35 research outputs found

    Preparation of Mesoporous V2O5@TiO2 Composites with Enhanced Photoactivity for Gaseous Benzene Degradation

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    AbstractMesoporous V2O5@TiO2 composites were fabricated by an ultrasonic method with V2O5 sol as the guest precursor. The prepared materials were characterized by powder X-ray diffraction, field emission-scanning electron microscopy, transmission electron microscope, X-ray photoelectron spectroscopy, UV-Vis spectroscopy and nitrogen sorption analysis. The results indicated that V2O5 nanoparticles dispersed well on/into the porous structure of TiO2 matrix. The composites presented typical IUPAC IV isotherms with type H2 hysteresis loops, revealing the mesoporous structure. It was observed that V2O5 loading led to red shift of the absorption edge to 540nm and reduced the band gap < 3.0eV. The V2O5@TiO2 composites with V/Ti molar ratio of 0.1 exhibited outstanding degradation efficiency of gaseous benzene

    A Planetary Microlensing Event with an Unusually Red Source Star: MOA-2011-BLG-291

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    We present the analysis of planetary microlensing event MOA-2011-BLG-291, which has a mass ratio of q=(3.8±0.7)×104q=(3.8\pm0.7)\times10^{-4} and a source star that is redder (or brighter) than the bulge main sequence. This event is located at a low Galactic latitude in the survey area that is currently planned for NASA's WFIRST exoplanet microlensing survey. This unusual color for a microlensed source star implies that we cannot assume that the source star is in the Galactic bulge. The favored interpretation is that the source star is a lower main sequence star at a distance of DS=4.9±1.3D_S=4.9\pm1.3\,kpc in the Galactic disk. However, the source could also be a turn-off star on the far side of the bulge or a sub-giant in the far side of the Galactic disk if it experiences significantly more reddening than the bulge red clump stars. However, these possibilities have only a small effect on our mass estimates for the host star and planet. We find host star and planet masses of Mhost=0.150.10+0.27MM_{\rm host} =0.15^{+0.27}_{-0.10}M_\odot and mp=1812+34Mm_p=18^{+34}_{-12}M_\oplus from a Bayesian analysis with a standard Galactic model under the assumption that the planet hosting probability does not depend on the host mass or distance. However, if we attempt to measure the host and planet masses with host star brightness measurements from high angular resolution follow-up imaging, the implied masses will be sensitive to the host star distance. The WFIRST exoplanet microlensing survey is expected to use this method to determine the masses for many of the planetary systems that it discovers, so this issue has important design implications for the WFIRST exoplanet microlensing survey

    Spectroscopic Mass and Host-star Metallicity Measurements for Newly Discovered Microlensing Planet OGLE-2018-BLG-0740Lb

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    We report the discovery of the microlensing planet OGLE-2018-BLG-0740Lb. The planet is detected with a very strong signal of Δχ24630\Delta\chi^2\sim 4630, but the interpretation of the signal suffers from two types of degeneracies. One type is caused by the previously known close/wide degeneracy, and the other is caused by an ambiguity between two solutions, in which one solution requires to incorporate finite-source effects, while the other solution is consistent with a point-source interpretation. Although difficult to be firmly resolved based on only the photometric data, the degeneracy is resolved in strong favor of the point-source solution with the additional external information obtained from astrometric and spectroscopic observations. The small astrometric offset between the source and baseline object supports that the blend is the lens and this interpretation is further secured by the consistency of the spectroscopic distance estimate of the blend with the lensing parameters of the point-source solution. The estimated mass of the host is 1.0±0.1 M1.0\pm 0.1~M_\odot and the mass of the planet is 4.5±0.6 MJ4.5\pm 0.6~M_{\rm J} (close solution) or 4.8±0.6 MJ4.8\pm 0.6~M_{\rm J} (wide solution) and the lens is located at a distance of 3.2±0.53.2\pm 0.5~kpc. The bright nature of the lens, with I17.1I\sim 17.1 (V18.2V\sim 18.2), combined with its dominance of the observed flux suggest that radial-velocity (RV) follow-up observations of the lens can be done using high-resolution spectrometers mounted on large telescopes, e.g., VLT/ESPRESSO, and this can potentially not only measure the period and eccentricity of the planet but also probe for close-in planets. We estimate that the expected RV amplitude would be 60sini m s1\sim 60\sin i ~{\rm m~s}^{-1}.Comment: 12 pages, 11 figures, 4 table

