5,172 research outputs found

    Stellar Variability in a Forming Massive Star Cluster

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    We present a near-infrared (NIR) variability analysis for an 6\arcmin ×\times 6\arcmin region, which encompasses the massive protocluster G286.21+0.17. The total sample comprises more than 5000 objects, of which 562 show signs of a circumstellar disk based on their infrared colors. The data includes HST observations taken in two epochs separated by 3 years in the F110W and F160W bands. 363 objects (7% of the sample) exhibit NIR variability at a significant level (Stetson index >1.7), and a higher variability fraction (14%) is found for the young stellar objects (YSOs) with disk excesses. We identified 4 high amplitude (>0.6 mag) variables seen in both NIR bands. Follow up and archival observations of the most variable object in this survey (G286.2032+0.1740) reveal a rising light curve over 8 years from 2011 to 2019, with a K band brightening of 3.5 mag. Overall the temporal behavior of G286.2032+0.1740 resembles that of typical FU Ori objects, however its pre-burst luminosity indicates it has a very low mass (<0.12M<0.12\:M_\odot), making it an extreme case of an outburst event that is still ongoing.Comment: 13 pages, 8 figures, accepted by Ap

    The Core Mass Function in the Massive Protocluster G286.21+0.17 revealed by ALMA

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    We study the core mass function (CMF) of the massive protocluster G286.21+0.17 with the Atacama Large Millimeter/submillimeter Array via 1.3~mm continuum emission at a resolution of 1.0\arcsec\ (2500~au). We have mapped a field of 5.3\arcmin×\times5.3\arcmin\ centered on the protocluster clump. We measure the CMF in the central region, exploring various core detection algorithms, which give source numbers ranging from 60 to 125, depending on parameter selection. We estimate completeness corrections due to imperfect flux recovery and core identification via artificial core insertion experiments. For masses M1MM\gtrsim1\:M_\odot, the fiducial dendrogram-identified CMF can be fit with a power law of the form dN/dlogMMα{\rm{d}}N/{\rm{d}}{\rm{log}}M\propto{M}^{-\alpha} with α1.24±0.17\alpha \simeq1.24\pm0.17, slightly shallower than, but still consistent with, the index of the Salpeter stellar initial mass function of 1.35. Clumpfind-identified CMFs are significantly shallower with α0.64±0.13\alpha\simeq0.64\pm0.13. While raw CMFs show a peak near 1M1\:M_\odot, completeness-corrected CMFs are consistent with a single power law extending down to 0.5M\sim 0.5\:M_\odot, with only a tentative indication of a shallowing of the slope around 1M\sim1\:M_\odot. We discuss the implications of these results for star and star cluster formation theories.Comment: 11 pages, accepted by Ap

    The Core Mass Function Across Galactic Environments. II. Infrared Dark Cloud Clumps

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    We study the core mass function (CMF) within 32 dense clumps in seven infrared dark clouds (IRDCs) with the Atacama Large Millimeter/submillimeter Array (ALMA) via 1.3~mm continuum emission at a resolution of \sim1". We have identified 107 cores with the dendrogram algorithm, with a median radius of about 0.02 pc. Their masses range from 0.261 to 178 MM_{\odot}. After applying completeness corrections, we fit the combined IRDC CMF with a power law of the form dN/dlogMMαd N / d\:{\rm log} M \propto M^{-\alpha} and derive an index of α0.86±0.11\alpha\simeq0.86\pm0.11 for M0.79MM \geq 0.79\:M_\odot and α0.70±0.13\alpha\simeq0.70\pm0.13 for M1.26MM\geq 1.26\:M_\odot, which is a significantly more top-heavy distribution than the Salpeter stellar initial mass function (IMF) index of 1.35. We also make a direct comparison of these IRDC clump CMF results to those measured in the more evolved protocluster G286 derived with similar methods, which have α1.29±0.19\alpha\simeq1.29\pm0.19 and 1.08±0.271.08\pm0.27 in these mass ranges, respectively. These results provide a hint that, especially for the M1.26MM\geq 1.26\:M_\odot range where completeness corrections are modest, the CMF in high pressure, early-stage environments of IRDC clumps may be top-heavy compared to that in the more evolved, global environment of the G286 protoclusters. However, larger samples of cores probing these different environments are needed to better establish the robustness of this potential CMF variation.Comment: Accepted to ApJ, 15 pages, 7 figure

