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Neutron Star Extreme Matter Observatory: A kilohertz-band gravitational-wave detector in the global network
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- K. Ackley, V. B. Adya, P. Agrawal, P. Altin, G. Ashton, M. Bailes, E. Baltinas, A. Barbuio, D. Beniwal, C. Blair, D. Blair, G. N. Bolingbroke, V. Bossilkov, S. Shachar Boublil, D. D. Brown, B. J. Burridge, J. Calderon Bustillo, J. Cameron, H. Tuong Cao, J. B. Carlin, S. Chang, P. Charlton, C. Chatterjee, D. Chattopadhyay, X. Chen, J. Chi, J. Chow, Q. Chu, A. Ciobanu, T. Clarke, P. Clearwater, J. Cooke, D. Coward, H. Crisp, R. J. Dattatri, A. T. Deller, D. A. Dobie, L. Dunn, P. J. Easter, J. Eichholz, R. Evans, C. Flynn, G. Foran, P. Forsyth, Y. Gai, S. Galaudage, D. K. Galloway, B. Gendre, B. Goncharov, S. Goode, D. Gozzard, B. Grace, A. W. Graham, A. Heger, F. Hernandez Vivanco, R. Hirai, N. A. Holland, Z. J. Holmes, E. Howard, E. Howell, G. Howitt, M. T. Hübner, J. Hurley, C. Ingram, V. Jaberian Hamedan, K. Jenner, L. Ju, D. P. Kapasi, T. Kaur, N. Kijbunchoo, M. Kovalam, R. Kumar Choudhary, P. D. Lasky, M. Y. M. Lau, J. Leung, J. Liu, K. Loh, A. Mailvagan, I. Mandel, J. J. McCann, D. E. McClelland, K. McKenzie, D. McManus, T. McRae, A. Melatos, P. Meyers, H. Middleton, M. T. Miles, M. Millhouse, Y. Lun Mong, B. Mueller, J. Munch, J. Musiov, S. Muusse, R. S. Nathan, Y. Naveh, C. Neijssel, B. Neil, S. W. S. Ng, V. Oloworaran, D. J. Ottaway, M. Page, J. Pan, M. Pathak, E. Payne, J. Powell, J. Pritchard, E. Puckridge, A. Raidani, V. Rallabhandi, D. Reardon, J. A. Riley, L. Roberts, I. M. Romero-Shaw, T. J. Roocke, G. Rowell, N. Sahu, N. Sarin, L. Sarre, H. Sattari, M. Schiworski, S. M. Scott, R. Sengar, D. Shaddock, R. Shannon, J. SHI, P. Sibley, B. J. J. Slagmolen, T. Slaven-Blair, R. J. E. Smith, J. Spollard, L. Steed, L. Strang, H. Sun, A. Sunderland, S. Suvorova, C. Talbot, E. Thrane, D. Töyrä, P. Trahanas, A. Vajpeyi, J. V. van Heijningen, A. F. Vargas, P. J. Veitch, A. Vigna-Gomez, A. Wade, K. Walker, Z. Wang, R. L. Ward, K. Ward, S. Webb, L. Wen, K. Wette, R. Wilcox, J. Winterflood, C. Wolf, B. Wu, M. Jet Yap, Z. You, H. Yu, J. Zhang, J. Zhang, C. Zhao, X. Zhu
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- Journal:
- Publications of the Astronomical Society of Australia / Volume 37 / 2020
- Published online by Cambridge University Press:
- 05 November 2020, e047
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Gravitational waves from coalescing neutron stars encode information about nuclear matter at extreme densities, inaccessible by laboratory experiments. The late inspiral is influenced by the presence of tides, which depend on the neutron star equation of state. Neutron star mergers are expected to often produce rapidly rotating remnant neutron stars that emit gravitational waves. These will provide clues to the extremely hot post-merger environment. This signature of nuclear matter in gravitational waves contains most information in the 2–4 kHz frequency band, which is outside of the most sensitive band of current detectors. We present the design concept and science case for a Neutron Star Extreme Matter Observatory (NEMO): a gravitational-wave interferometer optimised to study nuclear physics with merging neutron stars. The concept uses high-circulating laser power, quantum squeezing, and a detector topology specifically designed to achieve the high-frequency sensitivity necessary to probe nuclear matter using gravitational waves. Above 1 kHz, the proposed strain sensitivity is comparable to full third-generation detectors at a fraction of the cost. Such sensitivity changes expected event rates for detection of post-merger remnants from approximately one per few decades with two A+ detectors to a few per year and potentially allow for the first gravitational-wave observations of supernovae, isolated neutron stars, and other exotica.
15 - Laser-induced breakdown spectroscopy using sequential laser pulses
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- By Jack Pender, Department of Chemistry and Biochemistry, The University of South Carolina, USA, Bill Pearman, Department of Chemistry and Biochemistry, The University of South Carolina, USA, Jon Scaffidi, Department of Chemistry and Biochemistry, The University of South Carolina, USA, Scott R. Goode, Department of Chemistry and Biochemistry, The University of South Carolina, USA, S. Michael Angel, Department of Chemistry and Biochemistry, The University of South Carolina, USA
- Edited by Andrzej W. Miziolek, Vincenzo Palleschi, Israel Schechter, Technion - Israel Institute of Technology, Haifa
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- Book:
- Laser Induced Breakdown Spectroscopy
- Published online:
- 08 August 2009
- Print publication:
- 07 September 2006, pp 516-538
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Summary
Introduction
In laser-induced breakdown spectroscopy (LIBS), first reported by Brech and Cross in 1962 [1], a laser is used to ablate and atomize material from a sample and to form a plasma. Emission from the plasma is used to identify and quantify elements within the sample. The ability to form a plasma on unprepared samples makes LIBS an amazingly versatile analytical technique. It is one of the few techniques that can be used for non-contact elemental analysis, making LIBS uniquely suited to measurements of hazardous materials and materials in difficult-to-reach locations [2–16]. The sampling is virtually non-destructive, making LIBS useful for such unique applications as the analysis of priceless works of art and archeological relics [17–21]. Other applications that benefit from the unique advantages of LIBS include environmental [22–28], industrial [2–4, 23, 24, 29–36], geological [22, 25–27], planetary [22], art [28–42], medical [43, 44], and dental [45] measurements. Recently, many researchers have coupled LIBS with other techniques such as ICP-MS[12, 41, 42, 46–48].
Despite the increasing popularity of LIBS, the sensitivity and precision of the technique are relatively poor compared with other forms of atomic spectroscopy and there are significant matrix effects and relatively high background signals [49]. There are also many fundamental studies aimed at improving the sensitivity and precision of LIBS[34, 50–54]. These studies have led to investigations of multiple-pulse LIBS, which can give greatly enhanced emission signals and improved signal to background ratio [55–58].