5,096 results on '"Keller C"'
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2. Multi-scale, open-system magmatic and sub-solidus processes contribute to the chemical and isotopic characteristics of the Jurassic Guadalupe Igneous Complex, Sierra Nevada, California, USA
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Ratschbacher, Barbara C, Ardill, Katie, Keller, C Brenhin, Schoene, Blair, Paterson, Scott R, Putirka, Keith D, Lackey, Jade Star, and Paige, Matthew L
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Earth Sciences ,Geochemistry ,Geology ,Geophysics ,Geochemistry & Geophysics - Abstract
The chemical and isotopic characteristics of a solidified pluton represent the integration of magmatic and sub-solidus processes operating across a range of spatial and temporal scales during pluton construction, crystallization, and cooling. Disentangling these processes and understanding where chemical and isotopic signatures were acquired requires the combination of multiple tools tracing processes at different time and length scales. We combine whole-rock oxygen and Sr-Nd isotopes, zircon oxygen isotopes and trace elements, and mineral compositions with published high-precision U-Pb zircon geochronology to evaluate differentiation within the bimodal Guadalupe Igneous Complex, Sierra Nevada, California (USA). The complex was constructed in ~300 k.y. between 149 and 150 Ma. Felsic magmas crystallized as centimeter- to meter-sized segregations in gabbros in the lower part of the complex and as granites and granophyres structurally above the gabbros. A central mingling zone separates the mafic and felsic units. Pluton-wide δ18O(whole-rock), δ18O(zircon), and Sr-Nd isotopic ranges are too large to be explained by in situ, closed-system differentiation, instead requiring open-system behavior at all scales. Low δ18O(whole-rock) and δ18O(zircon) values indicate assimilation of hydrothermally altered marine host rocks during ascent and/or emplacement. In situ differentiation processes operated on a smaller scale (meters to tens of meters) for at least ~200 k.y. via (1) percolation and segregation of chemically and isotopically diverse silicic interstitial melt from a heterogeneous gabbro mush; (2) crystal accumulation; and (3) sub-solidus, high-temperature, hydrothermal alteration at the shallow roof of the complex to modify the chemical and isotopic characteristics. Whole-rock and mineral chemistry in combination with geochronology allows deciphering open-system differentiation processes at the outcrop to pluton scale from magmatic to sub-solidus temperatures over time scales of hundreds of thousands to millions of years.
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- 2024
3. An early giant planet instability recorded in asteroidal meteorites
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Edwards, Graham Harper, Keller, C. Brenhin, Newton, Elisabeth R., and Stewart, Cameron W.
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Astrophysics - Earth and Planetary Astrophysics - Abstract
Giant planet migration appears widespread among planetary systems in our Galaxy. However, the timescales of this process, which reflect the underlying dynamical mechanisms, are not well constrained, even within the solar system. Since planetary migration scatters smaller bodies onto intersecting orbits, it would have resulted in an epoch of enhanced bombardment in the solar system's asteroid belt. To accurately and precisely quantify the timescales of migration, we interrogate thermochronologic data from asteroidal meteorites, which record the thermal imprint of energetic collisions. We present a database of 40K-40Ar system ages from chondrite meteorites and evaluate it with an asteroid-scale thermal code coupled to a Markov chain Monte Carlo inversion. Simulations require bombardment in order to reproduce the observed age distribution and identify a bombardment event beginning 11.3 +9.5/-6.6 million years after the Sun formed (50% credible interval). Our results associate a giant planet instability in our solar system with the dissipation of the gaseous protoplanetary disk., Comment: 45 pages, 2 tables, 4 figures, 10 extended data items (8 figures, 2 tables). Twice reviewed and accepted in principle at Nature Astronomy
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- 2023
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4. InSPECtor: an end-to-end design framework for compressive pixelated hyperspectral instruments
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Stockmans, T. A., Snik, F., Esposito, M., van Dijk, C., and Keller, C. U.
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Electrical Engineering and Systems Science - Image and Video Processing ,Physics - Optics - Abstract
Classic designs of hyperspectral instrumentation densely sample the spatial and spectral information of the scene of interest. Data may be compressed after the acquisition. In this paper we introduce a framework for the design of an optimized, micro-patterned snapshot hyperspectral imager that acquires an optimized subset of the spatial and spectral information in the scene. The data is thereby compressed already at the sensor level, but can be restored to the full hyperspectral data cube by the jointly optimized reconstructor. This framework is implemented with TensorFlow and makes use of its automatic differentiation for the joint optimization of the layout of the micro-patterned filter array as well as the reconstructor. We explore the achievable compression ratio for different numbers of filter passbands, number of scanning frames, and filter layouts using data collected by the Hyperscout instrument. We show resulting instrument designs that take snapshot measurements without losing significant information while reducing the data volume, acquisition time, or detector space by a factor of 40 as compared to classic, dense sampling. The joint optimization of a compressive hyperspectral imager design and the accompanying reconstructor provides an avenue to substantially reduce the data volume from hyperspectral imagers., Comment: 23 pages, 12 figures, published in Applied Optics
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- 2023
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5. Polarization-dependent beam shifts upon metallic reflection in high-contrast imagers and telescopes
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van Holstein, R. G., Keller, C. U., Snik, F., and Bos, S. P.
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Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Earth and Planetary Astrophysics ,Physics - Optics - Abstract
(Abridged) Context. To directly image rocky exoplanets in reflected (polarized) light, future space- and ground-based high-contrast imagers and telescopes aim to reach extreme contrasts at close separations from the star. However, the achievable contrast will be limited by reflection-induced polarization aberrations. While polarization aberrations can be modeled numerically, such computations provide little insight into the full range of effects, their origin and characteristics, and possible ways to mitigate them. Aims. We aim to understand polarization aberrations produced by reflection off flat metallic mirrors at the fundamental level. Methods. We used polarization ray tracing to numerically compute polarization aberrations and interpret the results in terms of the polarization-dependent spatial and angular Goos-H\"anchen and Imbert-Federov shifts of the beam of light as described with closed-form mathematical expressions in the physics literature. Results. We find that all four beam shifts are fully reproduced by polarization ray tracing and study the origin, characteristics, sizes, and directions of the shifts. Of the four beam shifts, only the spatial Goos-H\"anchen and Imbert-Federov shifts are relevant for high-contrast imagers and telescopes because these shifts are visible in the focal plane and create a polarization structure in the PSF that reduces the performance of coronagraphs and the polarimetric speckle suppression close to the star. Conclusions. The beam shifts in an optical system can be mitigated by keeping the f-numbers large and angles of incidence small. Most importantly, mirror coatings should not be optimized for maximum reflectivity, but should be designed to have a retardance close to 180{\deg}. The insights from our study can be applied to improve the performance of current and future high-contrast imagers, especially those in space and on the ELTs., Comment: 19 pages, 13 figures, 1 table, final version as published in Astronomy & Astrophysics, 677, A150 (2023)
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- 2023
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6. Subgruppe der Multiplen Sklerose mit charakteristischer Autoantikörpersignatur im präklinischen Stadium
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Keller, C. W.
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- 2024
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7. The Enhanced Resolution Imager and Spectrograph for the VLT
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Davies, R., Absil, O., Agapito, G., Berbel, A. Agudo, Baruffolo, A., Biliotti, V., Bonaglia, M., Bonse, M., Briguglio, R., Campana, P., Cao, Y., Carbonaro, L., Cortes, A., Cresci, G., Dallilar, Y., Dannert, F., De Rosa, R. J., Deysenroth, M., Di Antonio, I., Di Cianno, A., Di Rico, G., Doelman, D., Dolci, M., Dorn, R., Eisenhauer, F., Esposito, S., Fantinel, D., Ferruzzi, D., Feuchtgruber, H., Finger, G., Schreiber, N. M. Förster, Gao, X., Gemperlein, H., Genzel, R., Gillessen, S., Ginski, C., Glauser, A. M., Glindemann, A., Grani, P., Hartl, M., Hayoz, J., Heida, M., Henry, D., Hofmann, R., Huber, H., Kasper, M., Keller, C., Kenworthy, M., Kravchenko, K., Kuntschner, H., Lacour, S., Lightfoot, J., Lunney, D., Lutz, D., Macintosh, M., Mannucci, F., Marsset, M., Modigliani, A., Neeser, M., de Xivry, G. Orban, Ott, T., Pallanca, L., Patapis, P., Pearson, D., Peña, E., Percheron, I., Puglisi, A., Quanz, S. P., Rabien, S., Rau, C., Riccardi, A., Salasnich, B., Schmid, H. -M., Schubert, J., Serra, B., Shimizu, T., Snik, F., Sturm, E., Tacconi, L., Taylor, W., Valentini, A., Waring, C., Wiezorrek, E., and Xompero, M.
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
ERIS, the Enhanced Resolution Imager and Spectrograph, is an instrument that both extends and enhances the fundamental diffraction limited imaging and spectroscopy capability for the VLT. It replaces two instruments that were being maintained beyond their operational lifetimes, combines their functionality on a single focus, provides a new wavefront sensing module for natural and laser guide stars that makes use of the Adaptive Optics Facility, and considerably improves on their performance. The observational modes ERIS provides are integral field spectroscopy at 1-2.5 {\mu}m, imaging at 1-5 {\mu}m with several options for high contrast imaging, and longslit spectroscopy at 3-4 {\mu}m, The instrument is installed at the Cassegrain focus of UT4 at the VLT and, following its commissioning during 2022, has been made available to the community., Comment: 20 pages with 29 figures; accepted for A&A (minor changes)
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- 2023
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8. Upgrading the high contrast imaging facility SPHERE: science drivers and instrument choices
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Boccaletti, A., Chauvin, G., Wildi, F., Milli, J., Stadler, E., Diolaiti, E., Gratton, R., Vidal, F., Loupias, M., Langlois, M., Cantalloube, F., N'Diaye, M., Gratadour, D., Ferreira, F., Tallon, M., Mazoyer, J., Segransan, D., Mouillet, D., Beuzit, J. -L., Bonnefoy, M., Galicher, R., Vigan, A., Snellen, I., Feldt, M., Desidera, S., Rousseau, S., Baruffolo, A., Goulas, C., Baudoz, P., Bechet, C., Benisty, M., Bianco, A., Carry, B., Cascone, E., Charnay, B., Choquet, E., Christiaens, V., Cortecchia, F., de Caprio, V., De Rosa, A., Desgrange, C., D'Orazi, V., Douté, S., Frangiamore, M., Gendron, E., Ginski, C., Huby, E., Keller, C., Kulcsár, C., Landman, R., Lagarde, S., Lagadec, E., Lagrange, A. -M., Kasper, M. Lombini M., Ménard, F., Magnard, Y., Malaguti, G., Maurel, D., Mesa, D., Morgante, G., Pantin, E., Pichon, T., Potier, A., Rabou, P., Rochat, S., Terenzi, L., Thiébaut, E., Tallon-Bosc, I., Raynaud, H. -F., Rouan, D., Sevin, A., Schiavone, F., Schreiber, L., and Zanutta, A.