    Gas Kinematics of the Massive Protocluster G286.21+0.17 Revealed by ALMA

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    We study the gas kinematics and dynamics of the massive protocluster G286.21+0.17 with the Atacama Large Millimeter/submillimeter Array using spectral lines of C18OC^{18}O(2-1), N2D+N_2D^+(3-2), DCO+DCO^+(3-2) and DCNDCN(3-2). On the parsec clump scale, C18OC^{18}O emission appears highly filamentary around the systemic velocity. N2D+N_2D^+ and DCO+DCO^+ are more closely associated with the dust continuum. DCNDCN is strongly concentrated towards the protocluster center, where no or only weak detection is seen for N2D+N_2D^+ and DCO+DCO^+, possibly due to this region being at a relatively evolved evolutionary stage. Spectra of 76 continuum defined dense cores, typically a few 1000 AU in size, are analysed to measure their centroid velocities and internal velocity dispersions. There are no statistically significant velocity offsets of the cores among the different dense gas tracers. Furthermore, the majority (71\%) of the dense cores have subthermal velocity offsets with respect to their surrounding, lower density C18OC^{18}O emitting gas. Within the uncertainties, the dense cores in G286 show internal kinematics that are consistent with being in virial equilibrium. On clumps scales, the core to core velocity dispersion is also similar to that required for virial equilibrium in the protocluster potential. However, the distribution in velocity of the cores is largely composed of two spatially distinct groups, which indicates that the dense molecular gas has not yet relaxed to virial equilibrium, perhaps due to there being recent/continuous infall into the system.Comment: 26 pages, 17 figures, accepted by Ap

    Large area growth and electrical properties of p-type WSe2 atomic layers.

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    Transition metal dichacogenides represent a unique class of two-dimensional layered materials that can be exfoliated into single or few atomic layers. Tungsten diselenide (WSe(2)) is one typical example with p-type semiconductor characteristics. Bulk WSe(2) has an indirect band gap (∼ 1.2 eV), which transits into a direct band gap (∼ 1.65 eV) in monolayers. Monolayer WSe(2), therefore, is of considerable interest as a new electronic material for functional electronics and optoelectronics. However, the controllable synthesis of large-area WSe(2) atomic layers remains a challenge. The studies on WSe(2) are largely limited by relatively small lateral size of exfoliated flakes and poor yield, which has significantly restricted the large-scale applications of the WSe(2) atomic layers. Here, we report a systematic study of chemical vapor deposition approach for large area growth of atomically thin WSe(2) film with the lateral dimensions up to ∼ 1 cm(2). Microphotoluminescence mapping indicates distinct layer dependent efficiency. The monolayer area exhibits much stronger light emission than bilayer or multilayers, consistent with the expected transition to direct band gap in the monolayer limit. The transmission electron microscopy studies demonstrate excellent crystalline quality of the atomically thin WSe(2). Electrical transport studies further show that the p-type WSe(2) field-effect transistors exhibit excellent electronic characteristics with effective hole carrier mobility up to 100 cm(2) V(-1) s(-1) for monolayer and up to 350 cm(2) V(-1) s(-1) for few-layer materials at room temperature, comparable or well above that of previously reported mobility values for the synthetic WSe(2) and comparable to the best exfoliated materials

    The effect of 14 weeks of vitamin D3 supplementation on antimicrobial peptides and proteins in athletes

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    Heavy training is associated with increased respiratory infection risk and antimicrobial proteins are important in defence against oral and respiratory tract infections. We examined the effect of 14 weeks of vitamin D3 supplementation (5000 IU/day) on the resting plasma cathelicidin concentration and the salivary secretion rates of secretory immunoglobulin A (SIgA), cathelicidin, lactoferrin and lysozyme in athletes during a winter training period. Blood and saliva were obtained at the start of the study from 39 healthy men who were randomly allocated to vitamin D3 supplement or placebo. Blood samples were also collected at the end of the study; saliva samples were collected after 7 and 14 weeks. Plasma total 25(OH)D concentration increased by 130% in the vitamin D3 group and decreased by 43% in the placebo group (both P=0.001). The percentage change of plasma cathelicidin concentration in the vitamin D3 group was higher than in the placebo group (P=0.025). Only in the vitamin D3 group, the saliva SIgA and cathelicidin secretion rates increased over time (both P=0.03). A daily 5000 IU vitamin D3 supplement has a beneficial effect in up-regulating the expression of SIgA and cathelicidin in athletes during a winter training period which could improve resistance to respiratory infections

    Final-State Phases in BB \to Baryon-Antibaryon Decays

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    The recent observation of the decay \ob \to \Lambda_c^+ \bar p suggests that related decays may soon be visible at e+ee^+ e^- colliders. It is shown how these decays can shed light on strong final-state phases and amplitudes involving the spectator quark, both of which are normally expected to be small in B decays.Comment: 14 pages, LaTeX, 2 figures, submitted to Phys. Rev. D, references and discussion of helicity amplitudes adde
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