78 results on '"S E Clark"'
Search Results
2. A New Constraint on the Relative Disorder of Magnetic Fields between Neutral Interstellar Medium Phases
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Minjie Lei and S. E. Clark
- Subjects
Interstellar medium ,Cold neutral medium ,Interstellar magnetic fields ,Interstellar dust ,Astrophysics ,QB460-466 - Abstract
Utilizing Planck polarized dust emission maps at 353 GHz and large-area maps of the neutral hydrogen (H i ) cold neutral medium (CNM) fraction ( f _CNM ), we investigate the relationship between dust polarization fraction ( p _353 ) and f _CNM in the diffuse high latitude ( $\left|b\right|\gt 30^\circ $ ) sky. We find that the correlation between p _353 and f _CNM is qualitatively distinct from the p _353 –H i column density ( N _H _i ) relationship. At low column densities ( N _H _i < 4 × 10 ^20 cm ^−2 ) where p _353 and N _H _i are uncorrelated, there is a strong positive p _353 – f _CNM correlation. We fit the p _353 – f _CNM correlation with data-driven models to constrain the degree of magnetic field disorder between phases along the line of sight. We argue that an increased magnetic field disorder in the warm neutral medium (WNM) relative to the CNM best explains the positive p _353 – f _CNM correlation in diffuse regions. Modeling the CNM-associated dust column as being maximally polarized, with a polarization fraction p _CNM ∼ 0.2, we find that the best-fit mean polarization fraction in the WNM-associated dust column is 0.22 p _CNM . The model further suggests that a significant f _CNM -correlated fraction of the non-CNM column (an additional 18.4% of the H i mass on average) is also more magnetically ordered, and we speculate that the additional column is associated with the unstable medium. Our results constitute a new large-area constraint on the average relative disorder of magnetic fields between the neutral phases of the interstellar medium, and are consistent with the physical picture of a more magnetically aligned CNM column forming out of a disordered WNM.
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- 2024
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- View/download PDF
3. Imprints of the Local Bubble and Dust Complexity on Polarized Dust Emission
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George Halal, S. E. Clark, and Mehrnoosh Tahani
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Interstellar dust ,Cosmic microwave background radiation ,Algorithms ,Interstellar magnetic fields ,Interstellar medium ,Galaxy magnetic fields ,Astrophysics ,QB460-466 - Abstract
Using 3D dust maps and Planck polarized dust emission data, we investigate the influence of the 3D geometry of the nearby interstellar medium (ISM) on the statistics of the dust polarization on large ( $80^{\prime} $ ) scales. We test recent models that assume that the magnetic field probed by the polarized dust emission is preferentially tangential to the Local Bubble wall, but we do not find an imprint of the Local Bubble geometry on the dust polarization fraction. We also test the hypothesis that the complexity of the 3D dust distribution drives some of the measured variation of the dust polarization fraction. We compare sight lines with similar total column densities and find that, on average, the dust polarization fraction decreases when the dust column is substantially distributed among multiple components at different distances. Conversely, the dust polarization fraction is higher for sight lines where the dust is more concentrated in 3D space. This finding is statistically significant for the dust within 1.25 kpc, but the effect disappears if we only consider dust within 270 pc. In conclusion, we find that the extended 3D dust distribution, rather than solely the dust associated with the Local Bubble, plays a role in determining the observed dust polarization fraction at 80′. This conclusion is consistent with a simple analytical prediction and remains robust under various modifications to the analysis. These results illuminate the relationship between the 3D geometry of the ISM and tracers of the interstellar magnetic field. We discuss implications for our understanding of the polarized dust foreground to the cosmic microwave background.
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- 2024
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4. Tensor-to-scalar ratio forecasts for extended LiteBIRD frequency configurations
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U. Fuskeland, J. Aumont, R. Aurlien, C. Baccigalupi, A. J. Banday, H. K. Eriksen, J. Errard, R. T. Génova-Santos, T. Hasebe, J. Hubmayr, H. Imada, N. Krachmalnicof, L. Lamagna, G. Pisano, D. Poletti, M. Remazeilles, K. L. Thompson, L. Vache, I. K. Wehus, S. Azzoni, M. Ballardini, R. B. Barreiro, N. Bartolo, A. Basyrov, D. Beck, M. Bersanelli, M. Bortolami, M. Brilenkov, E. Calabrese, A. Carones, F. J. Casas, K. Cheung, J. Chluba, S. E. Clark, L. Clermont, and E.J. Wollack
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Space Sciences (General) - Abstract
LiteBIRD is a planned JAXA-led cosmic microwave background (CMB) B-mode satellite experiment aiming for launch in the late 2020s, with a primary goal of detecting the imprint of primordial inflationary gravitational waves. Its current baseline focal-plane configuration includes 15 frequency bands between 40 and 402 GHz, fulfilling the mission requirements to detect the amplitude of gravitational waves with the total uncertainty on the tensor-to-scalar ratio, δr, down to δr < 0.001. A key aspect of this performance is accurate astrophysical component separation, and the ability to remove polarized thermal dust emission is particularly important. In this paper we note that the CMB frequency spectrum falls off nearly exponentially above 300 GHz relative to the thermal dust spectral energy distribution, and a relatively minor high frequency extension can therefore result in even lower uncertainties and better model reconstructions. Specifically, we compared the baseline design with five extended configurations, while varying the underlying dust modeling, in each of which the High-Frequency Telescope (HFT) frequency range was shifted logarithmically toward higher frequencies, with an upper cutoff ranging between 400 and 600 GHz. In each case, we measured the tensor-to-scalar ratio r uncertainty and bias using both parametric and minimum-variance component-separation algorithms. When the thermal dust sky model includes a spatially varying spectral index and temperature, we find that the statistical uncertainty on r after foreground cleaning may be reduced by as much as 30–50% by extending the upper limit of the frequency range from 400 to 600 GHz, with most of the improvement already gained at 500 GHz. We also note that a broader frequency range leads to higher residuals when fitting an incorrect dust model, but also it is easier to discriminate between models through higher χ2 sensitivity. Even in the case in which the fitting procedure does not correspond to the underlying dust model in the sky, and when the highest frequency data cannot be modeled with sufficient fidelity and must be excluded from the analysis, the uncertainty on r increases by only about 5% for a 500 GHz configuration compared to the baseline.
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- 2023
- Full Text
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5. BICEP/Keck. XVI. Characterizing Dust Polarization through Correlations with Neutral Hydrogen
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P. A. R. Ade, Z. Ahmed, M. Amiri, D. Barkats, R. Basu Thakur, C. A. Bischoff, D. Beck, J. J. Bock, H. Boenish, E. Bullock, V. Buza, J. R. Cheshire IV, S. E. Clark, J. Connors, J. Cornelison, M. Crumrine, A. Cukierman, E. V. Denison, M. Dierickx, L. Duband, M. Eiben, S. Fatigoni, J. P. Filippini, S. Fliescher, C. Giannakopoulos, N. Goeckner-Wald, D. C. Goldfinger, J. Grayson, P. Grimes, G. Hall, G. Halal, M. Halpern, E. Hand, S. Harrison, S. Henderson, S. R. Hildebrandt, J. Hubmayr, H. Hui, K. D. Irwin, J. Kang, K. S. Karkare, E. Karpel, S. Kefeli, S. A. Kernasovskiy, J. M. Kovac, C. L. Kuo, K. Lau, E. M. Leitch, A. Lennox, K. G. Megerian, L. Minutolo, L. Moncelsi, Y. Nakato, T. Namikawa, H. T. Nguyen, R. O’Brient, R. W. Ogburn IV, S. Palladino, M. A. Petroff, T. Prouve, C. Pryke, B. Racine, C. D. Reintsema, S. Richter, A. Schillaci, R. Schwarz, B. L. Schmitt, C. D. Sheehy, B. Singari, A. Soliman, T. St. Germaine, B. Steinbach, R. V. Sudiwala, G. P. Teply, K. L. Thompson, J. E. Tolan, C. Tucker, A. D. Turner, C. Umiltà, C. Vergès, A. G. Vieregg, A. Wandui, A. C. Weber, D. V. Wiebe, J. Willmert, C. L. Wong, W. L. K. Wu, H. Yang, K. W. Yoon, E. Young, C. Yu, L. Zeng, C. Zhang, S. Zhang, and BICEP/Keck Collaboration
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Interstellar dust ,Interstellar filaments ,Neutral hydrogen clouds ,Cosmic microwave background radiation ,Interstellar magnetic fields ,Interstellar medium ,Astrophysics ,QB460-466 - Abstract
We characterize Galactic dust filaments by correlating BICEP/Keck and Planck data with polarization templates based on neutral hydrogen (H i ) observations. Dust polarization is important for both our understanding of astrophysical processes in the interstellar medium (ISM) and the search for primordial gravitational waves in the cosmic microwave background (CMB). In the diffuse ISM, H i is strongly correlated with the dust and partly organized into filaments that are aligned with the local magnetic field. We analyze the deep BICEP/Keck data at 95, 150, and 220 GHz, over the low-column-density region of sky where BICEP/Keck has set the best limits on primordial gravitational waves. We separate the H i emission into distinct velocity components and detect dust polarization correlated with the local Galactic H i but not with the H i associated with Magellanic Stream i . We present a robust, multifrequency detection of polarized dust emission correlated with the filamentary H i morphology template down to 95 GHz. For assessing its utility for foreground cleaning, we report that the H i morphology template correlates in B modes at a ∼10%–65% level over the multipole range 20 < ℓ < 200 with the BICEP/Keck maps, which contain contributions from dust, CMB, and noise components. We measure the spectral index of the filamentary dust component spectral energy distribution to be β = 1.54 ± 0.13. We find no evidence for decorrelation in this region between the filaments and the rest of the dust field or from the inclusion of dust associated with the intermediate velocity H i . Finally, we explore the morphological parameter space in the H i -based filamentary model.
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- 2023
- Full Text
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6. Probing the Cold Neutral Medium through H I Emission Morphology with the Scattering Transform
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Minjie Lei and S. E. Clark
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Interstellar medium ,Cold neutral medium ,H I line emission ,Astrostatistics ,Wavelet analysis ,Astrophysics ,QB460-466 - Abstract
Neutral hydrogen (H I ) emission exhibits complex morphology that encodes rich information about the physics of the interstellar medium. We apply the scattering transform (ST) to characterize the H I emission structure via a set of compact and interpretable coefficients, and find a connection between the H I emission morphology and H I cold neutral medium (CNM) phase content. Where H I absorption measurements are unavailable, the H I phase structure is typically estimated from the emission via spectral line decomposition. Here, we present a new probe of the CNM content using measures that are solely derived from H I emission spatial information. We apply the ST to GALFA-H I data at high Galactic latitudes ( $\left|b\right|\gt 30^\circ $ ), and compare the resulting coefficients to CNM fraction measurements derived from archival H I emission and absorption spectra. We quantify the correlation between the ST coefficients and the measured CNM fraction ( f _CNM ), finding that the H I emission morphology encodes substantial f _CNM -correlating information and that ST-based metrics for small-scale linearity are particularly predictive of f _CNM . This is further corroborated by the enhancement of the I _857 / N _HI ratio with larger ST measures of small-scale linearity. These results are consistent with the picture of regions with higher CNM content being more populated by small-scale filamentary H I structures. Our work illustrates a physical connection between the H I morphology and phase content, and suggests that future phase decomposition methods can be improved by making use of both H I spectral and spatial information.
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- 2023
- Full Text
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7. Magnetic Misalignment of Interstellar Dust Filaments
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Ari J. Cukierman, S. E. Clark, and George Halal
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Interstellar medium ,Interstellar filaments ,Interstellar magnetic fields ,Interstellar atomic gas ,Neutral hydrogen clouds ,Magnetic fields ,Astrophysics ,QB460-466 - Abstract
We present evidence for scale-independent misalignment of interstellar dust filaments and magnetic fields. We estimate the misalignment by comparing millimeter-wave dust-polarization measurements from Planck with filamentary structures identified in neutral-hydrogen (H i ) measurements from H i 4PI. We find that the misalignment angle displays a scale independence (harmonic coherence) for features larger than the H i 4PI beamwidth (16.′2). We additionally find a spatial coherence on angular scales of ${ \mathcal O }(1^\circ )$ . We present several misalignment estimators formed from the auto- and cross-spectra of dust-polarization and H i -based maps, and we also introduce a map-space estimator. Applied to large regions of the high-Galactic-latitude sky, we find a global misalignment angle of ∼2°, which is robust to a variety of masking choices. By dividing the sky into small regions, we show that the misalignment angle correlates with the parity-violating TB cross-spectrum measured in the Planck dust maps. The misalignment paradigm also predicts a dust EB signal, which is of relevance in the search for cosmic birefringence but as yet undetected; the measurements of EB are noisier than those of TB , and our correlations of EB with misalignment angle are found to be weaker and less robust to masking choices. We also introduce an H i -based dust-polarization template constructed from the Hessian matrix of the H i intensity, which is found to correlate more strongly than previous templates with Planck dust B modes.