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Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Earth and Planetary Astrophysics - Abstract
SPHERE+ is a proposed upgrade of the SPHERE instrument at the VLT, which is intended to boost the current performances of detection and characterization for exoplanets and disks. SPHERE+ will also serve as a demonstrator for the future planet finder (PCS) of the European ELT. The main science drivers for SPHERE+ are 1/ to access the bulk of the young giant planet population down to the snow line ($3-10$ au), to bridge the gap with complementary techniques (radial velocity, astrometry); 2/ to observe fainter and redder targets in the youngest ($1-10$\,Myr) associations compared to those observed with SPHERE to directly study the formation of giant planets in their birth environment; 3/ to improve the level of characterization of exoplanetary atmospheres by increasing the spectral resolution in order to break degeneracies in giant planet atmosphere models. Achieving these objectives requires to increase the bandwidth of the xAO system (from $\sim$1 to 3\,kHz) as well as the sensitivity in the infrared (2 to 3\,mag). These features will be brought by a second stage AO system optimized in the infrared with a pyramid wavefront sensor. As a new science instrument, a medium resolution integral field spectrograph will provide a spectral resolution from 1000 to 5000 in the J and H bands. This paper gives an overview of the science drivers, requirements and key instrumental trade-off that were done for SPHERE+ to reach the final selected baseline concept., Comment: To appear in the Proceedings of the SPIE Astronomical Telescopes + Instrumentation (2022), 13 pages, 6 figure
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- 2022
9. Continental flood basalts drive Phanerozoic extinctions
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Green, Theodore, Renne, Paul R, and Keller, C Brenhin
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Earth Sciences ,Biological Sciences ,Ecology ,Geology ,Extinction ,Biological ,Silicates ,Volcanic Eruptions ,volcanology ,mass extinctions ,carbon cycle ,paleontology - Abstract
Refinements of the geological timescale driven by the increasing precision and accuracy of radiometric dating have revealed an apparent correlation between large igneous provinces (LIPs) and intervals of Phanerozoic faunal turnover that has been much discussed at a qualitative level. However, the extent to which such correlations are likely to occur by chance has yet to be quantitatively tested, and other kill mechanisms have been suggested for many mass extinctions. Here, we show that the degree of temporal correlation between continental LIPs and faunal turnover in the Phanerozoic is unlikely to occur by chance, suggesting a causal relationship linking extinctions and continental flood basalts. The relationship is stronger for LIPs with higher estimated eruptive rates and for stage boundaries with higher extinction magnitudes. This suggests LIP magma degassing as a primary kill mechanism for mass extinctions and other intervals of faunal turnover, which may be related to [Formula: see text], Cl, and F release. Our results suggest continental LIPs as a major, direct driver of extinctions throughout the Phanerozoic.
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- 2022
10. Influence of processing parameters on the fracture behaviour of 316L SS printed by laser powder bed fusion
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Wilson, T., Sealy, M., Cisa Bofarull, I., Keller, C., and Vieille, B.
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- 2024
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11. Regional trends and petrologic factors inhibit global interpretations of zircon trace element compositions
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Roberts, Nick M.W., Spencer, Christopher J., Puetz, Stephen, Keller, C. Brenhin, and Tapster, Simon
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- 2024
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12. Micromechanical analysis of a unimodal and a bimodal polycrystal with paired microstructures of ultrafine grains, 2D & 3D
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Calvat, M., Keller, C., and Barbe, F.
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- 2025
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13. Fracture behavior of a Ni-20 wt.%Cr binary alloy processed by Laser Powder Bed Fusion: Influence of the specimen building orientation and rotation angle between layers
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Benmabrouk, S., Vieille, B., Keller, C., Joshi, S.S., and Hug, E.
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- 2024
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14. A MUSE view of the asymmetric jet from HD 163296
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Xie, C., Haffert, S. Y., de Boer, J., Kenworthy, M. A., Brinchmann, J., Girard, J., Snellen, I. A. G., and Keller, C. U.
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Astrophysics - Solar and Stellar Astrophysics ,Astrophysics - Earth and Planetary Astrophysics ,Astrophysics - High Energy Astrophysical Phenomena - Abstract
Jets and outflows are thought to play important roles in regulating star formation and disk evolution. HD 163296 is a well-studied Herbig Ae star that hosts proto-planet candidates, a protoplanetary disk, a protostellar jet, and a molecular outflow, which makes it an excellent laboratory for studying jets. We aim to characterize the jet at the inner regions and check if there are large differences with the features at large separations. A secondary objective is to demonstrate the performance of Multi Unit Spectroscopic Explorer (MUSE) in high-contrast imaging of extended line emission. MUSE in the narrow field mode (NFM) can provide observations at optical wavelengths with high spatial ($\sim$75 mas) and medium spectral ($R\sim$2500) resolution. With the high-resolution spectral differential imaging (HRSDI) technique, we can characterize the kinematic structures and physical conditions of jets down to 100 mas. We detect multiple atomic lines in two new knots, B3 and A4, at distances of <4" from the host star with MUSE. The derived $\dot{M}_{\rm jet} / \dot{M}_{\rm acc}$ is about 0.08 and 0.06 for knots B3 and A4, respectively. The observed [Ca II]/[S II] ratios indicate that there is no sign of dust grains at distances of <4". Assuming the knot A4 traces the streamline, we set an upper limit of 2.2 au on the size of the launching region. Although MUSE has the ability to detect the velocity shifts caused by high- and low-velocity components, we found no significant evidence of velocity decrease transverse to the jet direction. Our work demonstrates the capability of using MUSE NFM observations for the detailed study of stellar jets in the optical down to 100~mas. The derived $\dot{M}_{\rm jet} / \dot{M}_{\rm acc}$, no dust grain, and jet radius at the star support the magneto-centrifugal models as a launching mechanism for the jet., Comment: Astronomy & Astrophysics, June 3, 2021; 9 pages, 4 Figures, 3 Tables
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- 2021
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15. S2k-Leitlinie: Diagnostik und Therapie myasthener Syndrome: Kurzfassung der Leitlinie der Deutschen Gesellschaft für Neurologie
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Meisel, A., Keller, C. W., Hoffmann, S., and Wiendl, H.
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- 2023
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16. The vector-apodizing phase plate coronagraph: design, current performance, and future development
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Doelman, D. S., Snik, F., Por, E. H., Bos, S. P., Otten, G. P. P. L., Kenworthy, M., Haffert, S. Y., Wilby, M., Bohn, A. J., Sutlieff, B. J., Miller, K., Ouellet, M., de Boer, J., Keller, C. U., Escuti, M. J., Shi, S., Warriner, N. Z., Hornburg, K. J., Birkby, J. L., Males, J., Morzinski, K. M., Close, L. M., Codona, J., Long, J., Schatz, L., Lumbres, J., Rodack, A., Van Gorkom, K., Hedglen, A, Guyon, O., Lozi, J., Groff, T., Chilcote, J., Jovanovic, N., Thibault, S., de Jonge, C., Allain, G., Vallée, C., Patel, D., Côté, O., Marois, C., Hinz, P., Stone, J., Skemer, A., Briesemeister, Z., Boehle, A., Glauser, A. M., Taylor, W., Baudoz, P., Huby, E., Absil, O., Carlomagno, B., and Delacroix, C.
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Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Earth and Planetary Astrophysics - Abstract
Over the last decade, the vector-apodizing phase plate (vAPP) coronagraph has been developed from concept to on-sky application in many high-contrast imaging systems on 8-m class telescopes. The vAPP is an geometric-phase patterned coronagraph that is inherently broadband, and its manufacturing is enabled only by direct-write technology for liquid-crystal patterns. The vAPP generates two coronagraphic PSFs that cancel starlight on opposite sides of the point spread function (PSF) and have opposite circular polarization states. The efficiency, that is the amount of light in these PSFs, depends on the retardance offset from half-wave of the liquid-crystal retarder. Using different liquid-crystal recipes to tune the retardance, different vAPPs operate with high efficiencies ($>96\%$) in the visible and thermal infrared (0.55 $\mu$m to 5 $\mu$m). Since 2015, seven vAPPs have been installed in a total of six different instruments, including Magellan/MagAO, Magellan/MagAO-X, Subaru/SCExAO, and LBT/LMIRcam. Using two integral field spectrographs installed on the latter two instruments, these vAPPs can provide low-resolution spectra (R$\sim$30) between 1 $\mu$m and 5 $\mu$m. We review the design process, development, commissioning, on-sky performance, and first scientific results of all commissioned vAPPs. We report on the lessons learned and conclude with perspectives for future developments and applications., Comment: 38 pages, 17 figures, accepted for publication in Applied Optics, added NSF grant acknowledgement
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- 2021
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17. A survey of the linear polarization of directly imaged exoplanets and brown dwarf companions with SPHERE-IRDIS. First polarimetric detections revealing disks around DH Tau B and GSC 6214-210 B
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van Holstein, R. G., Stolker, T., Jensen-Clem, R., Ginski, C., Milli, J., de Boer, J., Girard, J. H., Wahhaj, Z., Bohn, A. J., Millar-Blanchaer, M. A., Benisty, M., Bonnefoy, M., Chauvin, G., Dominik, C., Hinkley, S., Keller, C. U., Keppler, M., Langlois, M., Marino, S., Ménard, F., Perrot, C., Schmidt, T. O. B., Vigan, A., Zurlo, A., and Snik, F.
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Astrophysics - Earth and Planetary Astrophysics ,Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Solar and Stellar Astrophysics - Abstract
Young giant planets and brown dwarf companions emit near-infrared radiation that can be linearly polarized up to several percent. This polarization can reveal the presence of a circumsubstellar accretion disk, rotation-induced oblateness of the atmosphere, or an inhomogeneous distribution of atmospheric dust clouds. We measured the near-infrared linear polarization of 20 known directly imaged exoplanets and brown dwarf companions with the high-contrast imager SPHERE-IRDIS at the VLT. We reduced the data using the IRDAP pipeline to correct for the instrumental polarization and crosstalk with an absolute polarimetric accuracy <0.1% in the degree of polarization. We report the first detection of polarization originating from substellar companions, with a polarization of several tenths of a percent for DH Tau B and GSC 6214-210 B in H-band. By comparing the measured polarization with that of nearby stars, we find that the polarization is unlikely to be caused by interstellar dust. Because the companions have previously measured hydrogen emission lines and red colors, the polarization most likely originates from circumsubstellar disks. Through radiative transfer modeling, we constrain the position angles of the disks and find that the disks must have high inclinations. The presence of these disks as well as the misalignment of the disk of DH Tau B with the disk around its primary star suggest in situ formation of the companions. For the 18 other companions, we do not detect significant polarization and place subpercent upper limits on their degree of polarization. These non-detections may indicate the absence of circumsubstellar disks, a slow rotation rate of young companions, the upper atmospheres containing primarily submicron-sized dust grains, and/or limited cloud inhomogeneity. Finally, we present images of the circumstellar disks of DH Tau, GQ Lup, PDS 70, Beta Pic, and HD 106906., Comment: Accepted for publication in A&A. Shortened abstract. 29 pages, 22 figures
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- 2021
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18. Searching for proto-planets with MUSE
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Xie, C., Haffert, S. Y., de Boer, J., Kenworthy, M. A., Brinchmann, J., Girard, J., Snellen, I. A. G., and Keller, C. U.
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Astrophysics - Earth and Planetary Astrophysics ,Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Solar and Stellar Astrophysics - Abstract
Protoplanetary disks contain structures such as gaps, rings, and spirals, which are thought to be produced by the interaction between the disk and embedded protoplanets. However, only a few planet candidates are found orbiting within protoplanetary disks, and most of them are being challenged as having been confused with disk features. We aim to discover more proto-planetary candidates with MUSE, with a secondary aim of improving the high-resolution spectral differential imaging (HRSDI) technique by analyzing the instrumental residuals of MUSE. We analyzed MUSE observations of five young stars and applied the HRSDI technique to perform high-contrast imaging. With a 30 min integration time, MUSE can reach 5$\sigma$ detection limits in apparent H$\alpha$ line flux down to 10$^{-14}$ and 10$^{-15}$ erg s$^{-1}$ cm$^{-2}$ at 0.075" and 0.25", respectively. In addition to PDS 70 b and c, we did not detect any clear accretion signatures in PDS 70, J1850-3147, and V1094 Sco down to 0.1". MUSE avoids the small sample statistics problem by measuring the noise characteristics in the spatial direction at multiple wavelengths. We detected two asymmetric atomic jets in HD 163296. The HRSDI technique when applied to MUSE data allows us to reach the photon noise limit at small separations (i.e., < 0.5"). With a higher spectral resolution, MUSE can achieve fainter detection limits in apparent line flux than SPHERE/ZIMPOL by a factor of $\sim$5. MUSE has some instrumental issues that limit the contrast that appear in cases with strong point sources, which can be either a spatial point source due to high Strehl observations or a spectral point source due to a high line-to-continuum ratio. We modified the HRSDI technique to better handle the instrumental artifacts and improve the detection limits., Comment: 14 pages, 15 figures, 4 tables. Accepted for publication in A&A
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- 2020
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19. CS Cha B: A disc-obscured M-type star mimicking a polarised planetary companion
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Haffert, S. Y., van Holstein, R. G., Ginski, C., Brinchmann, J., Snellen, I. A. G., Milli, J., Stolker, T., Keller, C. U., and Girard, J.
