Not Available <P />
\n| 2018Wthr...73Q..35. | \nBook reviews | \n\n | Weather, vol. 73, issue 1, pp. 35-35 | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018Wthr...73Q..35. | \n
| 2018TDM.....5a0201F | \n2D Materials: maintaining editorial quality | \nFal\'ko, Vladimir; Thomas, Ceri-Wyn | \n2D Materials, Volume 5, Issue 1, article id. 010201 (2018). | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018TDM.....5a0201F | \n
| 2018Spin....877001P | \nObituary: In Memoriam Professor Dr. Shoucheng Zhang, Consulting Editor | \nParkin, Stuart; Chantrell, Roy; Chang, Ching-Ray | \nSpin, Volume 8, Issue 4, id. 1877001 | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018Spin....877001P | \n
| 2018SAAS...38.....D | \nMillimeter Astronomy | \nDessauges-Zavadsky, Miroslava; Pfenniger, Daniel | \nMillimeter Astronomy: Saas-Fee Advanced Course 38. Swiss Society for Astrophysics and Astronomy, Saas-Fee Advanced Course, Volume 38. ISBN 978-3-662-57545-1. Springer-Verlag GmbH Germany, part of Springer Nature, 2018 | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018SAAS...38.....D | \n
| 2018PhRvL.120b9901P | \nErratum: Quantum Criticality in Resonant Andreev Conduction [Phys. Rev. Lett. 119, 116802 (2017)] | \nPustilnik, M.; van Heck, B.; Lutchyn, R. M.; Glazman, L. I. | \nPhysical Review Letters, Volume 120, Issue 2, id.029901 | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018PhRvL.120b9901P | \n
| 2017PhDT........14C | \nResolving Gas-Phase Metallicity In Galaxies | \nCarton, David | \nPhD Thesis, Leiden University, 2017 | \n2017-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017PhDT........14C | \n
| 2017nova.pres.2388K | \nA 3D View of a Supernova Remnant | \nKohler, Susanna | \nAAS Nova Highlight, 14 Jun 2017, id.2388 | \n2017-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017nova.pres.2388K | \n
| 2017CBET.4403....2G | \nPotential New Meteor Shower from Comet C/2015 D4 (Borisov) | \nGreen, D. W. E. | \nCentral Bureau Electronic Telegrams, 4403, 2 (2017). Edited by Green, D. W. E. | \n2017-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017CBET.4403....2G | \n
| 2017ascl.soft06009C | \nsick: Spectroscopic inference crank | \nCasey, Andrew R. | \nAstrophysics Source Code Library, record ascl:1706.009 | \n2017-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017ascl.soft06009C | \n
| 2017yCat.113380453S | \nVizieR Online Data Catalog: BM CVn V-band differential light curve (Siltala+, 2017) | \nSiltala, J.; Jetsu, L.; Hackman, T.; Henry, G. W.; Immonen, L.; Kajatkari, P.; Lankinen, J.; Lehtinen, J.; Monira, S.; Nikbakhsh, S.; Viitanen, A.; Viuho, J.; Willamo, T. | \nVizieR On-line Data Catalog: J/AN/338/453. Originally published in: 2017AN....338..453S | \n2017-05-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017yCat.113380453S | \n
| 2017AAVSN.429....1W | \nV694 Mon (MWC 560) spectroscopy requested | \nWaagen, Elizabeth O. | \nAAVSO Special Notice #429 | \n2017-05-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017AAVSN.429....1W | \n
| 2017sptz.prop13168Y | \nConfirm the Nature of a TDE Candidate in ULIRG F01004-2237 Using Spitzer mid-IR Light Curves | \nYan, Lin | \nSpitzer Proposal ID 13168 | \n2017-04-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017sptz.prop13168Y | \n
| 2017MsT..........2A | \nSurface Accuracy and Pointing Error Prediction of a 32 m Diameter Class Radio Astronomy Telescope | \nAzankpo, Severin | \nMasters thesis, University of Stellenbosch, March 2017, 120 pages | \n2017-03-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017MsT..........2A | \n