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- 2023
- Full Text
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8. H<scp> i</scp>filaments as potential compass needles? Comparing the magnetic field structure of the Small Magellanic Cloud to the orientation of GASKAP-H <scp>i</scp>filaments
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Y K Ma, N M McClure-Griffiths, S E Clark, S J Gibson, J Th van Loon, J D Soler, M E Putman, J M Dickey, M -Y Lee, K E Jameson, L Uscanga, J Dempsey, H Dénes, C Lynn, and N M Pingel
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Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics - Astrophysics of Galaxies - Abstract
High-spatial-resolution HI observations have led to the realisation that the nearby (within few hundreds of parsecs) Galactic atomic filamentary structures are aligned with the ambient magnetic field. Enabled by the high quality data from the Australian Square Kilometre Array Pathfinder (ASKAP) radio telescope for the Galactic ASKAP HI (GASKAP-HI) survey, we investigate the potential magnetic alignment of the $\gtrsim 10\,{\rm pc}$-scale HI filaments in the Small Magellanic Cloud (SMC). Using the Rolling Hough Transform (RHT) technique that automatically identifies filamentary structures, combined with our newly devised ray-tracing algorithm that compares the HI and starlight polarisation data, we find that the HI filaments in the northeastern end of the SMC main body ("Bar" region) and the transition area between the main body and the tidal feature ("Wing" region) appear preferentially aligned with the magnetic field traced by starlight polarisation. Meanwhile, the remaining SMC volume lacks starlight polarisation data of sufficient quality to draw any conclusions. This suggests for the first time that filamentary HI structures can be magnetically aligned across a large spatial volume ($\gtrsim\,{\rm kpc}$) outside of the Milky Way. In addition, we generate maps of the preferred orientation of HI filaments throughout the entire SMC, revealing the highly complex gaseous structures of the galaxy likely shaped by a combination of the intrinsic internal gas dynamics, tidal interactions, and star formation feedback processes. These maps can further be compared with future measurements of the magnetic structures in other regions of the SMC., Comment: 24 pages, MNRAS accepted
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- 2023
- Full Text
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9. Probing Cosmic Inflation with the LiteBIRD Cosmic Microwave Background Polarization Survey
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Allys, E, Arnold, K, Aumont, J, Aurlien, R, Azzoni, S, Baccigalupi, C, J Banday, A, Banerji, R, B Barreiro, R, Bartolo, N, Bautista, L, Beck, D, Beckman, S, Bersanelli, M, Boulanger, F, Brilenkov, M, Bucher, M, Calabrese, E, Campeti, P, Carones, A, J Casas, F, Catalano, A, Chan, V, Cheung, K, Chinone, Y, E Clark, S, Columbro, F, D???alessandro, G, de??? Bernardis, P, de??? Haan, T, de??? la??? Hoz, E, De??? Petris, M, Della??? Torre, S, Diego-Palazuelos, P, Dobbs, M, Dotani, T, M Duval, J, Elleflot, T, K Eriksen, H, Errard, J, Essinger-Hileman, T, Finelli, F, Flauger, R, Franceschet, C, Fuskeland, U, Galloway, M, Ganga, K, Gerbino, M, Gervasi, M, T G??nova-Santos, R, Ghigna, T, Giardiello, S, Gjerl??w, E, Grain, J, Grupp, F, Gruppuso, A, E Gudmundsson, J, W Halverson, N, Hargrave, P, Hasebe, T, Hasegawa, M, Hazumi, M, Henrot-Versill??, S, Hensley, B, T Hergt, L, Herman, D, Hivon, E, A Hlozek, R, L Hornsby, A, Hoshino, Y, Hubmayr, J, Ichiki, K, Iida, T, Imada, H, Ishino, H, Jaehnig, G, Katayama, N, Kato, A, Keskitalo, R, Kisner, T, Kobayashi, Y, Kogut, A, Kohri, K, Komatsu, E, Komatsu, K, Konishi, K, Krachmalnicoff, N, L Kuo, C, Lamagna, L, Lattanzi, M, T Lee, A, Leloup, C, Levrier, F, Linder, E, Luzzi, G, Macias-Perez, J, Maciaszek, T, Maffei, B, Maino, D, Mandelli, S, Mart??nez-Gonz??lez, E, Masi, S, Massa, M, Matarrese, S, T Matsuda, F, Matsumura, T, Mele, L, Migliaccio, M, Minami, Y, Moggi, A, Montgomery, J, Montier, L, Morgante, G, Mot, B, Nagano, Y, Nagasaki, T, Nagata, R, Nakano, R, Namikawa, T, Nati, F, Natoli, P, Nerval, S, Noviello, F, Odagiri, K, Oguri, S, Ohsaki, H, Pagano, L, Paiella, A, Paoletti, D, Passerini, A, Patanchon, G, Piacentini, F, Piat, M, Polenta, G, Poletti, D, Prouv??, T, Puglisi, G, Rambaud, D, Raum, C, Realini, S, Reinecke, M, Remazeilles, M, Ritacco, A, Roudil, G, A Rubino-Martin, J, Russell, M, Sakurai, H, Sakurai, Y, Sasaki, M, Scott, D, Sekimoto, Y, Shinozaki, K, Shiraishi, M, Shirron, P, Signorelli, G, Spinella, F, Stever, S, Stompor, R, Sugiyama, S, M Sullivan, R, Suzuki, A, L Svalheim, T, Switzer, E, Takaku, R, Takakura, H, Takase, Y, Tartari, A, Terao, Y, Thermeau, J, Thommesen, H, L Thompson, K, Tomasi, M, Tominaga, M, Tristram, M, Tsuji, M, Tsujimoto, M, Vacher, L, Vielva, P, Vittorio, N, Wang, W, Watanuki, K, K Wehus, I, Weller, J, Westbrook, B, Wilms, J, J Wollack, E, Yumoto, J, Zannoni, M, E Allys, K Arnold, J Aumont, R Aurlien, S Azzoni, C Baccigalupi, A J Banday, R Banerji, R B Barreiro, N Bartolo, L Bautista, D Beck, S Beckman, M Bersanelli, F Boulanger, M Brilenkov, M Bucher, E Calabrese, P Campeti, A Carones, F J Casas, A Catalano, V Chan, K Cheung, Y Chinone, S E Clark, F Columbro, G D???Alessandro, P de??? Bernardis, T de??? Haan, E de??? la??? Hoz, M De??? Petris, S Della??? Torre, P Diego-Palazuelos, M Dobbs, T Dotani, J M Duval, T Elleflot, H K Eriksen, J Errard, T Essinger-Hileman, F Finelli, R Flauger, C Franceschet, U Fuskeland, M Galloway, K Ganga, M Gerbino, M Gervasi, R T G??nova-Santos, T Ghigna, S Giardiello, E Gjerl??w, J Grain, F Grupp, A Gruppuso, J E Gudmundsson, N W Halverson, P Hargrave, T Hasebe, M Hasegawa, M Hazumi, S Henrot-Versill??, B Hensley, L T Hergt, D Herman, E Hivon, R A Hlozek, A L Hornsby, Y Hoshino, J Hubmayr, K Ichiki, T Iida, H Imada, H Ishino, G Jaehnig, N Katayama, A Kato, R Keskitalo, T Kisner, Y Kobayashi, A Kogut, K Kohri, E Komatsu, K Komatsu, K Konishi, N Krachmalnicoff, C L Kuo, L Lamagna, M Lattanzi, A T Lee, C Leloup, F Levrier, E Linder, G Luzzi, J Macias-Perez, T Maciaszek, B Maffei, D Maino, S Mandelli, E Mart??nez-Gonz??lez, S Masi, M Massa, S Matarrese, F T Matsuda, T Matsumura, L Mele, M Migliaccio, Y Minami, A Moggi, J Montgomery, L Montier, G Morgante, B Mot, Y Nagano, T Nagasaki, R Nagata, R Nakano, T Namikawa, F Nati, P Natoli, S Nerval, F Noviello, K Odagiri, S Oguri, H Ohsaki, L Pagano, A Paiella, D Paoletti, A Passerini, G Patanchon, F Piacentini, M Piat, G Polenta, D Poletti, T Prouv??, G Puglisi, D Rambaud, C Raum, S Realini, M Reinecke, M Remazeilles, A Ritacco, G Roudil, J A Rubino-Martin, M Russell, H Sakurai, Y Sakurai, M Sasaki, D Scott, Y Sekimoto, K Shinozaki, M Shiraishi, P Shirron, G Signorelli, F Spinella, S Stever, R Stompor, S Sugiyama, R M Sullivan, A Suzuki, T L Svalheim, E Switzer, R Takaku, H Takakura, Y Takase, A Tartari, Y Terao, J Thermeau, H Thommesen, K L Thompson, M Tomasi, M Tominaga, M Tristram, M Tsuji, M Tsujimoto, L Vacher, P Vielva, N Vittorio, W Wang, K Watanuki, I K Wehus, J Weller, B Westbrook, J Wilms, E J Wollack, J Yumoto, M Zannoni, Allys, E, Arnold, K, Aumont, J, Aurlien, R, Azzoni, S, Baccigalupi, C, J Banday, A, Banerji, R, B Barreiro, R, Bartolo, N, Bautista, L, Beck, D, Beckman, S, Bersanelli, M, Boulanger, F, Brilenkov, M, Bucher, M, Calabrese, E, Campeti, P, Carones, A, J Casas, F, Catalano, A, Chan, V, Cheung, K, Chinone, Y, E Clark, S, Columbro, F, D???alessandro, G, de??? Bernardis, P, de??? Haan, T, de??? la??? Hoz, E, De??? Petris, M, Della??? Torre, S, Diego-Palazuelos, P, Dobbs, M, Dotani, T, M Duval, J, Elleflot, T, K Eriksen, H, Errard, J, Essinger-Hileman, T, Finelli, F, Flauger, R, Franceschet, C, Fuskeland, U, Galloway, M, Ganga, K, Gerbino, M, Gervasi, M, T G??nova-Santos, R, Ghigna, T, Giardiello, S, Gjerl??w, E, Grain, J, Grupp, F, Gruppuso, A, E Gudmundsson, J, W Halverson, N, Hargrave, P, Hasebe, T, Hasegawa, M, Hazumi, M, Henrot-Versill??, S, Hensley, B, T Hergt, L, Herman, D, Hivon, E, A Hlozek, R, L Hornsby, A, Hoshino, Y, Hubmayr, J, Ichiki, K, Iida, T, Imada, H, Ishino, H, Jaehnig, G, Katayama, N, Kato, A, Keskitalo, R, Kisner, T, Kobayashi, Y, Kogut, A, Kohri, K, Komatsu, E, Komatsu, K, Konishi, K, Krachmalnicoff, N, L Kuo, C, Lamagna, L, Lattanzi, M, T Lee, A, Leloup, C, Levrier, F, Linder, E, Luzzi, G, Macias-Perez, J, Maciaszek, T, Maffei, B, Maino, D, Mandelli, S, Mart??nez-Gonz??lez, E, Masi, S, Massa, M, Matarrese, S, T Matsuda, F, Matsumura, T, Mele, L, Migliaccio, M, Minami, Y, Moggi, A, Montgomery, J, Montier, L, Morgante, G, Mot, B, Nagano, Y, Nagasaki, T, Nagata, R, Nakano, R, Namikawa, T, Nati, F, Natoli, P, Nerval, S, Noviello, F, Odagiri, K, Oguri, S, Ohsaki, H, Pagano, L, Paiella, A, Paoletti, D, Passerini, A, Patanchon, G, Piacentini, F, Piat, M, Polenta, G, Poletti, D, Prouv??, T, Puglisi, G, Rambaud, D, Raum, C, Realini, S, Reinecke, M, Remazeilles, M, Ritacco, A, Roudil, G, A Rubino-Martin, J, Russell, M, Sakurai, H, Sakurai, Y, Sasaki, M, Scott, D, Sekimoto, Y, Shinozaki, K, Shiraishi, M, Shirron, P, Signorelli, G, Spinella, F, Stever, S, Stompor, R, Sugiyama, S, M Sullivan, R, Suzuki, A, L Svalheim, T, Switzer, E, Takaku, R, Takakura, H, Takase, Y, Tartari, A, Terao, Y, Thermeau, J, Thommesen, H, L Thompson, K, Tomasi, M, Tominaga, M, Tristram, M, Tsuji, M, Tsujimoto, M, Vacher, L, Vielva, P, Vittorio, N, Wang, W, Watanuki, K, K Wehus, I, Weller, J, Westbrook, B, Wilms, J, J Wollack, E, Yumoto, J, Zannoni, M, E Allys, K Arnold, J Aumont, R Aurlien, S Azzoni, C Baccigalupi, A J Banday, R Banerji, R B Barreiro, N Bartolo, L Bautista, D Beck, S Beckman, M Bersanelli, F Boulanger, M Brilenkov, M Bucher, E Calabrese, P Campeti, A Carones, F J Casas, A Catalano, V