    Spitzer + VLTI-GRAVITY Measure the Lens Mass of a Nearby Microlensing Event

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    We report the lens mass and distance measurements of the nearby microlensing event TCP J05074264+2447555 (Kojima-1). We measure the microlens parallax vector π_E using Spitzer and ground-based light curves with constraints on the direction of lens-source relative proper motion derived from Very Large Telescope Interferometer (VLTI) GRAVITY observations. Combining this π_E determination with the angular Einstein radius θ_E measured by VLTI-GRAVITY observations, we find that the lens is a star with mass M_L = 0.495±0.063 M⊙ at a distance D_L = 429 ± 21 pc. We find that the blended light basically all comes from the lens. The lens-source proper motion is Μ_(rel,hel) = 26.55±0.36 mas yr⁻¹, so with currently available adaptive-optics instruments, the lens and source can be resolved in 2021. This is the first microlensing event whose lens mass is unambiguously measured by interferometry + satellite-parallax observations, which opens a new window for mass measurements of isolated objects such as stellar-mass black holes

    Spitzer + VLTI-GRAVITY Measure the Lens Mass of a Nearby Microlensing Event

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    We report the lens mass and distance measurements of the nearby microlensing event TCP J05074264+2447555. We measure the microlens parallax vector πE{\pi}_{\rm E} using Spitzer and ground-based light curves with constraints on the direction of lens-source relative proper motion derived from Very Large Telescope Interferometer (VLTI) GRAVITY observations. Combining this πE{\pi}_{\rm E} determination with the angular Einstein radius θE\theta_{\rm E} measured by VLTI GRAVITY observations, we find that the lens is a star with mass ML=0.495±0.063 MM_{\rm L} = 0.495 \pm 0.063~M_{\odot} at a distance DL=429±21 pcD_{\rm L} = 429 \pm 21~{\rm pc}. We find that the blended light basically all comes from the lens. The lens-source proper motion is μrel,hel=26.55±0.36 masyr1\mu_{\rm rel,hel} = 26.55 \pm 0.36~{\rm mas\,yr^{-1}}, so with currently available adaptive-optics (AO) instruments, the lens and source can be resolved in 2021. This is the first microlensing event whose lens mass is unambiguously measured by interferometry + satellite parallax observations, which opens a new window for mass measurements of isolated objects such as stellar-mass black holes.Comment: 3 Figures and 6 Tables Submitted to AAS Journa

    Spitzer Parallax Of Ogle-2015-blg-0966: A Cold Neptune In The Galactic Disk

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    We report the detection of a cold Neptune mplanet = 21 ± 2 M? orbiting a 0.38 M? M dwarf lying 2.5–3.3 kpc toward the Galactic center as part of a campaign combining ground-based and Spitzer observations to measure the Galactic distribution of planets. This is the first time that the complex real-time protocols described by Yee et al., which aim to maximize planet sensitivity while maintaining sample integrity, have been carried out in practice. Multiple survey and follow up teams successfully combined their efforts within the framework of these protocols to detect this planet. This is the second planet in the Spitzer Galactic distribution sample. Both are in the near to mid-disk and are clearly not in the Galactic bulge

    Effect of internal surface structure of the north wall on Chinese solar greenhouse thermal microclimate based on computational fluid dynamics.

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    Chinese solar greenhouses are unique facility agriculture buildings and widely used in northeastern China, providing a favorable requirement for crop growth. The north wall configurations play an essential role in heat storage and thermal insulation and directly affect the management of the internal environment. This research is devoted to further improve the thermal performance of the greenhouse and explore the potential of the north wall. A mathematical model was designed to investigate the concave-convex wall configurations based on computational fluid dynamics. Four passive heat-storage north walls were analyzed by using the same constituent materials, including a plane wall, a vertical wall, a horizontal wall and an alveolate wall. The numerical model was validated by experimental measurements. The temperature distributions of the north walls were examined and a comparative analysis of the heat storage-release capabilities was carried out. The results showed that the heat-storage capacity of the north wall is affected by the surface structure. Moreover, the critical factor influencing the air temperature is the sum of the heat load released by the wall and the energy increment of greenhouse air. The results suggested that the alveolate wall has preferable thermal accumulation capacity. The concave-convex wall configurations have a wider range of heat transfer performance along the thickness direction, while the plane wall has a superior thermal environment. This study provides a basic theoretical reference to rationally design the internal surface structures of the north wall
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