| 2016emo6.rept.....R | \nThe penumbral Moon\'s eclipse form 16 september 2016 | \nRotaru, Adrian; Pteancu, Mircea; Zaharia, Cristian | \nhttp://www.astronomy.ro/forum/viewtopic.php?p=159287#159287 (Comments in Romanian) | \n2016-10-1 | \nhttps://ui.adsabs.harvard.edu/abs/2016emo6.rept.....R | \n
| 2016iac..talk..872V | \nLiving on the edge: Adaptive Optics+Lucky Imaging | \nVelasco, Sergio | \nIAC Talks, Astronomy and Astrophysics Seminars from the Instituto de Astrofísica de Canarias, 872 | \n2016-03-1 | \nhttps://ui.adsabs.harvard.edu/abs/2016iac..talk..872V | \n
| 2009bcet.book...65L | \nThe Diversity of Nuclear Magnetic Resonance Spectroscopy | \nLiu, Corey W.; Alekseyev, Viktor Y.; Allwardt, Jeffrey R.; Bankovich, Alexander J.; Cade-Menun, Barbara J.; Davis, Ronald W.; Du, Lin-Shu; Garcia, K. Christopher; Herschlag, Daniel; Khosla, Chaitan; Kraut, Daniel A.; Li, Qing; Null, Brian; Puglisi, Joseph D.; Sigala, Paul A.; Stebbins, Jonathan F.; Varani, Luca | \nBiophysics and the Challenges of Emerging Threats, NATO Science for Peace and Security Series B: Physics and Biophysics. ISBN 978-90-481-2367-4. Springer Netherlands, 2009, p. 65 | \n2009-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2009bcet.book...65L | \n
| 2007AAS...210.2104M | \nTime Domain Exploration with the Palomar-QUEST Sky Survey | \nMahabal, Ashish A.; Drake, A. J.; Djorgovski, S. G.; Donalek, C.; Glikman, E.; Graham, M. J.; Williams, R.; Baltay, C.; Rabinowitz, D.; PQ Team Caltech; Yale; NCSA; Indiana; , . . . | \nAmerican Astronomical Society Meeting 210, id.21.04 | \n2007-05-1 | \nhttps://ui.adsabs.harvard.edu/abs/2007AAS...210.2104M | \n
| 2007RJPh....1...35. | \nAnalysis of Thermal Losses in the Flat-Plate Collector of a Thermosyphon Solar Water Heater | \n., S. N. Agbo; ., E. C. Okoroigwe | \nResearch Journal of Physics, vol. 1, issue 1, pp. 35-41 | \n2007-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2007RJPh....1...35. | \n
| 1995ans..agar..390M | \nSpacecraft navigation requirements | \nMiller, Judy L. | \nIn AGARD, Aerospace Navigation Systems p 390-405 (SEE N96-13404 02-04) | \n1995-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/1995ans..agar..390M | \n
| 1995anda.book.....N | \nApplied nonlinear dynamics: analytical, computational and experimental methods | \nNayfeh, Ali H.; Balachandran, Balakumar | \nWiley series in nonlinear science, New York; Chichester: Wiley, |c1995 | \n1995-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/1995anda.book.....N | \n
| 1991hep.th....8028G | \nApplied Conformal Field Theory | \nGinsparg, Paul | \neprint arXiv:hep-th/9108028 | \n1988-11-1 | \nhttps://ui.adsabs.harvard.edu/abs/1991hep.th....8028G | \n
| 1983aiaa.meetY....K | \nAutonomous navigation using lunar beacons | \nKhatib, A. R.; Ellis, J.; French, J.; Null, G.; Yunck, T.; Wu, S. | \nAmerican Institute of Aeronautics and Astronautics, Aerospace Sciences Meeting, 21st, Reno, NV, Jan. 10-13, 1983. 7 p. | \n1983-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/1983aiaa.meetY....K | \n
| 2012ddsw.rept.....T | \nDaymet: Daily surface weather on a 1 km grid for North America, 1980-2008 | \nThornton, P. E.; Thornton, M. M.; Mayer, B. W.; Wilhelmi, N.; Wei, Y.; Devarakonda, R.; Cook, R. | \nOak Ridge National Laboratory (ORNL) Distributed Active Archive Center for Biogeochemical Dynamics (DAAC) | \n2012-04-1 | \nhttps://ui.adsabs.harvard.edu/abs/2012ddsw.rept.....T | \n