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Astrophysics - Earth and Planetary Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Astrophysics - Solar and Stellar Astrophysics - Abstract
Context. Direct imaging provides a steady flow of newly discovered giant planets and brown dwarf companions. These multi-object systems can provide information about the formation of low-mass companions in wide orbits and/or help us to speculate about possible migration scenarios. Accurate classification of companions is crucial for testing formation pathways. Aims. In this work we further characterise the recently discovered candidate for a planetary-mass companion CS Cha b and determine if it is still accreting. Methods. MUSE is a four-laser-adaptive-optics-assisted medium-resolution integral-field spectrograph in the optical part of the spectrum. We observed the CS Cha system to obtain the first spectrum of CS Cha b. The companion is characterised by modelling both the spectrum from 6300 $\unicode{x212B}$ to 9300 $\unicode{x212B}$ and the photometry using archival data from the visible to the near-infrared (NIR). Results. We find evidence of accretion and outflow signatures in H$\mathrm{\alpha}$ and OI emission. The atmospheric models with the highest likelihood indicate an effective temperature of $3450\pm50$ K with a $\log{g}$ of $3.6\pm0.5$ dex. Based on evolutionary models, we find that the majority of the object is obscured. We determine the mass of the faint companion with several methods to be between 0.07 $M_{\odot}$ and 0.71 $M_{\odot}$ with an accretion rate of $\dot{M} = 4 \times 10^{-11 \pm 0.4}$ Myr$^{-1}$. Conclusions. Our results show that CS Cha B is most likely a mid-M-type star that is obscured by a highly inclined disc, which has led to its previous classification using broadband NIR photometry as a planetary-mass companion. This shows that it is important and necessary to observe over a broad spectral range to constrain the nature of faint companions, Comment: 9 pages, 6 figures, accepted for publication by A&A
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- 2020
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20. SPHERE+: Imaging young Jupiters down to the snowline
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Boccaletti, A., Chauvin, G., Mouillet, D., Absil, O., Allard, F., Antoniucci, S., Augereau, J. -C., Barge, P., Baruffolo, A., Baudino, J. -L., Baudoz, P., Beaulieu, M., Benisty, M., Beuzit, J. -L., Bianco, A., Biller, B., Bonavita, B., Bonnefoy, M., Bos, S., Bouret, J. -C., Brandner, W., Buchschache, N., Carry, B., Cantalloube, F., Cascone, E., Carlotti, A., Charnay, B., Chiavassa, A., Choquet, E., Clenet, Y., Crida, A., De Boer, J., De Caprio, V., Desidera, S., Desert, J. -M., Delisle, J. -B., Delorme, P., Dohlen, K., Doelman, D., Dominik, C., Orazi, V. D, Dougados, C., Doute, S., Fedele, D., Feldt, M., Ferreira, F., Fontanive, C., Fusco, T., Galicher, R., Garufi, A., Gendron, E., Ghedina, A., Ginski, C., Gonzalez, J. -F., Gratadour, D., Gratton, R., Guillot, T., Haffert, S., Hagelberg, J., Henning, T., Huby, E., Janson, M., Kamp, I., Keller, C., Kenworthy, M., Kervella, P., Kral, Q., Kuhn, J., Lagadec, E., Laibe, G., Langlois, M., Lagrange, A. -M., Launhardt, R., Leboulleux, L., Coroller, H. Le, Causi, G. Li, Loupias, M., Maire, A. L., Marleau, G., Martinache, F., Martinez, P., Mary, D., Mattioli, M., Mazoyer, J., Meheut, H., Menard, F., Mesa, D., Meunier, N., Miguel, Y., Milli, J., Min, M., Molliere, P., Mordasini, C., Moretto, G., Mugnier, L., Arena, G. Muro, Nardetto, N., Diaye, M. N, Nesvadba, N., Pedichini, F., Pinilla, P., Por, E., Potier, A., Quanz, S., Rameau, J., Roelfsema, R., Rouan, D., Rigliaco, E., Salasnich, B., Samland, M., Sauvage, J. -F., Schmid, H. -M., Segransan, D., Snellen, I., Snik, F., Soulez, F., Stadler, E., Stam, D., Tallon, M., Thebault, P., Thiebaut, E., Tschudi, C., Udry, S., van Holstein, R., Vernazza, P., Vidal, F., Vigan, A., Waters, R., Wildi, F., Willson, M., Zanutta, A., Zavagno, A., and Zurlo, A.
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Astrophysics - Earth and Planetary Astrophysics ,Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Solar and Stellar Astrophysics - Abstract
SPHERE (Beuzit et al,. 2019) has now been in operation at the VLT for more than 5 years, demonstrating a high level of performance. SPHERE has produced outstanding results using a variety of operating modes, primarily in the field of direct imaging of exoplanetary systems, focusing on exoplanets as point sources and circumstellar disks as extended objects. The achievements obtained thus far with SPHERE (~200 refereed publications) in different areas (exoplanets, disks, solar system, stellar physics...) have motivated a large consortium to propose an even more ambitious set of science cases, and its corresponding technical implementation in the form of an upgrade. The SPHERE+ project capitalizes on the expertise and lessons learned from SPHERE to push high contrast imaging performance to its limits on the VLT 8m-telescope. The scientific program of SPHERE+ described in this document will open a new and compelling scientific window for the upcoming decade in strong synergy with ground-based facilities (VLT/I, ELT, ALMA, and SKA) and space missions (Gaia, JWST, PLATO and WFIRST). While SPHERE has sampled the outer parts of planetary systems beyond a few tens of AU, SPHERE+ will dig into the inner regions around stars to reveal and characterize by mean of spectroscopy the giant planet population down to the snow line. Building on SPHERE's scientific heritage and resounding success, SPHERE+ will be a dedicated survey instrument which will strengthen the leadership of ESO and the European community in the very competitive field of direct imaging of exoplanetary systems. With enhanced capabilities, it will enable an even broader diversity of science cases including the study of the solar system, the birth and death of stars and the exploration of the inner regions of active galactic nuclei., Comment: White paper submitted to ESO on Feb. 20th, 2020
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- 2020
21. The Young Suns Exoplanet Survey: Detection of a wide orbit planetary mass companion to a solar-type Sco-Cen member
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Bohn, A. J., Kenworthy, M. A., Ginski, C., Manara, C. F., Pecaut, M. J., de Boer, J., Keller, C. U., Mamajek, E. E., Meshkat, T., Reggiani, M., Todorov, K. O., and Snik, F.
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Astrophysics - Earth and Planetary Astrophysics ,Astrophysics - Solar and Stellar Astrophysics - Abstract
The Young Suns Exoplanet Survey (YSES) consists of a homogeneous sample of 70 young, solar-mass stars located in the Lower Centaurus-Crux subgroup of the Scorpius-Centaurus association with an average age of $15\pm3\,$Myr. We report the detection of a co-moving companion around the K3IV star TYC 8998-760-1 (2MASSJ13251211-6456207) that is located at a distance of $94.6\pm0.3\,$pc using SPHERE/IRDIS on the VLT. Spectroscopic observations with VLT/X-SHOOTER constrain the mass of the star to $1.00\pm0.02\,M_{\odot}$ and an age of $16.7\pm1.4\,$Myr. The companion TYC 8998-760-1 b is detected at a projected separation of 1.71'', which implies a projected physical separation of $162\,$au. Photometric measurements ranging from $Y$ to $M$ band provide a mass estimate of $14\pm3\,M_\mathrm{jup}$ by comparison to BT-Settl and AMES-dusty isochrones, corresponding to a mass ratio of $q=0.013\pm0.003$ with respect to the primary. We rule out additional companions to TYC 8998-760-1 that are more massive than $12\,M_\mathrm{jup}$ and farther than $12\,$au away from the host. Future polarimetric and spectroscopic observations of this system with ground and space based observatories will facilitate testing of formation and evolution scenarios shaping the architecture of the circumstellar environment around this 'young Sun'., Comment: Accepted for publication in MNRAS (15 pages, 9 figures)
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- 2019
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22. Synthesis and characterization of high-density biosynthetic fuels from myrtenal
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Garrison, Michael D., Luke Keller, C., Woodroffe, Josanne-Dee, Nagel, Eric M., and Harvey, Benjamin G.
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- 2023
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23. Spectral and polarimetric characterization of gazeous and telluric planets with SEE COAST
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Keller C.-U., Pinfield D., Doel P., Cavarroc C., Hough J., Stam D., Galicher R., Tinetti G., Schneider J., Mawet D., Baudoz P., Boccaletti A., Beuzit J.-L., Udry S., Ferrari A., Martin E., Ménard F., and Sein E.
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Physics ,QC1-999 - Abstract
SEE COAST stands for Super Earth Explorer – Coronagraphic Off-Axis Space Telescope. The concept was initially proposed to ESA for Cosmic Vision. None of the direct detection exoplanet proposals were selected in 2007 and we are now pursuing our efforts to consolidate the astrophysical program and the technical developments for the next call for proposal. The prime objective of SEE COAST is to contribute to the understanding of the formation and evolution of planetary systems. Exploring the diversity of these objects is therefore the main driver to define the instrumentation. In the next decade the improvement of radial velocity instruments and obviously temporal coverage will provide us with a large numbers of long period giants as well as telluric planets, namely Super Earths. Obtaining the spectral and polarimetric signatures of these objects in the visible range to measure atmospheric parameters (molecular composition, clouds, soils, …) will be unique and with important scientific returns. A space mission complementary to near IR instruments like SPHERE, GPI, JWST and later ELTs for the full characterization of giants and Super Earths is a first secure step towards the longer term goal that is the characterization of telluric planets with mass and atmosphere comparable to that of the Earth. An overview of the astrophysical motivation and the trade-off that lead to a simple integrated concept of a space-based high contrast imaging instrument are given here.
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- 2011
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24. The Paleogeography of Laurentia in Its Early Years: New Constraints From the Paleoproterozoic East‐Central Minnesota Batholith
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Swanson‐Hysell, Nicholas L, Avery, Margaret S, Zhang, Yiming, Hodgin, Eben B, Sherwood, Robert J, Apen, Francisco E, Boerboom, Terrence J, Keller, C Brenhin, and Cottle, John M
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geochronology ,North America ,Nuna ,paleogeography ,paleomagnetism ,plate motions ,Precambrian ,Proterozoic ,supercontinent ,superior craton ,Geology ,Geophysics ,Geochemistry & Geophysics - Abstract
The ca. 1.83 Ga Trans-Hudson orogeny resulted from collision of an upper plate consisting of the Hearne, Rae, and Slave provinces with a lower plate consisting of the Superior province. While the geologic record of ca. 1.83 Ga peak metamorphism within the orogen suggests that these provinces were a single amalgamated craton from this time onward, a lack of paleomagnetic poles from the Superior province following Trans-Hudson orogenesis has made this coherency difficult to test. We develop a high-quality paleomagnetic pole for northeast-trending diabase dikes of the post-Penokean orogen East-Central Minnesota Batholith (pole longitude: 265.8°; pole latitude: 20.4°; A95: 4.5°; K: 45.6 N: 23) whose age we constrain to be 1,779.1 ± 2.3 Ma (95% CI) with new U-Pb dates. Demagnetization and low-temperature magnetometry experiments establish dike remanence be held by low-Ti titanomagnetite. Thermochronology data constrain the intrusions to have cooled below magnetite blocking temperatures upon initial emplacement with a mild subsequent thermal history within the stable craton. The similarity of this new Superior province pole with poles from the Slave and Rae provinces establishes the coherency of Laurentia following Trans-Hudson orogenesis. This consistency supports interpretations that older discrepant 2.22–1.87 Ga pole positions between the provinces are the result of differential motion through mobile-lid plate tectonics. The new pole supports the northern Europe and North America connection between the Laurentia and Fennoscandia cratons. The pole can be used to jointly reconstruct these cratons ca. 1,780 Ma strengthening the paleogeographic position of these major constituents of the hypothesized late Paleoproterozoic supercontinent Nuna.
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- 2021
25. Passivation properties of ultrafine grain 316L stainless steels manufactured by ball milling and spark plasma sintering
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Hug, E. and Keller, C.
