1,167 research outputs found

    Sub-millimetre galaxies in cosmological hydrodynamic simulations: Source number counts and the spatial clustering

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    We use large cosmological Smoothed-Particle-Hydrodynamics simulations to study the formation and evolution of sub-millimetre galaxies (SMGs). In our previous work, we studied the statistical properties of ultra-violet selected star-forming galaxies at high redshifts. We populate the same cosmological simulations with SMGs by calculating the reprocess of stellar light by dust grains into far-infrared to millimetre wavebands in a self-consistent manner. We generate light-cone outputs to compare directly the statistical properties of the simulated SMGs with available observations. Our model reproduces the submm source number counts and the clustering amplitude. We show that bright SMGs with flux S>1S > 1 mJy reside in halos with mass of ∼1013M⊙\sim 10^{13} M_{\odot} and have stellar masses greater than 1011∼M⊙10^{11}\sim \rm M_{\odot}. The angular cross-correlation between the SMGs and Lyman-α\alpha emitters is significantly weaker than that between the SMGs and Lyman-break galaxies. The cross-correlation is also weaker than the auto-correlation of the SMGs. The redshift distribution of the SMGs shows a broad peak at z∼2z \sim 2, where Bright SMGs contribute significantly to the global cosmic star formation rate density. Our model predicts that there are hundreds of SMGs with S>0.1S > 0.1 mJy at z>5z > 5 per 1 square degree field. Such SMGs can be detected by ALMA.Comment: 11 pages, 13 figures, submitted to MNRA

    Physical Properties of UDF12 Galaxies in Cosmological simulations

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    We have performed a large cosmological hydrodynamics simulation tailored to the deep survey with the Hubble Space Telescope made in 2012, the so-called UDF12 campaign. After making a light-cone output, we have applied the same color selection criteria as the UDF12 campaign to select galaxies from our simulation, and then, have examined the physical properties of them as a proxy of the real observed UDF12 galaxies at z>7z > 7. As a result, we find that the halo mass is almost linearly proportional to the observed ultraviolet (UV) luminosity (4×1011 M⊙4 \times 10^{11}~{\rm M_{\odot}} at MUV=−21M_{\rm UV} = -21). The dust attenuation and UV slope β\beta well correlates with the observed UV luminosity, which is consistent with observations quantitatively. The star formation rate (SFR) is also linearly proportional to the stellar mass and the specific SFR shows only a weak dependency on the mass. We also find an increasing star formation history with a time-scale of ∼100\sim100 Myr in the high-zz galaxies. An average metallicity weighted by the Lyman continuum luminosity reaches up to >0.1>0.1 Solar even at z∼10z \sim 10, suggesting a rapid metal enrichment. We also expect ≥0.1\geq 0.1 mJy at 350 GHz of the dust thermal emission from the galaxies with H160≤27H_{160} \leq 27, which can be detectable with the Atacama Large Milimetre-submilimetre Array. The galaxies selected by the UDF12 survey contribute to only 52−−12%52--12\% of the cosmic SFR density from z∼7z \sim 7 to z∼10z \sim 10, respectively. The James Webb Space Telescope will push the detection fraction up to 77−−72%77--72\%.Comment: re-Submitted to MNRAS; 16 pages; 14 figures; 1 tables

    Nuclear prolate-shape dominance with the Woods-Saxon potential

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    We study the prolate-shape predominance of the nuclear ground-state deformation by calculating the masses of more than two thousand even-even nuclei using the Strutinsky method, modified by Kruppa, and improved by us. The influences of the surface thickness of the single-particle potentials, the strength of the spin-orbit potential, and the pairing correlations are investigated by varying the parameters of the Woods-Saxon potential and the pairing interaction. The strong interference between the effects of the surface thickness and the spin-orbit potential is confirmed to persist for six sets of the Woods-Saxon potential parameters. The observed behavior of the ratios of prolate, oblate, and spherical nuclei versus potential parameters are rather different in different mass regions. It is also found that the ratio of spherical nuclei increases for weakly bound unstable nuclei. Differences of the results from the calculations with the Nilsson potential are described in detail.Comment: 16 pages, 17 figure

    Clinical and Arthroscopic Findings of Acute Anterior Cruciate Ligament Tears of the Knee

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    Clinical, arthrographic, and arthroscopic findings in 53 patients with acutely torn anterior cruciate ligaments (ACLs) were documented. Arthroscopy and instability tests under anesthesia were performed on all patients within 2 weeks after the initial injury. Twenty-three patients complained of extension blocks, and localized tenderness on the medial side was revealed in 26 patients at the initial examination. Aspiration from joints exhibited hemarthrosis in 52 patients. Arthroscopy revealed ACL ruptures in all patients. Four Segond's fractures, 26 meniscus tears (8 medial and 18 lateral), 1 osteochondral fracture, and 19 medial collateral ligament ruptures were revealed. Arthroscopy detected only 1 of the 5 ruptures of the posteromedial corner of the medial meniscus, which were noted on arthrography. Three ACL stumps were protruding among the femorotibial joint, which seemed to be restricting full extension. Statistical analysis showed that tenderness on the medial side was not revealed more frequently in knees with medial collateral ligament injuries than in the others. The volume of aspirated fluids in knees with no leakage in arthrography significantly increased over those with leakages (p < 0.05). Diagnosis of ACL injuries should be completed by clinical, arthrographic, and arthroscopic examinations
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