Chan, K Cheung, Y Chinone, S E Clark, F Columbro, G D???Alessandro, P de??? Bernardis, T de??? Haan, E de??? la??? Hoz, M De??? Petris, S Della??? Torre, P Diego-Palazuelos, M Dobbs, T Dotani, J M Duval, T Elleflot, H K Eriksen, J Errard, T Essinger-Hileman, F Finelli, R Flauger, C Franceschet, U Fuskeland, M Galloway, K Ganga, M Gerbino, M Gervasi, R T G??nova-Santos, T Ghigna, S Giardiello, E Gjerl??w, J Grain, F Grupp, A Gruppuso, J E Gudmundsson, N W Halverson, P Hargrave, T Hasebe, M Hasegawa, M Hazumi, S Henrot-Versill??, B Hensley, L T Hergt, D Herman, E Hivon, R A Hlozek, A L Hornsby, Y Hoshino, J Hubmayr, K Ichiki, T Iida, H Imada, H Ishino, G Jaehnig, N Katayama, A Kato, R Keskitalo, T Kisner, Y Kobayashi, A Kogut, K Kohri, E Komatsu, K Komatsu, K Konishi, N Krachmalnicoff, C L Kuo, L Lamagna, M Lattanzi, A T Lee, C Leloup, F Levrier, E Linder, G Luzzi, J Macias-Perez, T Maciaszek, B Maffei, D Maino, S Mandelli, E Mart??nez-Gonz??lez, S Masi, M Massa, S Matarrese, F T Matsuda, T Matsumura, L Mele, M Migliaccio, Y Minami, A Moggi, J Montgomery, L Montier, G Morgante, B Mot, Y Nagano, T Nagasaki, R Nagata, R Nakano, T Namikawa, F Nati, P Natoli, S Nerval, F Noviello, K Odagiri, S Oguri, H Ohsaki, L Pagano, A Paiella, D Paoletti, A Passerini, G Patanchon, F Piacentini, M Piat, G Polenta, D Poletti, T Prouv??, G Puglisi, D Rambaud, C Raum, S Realini, M Reinecke, M Remazeilles, A Ritacco, G Roudil, J A Rubino-Martin, M Russell, H Sakurai, Y Sakurai, M Sasaki, D Scott, Y Sekimoto, K Shinozaki, M Shiraishi, P Shirron, G Signorelli, F Spinella, S Stever, R Stompor, S Sugiyama, R M Sullivan, A Suzuki, T L Svalheim, E Switzer, R Takaku, H Takakura, Y Takase, A Tartari, Y Terao, J Thermeau, H Thommesen, K L Thompson, M Tomasi, M Tominaga, M Tristram, M Tsuji, M Tsujimoto, L Vacher, P Vielva, N Vittorio, W Wang, K Watanuki, I K Wehus, J Weller, B Westbrook, J Wilms, E J Wollack, J Yumoto, and M Zannoni
- Published
- 2023
10. The Origin of Parity Violation in Polarized Dust Emission and Implications for Cosmic Birefringence
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S. E. Clark, Chang-Goo Kim, J. Colin Hill, and Brandon S. Hensley
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- 2021
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11. GASKAP Pilot Survey Science. II. ASKAP Zoom Observations of Galactic 21 cm Absorption
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John M. Dickey, J. M. Dempsey, N. M. Pingel, N. M. McClure-Griffiths, K. Jameson, J. R. Dawson, H. Dénes, S. E. Clark, G. Joncas, D. Leahy, Min-Young Lee, M.-A. Miville-Deschênes, S. Stanimirović, C. D. Tremblay, J. Th. van Loon, Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité)
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[SDU.ASTR]Sciences of the Universe [physics]/Astrophysics [astro-ph] ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Q1 ,Astrophysics - Astrophysics of Galaxies ,[SDU]Sciences of the Universe [physics] ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,QB460 ,Astrophysics::Earth and Planetary Astrophysics ,Astrophysics::Galaxy Astrophysics ,QB600 ,QB - Abstract
Using the Australian Square Kilometre Array Pathfinder to measure 21-cm absorption spectra toward continuum background sources, we study the cool phase of the neutral atomic gas in the far outer disk, and in the inner Galaxy near the end of the Galactic bar at longitude 340 degrees. In the inner Galaxy the cool atomic gas has a smaller scale height than in the solar neighborhood, similar to the molecular gas and the superthin stellar population in the bar. In the outer Galaxy the cool atomic gas is mixed with the warm, neutral medium, with the cool fraction staying roughly constant with Galactic radius. The mean spin temperature, i.e. the ratio of the emission brightness temperature to the absorption, is roughly constant for velocities corresponding to Galactic radius greater than about twice the solar circle radius. The ratio has a value of about 300 K, but this does not correspond to a physical temperature in the gas. If the gas causing the absorption has kinetic temperature of about 100 K, as in the solar neighborhood, then the value 300 K indicates that the fraction of the gas mass in this phase is one-third of the total HI mass., Comment: 29 pages, 12 figures, submitted to Astrophysical Journal
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- 2022
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12. Optical Characterization of OMT-Coupled TES Bolometers for LiteBIRD
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J. Hubmayr, P. A. R. Ade, A. Adler, E. Allys, D. Alonso, K. Arnold, D. Auguste, J. Aumont, R. Aurlien, J. E. Austermann, S. Azzoni, C. Baccigalupi, A. J. Banday, R. Banerji, R. B. Barreiro, N. Bartolo, S. Basak, E. Battistelli, L. Bautista, J. A. Beall, D. Beck, S. Beckman, K. Benabed, J. Bermejo-Ballesteros, M. Bersanelli, J. Bonis, J. Borrill, F. Bouchet, F. Boulanger, S. Bounissou, M. Brilenkov, M. L. Brown, M. Bucher, E. Calabrese, M. Calvo, P. Campeti, A. Carones, F. J. Casas, A. Catalano, A. Challinor, V. Chan, K. Cheung, Y. Chinone, C. Chiocchetta, S. E. Clark, L. Clermont, S. Clesse, J. Cliche, F. Columbro, J. A. Connors, A. Coppolecchia, W. Coulton, J. Cubas, A. Cukierman, D. Curtis, F. Cuttaia, G. D’Alessandro, K. Dachlythra, P. de Bernardis, T. de Haan, E. de la Hoz, M. De Petris, S. Della Torre, J. J. Daz Garca, C. Dickinson, P. Diego-Palazuelos, M. Dobbs, T. Dotani, D. Douillet, E. Doumayrou, L. Duband, A. Ducout, S. M. Duff, J. M. Duval, K. Ebisawa, T. Elleflot, H. K. Eriksen, J. Errard, T. Essinger-Hileman, S. Farrens, F. Finelli, R. Flauger, K. Fleury-Frenette, C. Franceschet, U. Fuskeland, L. Galli, S. Galli, M. Galloway, K. Ganga, J. R. Gao, R. T. Genova-Santos, M. Georges, M. Gerbino, M. Gervasi, T. Ghigna, S. Giardiello, E. Gjerlw, R. Gonzlez Gonzles, M. L. Gradziel, J. Grain, L. Grandsire, F. Grupp, A. Gruppuso, J. E. Gudmundsson, N. W. Halverson, J. Hamilton, P. Hargrave, T. Hasebe, M. Hasegawa, M. Hattori, M. Hazumi, S. Henrot-Versill, B. Hensley, D. Herman, D. Herranz, G. C. Hilton, E. Hivon, R. A. Hlozek, D. Hoang, A. L. Hornsby, Y. Hoshino, K. Ichiki, T. Iida, T. Ikemoto, H. Imada, K. Ishimura, H. Ishino, G. Jaehnig, M. Jones, T. Kaga, S. Kashima, N. Katayama, A. Kato, T. Kawasaki, R. Keskitalo, C. Kintziger, T. Kisner, Y. Kobayashi, N. Kogiso, A. Kogut, K. Kohri, E. Komatsu, K. Komatsu, K. Konishi, N. Krachmalnicoff, I. Kreykenbohm, C. L. Kuo, A. Kushino, L. Lamagna, J. V. Lanen, G. Laquaniello, M. Lattanzi, A. T. Lee, C. Leloup, F. Levrier, E. Linder, M. J. Link, A. I. Lonappan, T. Louis, G. Luzzi, J. Macias-Perez, T. Maciaszek, B. Maffei, D. Maino, M. Maki, S. Mandelli, M. Maris, B. Marquet, E. Martnez-Gonzlez, F. A. Martire, S. Masi, M. Massa, M. Masuzawa, S. Matarrese, F. T. Matsuda, T. Matsumura, L. Mele, A. Mennella, M. Migliaccio, Y. Minami, K. Mitsuda, A. Moggi, M. Monelli, A. Monfardini, J. Montgomery, L. Montier, G. Morgante, B. Mot, Y. Murata, J. A. Murphy, M. Nagai, Y. Nagano, T. Nagasaki, R. Nagata, S. Nakamura, R. Nakano, T. Namikawa, F. Nati, P. Natoli, S. Nerval, N. Neto Godry Farias, T. Nishibori, H. Nishino, F. Noviello, G. C. O’Neil, C. O’Sullivan, K. Odagiri, H. Ochi, H. Ogawa, S. Oguri, H. Ohsaki, I. S. Ohta, N. Okada, L. Pagano, A. Paiella, D. Paoletti, G. Pascual Cisneros, A. Passerini, G. Patanchon, V. Pelgrim, J. Peloton, V. Pettorino, F. Piacentini, M. Piat, G. Piccirilli, F. Pinsard, G. Pisano, J. Plesseria, G. Polenta, D. Poletti, T. Prouv, G. Puglisi, D. Rambaud, C. Raum, S. Realini, M. Reinecke, C. D. Reintsema, M. Remazeilles, A. Ritacco, P. Rosier, G. Roudil, J. Rubino-Martin, M. Russell, H. Sakurai, Y. Sakurai, M. Sandri, M. Sasaki, G. Savini, D. Scott, J. Seibert, Y. Sekimoto, B. Sherwin, K. Shinozaki, M. Shiraishi, P. Shirron, A. Shitvov, G. Signorelli, G. Smecher, F. Spinella, J. Starck, S. Stever, R. Stompor, R. Sudiwala, S. Sugiyama, R. Sullivan, A. Suzuki, J. Suzuki, T. Suzuki, T. L. Svalheim, E. Switzer, R. Takaku, H. Takakura, S. Takakura, Y. Takase, Y. Takeda, A. Tartari, D. Tavagnacco, A. Taylor, E. Taylor, Y. Terao, L. Terenzi, J. Thermeau, H. Thommesen, K. L. Thompson, B. Thorne, T. Toda, M. Tomasi, M. Tominaga, N. Trappe, M. Tristram, M. Tsuji, M. Tsujimoto, C. Tucker, R. Ueki, J. N. Ullom, K. Umemori, L. Vacher, J. Van Lanen, G. Vermeulen, P. Vielva, F. Villa, M. R. Vissers, N. Vittorio, B. Wandelt, W. Wang, I. K. Wehus, J. Weller, B. Westbrook, G. Weymann-Despres, J. Wilms, B. Winter, E. J. Wollack, N. Y. Yamasaki, T. Yoshida, J. Yumoto, K. Watanuki, A. Zacchei, M. Zannoni, A. Zonca, Hubmayr, J, Ade, P, Adler, A, Allys, E, Alonso, D, Arnold, K, Auguste, D, Aumont, J, Aurlien, R, Austermann, J, Azzoni, S, Baccigalupi, C, Banday, A, Banerji, R, Barreiro, R, Bartolo, N, Basak, S, Battistelli, E, Bautista, L, Beall, J, Beck, D, Beckman, S, Benabed, K, Bermejo-Ballesteros, J, Bersanelli, M, Bonis, J, Borrill, J, Bouchet, F, Boulanger, F, Bounissou, S, Brilenkov, M, Brown, M, Bucher, M, Calabrese, E, Calvo, M, Campeti, P, Carones, A, Casas, F, Catalano, A, Challinor, A, Chan, V, Cheung, K, Chinone, Y, Chiocchetta, C, Clark, S, Clermont, L, Clesse, S, Cliche, J, Columbro, F, Connors, J, Coppolecchia, A, Coulton, W, Cubas, J, Cukierman, A, Curtis, D, Cuttaia, F, D’Alessandro, G, Dachlythra, K, de Bernardis, P, de Haan, T, de la Hoz, E, De Petris, M, Della Torre, S, Daz