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- 2023
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26. Spatial variations in estimated chronic exposure to traffic-related air pollution in working populations: A simulation
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Cloutier-Fisher Denise, Keller C Peter, Setton Eleanor M, and Hystad Perry W
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Computer applications to medicine. Medical informatics ,R858-859.7 - Abstract
Abstract Background Chronic exposure to traffic-related air pollution is associated with a variety of health impacts in adults and recent studies show that exposure varies spatially, with some residents in a community more exposed than others. A spatial exposure simulation model (SESM) which incorporates six microenvironments (home indoor, work indoor, other indoor, outdoor, in-vehicle to work and in-vehicle other) is described and used to explore spatial variability in estimates of exposure to traffic-related nitrogen dioxide (not including indoor sources) for working people. The study models spatial variability in estimated exposure aggregated at the census tracts level for 382 census tracts in the Greater Vancouver Regional District of British Columbia, Canada. Summary statistics relating to the distributions of the estimated exposures are compared visually through mapping. Observed variations are explored through analyses of model inputs. Results Two sources of spatial variability in exposure to traffic-related nitrogen dioxide were identified. Median estimates of total exposure ranged from 8 μg/m3 to 35 μg/m3 of annual average hourly NO2 for workers in different census tracts in the study area. Exposure estimates are highest where ambient pollution levels are highest. This reflects the regional gradient of pollution in the study area and the relatively high percentage of time spent at home locations. However, for workers within the same census tract, variations were observed in the partial exposure estimates associated with time spent outside the residential census tract. Simulation modeling shows that some workers may have exposures 1.3 times higher than other workers residing in the same census tract because of time spent away from the residential census tract, and that time spent in work census tracts contributes most to the differences in exposure. Exposure estimates associated with the activity of commuting by vehicle to work were negligible, based on the relatively short amount of time spent in this microenvironment compared to other locations. We recognize that this may not be the case for pollutants other than NO2. These results represent the first time spatially disaggregated variations in exposure to traffic-related air pollution within a community have been estimated and reported. Conclusion The results suggest that while time spent in the home indoor microenvironment contributes most to between-census tract variation in estimates of annual average exposures to traffic-related NO2, time spent in the work indoor microenvironment contributes most to within-census tract variation, and time spent in transit by vehicle makes a negligible contribution. The SESM has potential as a policy evaluation tool, given input data that reflect changes in pollution levels or work flow patterns due to traffic demand management and land use development policy.
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- 2008
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27. Detecting life outside our solar system with a large high-contrast-imaging mission
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Snellen, Ignas A. G., Snik, F., Kenworthy, M., Albrecht, S., Anglada-Escudé, G., Baraffe, I., Baudoz, P., Benz, W., Beuzit, J.-L., Biller, B., Birkby, J. L., Boccaletti, A., van Boekel, R., de Boer, J., Brogi, Matteo, Buchhave, L., Carone, L., Claire, M., Claudi, R., Demory, B.-O., Désert, J.-M., Desidera, S., Gaudi, B. S., Gratton, R., Gillon, M., Grenfell, J. L., Guyon, O., Henning, T., Hinkley, S., Huby, E., Janson, M., Helling, C., Heng, K., Kasper, M., Keller, C. U., Krause, O., Kreidberg, L., Madhusudhan, N., Lagrange, A.-M., Launhardt, R., Lenton, T. M., Lopez-Puertas, M., Maire, A.-L., Mayne, N., Meadows, V., Mennesson, B., Micela, G., Miguel, Y., Milli, J., Min, M., de Mooij, E., Mouillet, D., N’Diaye, M., D’Orazi, V., Palle, E., Pagano, I., Piotto, G., Queloz, D., Rauer, H., Ribas, I., Ruane, G., Selsis, F., Sozzetti, A., Stam, D., Stark, C.C., Vigan, A., and de Visser, Pieter
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- 2022
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28. Opportunities for using spatial property assessment data in air pollution exposure assessments
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Keller C Peter, Hystad Perry W, and Setton Eleanor M
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Computer applications to medicine. Medical informatics ,R858-859.7 - Abstract
Abstract Background Many epidemiological studies examining the relationships between adverse health outcomes and exposure to air pollutants use ambient air pollution measurements as a proxy for personal exposure levels. When pollution levels vary at neighbourhood levels, using ambient pollution data from sparsely located fixed monitors may inadequately capture the spatial variation in ambient pollution. A major constraint to moving toward exposure assessments and epidemiological studies of air pollution at a neighbourhood level is the lack of readily available data at appropriate spatial resolutions. Spatial property assessment data are widely available in North America and may provide an opportunity for developing neighbourhood level air pollution exposure assessments. Results This paper provides a detailed description of spatial property assessment data available in the Pacific Northwest of Canada and the United States, and provides examples of potential applications of spatial property assessment data for improving air pollution exposure assessment at the neighbourhood scale, including: (1) creating variables for use in land use regression modelling of neighbourhood levels of ambient air pollution; (2) enhancing wood smoke exposure estimates by mapping fireplace locations; and (3) using data available on individual building characteristics to produce a regional air pollution infiltration model. Conclusion Spatial property assessment data are an extremely detailed data source at a fine spatial resolution, and therefore a source of information that could improve the quality and spatial resolution of current air pollution exposure assessments.
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- 2005
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29. RefPlanets: Search for reflected light from extra-solar planets with SPHERE/ZIMPOL
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Hunziker, S., Schmid, H. M., Mouillet, D., Milli, J., Zurlo, A., Delorme, P., Abe, L., Avenhaus, H., Baruffolo, A., Bazzon, A., Boccaletti, A., Baudoz, P., Beuzit, J. L., Carbillet, M., Chauvin, G., Claudi, R., Costille, A., Daban, J. B., Desidera, S., Dohlen, K., Dominik, C., Downing, M., Engler, N., Feldt, M., Fusco, T., Ginski, C., Gisler, D., Girard, J. H., Gratton, R., Henning, Th., Hubin, N., Kasper, M., Keller, C. U., Langlois, M., Lagadec, E., Martinez, P., Maire, A. L., Menard, F., Meyer, M. R., Pavlov, A., Pragt, J., Puget, P., Quanz, S. P., Rickman, E., Roelfsema, R., Salasnich, B., Sauvage, J. F., Siebenmorgen, R., Sissa, E., Snik, F., Suarez, M., Szulagyi, J., Thalmann, Ch., Turatto, M., Udry, S., van Holstein, R. G., Vigan, A., and Wildi, F.
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Astrophysics - Earth and Planetary Astrophysics ,Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Solar and Stellar Astrophysics - Abstract
RefPlanets is a guaranteed time observation (GTO) programme that uses the Zurich IMaging POLarimeter (ZIMPOL) of SPHERE/VLT for a blind search for exoplanets in wavelengths from 600-900 nm. The goals of this study are the characterization of the unprecedented high polarimetic contrast and polarimetric precision capabilities of ZIMPOL for bright targets, the search for polarized reflected light around some of the closest bright stars to the Sun and potentially the direct detection of an evolved cold exoplanet for the first time. For our observations of Alpha Cen A and B, Sirius A, Altair, Eps Eri and Tau Ceti we used the polarimetric differential imaging (PDI) mode of ZIMPOL which removes the speckle noise down to the photon noise limit for angular separations >0.6". We describe some of the instrumental effects that dominate the noise for smaller separations and explain how to remove these additional noise effects in post-processing. We then combine PDI with angular differential imaging (ADI) as a final layer of post-processing to further improve the contrast limits of our data at these separations. For good observing conditions we achieve polarimetric contrast limits of 15.0-16.3 mag at the effective inner working angle of about 0.13", 16.3-18.3 mag at 0.5" and 18.8-20.4 mag at 1.5". The contrast limits closer in (<0.6") depend significantly on the observing conditions, while in the photon noise dominated regime (>0.6"), the limits mainly depend on the brightness of the star and the total integration time. We compare our results with contrast limits from other surveys and review the exoplanet detection limits obtained with different detection methods. For all our targets we achieve unprecedented contrast limits. Despite the high polarimetric contrasts we are not able to find any additional companions or extended polarized light sources in the data that has been taken so far., Comment: 23 pages, 17 figures, 2 table, Accepted for publication in A&A
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- 2019
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30. The polarimetric imaging mode of VLT/SPHERE/IRDIS I: Description, data reduction and observing strategy
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de Boer, J., Langlois, M., van Holstein, R. G., Girard, J. H., Mouillet, D., Vigan, A., Dohlen, K., Snik, F., Keller, C. U., Ginski, C., Stam, D. M., Milli, J., Wahhaj, Z., Kasper, M., Schmid, H. M., Rabou, P., Gluck, L., Hugot, E., Perret, D., Martinez, P., Weber, L., Pragt, J., Sauvage, J. -F., Boccaletti, A., Coroller, H. Le, Dominik, C., Henning, T., Lagadec, E., Ménard, F., Turatto, M., Udry, S., Chauvin, G., Feldt, M., and Beuzit, J. -L.
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Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Earth and Planetary Astrophysics - Abstract
Context. Polarimetric imaging is one of the most effective techniques for high-contrast imaging and characterization of protoplanetary disks, and has the potential to be instrumental in characterizing exoplanets. VLT/SPHERE contains the InfraRed Dual-band Imager and Spectrograph (IRDIS) with a dual-beam polarimetric imaging (DPI) mode, which offers the capability to obtain linear polarization images at high contrast and resolution. Aims. We aim to provide an overview of IRDIS/DPI and study its optical design to improve observing strategies and data reduction. Methods. For H-band observations of TW Hya, we compare two data reduction methods that correct for instrumental polarization effects in different ways: a minimization of the noise image, and a polarimetric-model-based correction method that we present in Paper II of this study. Results. We use observations of TW Hya to illustrate the data reduction. In the images of the protoplanetary disk around this star we detect variability in the polarized intensity and angle of linear polarization with pointing-dependent instrument configuration. We explain these variations as instrumental polarization effects and correct for these effects using our model-based correction method. Conclusions. IRDIS/DPI has proven to be a very successful and productive high-contrast polarimetric imaging system. However, the instrument performance depends on the specific instrument configuration. We suggest adjustments to future observing strategies to optimize polarimetric efficiency in field tracking mode by avoiding unfavourable derotator angles. We recommend reducing on-sky data with the pipeline called IRDAP that includes the model-based correction method (described in Paper II) to optimally account for the remaining telescope and instrumental polarization effects and to retrieve the true polarization state of the incident light., Comment: 17 pages, 10 figures
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- 2019
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31. The polarimetric imaging mode of VLT/SPHERE/IRDIS II: Characterization and correction of instrumental polarization effects
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van Holstein, R. G., Girard, J. H., de Boer, J., Snik, F., Milli, J., Stam, D. M., Ginski, C., Mouillet, D., Wahhaj, Z., Schmid, H. M., Keller, C. U., Langlois, M., Dohlen, K., Vigan, A., Pohl, A., Carbillet, M., Fantinel, D., Maurel, D., Origné, A., Petit, C., Ramos, J., Rigal, F., Sevin, A., Boccaletti, A., Coroller, H. Le, Dominik, C., Henning, T., Lagadec, E., Ménard, F., Turatto, M., Udry, S., Chauvin, G., Feldt, M., and Beuzit, J. -L.
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Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Earth and Planetary Astrophysics - Abstract
Context. Circumstellar disks and self-luminous giant exoplanets or companion brown dwarfs can be characterized through direct-imaging polarimetry at near-infrared wavelengths. SPHERE/IRDIS at the Very Large Telescope has the capabilities to perform such measurements, but uncalibrated instrumental polarization effects limit the attainable polarimetric accuracy. Aims. We aim to characterize and correct the instrumental polarization effects of the complete optical system, i.e. the telescope and SPHERE/IRDIS. Methods. We create a detailed Mueller matrix model in the broadband filters Y-, J-, H- and Ks, and calibrate it using measurements with SPHERE's internal light source and observations of two unpolarized stars. We develop a data-reduction method that uses the model to correct for the instrumental polarization effects, and apply it to observations of the circumstellar disk of T Cha. Results. The instrumental polarization is almost exclusively produced by the telescope and SPHERE's first mirror and varies with telescope altitude angle. The crosstalk primarily originates from the image derotator (K-mirror). At some orientations, the derotator causes severe loss of signal (>90% loss in H- and Ks-band) and strongly offsets the angle of linear polarization. With our correction method we reach in all filters a total polarimetric accuracy of <0.1% in the degree of linear polarization and an accuracy of a few degrees in angle of linear polarization. Conclusions. The correction method enables us to accurately measure the polarized intensity and angle of linear polarization of circumstellar disks, and is a vital tool for detecting unresolved (inner) disks and measuring the polarization of substellar companions. We have incorporated the correction method in a highly-automatic end-to-end data-reduction pipeline called IRDAP which is publicly available at https://irdap.readthedocs.io., Comment: 28 pages, 25 figures
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- 2019
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32. Search for gas from the disintegrating rocky exoplanet K2-22b
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Ridden-Harper, A. R., Snellen, I. A. G., Keller, C. U., and Mollière, P.
