248 research outputs found

    Alteration of phospholipid at various growth phases of Escherichia coli

    Get PDF
    By inoculating E. coli B into the semisynthetic medium we conducted shaking culture, and observed alterations of the total phospholipid contents and the amounts of individual phospholipid components in various stages of growth. The results are briefly summarized as follows. 1. The total phospholipid content has been found to be greater during early culture period, while it decreases as the growth age advances. 2. Phosphatidyl ethanolamine gradually increase as the culture period approaches the stationary phase. 3. Phosphatidic acid and phosphatidyl glycerol decrease precipitously as growth age advances. 4. Cardiolipin shows the maximum content in the middle log phase when the growth rate is most speedy.</p

    Atmospheric Delay Reduction Using KARAT for GPS Analysis and Implications for VLBI

    Get PDF
    We have been developing a state-of-the-art tool to estimate the atmospheric path delays by raytracing through mesoscale analysis (MANAL) data, which is operationally used for numerical weather prediction by the Japan Meteorological Agency (JMA). The tools, which we have named KAshima RAytracing Tools (KARAT)', are capable of calculating total slant delays and ray-bending angles considering real atmospheric phenomena. The KARAT can estimate atmospheric slant delays by an analytical 2-D ray-propagation model by Thayer and a 3-D Eikonal solver. We compared PPP solutions using KARAT with that using the Global Mapping Function (GMF) and Vienna Mapping Function 1 (VMF1) for GPS sites of the GEONET (GPS Earth Observation Network System) operated by Geographical Survey Institute (GSI). In our comparison 57 stations of GEONET during the year of 2008 were processed. The KARAT solutions are slightly better than the solutions using VMF1 and GMF with linear gradient model for horizontal and height positions. Our results imply that KARAT is a useful tool for an efficient reduction of atmospheric path delays in radio-based space geodetic techniques such as GNSS and VLBI

    Study on Constructions with English Verb get: Reflexive Pronouns and the Attenuation of Subject NP\u27s Force

    Get PDF
    13301乙第2084号博士(社会環境学)金沢大学博士論文本文Ful

    Study on Constructions with English Verb get: Reflexive Pronouns and the Attenuation of Subject NP\u27s Force

    Get PDF
    13301乙第2084号博士(社会環境学)金沢大学博士論文要旨Abstrac

    Scan-Less, Kilo-Pixel, Line-Field Confocal Phase Imaging with Spectrally Encoded Dual-Comb Microscopy

    Get PDF
    Confocal laser microscopy (CLM) is a powerful tool in life science research and industrial inspection, and its image acquisition rate is boosted by scan-less imaging techniques. However, the optical-intensity-based image contrast in CLM makes it difficult to visualize transparent non-fluorescent objects or reflective objects with nanometer unevenness. In this paper, we introduce an optical frequency comb (OFC) to scan-less CLM to give the optical-phase-based image contrast. One-dimensional (1D) image pixels of a sample are separately encoded onto OFC modes via 1D spectral encoding by using OFC as an optical carrier of amplitude and phase with a vast number of discrete frequency channels. Then, line-field confocal information of amplitude and phase are decoded from a mode-resolved OFC amplitude and phase spectra obtained by dual-comb spectroscopy. The proposed confocal phase imaging will further expand the application fields of CLM

    Scan-Less, Kilo-Pixel, Line-Field Confocal Phase Imaging with Spectrally Encoded Dual-Comb Microscopy

    Get PDF
    Confocal laser microscopy (CLM) is a powerful tool in life science research and industrial inspection, and its image acquisition rate is boosted by scan-less imaging techniques. However, the optical-intensity-based image contrast in CLM makes it difficult to visualize transparent non-fluorescent objects or reflective objects with nanometer unevenness. In this paper, we introduce an optical frequency comb (OFC) to scan-less CLM to give the optical-phase-based image contrast. One-dimensional (1D) image pixels of a sample are separately encoded onto OFC modes via 1D spectral encoding by using OFC as an optical carrier of amplitude and phase with a vast number of discrete frequency channels. Then, line-field confocal information of amplitude and phase are decoded from a mode-resolved OFC amplitude and phase spectra obtained by dual-comb spectroscopy. The proposed confocal phase imaging will further expand the application fields of CLM

    SDSSp J104433.04-012502.2 at z=5.74z=5.74 is Gravitationally Magnified by an Intervening Galaxy

    Get PDF
    During the course of our optical deep survey program on Lα\alpha emitters at z5.7z \approx 5.7 in the sky area surrounding the quasar SDSSp J104433.04-012502.2 at z=5.74z=5.74, we found that a faint galaxy with mBm_B(AB) 25\approx 25 is located at \timeform{1".9} southwest of the quasar. Its broad-band color properties from BB to zz^\prime suggest that the galaxy is located at a redshift of z1.5z \sim 1.5 -- 2.5. This is consistent with no strong emission line in our optical spectroscopy. Since the counter image of the quasar cannot be seen in our deep optical images, the magnification factor seems not to be very high. Our modest estimate is that this quasar is gravitationally magnified by a factor of 2.Comment: 11 pages, 5 figures, PASJ, in pres

    The Discovery of a Very Narrow-Line Star Forming Obat a Redshift of 5.66ject

    Full text link
    We report on the discovery of a very narrow-line star forming object beyond redshift of 5. Using the prime-focus camera, Suprime-Cam, on the 8.2 m Subaru telescope together with a narrow-passband filter centered at λc\lambda_{\rm c} = 8150 \AA with passband of Δλ\Delta\lambda = 120 \AA, we have obtained a very deep image of the field surrounding the quasar SDSSp J104433.04-012502.2 at a redshift of 5.74. Comparing this image with optical broad-band images, we have found an object with a very strong emission line. Our follow-up optical spectroscopy has revealed that this source is at a redshift of z=5.655±0.002z=5.655\pm0.002, forming stars at a rate 13 h0.72 M\sim 13 ~ h_{0.7}^{-2} ~ M_\odot yr1^{-1}. Remarkably, the velocity dispersion of Lyα\alpha-emitting gas is only 22 km s1^{-1}. Since a blue half of the Lyα\alpha emission could be absorbed by neutral hydrogen gas, perhaps in the system, a modest estimate of the velocity dispersion may be \gtrsim 44 km s1^{-1}. Together with a linear size of 7.7 h0.71h_{0.7}^{-1} kpc, we estimate a lower limit of the dynamical mass of this object to be 2×109M\sim 2 \times 10^9 M_\odot. It is thus suggested that LAE J1044-0123 is a star-forming dwarf galaxy (i.e., a subgalactic object or a building block) beyond redshift 5 although we cannot exclude a possibility that most Lyα\alpha emission is absorbed by the red damping wing of neutral intergalactic matter.Comment: 6 pages, 2 figures. ApJ Letters, in pres
    corecore