Garca, J, Dickinson, C, Diego-Palazuelos, P, Dobbs, M, Dotani, T, Douillet, D, Doumayrou, E, Duband, L, Ducout, A, Duff, S, Duval, J, Ebisawa, K, Elleflot, T, Eriksen, H, Errard, J, Essinger-Hileman, T, Farrens, S, Finelli, F, Flauger, R, Fleury-Frenette, K, Franceschet, C, Fuskeland, U, Galli, L, Galli, S, Galloway, M, Ganga, K, Gao, J, Genova-Santos, R, Georges, M, Gerbino, M, Gervasi, M, Ghigna, T, Giardiello, S, Gjerlw, E, Gonzles, R, Gradziel, M, Grain, J, Grandsire, L, Grupp, F, Gruppuso, A, Gudmundsson, J, Halverson, N, Hamilton, J, Hargrave, P, Hasebe, T, Hasegawa, M, Hattori, M, Hazumi, M, Henrot-Versill, S, Hensley, B, Herman, D, Herranz, D, Hilton, G, Hivon, E, Hlozek, R, Hoang, D, Hornsby, A, Hoshino, Y, Ichiki, K, Iida, T, Ikemoto, T, Imada, H, Ishimura, K, Ishino, H, Jaehnig, G, Jones, M, Kaga, T, Kashima, S, Katayama, N, Kato, A, Kawasaki, T, Keskitalo, R, Kintziger, C, Kisner, T, Kobayashi, Y, Kogiso, N, Kogut, A, Kohri, K, Komatsu, E, Komatsu, K, Konishi, K, Krachmalnicoff, N, Kreykenbohm, I, Kuo, C, Kushino, A, Lamagna, L, Lanen, J, Laquaniello, G, Lattanzi, M, Lee, A, Leloup, C, Levrier, F, Linder, E, Link, M, Lonappan, A, Louis, T, Luzzi, G, Macias-Perez, J, Maciaszek, T, Maffei, B, Maino, D, Maki, M, Mandelli, S, Maris, M, Marquet, B, Martnez-Gonzlez, E, Martire, F, Masi, S, Massa, M, Masuzawa, M, Matarrese, S, Matsuda, F, Matsumura, T, Mele, L, Mennella, A, Migliaccio, M, Minami, Y, Mitsuda, K, Moggi, A, Monelli, M, Monfardini, A, Montgomery, J, Montier, L, Morgante, G, Mot, B, Murata, Y, Murphy, J, Nagai, M, Nagano, Y, Nagasaki, T, Nagata, R, Nakamura, S, Nakano, R, Namikawa, T, Nati, F, Natoli, P, Nerval, S, Neto Godry Farias, N, Nishibori, T, Nishino, H, Noviello, F, O’Neil, G, O’Sullivan, C, Odagiri, K, Ochi, H, Ogawa, H, Oguri, S, Ohsaki, H, Ohta, I, Okada, N, Pagano, L, Paiella, A, Paoletti, D, Pascual Cisneros, G, Passerini, A, Patanchon, G, Pelgrim, V, Peloton, J, Pettorino, V, Piacentini, F, Piat, M, Piccirilli, G, Pinsard, F, Pisano, G, Plesseria, J, Polenta, G, Poletti, D, Prouv, T, Puglisi, G, Rambaud, D, Raum, C, Realini, S, Reinecke, M, Reintsema, C, Remazeilles, M, Ritacco, A, Rosier, P, Roudil, G, Rubino-Martin, J, Russell, M, Sakurai, H, Sakurai, Y, Sandri, M, Sasaki, M, Savini, G, Scott, D, Seibert, J, Sekimoto, Y, Sherwin, B, Shinozaki, K, Shiraishi, M, Shirron, P, Shitvov, A, Signorelli, G, Smecher, G, Spinella, F, Starck, J, Stever, S, Stompor, R, Sudiwala, R, Sugiyama, S, Sullivan, R, Suzuki, A, Suzuki, J, Suzuki, T, Svalheim, T, Switzer, E, Takaku, R, Takakura, H, Takakura, S, Takase, Y, Takeda, Y, Tartari, A, Tavagnacco, D, Taylor, A, Taylor, E, Terao, Y, Terenzi, L, Thermeau, J, Thommesen, H, Thompson, K, Thorne, B, Toda, T, Tomasi, M, Tominaga, M, Trappe, N, Tristram, M, Tsuji, M, Tsujimoto, M, Tucker, C, Ueki, R, Ullom, J, Umemori, K, Vacher, L, Van Lanen, J, Vermeulen, G, Vielva, P, Villa, F, Vissers, M, Vittorio, N, Wandelt, B, Wang, W, Wehus, I, Weller, J, Westbrook, B, Weymann-Despres, G, Wilms, J, Winter, B, Wollack, E, Yamasaki, N, Yoshida, T, Yumoto, J, Watanuki, K, Zacchei, A, Zannoni, M, Zonca, A, and National Aeronautics and Space Administration (US)
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CMB ,TES ,OMT ,Low temperature detector ,Bolometer ,FIS/05 - ASTRONOMIA E ASTROFISICA ,Settore FIS/05 - Astronomia e Astrofisica ,General Materials Science ,Condensed Matter Physics ,CMB, TES, OMT, Low temperature detector, Bolometer ,Atomic and Molecular Physics, and Optics - Abstract
et al., Feedhorn- and orthomode transducer- (OMT) coupled transition edge sensor (TES) bolometers have been designed and micro-fabricated to meet the optical specifications of the LiteBIRD high frequency telescope (HFT) focal plane. We discuss the design and optical characterization of two LiteBIRD HFT detector types: dual-polarization, dual-frequency-band pixels with 195/280 GHz and 235/337 GHz band centers. Results show well-matched passbands between orthogonal polarization channels and frequency centers within 3% of the design values. The optical efficiency of each frequency channel is conservatively reported to be within the range 0.64−0.72, determined from the response to a cryogenic, temperature-controlled thermal source. These values are in good agreement with expectations and either exceed or are within 10% of the values used in the LiteBIRD sensitivity forecast. Lastly, we report a measurement of loss in Nb/SiNx/Nb microstrip at 100 mK and over the frequency range 200–350 GHz, which is comparable to values previously reported in the literature., This work is supported by NASA under grant no. 80NSSC18K0132.
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- 2022
13. GASKAP-HI Pilot Survey Science I: ASKAP Zoom Observations of HI Emission in the Small Magellanic Cloud
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N. M. Pingel, J. Dempsey, N. M. McClure-Griffiths, J. M. Dickey, K. E. Jameson, H. Arce, G. Anglada, J. Bland-Hawthorn, S. L. Breen, F. Buckland-Willis, S. E. Clark, J. R. Dawson, H. Dénes, E. M. Di Teodoro, B.-Q. For, Tyler J. Foster, J. F. Gómez, H. Imai, G. Joncas, C.-G. Kim, M.-Y. Lee, C. Lynn, D. Leahy, Y. K. Ma, A. Marchal, D. McConnell, M.-A. Miville-Deschènes, V. A. Moss, C. E. Murray, D. Nidever, J. Peek, S. Stanimirović, L. Staveley-Smith, T. Tepper-Garcia, C. D. Tremblay, L. Uscanga, J. Th. van Loon, E. Vázquez-Semadeni, J. R. Allison, C. S. Anderson, Lewis Ball, M. Bell, D. C.-J. Bock, J. Bunton, F. R. Cooray, T. Cornwell, B. S. Koribalski, N. Gupta, D. B. Hayman, L. Harvey-Smith, K. Lee-Waddell, A. Ng, C. J. Phillips, M. Voronkov, T. Westmeier, M. T. Whiting, Ministerio de Ciencia e Innovación (España), European Commission, and Australian Research Council
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Astrophysics::Instrumentation and Methods for Astrophysics ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astronomy & Astrophysics ,Q1 ,Astrophysics - Astrophysics of Galaxies ,HI line emission ,Space and Planetary Science ,Interstellar medium ,Astrophysics of Galaxies (astro-ph.GA) ,Dwarf irregular galaxies ,QB460 ,Small Magellanic Cloud ,0201 Astronomical and Space Sciences, 0299 Other Physical Sciences ,QB600 ,Astrophysics::Galaxy Astrophysics ,QB - Abstract
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.--Full list of authors: Pingel, N. M.; Dempsey, J.; McClure-Griffiths, N. M.; Dickey, J. M.; Jameson, K. E.; Arce, H.; Anglada, G.; Bland-Hawthorn, J.; Breen, S. L.; Buckland-Willis, F.; Clark, S. E.; Dawson, J. R.; Denes, H.; Di Teodoro, E. M.; For, B-Q; Foster, Tyler J.; Gomez, J. F.; Imai, H.; Joncas, G.; Kim, C-G; Lee, M-Y; Lynn, C.; Leahy, D.; Ma, Y. K.; Marchal, A.; McConnell, D.; Miville-Deschenes, M-A; Moss, V. A.; Murray, C. E.; Nidever, D.; Peek, J.; Staveley-Smith, L.; Tepper-Garcia, T.; Tremblay, C. D.; Uscanga, L.; van Loon, J. Th; Vazquez-Semadeni, E.; Allison, J. R.; Anderson, C. S.; Ball, Lewis; Bell, M.; Bock, D. C-J; Bunton, J.; Cooray, F. R.; Cornwell, T.; Koribalski, B. S.; Gupta, N.; Hayman, D. B.; Harvey-Smith, L.; Lee-Waddell, K.; Ng, A.; Phillips, C. J.; Voronkov, M.; Westmeier, T.; Whiting, M. T.; Stanimirovic, S., We present the most sensitive and detailed view of the neutral hydrogen ( HI ) emission associated with the Small Magellanic Cloud (SMC), through the combination of data from the Australian Square Kilometre Array Pathfinder (ASKAP) and Parkes (Murriyang), as part of the Galactic Australian Square Kilometre Array Pathfinder (GASKAP) pilot survey. These GASKAP-HI pilot observations, for the first time, reveal HI in the SMC on similar physical scales as other important tracers of the interstellar medium, such as molecular gas and dust. The resultant image cube possesses an rms noise level of 1.1 K ( 1.6mJy beam−1 ) per 0.98km s−1 spectral channel with an angular resolution of 30′′ ( ∼10pc ). We discuss the calibration scheme and the custom imaging pipeline that utilises a joint deconvolution approach, efficiently distributed across a computing cluster, to accurately recover the emission extending across the entire ∼25deg2 field-of-view. We provide an overview of the data products and characterise several aspects including the noise properties as a function of angular resolution and the represented spatial scales by deriving the global transfer function over the full spectral range. A preliminary spatial power spectrum analysis on individual spectral channels reveals that the power law nature of the density distribution extends down to scales of 10 pc. We highlight the scientific potential of these data by comparing the properties of an outflowing high-velocity cloud with previous ASKAP+Parkes HI test observations. c The Author(s), 2022. Published by Cambridge University Press on behalf of the Astronomical Society of Australia., The Australian SKA Pathfinder is part of the Australia Telescope National Facility which is managed by CSIRO. Operation of ASKAP is funded by the Australian Government with support from the National Collaborative Research Infrastructure Strategy. ASKAP uses the resources of the Pawsey Supercomputing Centre. Establishment of ASKAP, the Murchison Radio-astronomy Observatory and the Pawsey Supercomputing Centre are initiatives of the Australian Government, with support from the Government of Western Australia and the Science and Industry Endowment Fund. We acknowledge the Wajarri Yamatji people as the traditional owners of the Observatory site. Pipeline development was tested on the OzSTAR supercomputer under the project code, oz145, which is available through Swinburne University’s Centre of Astrophysics and Supercomputing. This research was supported by the Australian Research Council (ARC) through grant DP190101571. N.M.-G. acknowledges the support of the ARC through Future Fellowship FT150100024. G. A. and J. F. G. acknowledge support from the State Agency for Research (10.13039/501100011033) of the Spanish MCIU, through grants AYA2017-84390-C2-1-R and PID2020-114461GB-I00 (co-funded by FEDER) and the ‘Center of Excellence Severo Ochoa’ award for the Instituto de Astrofsica de Andaluca (SEV-2017-0709). C. E. M. is supported by an NSF Astronomy and Astrophysics Postdoctoral Fellowship under award AST-1801471.