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Astrophysics - Earth and Planetary Astrophysics - Abstract
[Abridged] Aims. We searched for circumplanetary sodium and ionized calcium gas around the disintegrating rocky exoplanet K2-22 b to constrain its gas-loss and sublimation processes. Methods. We observed four transits of K2-22 b with X-shooter on ESO's Very Large Telescope to obtain time-series of intermediate-resolution (R $\sim$ 11400) spectra. Our analysis focused on the two sodium D lines (588.995 nm and 589.592 nm) and the Ca$^{+}$ triplet (849.802 nm, 854.209 nm and 866.214 nm). Planet-related absorption is searched for in the velocity rest frame of the planet, which changes from $\pm$66 kms$^{-1}$ during the transit. Results. Since K2-22 b exhibits highly variable transit depths, we analyzed the individual nights and their average. By injecting signals we reached 5$\sigma$ upper-limits on the individual nights that ranged from 11% - 13% and 1.7% - 2.0% for the tail's sodium and ionized calcium absorption, respectively. Night 1 was contaminated by its companion star so we considered weighted averages with and without Night 1 and quote conservative 5$\sigma$ limits without Night 1 of 9% and 1.4%, respectively. Assuming their mass fractions to be similar to those in the Earth's crust, these limits correspond to scenarios in which 0.04% and 35% of the transiting dust is sublimated and observed as absorbing gas. However, this assumes the gas to be co-moving with the planet. We show that for the high irradiation environment of K2-22 b, sodium and ionized calcium could be quickly accelerated to 100s of km s$^{-1}$ due to radiation pressure and entrainment by the stellar wind, making them much more difficult to detect. No evidence for such possibly broad and blue-shifted signals are seen in our data. Conclusions. Future observations aimed at observing circumplanetary gas should take into account the possible broad and blue-shifted velocity field of atomic and ionized species., Comment: Accepted on 7 June 2019 for publication in Astronomy and Astrophysics (A&A). 17 pages, 11 figures. Submission updated after language editing by A&A
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- 2019
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33. Two accreting protoplanets around the young star PDS 70
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Haffert, S. Y., Bohn, A. J., de Boer, J., Snellen, I. A. G., Brinchmann, J., Girard, J. H., Keller, C. U., and Bacon, R.
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Astrophysics - Earth and Planetary Astrophysics - Abstract
Newly forming proto-planets are expected to create cavities and substructures in young, gas-rich proto-planetary disks, but they are difficult to detect as they could be confused with disk features affected by advanced image-analysis techniques. Recently, a planet was discovered inside the gap of the transitional disk of the T-Tauri star PDS 70. Here we report on the detection of strong H-alpha emission from two distinct locations in the PDS 70 system, one corresponding to the previously discovered planet PDS 70 b, which confirms the earlier H$\alpha$ detection, and another located close to the outer-edge of the gap, coinciding with a previously identified bright dust spot in the disk and with a small opening in a ring of molecular emission. We identify this second H$\alpha$ peak as a second proto-planet in the PDS 70 system. The H$\alpha$ emission spectra of both proto-planets indicate ongoing accretion onto the proto-planets, which appear to be near a 2:1 mean motion resonance. Our observations show that adaptive-optics-assisted, medium-resolution, integral-field spectroscopy with MUSE targeting accretion signatures will be a powerful way to trace ongoing planet formation in transitional disks at different stages of their evolution. Finding more young planetary systems in mean motion resonance would give credibility to the Grand Tack hypothesis in which Jupiter and Saturn migrated in a resonance orbit during the early formation period of our Solar System., Comment: Nature Astronomy, June 3, 2019; 15 pages, 3 Figs, 1 Table
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- 2019
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34. Discovery of a directly imaged disk in scattered light around the Sco-Cen member Wray 15-788
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Bohn, A. J., Kenworthy, M. A., Ginski, C., Benisty, M., de Boer, J., Keller, C. U., Mamajek, E. E., Meshkat, T., Muro-Arena, G. A., Pecaut, M. J., Snik, F., Wolff, S. G., and Reggiani, M.
- Subjects
Astrophysics - Solar and Stellar Astrophysics ,Astrophysics - Earth and Planetary Astrophysics - Abstract
As part of our on-going survey we have carried out high-contrast imaging with VLT/SPHERE/IRDIS to obtain polarized and total intensity images of the young ($11^{+16}_{-7}$Myr old) K3IV star Wray 15-788 within the Lower Centaurus Crux subgroup of Sco-Cen. For the total intensity images, we remove the stellar halo by an approach based on reference star differential imaging in combination with principal component analysis. Both total intensity and polarimetric data resolve a disk around Wray 15-788. Modeling of the stellar spectral energy distribution suggests that this is a protoplanetary disk at a transition stage. We detect a bright, outer ring at a projected separation of $\sim$370mas ($\approx$56au), hints for inner substructures at $\sim$170mas ($\approx$28au) and a gap in between. Only within a position angle range of $60^\circ<\varphi<240^\circ$, we are confident at 5$\sigma$ level to detect actual scattered light flux from the outer ring of the disk; the remaining part is indistinguishable from background noise. For the detected part of the outer ring we determine a disk inclination of $i$=21$^\circ\pm$6$^\circ$ and a position angle of $\varphi$=76$^\circ\pm$16$^\circ$. Furthermore, we find that Wray 15-788 is part of a binary system with the A2V star HD 98363 at a separation of $\sim$50'' ($\approx$6900au). The detection of only half of the outer ring might be due to shadowing by a misaligned inner disk. A potential substellar companion can cause the misalignment of the inner structures and can be responsible for clearing the detected gap from scattering material. We can not, however, rule out the possibility of a non-detection due to our limited signal to noise ratio, combined with brightness azimuthal asymmetry. From our data, we can exclude companions more massive than 10$M_\mathrm{jup}$ within the gap at a separation of $\sim$230mas ($\approx$35au)., Comment: Accepted for publication in A&A (16 pages, 11 figures)
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- 2019
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35. Soil CO2 in organic and no-till agroecosystems
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Lockhart, Summer R.A., Keller, C. Kent, Evans, R. David, Carpenter-Boggs, Lynne A., and Huggins, David R.
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- 2023
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36. Constraining crustal silica on ancient Earth
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Keller, C Brenhin and Harrison, T Mark
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Earth Sciences ,Geochemistry ,Geology ,Geophysics ,continental crust ,plate tectonics ,Archean ,Hadean - Abstract
Accurately quantifying the composition of continental crust on Hadean and Archean Earth is critical to our understanding of the physiography, tectonics, and climate of our planet at the dawn of life. One longstanding paradigm involves the growth of a relatively mafic planetary crust over the first 1 to 2 billion years of Earth history, implying a lack of modern plate tectonics and a paucity of subaerial crust, and consequently lacking an efficient mechanism to regulate climate. Others have proposed a more uniformitarian view in which Archean and Hadean continents were only slightly more mafic than at present. Apart from complications in assessing early crustal composition introduced by crustal preservation and sampling biases, effects such as the secular cooling of Earth's mantle and the biologically driven oxidation of Earth's atmosphere have not been fully investigated. We find that the former complicates efforts to infer crustal silica from compatible or incompatible element abundances, while the latter undermines estimates of crustal silica content inferred from terrigenous sediments. Accounting for these complications, we find that the data are most parsimoniously explained by a model with nearly constant crustal silica since at least the early Archean.
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- 2020
37. Global, regional, and national burden of disorders affecting the nervous system, 1990–2021: a systematic analysis for the Global Burden of Disease Study 2021