| 2018Wthr...73Q..35. | \nBook reviews | \n\n | Weather, vol. 73, issue 1, pp. 35-35 | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018Wthr...73Q..35. | \n
| 2018TDM.....5a0201F | \n2D Materials: maintaining editorial quality | \nFal\'ko, Vladimir; Thomas, Ceri-Wyn | \n2D Materials, Volume 5, Issue 1, article id. 010201 (2018). | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018TDM.....5a0201F | \n
| 2018Spin....877001P | \nObituary: In Memoriam Professor Dr. Shoucheng Zhang, Consulting Editor | \nParkin, Stuart; Chantrell, Roy; Chang, Ching-Ray | \nSpin, Volume 8, Issue 4, id. 1877001 | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018Spin....877001P | \n
| 2018SAAS...38.....D | \nMillimeter Astronomy | \nDessauges-Zavadsky, Miroslava; Pfenniger, Daniel | \nMillimeter Astronomy: Saas-Fee Advanced Course 38. Swiss Society for Astrophysics and Astronomy, Saas-Fee Advanced Course, Volume 38. ISBN 978-3-662-57545-1. Springer-Verlag GmbH Germany, part of Springer Nature, 2018 | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018SAAS...38.....D | \n
| 2018PhRvL.120b9901P | \nErratum: Quantum Criticality in Resonant Andreev Conduction [Phys. Rev. Lett. 119, 116802 (2017)] | \nPustilnik, M.; van Heck, B.; Lutchyn, R. M.; Glazman, L. I. | \nPhysical Review Letters, Volume 120, Issue 2, id.029901 | \n2018-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2018PhRvL.120b9901P | \n
| 2017PhDT........14C | \nResolving Gas-Phase Metallicity In Galaxies | \nCarton, David | \nPhD Thesis, Leiden University, 2017 | \n2017-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017PhDT........14C | \n
| 2017nova.pres.2388K | \nA 3D View of a Supernova Remnant | \nKohler, Susanna | \nAAS Nova Highlight, 14 Jun 2017, id.2388 | \n2017-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017nova.pres.2388K | \n
| 2017CBET.4403....2G | \nPotential New Meteor Shower from Comet C/2015 D4 (Borisov) | \nGreen, D. W. E. | \nCentral Bureau Electronic Telegrams, 4403, 2 (2017). Edited by Green, D. W. E. | \n2017-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017CBET.4403....2G | \n
| 2017ascl.soft06009C | \nsick: Spectroscopic inference crank | \nCasey, Andrew R. | \nAstrophysics Source Code Library, record ascl:1706.009 | \n2017-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017ascl.soft06009C | \n
| 2017yCat.113380453S | \nVizieR Online Data Catalog: BM CVn V-band differential light curve (Siltala+, 2017) | \nSiltala, J.; Jetsu, L.; Hackman, T.; Henry, G. W.; Immonen, L.; Kajatkari, P.; Lankinen, J.; Lehtinen, J.; Monira, S.; Nikbakhsh, S.; Viitanen, A.; Viuho, J.; Willamo, T. | \nVizieR On-line Data Catalog: J/AN/338/453. Originally published in: 2017AN....338..453S | \n2017-05-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017yCat.113380453S | \n
| 2017AAVSN.429....1W | \nV694 Mon (MWC 560) spectroscopy requested | \nWaagen, Elizabeth O. | \nAAVSO Special Notice #429 | \n2017-05-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017AAVSN.429....1W | \n
| 2017sptz.prop13168Y | \nConfirm the Nature of a TDE Candidate in ULIRG F01004-2237 Using Spitzer mid-IR Light Curves | \nYan, Lin | \nSpitzer Proposal ID 13168 | \n2017-04-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017sptz.prop13168Y | \n