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- 2021
14. The width of Herschel filaments varies with distance (Corrigendum)
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G. V. Panopoulou, S. E. Clark, A. Hacar, F. Heitsch, J. Kainulainen, E. Ntormousi, D. Seifried, and R. J. Smith
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Space and Planetary Science ,Astronomy and Astrophysics - Published
- 2022
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15. A Comparison of Multi-Phase Magnetic Field Tracers in a High-Galactic Latitude Region of the Filamentary Interstellar Medium
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J. L. Campbell, S. E. Clark, B. M. Gaensler, A. Marchal, C. L. Van Eck, A. A. Deshpande, S. J. George, S. J. Gibson, R. Ricci, J. M. Stil, and A. R. Taylor
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Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Astrophysics::Galaxy Astrophysics - Abstract
Understanding how the Galactic magnetic field threads the multi-phase interstellar medium (ISM) remains a considerable challenge, as different magnetic field tracers probe dissimilar phases and field components. We search for evidence of a common magnetic field shared between the ionized and neutral ISM by comparing 1.4 GHz radio continuum polarization and HI line emission from the Galactic Arecibo L-Band Feed Array Continuum Transit Survey (GALFACTS) and Galactic Arecibo L-Band Feed Array HI (GALFA-HI) survey, respectively. We compute the polarization gradient of the continuum emission and search for associations with diffuse/translucent HI structures. The polarization gradient is sensitive to changes in the integrated product of the thermal electron density and line-of-sight field strength ($B_\parallel$) in warm ionized gas, while narrow HI structures highlight the plane-of-sky field orientation in cold neutral gas. We identified one region in the high-Galactic latitude Arecibo sky, G216+26 centered on $(\ell,b)\sim(216\deg,+26\deg)$, containing filaments in the polarization gradient that are aligned with narrow HI structures roughly parallel to the Galactic plane. We present a comparison of multi-phase observations and magnetic field tracers of this region, demonstrating that the warm ionized and cold neutral media are connected likely via a common magnetic field. We quantify the physical properties of a polarization gradient filament associated with H$\alpha$ emission, measuring a line-of-sight field strength $B_\parallel=6{\pm}4 \mu$G and a plasma beta $\beta=2.1^{+3.1}_{-2.1}$. We discuss the lack of widespread multi-phase magnetic field alignments and consider whether this region is associated with a short-timescale or physically rare phenomenon. This work highlights the utility of multi-tracer analyses for understanding the magnetized ISM., Comment: 30 pages, 17 figures, minor edits to reflect published version
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- 2021
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16. The current referral patterns for temporomandibular joint disorders (TMD) in Greater Manchester
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R, Hamad, A S E, Clark, and I A, Pretty
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Quality of Life ,Humans ,Chronic Pain ,Temporomandibular Joint Disorders ,Referral and Consultation ,Retrospective Studies - Abstract
Temporomandibular joint disorders (TMD) affect up to 50% of the population. Chronic TMD may have a significant impact on patients' quality of life and is associated with a significant cost burden to health services.The aim of this study was to investigate the incidence of TMD in Greater Manchester and to determine the most appropriate setting for its management.Data were retrospectively collected on the demographics, symptoms and management provided to patients referred for TMD.There were 789 referrals analysed; 616 to a Tertiary Centre and 173 to a District General Hospital (DGH). The most common reason for referral was pain (82%), followed by limitation in opening (55%) and clicks or sounds (44%). 27% of referrals were managed with a splint and 12% were provided with advice or a patient information leaflet prior to referral.The effect of chronic pain on patients' quality of life and the cost burden of its management compels us to review current practices in referral and management of TMD. Barriers to provision of treatment in primary care may include a lack of training, remuneration or confidence. These may be overcome with the development of self-care plans for patients and a care pathway for practitioners.Based on existing evidence, timely and conservative management of TMD should be encouraged in primary care, enabling better outcomes to be achieved for patients and the maintenance of the experience and skill level of specialist services in secondary care.
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- 2020
17. Collisionless momentum transfer in space and astrophysical explosions
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Erik Everson, Carmen Constantin, B. Van Compernolle, Shreekrishna Tripathi, S. E. Clark, Stephen Vincena, B. R. Lee, Dan Winske, Derek Schaeffer, Christoph Niemann, and A. S. Bondarenko
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Physics ,Momentum transfer ,General Physics and Astronomy ,Plasma ,01 natural sciences ,010305 fluids & plasmas ,Magnetic field ,Ion ,Momentum ,Solar wind ,Deflection (physics) ,Physics::Plasma Physics ,Physics::Space Physics ,0103 physical sciences ,Physics::Atomic Physics ,Interplanetary magnetic field ,Atomic physics ,010306 general physics - Abstract
Larmor coupling is a collisionless momentum exchange mechanism believed to occur in various astrophysical and space-plasma environments. The phenomenon is now observed in a laboratory experiment. The AMPTE (Active Magnetospheric Particle Tracer Explorers) mission provided in situ measurements of collisionless momentum and energy exchange between an artificial, photo-ionized barium plasma cloud and the streaming, magnetized hydrogen plasma of the solar wind 1,2,3. One of its most significant findings was the unanticipated displacement of the barium ion ‘comet head’ (and an oppositely directed deflection of the streaming hydrogen ions) transverse to both the solar wind flow and the interplanetary magnetic field, defying the conventional expectation that the barium ions would simply move downwind4. While subsequent theoretical and computational efforts5,6,7 to understand the cause of the transverse motion reached differing conclusions, several authors5 attributed the observations to Larmor coupling8,9, a collisionless momentum exchange mechanism believed to occur in various astrophysical and space-plasma environments10,11 and to participate in cosmic magnetized collisionless shock formation12,13,14. Here we present the detection of Larmor coupling in a reproducible laboratory experiment that combines an explosive laser-produced plasma cloud with preformed, magnetized ambient plasma in a parameter regime relevant to the AMPTE barium releases. In our experiment, time-resolved Doppler spectroscopy reveals ambient ion acceleration transverse to both the laser-produced plasma flow and the background magnetic field. Utilizing a detailed numerical simulation, we demonstrate that the ambient ion velocity distribution corresponding to the measured Doppler-shifted spectrum is qualitatively and quantitatively consistent with Larmor coupling.
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- 2017
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18. Rapid assessment of the physiological impacts caused by catch-and-release angling on blue-finned mahseer (Torsp.) of the Cauvery River, India
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S. J. Cooke, Shannon D. Bower, Adrian C. Pinder, S. E. Clark-Danylchuk, Rajeev Raghavan, and Andy J. Danylchuk
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0106 biological sciences ,Veterinary medicine ,Ecology ,biology ,010604 marine biology & hydrobiology ,Fishing ,Aquatic Science ,biology.organism_classification ,010603 evolutionary biology ,01 natural sciences ,Rapid assessment ,Fishery ,Bycatch ,Air exposure ,Blood lactate ,%22">Fish ,14. Life underwater ,Major injury ,Mahseer - Abstract
Forty-nine blue-finned mahseer (Tor sp.; mean total length 458 ± 20 mm) were angled using a range of bait/lure types, angling and air exposure times in water that averaged 27 ± 2 °C over the course of the assessment. No cases of mortality were observed, and rates of moderate and major injury were low, with 91% of mahseer hooked in the mouth. More extreme physiological disturbances (i.e. blood lactate, glucose, pH) in mahseer were associated with longer angling times. Sixteen fish (33%) exhibited at least one form of reflex impairment. Moreover, longer air exposures and angling times resulted in significant likelihood of reflex impairment. Findings suggest that blue-finned mahseer are robust to catch-and-release, but that anglers should avoid unnecessarily long fight times and minimise air exposure to decrease the likelihood of sub-lethal effects that could contribute to post-release mortality.
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- 2016
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19. Observation of collisionless shocks in a large current-free laboratory plasma
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Erik Everson, Derek Schaeffer, Dan Winske, A. S. Bondarenko, Carmen Constantin, Christoph Niemann, B. Van Compernolle, Stephen Vincena, S. E. Clark, Patrick Pribyl, and Walter Gekelman
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Physics ,Plasma ,Astrophysics ,Dissipation ,law.invention ,Computational physics ,Shock (mechanics) ,Magnetic field ,Ion ,Shock waves in astrophysics ,Piston ,Coupling (physics) ,Geophysics ,Physics::Plasma Physics ,law ,Physics::Space Physics ,General Earth and Planetary Sciences - Abstract
We report the first measurements of the formation and structure of a magnetized collisionless shock by a laser-driven magnetic piston in a current-free laboratory plasma. This new class of experiments combines a high-energy laser system and a large magnetized plasma to transfer energy from a laser plasma plume to the ambient ions through collisionless coupling, until a self-sustained MA∼ 2 magnetosonic shock separates from the piston. The ambient plasma is highly magnetized, current free, and large enough (17 m × 0.6 m) to support Alfven waves. Magnetic field measurements of the structure and evolution of the shock are consistent with two-dimensional hybrid simulations, which show Larmor coupling between the debris and ambient ions and the presence of reflected ions, which provide the dissipation. The measured shock formation time confirms predictions from computational work.
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- 2014
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20. Molecular subtyping of DCIS: heterogeneity of breast cancer reflected in pre-invasive disease
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Jane Warwick, S E Clark, R Carpenter, J L Jones, Stephen W. Duffy, and R L Bowen
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Adult ,Oncology ,Cancer Research ,medicine.medical_specialty ,Pathology ,DCIS ,Receptor, ErbB-2 ,Breast Neoplasms ,Disease ,Biology ,triple negative ,RC0254 ,Immunoenzyme Techniques ,Breast cancer ,Internal medicine ,basal ,Biomarkers, Tumor ,Carcinoma ,medicine ,Humans ,Neoplasm Invasiveness ,intrinsic subtypes ,skin and connective tissue diseases ,Molecular Diagnostics ,neoplasms ,Survival rate ,Aged ,Neoplasm Staging ,Aged, 80 and over ,Invasive disease ,Follow up studies ,Middle Aged ,Prognosis ,medicine.disease ,Subtyping ,ErbB Receptors ,Survival Rate ,body regions ,Carcinoma, Intraductal, Noninfiltrating ,Proto-Oncogene Proteins c-bcl-2 ,Receptors, Estrogen ,Tissue Array Analysis ,Progesterone metabolism ,Keratins ,Female ,Bcl-2 ,Receptors, Progesterone ,Follow-Up Studies - Abstract
Background: Molecular profiling has identified at least four subtypes of invasive breast carcinoma, which exhibit distinct clinical behaviour. There is good evidence now that DCIS represents the non-obligate precursor to invasive breast cancer and therefore it should be possible to identify similar molecular subtypes at this stage. In addition to a limited five-marker system to identify molecular subtypes in invasive breast cancer, it is evident that other biological molecules may identify distinct tumour subsets, though this has not been formally evaluated in DCIS.\ud \ud Methods: Tissue microarrays were constructed for 188 cases of DCIS. Immunohistochemistry was performed to examine the expression patterns of oestrogen receptor (ER), progesterone receptor (PR), Her2, EGFR, cytokeratin (CK) 5/6, CK14, CK17, CK18, β4-integrin, β6-integrin, p53, SMA, maspin, Bcl-2, topoisomerase IIα and P-cadherin. Hierarchical clustering analysis was undertaken to identify any natural groupings, and the findings were validated in an independent sample series.\ud \ud Results: Each of the intrinsic molecular subtypes described for invasive breast cancer can be identified in DCIS, though there are differences in the relative frequency of subgroups, in particular, the triple negative and basal-like phenotype is very uncommon in DCIS. Hierarchical cluster analysis identified three main subtypes of DCIS determined largely by ER, PR, Her2 and Bcl-2, and this classification is related to conventional prognostic indicators. These subtypes were confirmed in an analysis on independent series of DCIS cases.\ud \ud Conclusion: This study indicates that DCIS may be classified in a similar manner to invasive breast cancer, and determining the relative frequency of different subtypes in DCIS and invasive disease may shed light on factors determining disease progression. It also demonstrates a role for Bcl-2 in classifying DCIS, which has recently been identified in invasive breast cancer.