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D., Seeher K. M., Schiess N., Nichols E., Cao B., Servili C., Cavallera V., Cousin E., Hagins H., Moberg M. E., Mehlman M. L., Abate Y. H., Abbas J., Abbasi M. A., Abbasian M., Abbastabar H., Abdelmasseh M., Abdollahi M., Abdollahifar M. -A., Abd-Rabu R., Abdulah D. M., Abdullahi A., Abedi A., Abedi V., Abeldano Zuniga R. A., Abidi H., Abiodun O., Aboagye R. G., Abolhassani H., Aboyans V., Abrha W. A., Abualhasan A., Abu-Gharbieh E., Aburuz S., Adamu L. H., Addo I. Y., Adebayo O. M., Adekanmbi V., Adekiya T. A., Adikusuma W., Adnani Q. E. S., Adra S., Afework T., Afolabi A. A., Afraz A., Afzal S., Aghamiri S., Agodi A., Agyemang-Duah W., Ahinkorah B. O., Ahmad A., Ahmad D., Ahmad S., Ahmadzade A. M., Ahmed A., Ahmed H., Ahmed J. Q., Ahmed L. A., Ahmed M. B., Ahmed S. A., Ajami M., Aji B., Ajumobi O., Akade S., Akbari M., Akbarialiabad H., Akhlaghi S., Akinosoglou K., Akinyemi R. O., Akonde M., Al Hasan S. M., Alahdab F., Al-Ahdal T. M. A., Al-Amer R. M., Albashtawy M., AlBataineh M. T., Aldawsari K. A., Alemi H., Alemi S., Algammal A. M., Al-Gheethi A. A. S., Alhalaiqa F. A. N., Alhassan R. K., Ali A., Ali E. A., Ali L., Ali M. U., Ali M. M., Ali R., Ali S., Shujait Ali S. S., Ali Z., Alif S. M., Alimohamadi Y., Aliyi A. A., Aljofan M., Aljunid S. M., Alladi S., Almazan J. U., Almustanyir S., Al-Omari B., Alqahtani J. S., Alqasmi I., Alqutaibi A. Y., Al-Shahi Salman R., Altaany Z., Al-Tawfiq J. A., Altirkawi K. A., Alvis-Guzman N., Al-Worafi Y. M., Aly H., Aly S., Alzoubi K. H., Amani R., Amindarolzarbi A., Amiri S., Amirzade-Iranaq M. H., Amu H., Amugsi D. A., Amusa G. A., Amzat J., Ancuceanu R., Anderlini D., Anderson D. B., Andrei C. L., Androudi S., Angappan D., Angesom T. W., Anil A., Ansari-Moghaddam A., Anwer R., Arafat M., Aravkin A. Y., Areda D., Ariffin H., Arifin H., Arkew M., Arnlov J., Arooj M., Artamonov A. A., Artanti K. D., Aruleba R. T., Asadi-Pooya A. A., Asena T. F., Asghari-Jafarabadi M., Ashraf M., Ashraf T., Atalell K. A., Athari S. S., Atinafu B. T. T., Atorkey P., Atout M. M. W., Atreya A., Aujayeb A., Avan A., Ayala Quintanilla B. P. A., Ayatollahi H., Ayinde O. O., Mohammad Ayyoubzadeh S., Azadnajafabad S., Azizi Z., Azizian K., Azzam A. Y., Babaei M., Badar M., Badiye A. D., Baghdadi S., Bagherieh S., Bai R., Baig A. A., Balakrishnan S., Balalla S., Baltatu O. C., Banach M., Bandyopadhyay S., Banerjee I., Baran M. F., Barboza M. A., Barchitta M., Bardhan M., Barker-Collo S. L., Barnighausen T. W., Barrow A., Bashash D., Bashiri H., Bashiru H. A., Basiru A., Basso J., Basu S., Batiha A. M. M., Batra K., Baune B. T., Bedi N., Begde A., Begum T., Behnam B., Behnoush A. H., Beiranvand M., Bejot Y., Bekele A., Belete M. A., Belgaumi U. I., Bemanalizadeh M., Bender R. G., Benfor B., Bennett D. A., Bensenor I. M., Berice B., Bettencourt P. J. G., Beyene K. A., Bhadra A., Bhagat D. S., Bhangdia K., Bhardwaj N., Bhardwaj P., Bhargava A., Bhaskar S., Bhat A. N., Bhat V., Bhatti G. K., Bhatti J. S., Bhatti R., Bijani A., Bikbov B., Bilalaga M. M., Biswas A., Bitaraf S., Bitra V. R., Bjorge T., Bodolica V., Bodunrin A. O., Boloor A., Braithwaite D., Brayne C., Brenner H., Briko A., Bringas Vega M. L., Brown J., Budke C. M., Buonsenso D., Burkart K., Burns R. A., Bustanji Y., Butt M. H., Butt N. S., Butt Z. A., Cabral L. S., dos Santos F. L. C., Calina D., Campos-Nonato I. R., Cao C., Carabin H., Cardenas R., Carreras G., Carvalho A. F., Castaneda-Orjuela C. A., Casulli A., Catala-Lopez F., Catapano A. L., Caye A., Cegolon L., Cenderadewi M., Cerin E., Chacon-Uscamaita P. R. U., Chan J. S. K., Chanie G. S., Charan J., Chattu V. K., Chekol Abebe E., Chen H., Chen J., Chi G., Chichagi F., Chidambaram S. B., Chimoriya R., Ching P. R., Chitheer A., Chong Y. Y., Chopra H., Choudhari S. G., Chowdhury E. K., Chowdhury R., Christensen H., Chu D. -T., Chukwu I. S., Chung E., Coberly K., Columbus A., Comachio J., Conde J., Cortesi P. A., Costa V. M., Couto R. A. S., Criqui M. H., Cruz-Martins N., Dabbagh Ohadi M. A., Dadana S., Dadras O., Dai X., Dai Z., D'Amico E., Danawi H. A., Dandona L., Dandona R., Darwish A. H., Das S., Dascalu A. M., Dash N. R., Dashti M., De la Hoz F. P., de la Torre-Luque A., De Leo D., Dean F. E., Dehghan A., Dejene H., Demant D., Demetriades A. K., Demissie S., Deng X., Desai H. D., Devanbu V. G. C., Dhama K., Dharmaratne S. D., Dhimal M., Dias da Silva D., Diaz D., Dibas M., Ding D. D., Dinu M., Dirac M. A., Diress M., Do T. C., Do T. H. P., Doan K. D. K., Dodangeh M., Doheim M. F., Dokova K. G., Dongarwar D., Dsouza H. L., Dube J., Duraisamy S., Durojaiye O. C., Dutta S., Dziedzic A. M., Edinur H. A., Eissazade N., Ekholuenetale M., Ekundayo T. C., El Nahas N., El Sayed I. E., Elahi Najafi M. A. E., Elbarazi I., Elemam N. M., Elgar F. J., Elgendy I. Y., Elhabashy H. R., Elhadi M., Elilo L. T., Ellenbogen R. G., Elmeligy O. A. A., Elmonem M. A., Elshaer M., Elsohaby I., Emamverdi M., Emeto T. I., Endres M., Esezobor C. I., Eskandarieh S., Fadaei A., Fagbamigbe A. F., Fahim A., Faramarzi A., Fares J., Farjoud Kouhanjani M., Faro A., Farzadfar F., Fatehizadeh A., Fathi M., Fathi S., Fatima S. A. F., Feizkhah A., Fereshtehnejad S. -M., Ferrari A. J., Ferreira N., Fetensa G., Firouraghi N., Fischer F., Fonseca A. C., Force L. M., Fornari A., Foroutan B., Fukumoto T., Gadanya M. A., Gaidhane A. M., Galali Y., Galehdar N., Gan Q., Gandhi A. P., Ganesan B., Gardner W. M., Garg N., Gau S. -Y., Gautam R. K., Gebre T., Gebrehiwot M., Gebremeskel G. G., Gebreslassie H. G., Getacher L., Ghaderi Yazdi B., Ghadirian F., Ghaffarpasand F., Ghanbari R., Ghasemi M., Ghazy R. M., Ghimire S., Gholami A., Gholamrezanezhad A., Ghotbi E., Ghozy S., Gialluisi A., Gill P. S., Glasstetter L. M., Gnedovskaya E. V., Golchin A., Golechha M., Goleij P., Golinelli D., Gomes-Neto M., Goulart A. C., Goyal A., Gray R. J., Grivna M., Guadie H. A., Guan B., Guarducci G., Guicciardi S., Gunawardane D. A., Guo H., Gupta B., Gupta R., Gupta S., Gupta V. B., Gupta V. K., Gutierrez R. A., Habibzadeh F., Hachinski V., Haddadi R., Hadei M., Hadi N. R., Haep N., Haile T. G., Haj-Mirzaian A., Hall B. J., Halwani R., Hameed S., Hamiduzzaman M., Hammoud A., Han H., Hanifi N., Hankey G. J., Hannan M. A., Hao J., Harapan H., Hareru H. E., Hargono A., Harlianto N. I., Haro J. M., Hartman N. N., Hasaballah A. I., Hasan F., Hasani H., Hasanian M., Hassan A., Hassan S., Hassanipour S., Hassankhani H., Hassen M. B., Haubold J., Hay S. I., Hayat K., Hegazy M. I., Heidari G., Heidari M., Heidari-Soureshjani R., Hesami H., Hezam K., Hiraike Y., Hoffman H. J., Holla R., Hopf K. P., Horita N., Hossain M. M., Hossain M. B., Hossain S., Hosseinzadeh H., Hosseinzadeh M., Hostiuc S., Hu C., Huang J., Huda M. N., Hussain J., Hussein N. R., Huynh H. -H., Hwang B. -F., Ibitoye S. E., Ilaghi M., Ilesanmi O. S., Ilic I. M., Ilic M. D., Immurana M., Iravanpour F., Islam S. M. S., Ismail F., Iso H., Isola G., Iwagami M., Iwu C. C. D., Iyer M., Jaan A., Jacob L., Jadidi-Niaragh F., Jafari M., Jafarinia M., Jafarzadeh A., Jahankhani K., Jahanmehr N., Jahrami H., Jaiswal A., Jakovljevic M., Jamora R. D. G., Jana S., Javadi N., Javed S., Javeed S., Jayapal S. K., Jayaram S., Jiang H., Johnson C. O., Johnson W. D., Jokar M., Jonas J. B., Joseph A., Joseph N., Joshua C. E., Jurisson M., Kabir A., Kabir Z., Kabito G. G., Kadashetti V., Kafi F., Kalani R., Kalantar F., Kaliyadan F., Kamath A., Kamath S., Kanchan T., Kandel A., Kandel H., Kanmodi K. K., Karajizadeh M., Karami J., Karanth S. D., Karaye I. M., Karch A., Karimi A., Karimi H., Karimi Behnagh A., Kasraei H., Kassebaum N. J., Kauppila J. H., Kaur H., Kaur N., Kayode G. A., Kazemi F., Keikavoosi-Arani L., Keller C., Keykhaei M., Khadembashiri M. A., Khader Y. S., Khafaie M. A., Khajuria H., Khalaji A., Khamesipour F., Khammarnia M., Khan M., Khan M. A. B., Khan Y. H., Suheb M. Z. K., Khanmohammadi S., Khanna T., Khatab K., Khatatbeh H., Khatatbeh M. M., Khateri S., Khatib M. N., Khayat Kashani H. R., Khonji M. S., Khorashadizadeh F., Khormali M., Khubchandani J., Kian S., Kim G., Kim J., Kim M. S., Kim Y. J., Kimokoti R. W., Kisa A., Kisa S., Kivimaki M., Kochhar S., Kolahi A. -A., Koly K. N., Kompani F., Koroshetz W. J., Kosen S., Kourosh Arami M., Koyanagi A., Kravchenko M. A., Krishan K., Krishnamoorthy V., Defo B. K., Kuddus M. A., Kumar A., Kumar G. A., Kumar M., Kumar N., Kumsa N. B., Kundu S., Kurniasari M. D., Kusuma D., Kuttikkattu A., Kyu H. H., La Vecchia C., Ladan M. A., Lahariya C., Laksono T., Lal D. K., Lallukka T., Lam J., Lami F. H., Landires I., Langguth B., Lasrado S., Latief K., Latifinaibin K., Lau K. M. -M., Laurens M. B., Lawal B. K., Le L. K. D., Le T. T. T., Ledda C., Lee M., Lee S. -W., Lee S. W., Lee W. -C., Lee Y. H., Leonardi M., Lerango T. L., Li M. -C., Li W., Ligade V. S., Lim S. S., Linehan C., Liu C., Liu J., Liu W., Lo C. -H., Lo W. D., Lobo S. W., Logroscino G., Lopes G., Lopukhov P. D., Lorenzovici L., Lorkowski S., Loureiro J. A., Lubinda J., Lucchetti G., Saute R. L., Ma Z. F., Mabrok M., Machoy M., Madadizadeh F., El Razek M. M. A., Maghazachi A. A., Maghbouli N., Mahjoub S., Mahmoudi M., Majeed A., Malagon-Rojas J. N., Malakan Rad E., Malhotra K., Malik A. A., Malik I., Mallhi T. H., Malta D. C., Manilal A., Mansouri V., Mansournia M. A., Marasini B. P., Marateb H. R., Maroufi S. F., Martinez-Raga J., Martini S., Martins-Melo F. R., Martorell M., Marz W., Marzo R. R., Massano J., Mathangasinghe Y., Mathews E., Maude R. J., Maugeri A., Maulik P. K., Mayeli M., Mazaheri M., McAlinden C., McGrath J. J., Meena J. K., Mehndiratta M. M., Mendez-Lopez M. A. M., Mendoza W., Mendoza-Cano O., Menezes R. G., Merati M., Meretoja A., Merkin A., Mersha A. M., Mestrovic T., Mi T., Miazgowski T., Michalek I. M., Mihretie E. T., Minh L. H. N., Mirfakhraie R., Mirica A., Mirrakhimov E. M., Mirzaei M., Misganaw A., Misra S., Mithra P., Mizana B. A., Mohamadkhani A., Mohamed N. S., Mohammadi E., Mohammadi H., Mohammadi S., Mohammadshahi M., Mohammed M., Mohammed S., Mohan S., Mojiri-Forushani H., Moka N., Mokdad A. H., Molinaro S., Moller H., Monasta L., Moniruzzaman M., Montazeri F., Moradi M., Moradi Y., Moradi-Lakeh M., Moraga P., Morovatdar N., Morrison S. D., Mosapour A., Mosser J. F., Mossialos E., Motaghinejad M., Mousavi P., Ehsan Mousavi S., Mubarik S., Muccioli L., Mughal F., Mukoro G. D., Mulita A., Mulita F., Musaigwa F., Mustafa A., Mustafa G., Muthu S., Nagarajan A. J., Naghavi P., Naik G. R., Nainu F., Nair T. S., Najmuldeen H. H. R., Nakhostin Ansari N., Nambi G., Namdar Areshtanab H., Nargus S., Nascimento