 deg2). Here we describe the instrument, the science goals of the survey, and the survey strategy and data processing. This paper serves as an introduction to a special issue of the Publications of the Astronomical Society of Japan, which includes a large number of technical and scientific papers describing results from the early phases of this survey
Seismic exploration at Fuji volcano with active sources : The outline of the experiment and the arrival time data
Fuji volcano (altitude 3,776m) is the largest basaltic stratovolcano in Japan. In late August and early September 2003, seismic exploration was conducted around Fuji volcano by the detonation of 500 kg charges of dynamite to investigate the seismic structure of that area. Seismographs with an eigenfrequency of 2 Hz were used for observation, positioned along a WSW-ENE line passing through the summit of the mountain. A total of 469 seismic stations were installed at intervals of 250-500 m. The data were stored in memory on-site using data loggers. The sampling interval was 4 ms. Charges were detonated at 5 points, one at each end of the observation line and 3 along its length. The first arrival times and the later-phase arrival times at each station for each detonation were recorded as data. P-wave velocities in the surface layer were estimated from the travel time curves near the explosion points, with results of 2.5 km/s obtained for the vicinity of Fuji volcano and 4.0 km5/s elsewhere
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