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- 2010
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21. Laboratory study of collisionless coupling between explosive debris plasma and magnetized ambient plasma
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Derek Schaeffer, A. S. Bondarenko, Carmen Constantin, B. R. Lee, Shreekrishna Tripathi, C. Niemann, S. E. Clark, Stephen Vincena, Dan Winske, Erik Everson, and B. Van Compernolle
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Physics ,Dense plasma focus ,010504 meteorology & atmospheric sciences ,Explosive material ,chemistry.chemical_element ,Plasma ,Condensed Matter Physics ,01 natural sciences ,7. Clean energy ,010305 fluids & plasmas ,Computational physics ,Coupling (physics) ,chemistry ,Physics::Plasma Physics ,Physics::Space Physics ,0103 physical sciences ,Plasma diagnostics ,Emission spectrum ,Atomic physics ,Helium ,Large Plasma Device ,0105 earth and related environmental sciences - Abstract
The explosive expansion of a localized plasma cloud into a relatively tenuous, magnetized, ambient plasma characterizes a variety of astrophysical and space phenomena. In these rarified environments, collisionless electromagnetic processes rather than Coulomb collisions typically mediate the transfer of momentum and energy from the expanding “debris” plasma to the surrounding ambient plasma. In an effort to better understand the detailed physics of collisionless coupling mechanisms, compliment in situ measurements of space phenomena, and provide validation of previous computational and theoretical work, the present research jointly utilizes the Large Plasma Device and the Raptor laser facility at the University of California, Los Angeles to study the super-Alfvenic, quasi-perpendicular expansion of laser-produced carbon (C) and hydrogen (H) debris plasma through preformed, magnetized helium (He) ambient plasma via a variety of diagnostics, including emission spectroscopy, wavelength-filtered imaging, and ...
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- 2017
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22. Effects of Site Characteristics and Release History on Establishment of Agapeta zoegana (Lepidoptera: Cochylidae) and Cyphocleonus achates (Coleoptera: Curculionidae), Root-Feeding Herbivores of Spotted Knapweed, Centaurea maculosa
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R. G. Van Driesche, N. Sturdevant, J. S. Elkinton, John P. Buonaccorsi, and S. E. Clark
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Herbivore ,Centaurea maculosa ,Cyphocleonus achates ,biology ,Weevil ,biology.organism_classification ,Soil type ,medicine.disease_cause ,Agronomy ,Insect Science ,Curculionidae ,Infestation ,medicine ,Agapeta zoegana ,Agronomy and Crop Science - Abstract
We evaluated several factors to identify features or practices that might increase the probability of establishment following the release of two root-feeding insects (the cochylid moth Agapeta zoegana L. and the weevil Cyphocleonus achates Fahraeus) that attack the invasive plant, spotted knapweed (Centaurea maculosa Lamarck). At each of 99 sites where releases had been made in previous years, we assessed (1) the number of insects of each species released, (2) the number of years in which releases were made, (3) the number of years since the first release, (4) the size of the knapweed infestation, (5) its shape (linear, large single patch, many small patches), (6) the knapweed plant density, and (7–18) 12 physical site characteristics: habitat type, elevation, percentage slope, aspect, topographic type, forest structure at or by the site, disturbance factors, land use category, percentage forest canopy at or near site, percentage bare soil, annual precipitation, and soil type. We found that continuous, nonlinear patches of spotted knapweed on loamy soil that were surrounded by even-age forest stands had the highest rates of establishment for A. zoegana, but likelihood of establishment was not greater for larger releases (>200 adults). This suggests that roadside strips of knapweed should not be selected as release sites and that many, smaller releases (100–200 adults) are better than fewer, larger releases (300–500 adults or greater). For the weevil C. achates, we found that the probability of establishment was also greatest in continuous knapweed patches, rather than in strips, and that larger infestations (>2 ha) were better than smaller infestations. Establishment was also highest at mid-elevations (750–1500 m), compared to higher or lower locations.
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- 2001
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23. Comparative Efficacy of Adult and Larval Sampling for Detection of the Root-Boring InsectsAgapeta zoegana(Lepidoptera: Cochylidae) andCyphocleonus achates(Coleoptera: Curculionidae) Released for Biological Control of Spotted Knapweed
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N. Sturdevant, S. E. Clark, R. G. Van Driesche, and Sandra J. Kegley
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Larva ,Centaurea maculosa ,Cyphocleonus achates ,Ecology ,biology ,Biological pest control ,Sampling (statistics) ,biology.organism_classification ,Lepidoptera genitalia ,Animal science ,Insect Science ,Curculionidae ,Botany ,Agapeta zoegana ,Ecology, Evolution, Behavior and Systematics - Abstract
In biological control projects, establishment of released natural enemies is a key step and must be efficiently detected. We studied the relative efficacy of larval versus adult sampling to detect establishment on spotted knapweed, Centaurea maculosa Lamarck, of the two root feeding insects Agapeta zoegana L. and Cyphocleonus achates (Fahraeus). Larval sampling was based on excavation and dissection of plant roots. Adult sampling consisted of either sighting adults along transects at release sites or collection of adults by sweep netting. Recovery rates for A. zoegana were higher through adult visual sampling (54.8%) than through larval sampling via root dissection (43.0%). Adult visual sampling required less time (30 min/site) than did root dissection (130 min/site). Sweep net sampling, although having the lowest detection rate (38.1%), required even less time (10 min/site) and was the most effective method per unit time. In contrast, for C. achates, larval sampling was the most effective method, with a recovery rate of 35.6%, compared with 8.9% for adult visual sampling. Sweep netting was more effective than visual sampling, with a detection rate of 18.1%. Adult visual sampling required less time (44 min/site) than did root dissection (130 min/site). Sweep net sampling, although having the lowest detection rate (18.1%), required even less time (10 min/site) and was the most effective method per unit time. However, other factors such as weather, travel time, and training levels needed for sampling make root sampling a more effective method, in a larger sense, for both of these insects.
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- 2001
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24. Postnatal alterations of GABA receptor profiles in the rat superior colliculus
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Bettina Platt, Maurice Garret, and S. E. Clark
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Aging ,Superior Colliculi ,medicine.medical_specialty ,Synaptophysin ,Cell Count ,GABAB receptor ,Biology ,gamma-Aminobutyric acid ,GABAA-rho receptor ,Rats, Sprague-Dawley ,Receptors, GABA ,GABA receptor ,Internal medicine ,medicine ,Animals ,Receptor ,gamma-Aminobutyric Acid ,Neurons ,GABAA receptor ,General Neuroscience ,Superior colliculus ,Cell Differentiation ,Receptors, GABA-A ,Immunohistochemistry ,Rats ,Endocrinology ,Animals, Newborn ,Receptors, GABA-B ,nervous system ,GABAergic ,medicine.drug - Abstract
Midbrain sections taken from Sprague-Dawley rats of varying ages within the first four postnatal weeks were used to determine, immunocytochemically, putative changes of GABA(A) receptor beta2/3 subunits, GABA(B) receptor (R1a and R1b splice variants), and GABA(C) receptor rho1 subunit expression and distribution in the superficial, visual layers of the superior colliculus. Immunoreactivity for the GABA(A) receptor beta2/3 subunits was found in the superficial grey layer from birth. The labelling changed with age, with an overall continuous reduction in the number of cells labelled and a significant increase in the labelling intensity distribution (neuropil vs soma). Further analysis revealed an initial increase in the labelling intensity between postnatal days 0 and 7 in parallel with an overall reduction of labelled neurones. This was followed by a significant decrease in labelling intensity distribution between postnatal days 7 and 16, and a subsequent increase in intensity between postnatal days 16 and 28. The labelling profiles for GABA(B) receptors (R1a and R1b splice variants) and GABA(C) receptors (rho1 subunit) showed similar patterns. Both receptors could be found in the superficial layers of the superior colliculus from birth, and the intensity and distribution of labelling remained constant during the first postnatal month. However, the cell body count showed a significant decrease between postnatal days 7 and 16. These changes may be related to the time-point of eye opening, which occurred approximately two weeks after birth. For all three receptor types, the cell body count remained constant after postnatal day 16. By four weeks of age, there was no significant difference between the cell numbers obtained for the different receptors. Both GABA itself and neurofilament labelling were also obtained in the superficial superior colliculus at birth. Neurofilament, although found at birth, showed very little ordered arrangement until 16days after birth. When slices were double labelled for GABA(C) receptors and neurofilament, some overlap was observed. Double labelling for the presynaptic protein synaptophysin and GABA(C) receptors showed proximity in some places, indicative of a partly synaptic location of GABA(C) receptors. When GABA(C) and GABA(A) receptors were labelled simultaneously, some but not all neurones showed immunoreactivity for both receptor types. In conclusion, all three GABA receptor types were found to be present in the superior colliculus from birth, and all show some form of postnatal modification, with GABA(A) receptors demonstrating the most dramatic changes. However, GABA(B) and GABA(C) receptors are modified significantly around the onset of input-specific activity. Together, this points towards a contribution of the GABAergic system to processes of postnatal maturation in the superficial superior colliculus.
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- 2001
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25. [Untitled]
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Robin A. McGee, D K Symons, and S E Clark
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endocrine system diseases ,Psychometrics ,Cognition ,Test validity ,medicine.disease ,digestive system diseases ,Developmental psychology ,Auditory Continuous Performance Test ,Psychiatry and Mental health ,El Niño ,Phonological awareness ,Auditory attention ,Developmental and Educational Psychology ,medicine ,Attention deficit hyperactivity disorder ,heterocyclic compounds ,Psychology ,neoplasms - Abstract
The performance of clinic-referred children aged 6-11 (N = 100) was examined using the Conners' Continuous Performance Test (CPT) and measures of auditory attention (Auditory Continuous Performance Test; ACPT), phonological awareness, visual processing speed, and visual-motor competence. The Conners' CPT overall index was unrelated to measures of visual processing speed or visual-motor competence. Although the Conners' CPT converged with the ACPT, the latter demonstrated age and order effects. Significant variance in Conners' CPT parameters was predicted by phonological awareness measures, suggesting that Reading Disordered (RD) children could be "false positives" on the Conners' CPT. The Conners' CPT overall index, phonological awareness, and visual-motor measures were submitted to a 2 x 2 MANCOVA (ADHD vs. RD, covarying for age and socioeconomic status): a main effect for RD status was found. Children with ADHD did not have higher Conners' CPT scores than did clinical controls; however, children with Reading Disorders did. Phonological measures distinguished RD children from ADHD children and other clinical controls. ADHD children who failed the Conners' CPT were rated by teachers as more hyperactive. Despite the strengths of the Conners' CPT, its utility for differential diagnosis of ADHD is questioned.
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- 2000
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26. Enhanced collisionless shock formation in a magnetized plasma containing a density gradient
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Derek Schaeffer, A. S. Bondarenko, Carmen Constantin, Dan Winske, Erik Everson, Christoph Niemann, and S. E. Clark
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Coupling ,Physics ,Laser ablation ,Density gradient ,Physics::Plasma Physics ,Physics::Space Physics ,Cylinder ,Plasma ,Atomic physics ,Molecular physics ,Magnetic flux ,Shock (mechanics) ,Ion - Abstract
Two-dimensional hybrid simulations of super-Alfv\'enic expanding debris plasma interacting with an inhomogeneous ambient plasma are presented. The simulations demonstrate improved collisionless coupling of energy to the ambient ions when encountering a density gradient. Simulations of an expanding cylinder running into a step function gradient are performed and compared to a simple analytical theory. Magnetic flux probe data from a laboratory shock experiment are compared to a simulation with a more realistic debris expansion and ambient ion density. The simulation confirms that a shock is formed and propagates within the high density region of ambient plasma.
- Published
- 2014
27. Characterization of laser-produced carbon plasmas relevant to laboratory astrophysics
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Erik Everson, A. S. Bondarenko, Carmen Constantin, S. E. Clark, Derek Schaeffer, and Christoph Niemann
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Physics ,Isentropic process ,General Physics and Astronomy ,Charge (physics) ,Astrophysics ,Plasma ,Laser ,7. Clean energy ,01 natural sciences ,010305 fluids & plasmas ,law.invention ,Ion ,law ,0103 physical sciences ,Plasma diagnostics ,Astrophysical plasma ,Atomic physics ,010306 general physics ,Adiabatic process - Abstract
Experiments, analytic modeling, and numerical simulations are presented to characterize carbon plasmas produced by high-intensity ( 109−1013 W cm−2) lasers relevant to experimental laboratory astrophysics. In the large-scale limit, the results agree well with a self-similar isentropic, adiabatic fluid model. Laser-target simulations, however, show small-scale structure in the velocity distribution of different ion species, which is also seen in experiments. These distributions indicate that most of the plasma energy resides in moderate charge states (C+3–C+4), most of the mass resides in the lowest charge states, and the highest charge states move fastest.
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- 2016
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28. Feasibility of characterizing laser-ablated carbon plasmas via planar laser induced fluorescence
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Erik Everson, S. E. Clark, A. S. Bondarenko, Carmen Constantin, C. Niemann, and Derek Schaeffer
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Materials science ,Laser ablation ,Context (language use) ,Plasma ,Laser ,law.invention ,Ion ,Physics::Plasma Physics ,Planar laser-induced fluorescence ,law ,Physics::Space Physics ,Atom ,Plasma diagnostics ,Atomic physics ,Instrumentation - Abstract
Planar laser induced fluorescence (PLIF) imaging can potentially assess ion distributions and coupling in the context of super-Alfvenic ablation plasma expansions into magnetized background plasmas. In this feasibility study, we consider the application of PLIF to rapidly expanding carbon plasmas generated via energetic laser ablation of graphite. By utilizing hydrodynamic and collisional-radiative simulations, we identify schemes accessible to commercially available tunable lasers for the C I atom, the C II ion, and the C V ion. We then estimate the signal-to-noise ratios yielded by the schemes under reasonable experimental configurations.