B. R., Naser A. Y., Nashwan A. J. J., Nasoori H., Nasreldein A., Natto Z. S., Nauman J., Nayak B. P., Nazri-Panjaki A., Negaresh M., Negash H., Negoi I., Negoi R. I., Negru S. M., Nejadghaderi S. A., Nematollahi M. H., Nesbit O. D., Newton C. R. J., Nguyen D. H., Nguyen H. T. H., Nguyen H. Q., Nguyen N. -T. T., Nguyen P. T., Nguyen V. T., Niazi R. K., Nikolouzakis T. K., Niranjan V., Nnyanzi L. A., Noman E. A., Noroozi N., Norrving B., Noubiap J. J., Nri-Ezedi C. A., Ntaios G., Nunez-Samudio V., Nurrika D., Oancea B., Odetokun I. A., O'Donnell M. J., Ogunsakin R. E., Oguta J. O., Oh I. -H., Okati-Aliabad H., Okeke S. R., Okekunle A. P., Okonji O. C., Okwute P. G., Olagunju A. T., Olaiya M. T., Olana M. D., Olatubi M. I., Oliveira G. M. M., Olufadewa I. I., Olusanya B. O., Bali A. O., Ong S., Onwujekwe O. E., Ordak M., Orji A. U., Ortega-Altamirano D. V., Osuagwu U. L., Otstavnov N., Otstavnov S. S., Ouyahia A., Owolabi M. O., Mahesh Padukudru P. A., Pacheco-Barrios K., Padubidri J. R., Pal P. K., Palange P. N., Palladino C., Palladino R., Palma-Alvarez R. F., Pan F., Panagiotakos D., Panda-Jonas S., Pandey A., Pandian J. D., Pangaribuan H. U., Pantazopoulos I., Pardhan S., Parija P. P., Parikh R. R., Park S., Parthasarathi A., Pashaei A., Patel J., Patil S., Patoulias D., Pawar S., Pedersini P., Pensato U., Pereira D. M., Pereira J., Pereira M. O., Peres M. F. P., Perico N., Perna S., Petcu I. -R., Petermann-Rocha F. E., Pham H. T., Phillips M. R., Pinilla-Monsalve G. D., Piradov M. A., Plotnikov E., Poddighe D., Polat B., Poluru R., Pond C. D., Poudel G. R., Pouramini A., Pourbagher-Shahri A. M., Pourfridoni M., Pourtaheri N., Prakash P. Y., Prakash S., Prakash V., Prates E. J. S., Pritchett N., Purnobasuki H., Qasim N. H., Qattea I., Qian G., Radhakrishnan V., Raee P., Shahraki H. R., Rafique I., Raggi A., Raghav P. R., Rahati M. M., Rahim F., Rahimi Z., Rahimifard M., Rahman M. O., Rahman M. H. U., Rahman M., Rahman M. A., Rahmani A. M., Rahmani S., Youshanlouei H. R., Rahmati M., Raj Moolambally S., Rajabpour-Sanati A., Ramadan H., Ramasamy S. K., Ramasubramani P., Ramazanu S., Rancic N., Rao I. R., Rao S. J., Rapaka D., Rashedi V., Rashid A. M., Rashidi M. -M., Rashidi Alavijeh M., Rasouli-Saravani A., Rawaf S., Razo C., Redwan E. M. M., Bana A. R., Remuzzi G., Rezaei N., Rezaeian M., Rhee T. G., Riad A., Robinson S. R., Rodrigues M., Rodriguez J. A. B., Roever L., Rogowski E. L. B., Romoli M., Ronfani L., Roy P., Pramanik K. R., Rubagotti E., Ruiz M. A., Russ T. C., Sunnerhagen K. S., Saad A. M. A., Saadatian Z., Saber K., SaberiKamarposhti M., Sacco S., Saddik B., Sadeghi E., Sadeghian S., Saeed U., Safdarian M., Safi S. Z., Sagar R., Sagoe D., Saheb Sharif-Askari F. S., Saheb Sharif-Askari N., Sahebkar A., Sahoo S. S., Sahraian M. A., Sajedi S. A., Sakshaug J. W., Saleh M. A., Salehi Omran H., Salem M. R., Salimi S., Samadi Kafil H., Samadzadeh S., Samargandy S., Samodra Y. L., Samuel V. P., Samy A. M., Sanadgol N., Sanjeev R. K., Sanmarchi F., Santomauro D. F., Santri I. N., Santric-Milicevic M. M., Saravanan A., Sarveazad A., Satpathy M., Saylan M., Sayyah M., Scarmeas N., Schlaich M. P., Schuermans A., Schwarzinger M., Schwebel D. C., Selvaraj S., Sendekie A. K., Sengupta P., Senthilkumaran S., Serban D., Sergindo M. T., Sethi Y., SeyedAlinaghi S., Seylani A., Shabani M., Shabany M., Shafie M., Shahabi S., Shahbandi A., Shahid S., Shahraki-Sanavi F., Shahsavari H. R., Shahwan M. J., Shaikh M. A., Shaji K. S., Sham S., Shama A. T. T., Shamim M. A., Shams-Beyranvand M., Shamsi M. A., Shanawaz M., Sharath M., Sharfaei S., Sharifan A., Sharma M., Sharma R., Shashamo B. B., Shayan M., Sheikhi R. A., Shekhar S., Shen J., Shenoy S. M., Shetty P. H., Shiferaw D. S., Shigematsu M., Shiri R., Shittu A., Shivakumar K. M., Shokri F., Shool S., Shorofi S. A., Shrestha S., Siankam Tankwanchi A. B., Siddig E. E., Sigfusdottir I. D., Silva J. P., Silva L. M. L. R., Sinaei E., Singh B. B., Singh G., Singh P., Singh S., Sirota S. B., Sivakumar S., Sohag A. A. M., Solanki R., Soleimani H., Solikhah S., Solomon Y., Song S., Song Y., Sotoudeh H., Spartalis M., Stark B. A., Starnes J. R., Starodubova A. V., Stein D. J., Steiner T. J., Stovner L. J., Suleman M., Abdulkader R. S., Sultana A., Sun J., Sunkersing D., Sunny A., Susianti H., Swain C. K., Szeto M. D., Tabares-Seisdedos R., Tabatabaei S. M., Tabatabai S., Tabish M., Taheri M., Tahvildari A., Tajbakhsh A., Tampa M., Lukenze Tamuzi J. J. L., Tan K. -K., Tang H., Tareke M., Tarigan I. U., Tat N. Y., Tat V. Y., Tavakoli Oliaee R., Tavangar S. M., Tavasol A., Tefera Y. M., Tehrani-Banihashemi A., Temesgen W. A., Temsah M. -H., Teramoto M., Tesfaye A. H., Tesfaye E. G., Tesler R., Thakali O., Thangaraju P., Thapa R., Thapar R., Thomas N. K., Thrift A. G., Ticoalu J. H. V., Tillawi T., Toghroli R., Tonelli M., Tovani-Palone M. R., Traini E., Tran N. M., Tran N. -H., Van Tran P., Tromans S. J., Truelsen T. C., Truyen T. T. T. T., Tsatsakis A., Tsegay G. M., Tsermpini E. E., Tualeka A. R., Tufa D. G., Ubah C. S., Udoakang A. J., Ulhaq I., Umair M., Umakanthan S., Umapathi K. K., Unim B., Unnikrishnan B., Vaithinathan A. G., Vakilian A., Tahbaz S. V., Valizadeh R., Van den Eynde J., Vart P., Varthya S. B., Vasankari T. J., Vaziri S., Vellingiri B., Venketasubramanian N., Verras G. -I., Vervoort D., Villafane J. H., Villani L., Veloz A. F. V., Viskadourou M., Vladimirov S. K., Vlassov V., Volovat S. R., Vu L. T., Vujcic I. S., Wagaye B., Waheed Y., Wahood W., Walde M. T., Wang F., Wang S., Wang Y., Wang Y. -P., Waqas M., Waris A., Weerakoon K. G., Weintraub R. G., Weldemariam A. H., Westerman R., Whisnant J. L., Wickramasinghe D. P., Wickramasinghe N. D., Willekens B., Wilner L. B., Winkler A. S., Wolfe C. D. A., Wu A. -M., Wulf Hanson S., Xu S., Xu X., Yadollahpour A., Yaghoubi S., Yahya G., Yamagishi K., Yang L., Yano Y., Yao Y., Yehualashet S. S., Yeshaneh A., Yesiltepe M., Yi S., Yigit A., Yigit V., Yon D. K., Yonemoto N., You Y., Younis M. Z., Yu C., Yusuf H., Zadey S., Zahedi M., Zakham F., Zaki N., Zali A., Zamagni G., Zand R., Zandieh G. G. Z., Zangiabadian M., Zarghami A., Zastrozhin M. S., Zeariya M. G. M., Zegeye Z. B., Zeukeng F., Zhai C., Zhang C., Zhang H., Zhang Y., Zhang Z. -J., Zhao H., Zhao Y., Zheng P., Zhou H., Zhu B., Zhumagaliuly A., Zielinska M., Zikarg Y. T., Zoladl M., Murray C. J. L., Ong K. L., Feigin V. L., Vos T., and Dua T.
- Abstract
Background: Disorders affecting the nervous system are diverse and include neurodevelopmental disorders, late-life neurodegeneration, and newly emergent conditions, such as cognitive impairment following COVID-19. Previous publications from the Global Burden of Disease, Injuries, and Risk Factor Study estimated the burden of 15 neurological conditions in 2015 and 2016, but these analyses did not include neurodevelopmental disorders, as defined by the International Classification of Diseases (ICD)-11, or a subset of cases of congenital, neonatal, and infectious conditions that cause neurological damage. Here, we estimate nervous system health loss caused by 37 unique conditions and their associated risk factors globally, regionally, and nationally from 1990 to 2021. Methods: We estimated mortality, prevalence, years lived with disability (YLDs), years of life lost (YLLs), and disability-adjusted life-years (DALYs), with corresponding 95% uncertainty intervals (UIs), by age and sex in 204 countries and territories, from 1990 to 2021. We included morbidity and deaths due to neurological conditions, for which health loss is directly due to damage to the CNS or peripheral nervous system. We also isolated neurological health loss from conditions for which nervous system morbidity is a consequence, but not the primary feature, including a subset of congenital conditions (ie, chromosomal anomalies and congenital birth defects), neonatal conditions (ie, jaundice, preterm birth, and sepsis), infectious diseases (ie, COVID-19, cystic echinococcosis, malaria, syphilis, and Zika virus disease), and diabetic neuropathy. By conducting a sequela-level analysis of the health outcomes for these conditions, only cases where nervous system damage occurred were included, and YLDs were recalculated to isolate the non-fatal burden directly attributable to nervous system health loss. A comorbidity correction was used to calculate total prevalence of all conditions that affect the nervous s
- Published
- 2024
38. Timescales for pluton growth, magma-chamber formation and super-eruptions
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van Zalinge, M. E., Mark, D. F., Sparks, R. S. J., Tremblay, M. M., Keller, C. B., Cooper, F. J., and Rust, A.
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- 2022
- Full Text
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39. SPHERE / ZIMPOL high resolution polarimetric imager. I. System overview, PSF parameters, coronagraphy, and polarimetry
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Schmid, H. M., Bazzon, A., Roelfsema, R., Mouillet, D., Milli, J., Menard, F., Gisler, D., Hunziker, S., Pragt, J., Dominik, C., Boccaletti, A., Ginski, C., Abe, L., Antoniucci, S., Avenhaus, H., Baruffolo, A., Baudoz, P., Beuzit, J. L., Carbillet, M., Chauvin, G., Claudi, R., Costille, A., Daban, J. B., de Haan, M., Desidera, S., Dohlen, K., Downing, M., Elswijk, E., Engler, N., Feldt, M., Fusco, T., Girard, J. H., Gratton, R., Hanenburg, H., Henning, Th., Hubin, N., Joos, F., Kasper, M., Keller, C. U., Langlois, M., Lagadec, E., Martinez, P., Mulder, E., Pavlov, A., Podio, L., Puget, P., Quanz, S., Rigal, F., Salasnich, B., Sauvage, J. F., Schuil, M., Siebenmorgen, R., Sissa, E., Snik, F., Suarez, M., Thalmann, Ch., Turatto, M., Udry, S., van Duin, A., van Holstein, R., Vigan, A., and Wildi, F.