| 2017MsT..........2A | \nSurface Accuracy and Pointing Error Prediction of a 32 m Diameter Class Radio Astronomy Telescope | \nAzankpo, Severin | \nMasters thesis, University of Stellenbosch, March 2017, 120 pages | \n2017-03-1 | \nhttps://ui.adsabs.harvard.edu/abs/2017MsT..........2A | \n
| 2016emo6.rept.....R | \nThe penumbral Moon\'s eclipse form 16 september 2016 | \nRotaru, Adrian; Pteancu, Mircea; Zaharia, Cristian | \nhttp://www.astronomy.ro/forum/viewtopic.php?p=159287#159287 (Comments in Romanian) | \n2016-10-1 | \nhttps://ui.adsabs.harvard.edu/abs/2016emo6.rept.....R | \n
| 2016iac..talk..872V | \nLiving on the edge: Adaptive Optics+Lucky Imaging | \nVelasco, Sergio | \nIAC Talks, Astronomy and Astrophysics Seminars from the Instituto de Astrofísica de Canarias, 872 | \n2016-03-1 | \nhttps://ui.adsabs.harvard.edu/abs/2016iac..talk..872V | \n
| 2009bcet.book...65L | \nThe Diversity of Nuclear Magnetic Resonance Spectroscopy | \nLiu, Corey W.; Alekseyev, Viktor Y.; Allwardt, Jeffrey R.; Bankovich, Alexander J.; Cade-Menun, Barbara J.; Davis, Ronald W.; Du, Lin-Shu; Garcia, K. Christopher; Herschlag, Daniel; Khosla, Chaitan; Kraut, Daniel A.; Li, Qing; Null, Brian; Puglisi, Joseph D.; Sigala, Paul A.; Stebbins, Jonathan F.; Varani, Luca | \nBiophysics and the Challenges of Emerging Threats, NATO Science for Peace and Security Series B: Physics and Biophysics. ISBN 978-90-481-2367-4. Springer Netherlands, 2009, p. 65 | \n2009-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2009bcet.book...65L | \n
| 2007AAS...210.2104M | \nTime Domain Exploration with the Palomar-QUEST Sky Survey | \nMahabal, Ashish A.; Drake, A. J.; Djorgovski, S. G.; Donalek, C.; Glikman, E.; Graham, M. J.; Williams, R.; Baltay, C.; Rabinowitz, D.; PQ Team Caltech; Yale; NCSA; Indiana; , . . . | \nAmerican Astronomical Society Meeting 210, id.21.04 | \n2007-05-1 | \nhttps://ui.adsabs.harvard.edu/abs/2007AAS...210.2104M | \n
| 2007RJPh....1...35. | \nAnalysis of Thermal Losses in the Flat-Plate Collector of a Thermosyphon Solar Water Heater | \n., S. N. Agbo; ., E. C. Okoroigwe | \nResearch Journal of Physics, vol. 1, issue 1, pp. 35-41 | \n2007-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/2007RJPh....1...35. | \n
| 1995ans..agar..390M | \nSpacecraft navigation requirements | \nMiller, Judy L. | \nIn AGARD, Aerospace Navigation Systems p 390-405 (SEE N96-13404 02-04) | \n1995-06-1 | \nhttps://ui.adsabs.harvard.edu/abs/1995ans..agar..390M | \n
| 1995anda.book.....N | \nApplied nonlinear dynamics: analytical, computational and experimental methods | \nNayfeh, Ali H.; Balachandran, Balakumar | \nWiley series in nonlinear science, New York; Chichester: Wiley, |c1995 | \n1995-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/1995anda.book.....N | \n
| 1991hep.th....8028G | \nApplied Conformal Field Theory | \nGinsparg, Paul | \neprint arXiv:hep-th/9108028 | \n1988-11-1 | \nhttps://ui.adsabs.harvard.edu/abs/1991hep.th....8028G | \n
| 1983aiaa.meetY....K | \nAutonomous navigation using lunar beacons | \nKhatib, A. R.; Ellis, J.; French, J.; Null, G.; Yunck, T.; Wu, S. | \nAmerican Institute of Aeronautics and Astronautics, Aerospace Sciences Meeting, 21st, Reno, NV, Jan. 10-13, 1983. 7 p. | \n1983-01-1 | \nhttps://ui.adsabs.harvard.edu/abs/1983aiaa.meetY....K | \n