- Published
- 2012
29. UV Seeding of IR Laser Induced Damage
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David C. Emmony, S E Clark, and N C Kerr
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Soda-lime glass ,Fused quartz ,Materials science ,Silicon ,business.industry ,chemistry.chemical_element ,Laser ,law.invention ,Wavelength ,Optics ,chemistry ,law ,business ,Quartz ,Order of magnitude ,Beam (structure) - Abstract
The values of the laser induced surface damage thresholds for samples of silicon, fused quartz and soda lime glass at both 0.248pm (UV) and 10.6pm (IR) are presented. Experiments are then described where laser damage is induced using crossed UV-IR beams, with varying time delays imposed between the arrivals of the two laser pulses at the sample surface. The results of these crossed beam experiments are then discussed. Order of magnitude reductions in the IR damage thresholds of silicon and glass are observed when the beams are crossed, no such reduction is observed for quartz. Further, only in the case of glass samples is a reduction in the UV damage threshold seen when the beams are crossed. The reduction in IR threshold on silicon has been seen with delays between the laser pulses of up to 100ns. The reduction in IR threshold for glass was seen for delays up to 1.2ms. These results lead to a discussion of the role of so-called seed electrons in the damage process and the mechanisms operative at the different wavelengths.
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- 2009
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30. IR Laser Beam Profiling Using Quenched Fluorescence
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S E Clark, David C. Emmony, and N C Kerr
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Materials science ,business.industry ,Resolution (electron density) ,Video camera ,Laser ,Pulse (physics) ,law.invention ,Pyroelectricity ,Optics ,law ,Optoelectronics ,Laser beam quality ,business ,Luminescence ,Beam (structure) - Abstract
The construction and performance of a system for the spatial characterization of a CO2 pulsed laser beam is described. Using thermally quenched fluorescence a direct imaging technique has been developed for single shot CO2 laser pulse beam profiling. A CCD video camera and framestore interfaced to a PC computer are used to image the spatial intensity distribution produced by a CO2 pulse incident upon a temperature dependent luminescent screen. The resolution is similar to much more expensive pyroelectric detector array techniques with all the advantages of two dimensional beam processing.
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- 2009
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31. The topography of laser-induced ripple structures
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S E Clark, B.A. Omar, N C Kerr, and David C. Emmony
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Fused quartz ,Materials science ,Acoustics and Ultrasonics ,business.industry ,Ripple ,chemistry.chemical_element ,Germanium ,Condensed Matter Physics ,Laser ,Plasma oscillation ,Surfaces, Coatings and Films ,Electronic, Optical and Magnetic Materials ,law.invention ,Interferometry ,Wavelength ,Optics ,chemistry ,law ,Irradiation ,business - Abstract
The authors present results which show the topography of the laser-induced periodic surface structures formed upon samples of germanium, which had been irradiated at a wavelength of 248 nm, and fused quartz irradiated at 10.6 mu m. Surface profiles are obtained from phaseshifting interferometry measurements. A slight modification to a theory which models the development of the surface contour during resolidification of a molten surface can be successfully employed to explain their observations upon germanium. To explain the profiles obtained on fused quartz they suggest that plasma oscillations at the surface may be involved.
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- 1990
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32. Crossed UV-IR laser beam studies of laser-induced surface damage to optical materials
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N C Kerr, S E Clark, and David C. Emmony
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Soda-lime glass ,Fused quartz ,Materials science ,Acoustics and Ultrasonics ,Silicon ,business.industry ,chemistry.chemical_element ,Electron ,Condensed Matter Physics ,Laser ,complex mixtures ,Surfaces, Coatings and Films ,Electronic, Optical and Magnetic Materials ,law.invention ,Wavelength ,Optics ,chemistry ,law ,business ,Quartz ,Beam (structure) - Abstract
The values of the laser-induced surface damage thresholds for samples of silicon, fused quartz and soda lime glass at both 0.248 mu m (UV) and 10.6 mu m (IR) are presented. Experiments are then described where laser damage is induced using crossed UV-IR beams, with varying time delays imposed between the arrivals of the two laser pulses at the sample surface. Order of magnitude reductions in the IR damage thresholds of silicon and glass are observed when the beams are crossed, no such reduction is observed for quartz. Further, only in the case of glass samples is a reduction in the UV damage threshold seen when the beams are crossed. The reduction in IR threshold on silicon has been seen with delays between the laser pulses of up to 100 ns. The reduction in IR threshold for glass was seen for delays up to 1.2 ms. These results lead to a discussion of the influence of 'seeding electrons' on the development of laser-induced damage as well as to determine whether the damage mechanisms are similar at each wavelength.
- Published
- 1990
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33. Experimental study of subcritical laboratory magnetized collisionless shocks using a laser-driven magnetic piston
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Erik Everson, Walter Gekelman, Christoph Niemann, Derek Schaeffer, Carmen Constantin, A. S. Bondarenko, Dan Winske, and S. E. Clark
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Physics ,Thomson scattering ,Astrophysics::High Energy Astrophysical Phenomena ,Plasma ,Mechanics ,Condensed Matter Physics ,Laser ,law.invention ,Shock (mechanics) ,Magnetic field ,Shock waves in astrophysics ,Piston ,law ,Plasma diagnostics ,Atomic physics ,Astrophysics::Galaxy Astrophysics - Abstract
Recent experiments at the University of California, Los Angeles have successfully generated subcritical magnetized collisionless shocks, allowing new laboratory studies of shock formation relevant to space shocks. The characteristics of these shocks are compared with new data in which no shock or a pre-shock formed. The results are consistent with theory and 2D hybrid simulations and indicate that the observed shock or shock-like structures can be organized into distinct regimes by coupling strength. With additional experiments on the early time parameters of the laser plasma utilizing Thomson scattering, spectroscopy, and fast-gate filtered imaging, these regimes are found to be in good agreement with theoretical shock formation criteria.
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- 2015
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34. Applying a Vadose Zone Model to Stormwater Infiltration
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K. H. Baker, S. E. Clark, and J. B. Mikula
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Pollutant ,Infiltration (hydrology) ,Environmental chemistry ,Soil water ,Vadose zone ,Stormwater ,Environmental engineering ,Environmental science ,Groundwater recharge ,Surface runoff ,Groundwater - Abstract
Urbanization has been responsible for an increase in the amount of impervious surfaces, leading to an increase in stormwater runoff and a decrease in groundwater recharge. Stormwater runoff contains pollutants, such as nutrients, pathogens, heavy metals, solids, organic compounds, pesticides, and chlorides, which have greatly contributed to the degradation of receiving waters due to surface discharge of stormwater. This has prompted stormwater managers to consider implementing more infiltration practices into their designs. However, past studies have shown that infiltrating stormwater could contaminate the groundwater, and in some cases contamination actually has occurred. Therefore, methods for easily predicting contamination potential need to be developed. Stormwater pollutants interact with the soils in the unsaturated zone as they migrate towards the groundwater. The specific type of soil and its properties have a profound effect on the movement of water and pollutants. Zinc and sodium chloride were chosen to be the pollutants of interest because of their prevalence in stormwater, solubility, and differing migration rates. Through the use of the SESOIL model, factors such as pollutant concentration, rainfall, vadose zone thickness, intrinsic permeability, organic content, and soil pH were evaluated to determine which ones have the greatest influence on pollutant migration. A factorial analysis (2 6 full factorial) was used to evaluate the effects of these factors on the maximum penetration depth of zinc and sodium chloride. High and low values for the factors were selected from the literature and the NRCS soils database. The pollutants were treated as separate ions (Zn +2 , Na + , Cl - ), and the length of each simulation was set at 1 year. Results indicated that rainfall was a common factor controlling Zn +2 , Na + , and Cl - migration. Concentration was also influential in Zn +2 migration, while intrinsic permeability affected Na + and Cl - .
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- 2006
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35. Simulating Radiating and Magnetized Flows in Multi-Dimensions with ZEUS-MP
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Michael L. Norman, Mordecai-Mark Mac Low, John C. Hayes, R. A. Fiedler, Pak Shing Li, Asif ud-Doula, S. E. Clark, and James Bordner
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Physics ,Scale (ratio) ,Fast Fourier transform ,Astrophysics (astro-ph) ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics ,Function (mathematics) ,Zeus (malware) ,Computational science ,Multigrid method ,Method of characteristics ,Space and Planetary Science ,Code (cryptography) ,Massively parallel - Abstract
This paper describes ZEUS-MP, a multi-physics, massively parallel, message- passing implementation of the ZEUS code. ZEUS-MP differs significantly from the ZEUS-2D code, the ZEUS-3D code, and an early "version 1" of ZEUS-MP distributed publicly in 1999. ZEUS-MP offers an MHD algorithm better suited for multidimensional flows than the ZEUS-2D module by virtue of modifications to the Method of Characteristics scheme first suggested by Hawley and Stone (1995), and is shown to compare quite favorably to the TVD scheme described by Ryu et. al (1998). ZEUS-MP is the first publicly-available ZEUS code to allow the advection of multiple chemical (or nuclear) species. Radiation hydrodynamic simulations are enabled via an implicit flux-limited radiation diffusion (FLD) module. The hydrodynamic, MHD, and FLD modules may be used in one, two, or three space dimensions. Self gravity may be included either through the assumption of a GM/r potential or a solution of Poisson's equation using one of three linear solver packages (conjugate-gradient, multigrid, and FFT) provided for that purpose. Point-mass potentials are also supported. Because ZEUS-MP is designed for simulations on parallel computing platforms, considerable attention is paid to the parallel performance characteristics of each module. Strong-scaling tests involving pure hydrodynamics (with and without self-gravity), MHD, and RHD are performed in which large problems (256^3 zones) are distributed among as many as 1024 processors of an IBM SP3. Parallel efficiency is a strong function of the amount of communication required between processors in a given algorithm, but all modules are shown to scale well on up to 1024 processors for the chosen fixed problem size., Comment: Accepted for publication in the ApJ Supplement. 42 pages with 29 inlined figures; uses emulateapj.sty. Discussions in sections 2 - 4 improved per referee comments; several figures modified to illustrate grid resolution. ZEUS-MP source code and documentation available from the Laboratory for Computational Astrophysics at http://lca.ucsd.edu/codes/currentcodes/zeusmp2/
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- 2005
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36. Spectroscopic measurement of high-frequency electric fields in the interaction of explosive debris plasma with magnetized background plasma
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Christoph Niemann, Erik Everson, Derek Schaeffer, Carmen Constantin, A. S. Bondarenko, and S. E. Clark
- Subjects
Physics ,Dense plasma focus ,Two-stream instability ,Physics::Plasma Physics ,Waves in plasmas ,Physics::Space Physics ,Electromagnetic electron wave ,Astrophysical plasma ,Plasma ,Inductively coupled plasma ,Atomic physics ,Condensed Matter Physics ,Large Plasma Device - Abstract
The collision-less transfer of momentum and energy from explosive debris plasma to magnetized background plasma is a salient feature of various astrophysical and space environments. While much theoretical and computational work has investigated collision-less coupling mechanisms and relevant parameters, an experimental validation of the results demands the measurement of the complex, collective electric fields associated with debris-background plasma interaction. Emission spectroscopy offers a non-interfering diagnostic of electric fields via the Stark effect. A unique experiment at the University of California, Los Angeles, that combines the Large Plasma Device (LAPD) and the Phoenix laser facility has investigated the marginally super-Alfvenic, quasi-perpendicular expansion of a laser-produced carbon (C) debris plasma through a preformed, magnetized helium (He) background plasma via emission spectroscopy. Spectral profiles of the He II 468.6 nm line measured at the maximum extent of the diamagnetic cavity are observed to intensify, broaden, and develop equally spaced modulations in response to the explosive C debris, indicative of an energetic electron population and strong oscillatory electric fields. The profiles are analyzed via time-dependent Stark effect models corresponding to single-mode and multi-mode monochromatic (single frequency) electric fields, yielding temporally resolved magnitudes and frequencies. The proximity of the measured frequencies to the expected electron plasma frequency suggests the development of the electron beam-plasma instability, and a simple saturation model demonstrates that the measured magnitudes are feasible provided that a sufficiently fast electron population is generated during C debris–He background interaction. Potential sources of the fast electrons, which likely correspond to collision-less coupling mechanisms, are briefly considered.