- Subjects
Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
We describe the Zurich Imaging Polarimeter (ZIMPOL), the visual focal plane subsystem of the SPHERE "VLT planet finder", which pushes the limits of current AO systems to shorter wavelengths, higher spatial resolution, and much improved polarimetric performance. We provide new benchmarks for the performance of high contrast instruments, in particular for polarimetric differential imaging. We have analyzed SPHERE/ZIMPOL point spread functions and measure the peak surface brightness, the encircled energy, and the full width half maximum (FWHM) for different wavelengths, atmospheric conditions, star brightness, and instrument modes. Coronagraphic images are described and analized and the performance for different coronagraphs is compared with tests for the binary alpha Hyi with a separation of 92 mas and a contrast of 6 mag. For the polarimetric mode we made the instrument calibrations using zero polarization and high polarization standard stars and here we give a recipe for the absolute calibration of polarimetric data. The data show a small <1 mas but disturbing differential polarimetric beam shifts, which can be explained as Goos-H\"ahnchen shifts from the inclined mirrors, and we discuss how to correct this effect. The polarimetric sensitivity is investigated with non-coronagraphic and deep, coronagraphic observations of the dust scattering around the symbiotic Mira variable R Aqr. SPHERE/ZIMPOL achieves imaging performances in the visual range with unprecedented characteristics, in particular very high spatial resolution and very high polarimetric contrast. This instrument opens up many new research opportunities for the detailed investigation of circumstellar dust, in scattered and therefore polarized light, for the investigation of faint companions, and for the mapping of circumstellar Halpha emission., Comment: 38 pages with 33 figurs, accepted for publication in Astron. Astrophys
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- 2018
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- View/download PDF
40. Chromatic transit light curves of disintegrating rocky planets
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Ridden-Harper, A. R., Keller, C. U., Min, M., van Lieshout, R., and Snellen, I. A. G.
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Astrophysics - Earth and Planetary Astrophysics - Abstract
Context. Kepler observations have revealed a class of short period exoplanets, of which Kepler-1520 b is the prototype, which have comet-like dust tails thought to be the result of small, rocky planets losing mass. The shape and chromaticity of the transits constrain the properties of the dust particles originating from the planet's surface, offering a unique opportunity to probe the composition and geophysics of rocky exoplanets. Aims. We aim to approximate the average Kepler long-cadence light curve of Kepler-1520 b and investigate how the optical thickness and transit cross-section of a general dust tail can affect the observed wavelength dependence and depth of transit light curves. Methods. We developed a new 3D model that ejects sublimating particles from the planet surface to build up a dust tail, assuming it to be optically thin, and used 3D radiative transfer computations that fully treat scattering using the distribution of hollow spheres (DHS) method, to generate transit light curves between 0.45 and 2.5 $\mu$m. Results. We show that the transit depth is wavelength independent for optically thick tails, potentially explaining why only some observations indicate a wavelength dependence. From the 3D nature of our simulated tails, we show that their transit cross-sections are related to the component of particle ejection velocity perpendicular to the planet's orbital plane and use this to derive a minimum ejection velocity of 1.2 kms$^{-1}$. To fit the average transit depth of Kepler-1520 b of 0.87%, we require a high dust mas-loss rate of 7 $-$ 80 M$_\oplus$ Gyr$^{-1}$ which implies planet lifetimes that may be inconsistent with the observed sample. Therefore, these mass-loss rates should be considered to be upper limits., Comment: 22 pages, 22 figures, accepted for publication in A&A
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- 2018
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41. Review of high-contrast imaging systems for current and future ground- and space-based telescopes I. Coronagraph design methods and optical performance metrics
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Ruane, G., Riggs, A., Mazoyer, J., Por, E. H., N'Diaye, M., Huby, E., Baudoz, P., Galicher, R., Douglas, E., Knight, J., Carlomagno, B., Fogarty, K., Pueyo, L., Zimmerman, N., Absil, O., Beaulieu, M., Cady, E., Carlotti, A., Doelman, D., Guyon, O., Haffert, S., Jewell, J., Jovanovic, N., Keller, C., Kenworthy, M. A., Kühn, J., Miller, K., Sirbu, D., Snik, F., Wallace, J. Kent, Wilby, M., and Ygouf, M.
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
The Optimal Optical Coronagraph (OOC) Workshop at the Lorentz Center in September 2017 in Leiden, the Netherlands gathered a diverse group of 25 researchers working on exoplanet instrumentation to stimulate the emergence and sharing of new ideas. In this first installment of a series of three papers summarizing the outcomes of the OOC workshop, we present an overview of design methods and optical performance metrics developed for coronagraph instruments. The design and optimization of coronagraphs for future telescopes has progressed rapidly over the past several years in the context of space mission studies for Exo-C, WFIRST, HabEx, and LUVOIR as well as ground-based telescopes. Design tools have been developed at several institutions to optimize a variety of coronagraph mask types. We aim to give a broad overview of the approaches used, examples of their utility, and provide the optimization tools to the community. Though it is clear that the basic function of coronagraphs is to suppress starlight while maintaining light from off-axis sources, our community lacks a general set of standard performance metrics that apply to both detecting and characterizing exoplanets. The attendees of the OOC workshop agreed that it would benefit our community to clearly define quantities for comparing the performance of coronagraph designs and systems. Therefore, we also present a set of metrics that may be applied to theoretical designs, testbeds, and deployed instruments. We show how these quantities may be used to easily relate the basic properties of the optical instrument to the detection significance of the given point source in the presence of realistic noise., Comment: To appear in Proceedings of the SPIE, vol. 10698
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- 2018
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42. First direct detection of a polarized companion outside of a resolved circumbinary disk around CS Cha
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Ginski, C., Benisty, M., van Holstein, R. G., Juhász, A., Schmidt, T. O. B., Chauvin, G., de Boer, J., Wilby, M., Manara, C. F., Delorme, P., Ménard, F., Pinilla, P., Birnstiel, T., Flock, M., Keller, C., Kenworthy, M., Milli, J., Olofsson, J., Pérez, L., Snik, F., and Vogt, N.
- Subjects
Astrophysics - Earth and Planetary Astrophysics - Abstract
In the present study we aim to investigate the circumstellar environment of the spectroscopic binary T Tauri star CS Cha. From unresolved mid- to far-infrared photometry it is predicted that CS Cha hosts a disk with a large cavity. In addition, SED modeling suggests significant dust settling, pointing towards an evolved disk that may show signs of ongoing or completed planet formation. We observed CS Cha with the high contrast imager VLT/SPHERE in polarimetric differential imaging mode to resolve the circumbinary disk in near infrared scattered light. These observations were followed-up by VLT/NACO L-band observations and complemented by archival VLT/NACO K-band and HST/WFPC2 I-band data. We resolve the compact circumbinary disk around CS Cha for the first time in scattered light. We find a smooth, low inclination disk with an outer radius of $\sim$55 au (at 165 pc). We do not detect the inner cavity but find an upper limit for the cavity size of $\sim$15 au. Furthermore, we find a faint co-moving companion with a projected separation of 210 au from the central binary outside of the circumbinary disk. The companion is detected in polarized light and shows an extreme degree of polarization (13.7$\pm$0.4 \% in J-band). The companion's J- and H-band magnitudes are compatible with masses of a few M$_\mathrm{Jup}$. However, K-, L- and I-band data draw this conclusion into question. We explore with radiative transfer modeling whether an unresolved circum-companion disk can be responsible for the high polarization and complex photometry. We find that the set of observations is best explained by a heavily extincted low mass ($\sim 20 \mathrm{M}_\mathrm{Jup}$) brown dwarf or high mass planet with an unresolved disk and dust envelope., Comment: 19 pages, 15 figures, accepted for publication in A&A as of 27.04.2018
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- 2018
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- View/download PDF
43. The Single-mode Complex Amplitude Refinement (SCAR) coronagraph: II. Lab verification, and toward the characterization of Proxima b
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Haffert, S. Y., Por, E. H., Keller, C. U., Kenworthy, M. A., Doelman, D. S., Snik, F., and Escuti, M. J.
- Subjects
Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - Earth and Planetary Astrophysics - Abstract
We present the monochromatic lab verification of the newly developed SCAR coronagraph that combines a phase plate (PP) in the pupil with a microlens-fed single-mode fiber array in the focal plane. The two SCAR designs that have been measured, create respectively a 360 degree and 180 degree dark region from 0.8-2.4 \lambda/D around the star. The 360 SCAR has been designed for a clear aperture and the 180 SCAR has been designed for a realistic aperture with central obscuration and spiders. The 360 SCAR creates a measured stellar null of $2-3 \times 10^{-4}$ , and the 180 SCAR reaches a null of $1 \times 10^{-4}$ . Their monochromatic contrast is maintained within a range of $\pm$ 0.16 \lambda/D peak-to-valley tip-tilt, which shows the robustness against tip-tilt errors. The small inner working angle and tip-tilt stability makes the SCAR coronagraph a very promising technique for an upgrade of current high-contrast instruments to characterize and detect exoplanets in the solar neighborhood., Comment: 9 pages, 11 figures. accepted by A&A
- Published
- 2018
44. Neoproterozoic glacial origin of the Great Unconformity
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Keller, C Brenhin, Husson, Jon M, Mitchell, Ross N, Bottke, William F, Gernon, Thomas M, Boehnke, Patrick, Bell, Elizabeth A, Swanson-Hysell, Nicholas L, and Peters, Shanan E
- Subjects
Earth Sciences ,Physical Geography and Environmental Geoscience ,Geology ,Geophysics ,Great Unconformity ,snowball Earth ,glacial erosion ,zircon ,Cambrian explosion - Abstract
The Great Unconformity, a profound gap in Earth's stratigraphic record often evident below the base of the Cambrian system, has remained among the most enigmatic field observations in Earth science for over a century. While long associated directly or indirectly with the occurrence of the earliest complex animal fossils, a conclusive explanation for the formation and global extent of the Great Unconformity has remained elusive. Here we show that the Great Unconformity is associated with a set of large global oxygen and hafnium isotope excursions in magmatic zircon that suggest a late Neoproterozoic crustal erosion and sediment subduction event of unprecedented scale. These excursions, the Great Unconformity, preservational irregularities in the terrestrial bolide impact record, and the first-order pattern of Phanerozoic sedimentation can together be explained by spatially heterogeneous Neoproterozoic glacial erosion totaling a global average of 3-5 vertical kilometers, along with the subsequent thermal and isostatic consequences of this erosion for global continental freeboard.
- Published
- 2019
45. Insights into ENGO activities in the Salish Sea: A call for more coordination, communication, and potential for communities of practice
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Jones, Jacob, Keller, C. Peter, and van der Flier Keller, Eileen
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- 2022
- Full Text
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46. Experimental and numerical investigations of plastic strain mechanisms of AISI 316L alloys with bimodal grain size distribution
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Keller, C., Calvat, M., Flipon, B., and Barbe, F.
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- 2022
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47. Solvent-free dehydration, cyclization, and hydrogenation of linalool with a dual heterogeneous catalyst system to generate a high-performance sustainable aviation fuel
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Keller, C. Luke, Doppalapudi, Karan R., Woodroffe, Josanne-Dee, and Harvey, Benjamin G.
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- 2022
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48. Neue Studie zur spatiotemporalen Verteilung von Remyelinisierungsprozessen bei multipler Sklerose
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Keller, C. W.
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- 2023
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49. Heterogeneous Hadean crust with ambient mantle affinity recorded in detrital zircons of the Green Sandstone Bed, South Africa
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Drabon, Nadja, Byerly, Benjamin L., Byerly, Gary R., Wooden, Joseph L., Keller, C. Brenhin, and Lowe, Donald R.
- Published
- 2021
50. New measurement of the 238U decay constant with inductively coupled plasma mass spectrometry
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Parsons-Davis, Tashi, Wimpenny, Josh, Keller, C Brenhin, Thomas, Keenan, Samperton, Kyle M, Renne, Paul R, Mundil, Roland, Moody, Ken, Knight, Kim, Kristo, Michael J, and Williams, Ross
- Subjects
Uranium ,Thorium ,Half-life ,Decay constant ,Radiochronometry ,Inductively coupled plasma mass spectrometry ,Analytical Chemistry ,Inorganic Chemistry ,Physical Chemistry (incl. Structural) ,Inorganic & Nuclear Chemistry - Abstract
The 238U decay constant (λU-238) is fundamental to radioisotope-based chronometry in the Earth and planetary sciences, yet only a single published λU-238 value (Jaffey et al. in Phys Rev C 4(5):1889–1906, 1971) is widely applied. We have determined λU-238 via the novel approach of measuring of 234Th ingrowth in high-purity 238U solutions, using isotope dilution mass spectrometry (ID-MS). The 234Th decay constant (λTh-234) was measured via decay counting with high-purity Ge (HPGe) γ detectors. Preliminary results for λU-238 agree with the value determined by α-counting [1] within the elevated uncertainty of 0.462% (k = 2). Ongoing efforts to reproduce λU-238 with reduced experimental uncertainties will inform future conclusions.
- Published
- 2018
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