- Published
- 2014
- Full Text
- View/download PDF
37. Laser-driven, magnetized quasi-perpendicular collisionless shocks on the Large Plasma Device
- Author
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Erik Everson, Carmen Constantin, Walter Gekelman, C. Niemann, S. E. Clark, S. T. Vincena, Shreekrishna Tripathi, A. S. Bondarenko, B. Van Compernolle, Dan Winske, and Derek Schaeffer
- Subjects
Physics ,Microphysics ,Plasma ,Condensed Matter Physics ,Computational physics ,law.invention ,Shock (mechanics) ,Shock waves in astrophysics ,Coupling (physics) ,Piston ,symbols.namesake ,Classical mechanics ,Mach number ,Physics::Plasma Physics ,law ,Physics::Space Physics ,symbols ,Large Plasma Device - Abstract
The interaction of a laser-driven super-Alfvenic magnetic piston with a large, preformed magnetized ambient plasma has been studied by utilizing a unique experimental platform that couples the Raptor kJ-class laser system [Niemann et al., J. Instrum. 7, P03010 (2012)] to the Large Plasma Device [Gekelman et al., Rev. Sci. Instrum. 62, 2875 (1991)] at the University of California, Los Angeles. This platform provides experimental conditions of relevance to space and astrophysical magnetic collisionless shocks and, in particular, allows a detailed study of the microphysics of shock formation, including piston-ambient ion collisionless coupling. An overview of the platform and its capabilities is given, and recent experimental results on the coupling of energy between piston and ambient ions and the formation of collisionless shocks are presented and compared to theoretical and computational work. In particular, a magnetosonic pulse consistent with a low-Mach number collisionless shock is observed in a quasi-perpendicular geometry in both experiments and simulations.
- Published
- 2014
- Full Text
- View/download PDF
38. Signaling through the CLAVATA1 receptor complex
- Author
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B J, DeYoung and S E, Clark
- Subjects
Sequence Homology, Amino Acid ,Arabidopsis Proteins ,Molecular Sequence Data ,Receptor Protein-Tyrosine Kinases ,Amino Acid Sequence ,Protein Serine-Threonine Kinases ,Plant Proteins ,Signal Transduction - Published
- 2001
39. Does the Conners' Continuous Performance Test aid in ADHD diagnosis?
- Author
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R A, McGee, S E, Clark, and D K, Symons
- Subjects
Male ,Psychiatric Status Rating Scales ,Hyperkinesis ,Neuropsychological Tests ,Diagnosis, Differential ,Dyslexia ,Refractory Period, Psychological ,Cognition ,Reading ,Attention Deficit Disorder with Hyperactivity ,Phonetics ,Predictive Value of Tests ,Case-Control Studies ,Humans ,Attention ,Female ,Child - Abstract
The performance of clinic-referred children aged 6-11 (N = 100) was examined using the Conners' Continuous Performance Test (CPT) and measures of auditory attention (Auditory Continuous Performance Test; ACPT), phonological awareness, visual processing speed, and visual-motor competence. The Conners' CPT overall index was unrelated to measures of visual processing speed or visual-motor competence. Although the Conners' CPT converged with the ACPT, the latter demonstrated age and order effects. Significant variance in Conners' CPT parameters was predicted by phonological awareness measures, suggesting that Reading Disordered (RD) children could be "false positives" on the Conners' CPT. The Conners' CPT overall index, phonological awareness, and visual-motor measures were submitted to a 2 x 2 MANCOVA (ADHD vs. RD, covarying for age and socioeconomic status): a main effect for RD status was found. Children with ADHD did not have higher Conners' CPT scores than did clinical controls; however, children with Reading Disorders did. Phonological measures distinguished RD children from ADHD children and other clinical controls. ADHD children who failed the Conners' CPT were rated by teachers as more hyperactive. Despite the strengths of the Conners' CPT, its utility for differential diagnosis of ADHD is questioned.
- Published
- 2000
40. Genetic and physical characterization of a region of Arabidopsis chromosome 1 containing the CLAVATA1 gene
- Author
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R W, Williams, S E, Clark, and E M, Meyerowitz
- Subjects
DNA, Plant ,Arabidopsis Proteins ,Molecular Sequence Data ,Restriction Mapping ,Arabidopsis ,Phosphoprotein Phosphatases ,Chromosome Mapping ,Protein Serine-Threonine Kinases ,Chromosomes, Artificial, Yeast ,Chromosomes ,Polymorphism, Restriction Fragment Length ,Signal Transduction - Abstract
With the advance of Arabidopsis as a model system for understanding plant genetics, development and biochemistry, a detailed description of the genome is necessary. As such, focused projects are underway to map and sequence the Arabidopsis nuclear genome. We have characterized a region of chromosome 1, surrounding the CLAVATA1 (CLV1) locus. Three (RFLP) clones were mapped relative to clv1-1, and were used to construct an ca. 700 kb yeast artificial chromosome (YAC) contig. Three cosmids spanning the CLV1 locus were analyzed and ca. 24 kb of genomic DNA was sequenced, including a continuous stretch of 18 kb. In addition to generating clones in this region of chromosome 1, we have analyzed the size, spacing and organization of several contiguous genes.
- Published
- 1999
41. Dynamics of exploding plasmas in a large magnetized plasma
- Author
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Carmen Constantin, Walter Gekelman, Alex Zylstra, S. E. Clark, A. S. Bondarenko, David Larson, Siegfried Glenzer, Christoph Niemann, Patrick Pribyl, Dan Winske, Erik Everson, Shreekrishna Tripathi, and Derek Schaeffer
- Subjects
Physics ,Magnetic energy ,Magnetism ,Plasma ,Condensed Matter Physics ,Magnetic flux ,Magnetic field ,symbols.namesake ,Physics::Plasma Physics ,Physics::Space Physics ,symbols ,Langmuir probe ,Diamagnetism ,Magnetohydrodynamics ,Atomic physics - Abstract
The dynamics of an exploding laser-produced plasma in a large ambient magneto-plasma was investigated with magnetic flux probes and Langmuir probes. Debris-ions expanding at super-Alfvenic velocity (up to MA=1.5) expel the ambient magnetic field, creating a large (>20 cm) diamagnetic cavity. We observe a field compression of up to B/B0=1.5 as well as localized electron heating at the edge of the bubble. Two-dimensional hybrid simulations reproduce these measurements well and show that the majority of the ambient ions are energized by the magnetic piston and swept outside the bubble volume. Nonlinear shear-Alfven waves (δB/B0>25%) are radiated from the cavity with a coupling efficiency of 70% from magnetic energy in the bubble to the wave.
- Published
- 2013
- Full Text
- View/download PDF
42. Confocal microscopy of the shoot apex
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M P, Running, S E, Clark, and E M, Meyerowitz
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Microscopy, Confocal ,Arabidopsis ,Plant Shoots ,Propidium ,Specimen Handling - Published
- 1995
43. Flowers
- Author
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J. L. Bowman, D. R. Smyth, J. P. Hill, E. M. Lord, S. Craig, A. Chaudhary, A. R. Davis, M. Koorneef, K. Okada, Y. Shimura, J. Alvarez, G. Bossinger, D. Weigel, E. M. Meyerowitz, S. E. Clark, H. Sakai, and W. Crone
- Published
- 1994
- Full Text
- View/download PDF
44. A support group for people bereaved through suicide
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S E, Clark, H E, Jones, K, Quinn, R D, Goldney, and P J, Cooling
- Subjects
Adult ,Male ,Adolescent ,Middle Aged ,Group Processes ,Leadership ,Self-Help Groups ,Suicide ,Adaptation, Psychological ,Humans ,Organizational Objectives ,Female ,Program Development ,Child ,Aged ,Bereavement ,Program Evaluation - Abstract
Although much research has been performed in recent years on the prevention of suicide, less attention has been focused on helping the persons left behind. This article outlines the history of establishing a support group for people who have been bereaved through suicide in an Australian city. It describes the difficulties in establishing the group, its structure, management, and helping functions, and the experiences gained from the initial 7 years of operation. The article has been written in response to requests from medical, social, and lay agencies for information in establishing similar support groups.
- Published
- 1993
45. A Contralateral Complication of Extra-peritoneal Laparoscopic Inguinal Hernia Repair
- Author
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S Jacob, M Hanson, and S E Clark
- Subjects
medicine.medical_specialty ,lcsh:Surgery ,Upper GI Surgery ,complication ,hernia ,laparoscopic ,medicine ,Direct Inguinal Hernia ,business.industry ,Femoral canal ,lcsh:RD1-811 ,medicine.disease ,Femoral hernia ,digestive system diseases ,Surgery ,Inguinal hernia ,Dissection ,stomatognathic diseases ,medicine.anatomical_structure ,surgical procedures, operative ,inguinal ,repair ,Extraperitoneal space ,Complication ,business - Abstract
A 63 year old female underwent an uncomplicated total extraperitoneal repair of a right direct inguinal hernia. One week later she presented with a strangulated left femoral hernia. We believe the dissection of the extraperitoneal space caused bleeding which tracked down through the femoral canal resulting in a femoral hernia. To date there are no reports of such a complication following total extraperitoneal inguinal hernia repair in the literature.
- Published
- 2010
46. Adults with congenital heart disease
- Author
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F, Cetta, R C, Lichtenberg, and S E, Clark
- Subjects
Adult ,Heart Defects, Congenital ,Heart Septal Defects, Ventricular ,Male ,Pregnancy ,Pregnancy Complications, Cardiovascular ,Age Factors ,Infant, Newborn ,Tetralogy of Fallot ,Humans ,Female ,Prognosis ,Aortic Coarctation - Published
- 1992
47. High Resolution Image Reconstruction from Sparse Random Arrays
- Author
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S E Clark and L F Desandre
- Abstract
In order to overcome such limitations as resolution, receiver weight and response time associated with large heavy monolithic laser radar receivers, a significant amount of work1-5 has been performed into the potential of array based systems to provide high resolution lightweight fast receivers. In order to achieve image resolution consistent with the overall size of the array, the amplitude and phase at each point in the array must be determined. As has been demonstrated in the microwave region6,7, the problem of phase errors due to errors in detector positioning and variations in the reference wavefront that are associated with the heterodyne detection process used to determine the phase, can be overcome in an adaptive way prior to using the array for imaging.
- Published
- 1992
- Full Text
- View/download PDF
48. Laser Radar Imaging with a Sparse Random Array Receiver
- Author
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S E Clark and L F Desandre
- Abstract
Over the last few years, there has been considerable interest1-4 in using multiple aperture receiver arrays in laser radar systems where low cost lightweight sensor systems of low power consumption and high angular resolution for tracking and imaging are required. As has been previously demonstrated2-4, the problem of determining the target phase from the measured phase which is corrupted by positional and reference wavefront errors can be overcome in an adaptive way prior to using the array for imaging.
- Published
- 1992
- Full Text
- View/download PDF
49. Phasing-up Multiple Aperture Laser Radar Receivers using Extended Soures
- Author
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S E Clark, L R Jones, and L F Desandre
- Abstract
Currently, there is substantial interest in using multiple apterture receiver arrays at laser wavelengths where lightweight structures and high angular resolution (tracking/imaging) are required. In order to achieve image resolution consistent with the overall size of the array, the amplitude and phase at each point in the array must be determined. Determination of the phase can be carried out either by performing heterodyne detection1,2 or by using direct detection combined with phase retrieval3 techniques. Since phase retrieval uses only the incident intensity, it does not suffer as does heterodyne detection from corruption of the incident phase due to errors in detector positioning and phase variations in the reference wavefront.
- Published
- 1991
- Full Text
- View/download PDF
50. List-strength effect: I. Data and discussion
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R, Ratcliff, S E, Clark, and R M, Shiffrin
- Subjects
Time Factors ,Memory ,Mental Recall ,Imagination ,Humans ,Cues ,Models, Psychological ,Serial Learning - Abstract
Extra items added to a list cause memory for the other items to decrease (the list-length effect). In one of the present studies we show that strengthening (or weakening) some items on a list harms (helps) free recall of the remaining list items. This is termed the list-strength effect. However, in seven recognition studies the list-strength effect was either absent or negative. This held whether strengthening was accomplished by extra study time or extra repetitions. The seven studies used various means to control rehearsal strategies, thereby providing evidence against the possibility that the findings were due to redistribution of rehearsal or effort from stronger to weaker items within a list. Current models appear unable to predict these results. We suggest that different retrieval operations underlie recall and recognition, as in the SAM model of Gillund and Shiffrin (1984), which can be made to fit the results with certain relatively minor modifications.
- Published
- 1990
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