| 2012ddsw.rept.....T | \nDaymet: Daily surface weather on a 1 km grid for North America, 1980-2008 | \nThornton, P. E.; Thornton, M. M.; Mayer, B. W.; Wilhelmi, N.; Wei, Y.; Devarakonda, R.; Cook, R. | \nOak Ridge National Laboratory (ORNL) Distributed Active Archive Center for Biogeochemical Dynamics (DAAC) | \n2012-04-1 | \nhttps://ui.adsabs.harvard.edu/abs/2012ddsw.rept.....T | \n
| 2020EPJC...80...96D | \nGeneralized Lomb–Scargle analysis of 36Cl decay rate measurements at PTB and BNL | \nDhaygude, Akanksha; Desai, Shantanu | \nThe European Physical Journal C, Volume 80, Issue 2, article id.96 | \n2020-02-1 | \nhttps://ui.adsabs.harvard.edu/abs/2020EPJC...80...96D | \n
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\nChapter 2: As part of the Bluedisk survey we analyse the radial gas-phase metallicity profiles of 50 late-type galaxies. We compare the metallicity profiles of a sample of HI-rich galaxies against a control sample of HI-\'normal\' galaxies. We find the metallicity gradient of a galaxy to be strongly correlated with its HI mass fraction {M}{HI}) / {M}_{\\ast}). We note that some galaxies exhibit a steeper metallicity profile in the outer disc than in the inner disc. These galaxies are found in both the HI-rich and control samples. This contradicts a previous indication that these outer drops are exclusive to HI-rich galaxies. These effects are not driven by bars, although we do find some indication that barred galaxies have flatter metallicity profiles. By applying a simple analytical model we are able to account for the variety of metallicity profiles that the two samples present. The success of this model implies that the metallicity in these isolated galaxies may be in a local equilibrium, regulated by star formation. This insight could provide an explanation of the observed local mass-metallicity relation. <P />Chapter 3 We present a method to recover the gas-phase metallicity gradients from integral field spectroscopic (IFS) observations of barely resolved galaxies. We take a forward modelling approach and compare our models to the observed spatial distribution of emission line fluxes, accounting for the degrading effects of seeing and spatial binning. The method is flexible and is not limited to particular emission lines or instruments. We test the model through comparison to synthetic observations and use downgraded observations of nearby galaxies to validate this work. As a proof of concept we also apply the model to real IFS observations of high-redshift galaxies. From our testing we show that the inferred metallicity gradients and central metallicities are fairly insensitive to the assumptions made in the model and that they are reliably recovered for galaxies with sizes approximately equal to the half width at half maximum of the point-spread function. However, we also find that the presence of star forming clumps can significantly complicate the interpretation of metallicity gradients in moderately resolved high-redshift galaxies. Therefore we emphasize that care should be taken when comparing nearby well-resolved observations to high-redshift observations of partially resolved galaxies. <P />Chapter 4 We present gas-phase metallicity gradients for 94 star-forming galaxies between (0.08 < z < 0.84). We find a negative median metallicity gradient of (-0.043^{+0.009}_{-0.007}, dex/kpc)/span>, i.e. on average we find the centres of these galaxies to be more metal-rich than their outskirts. However, there is significant scatter underlying this and we find that 10% (9) galaxies have significantly positive metallicity gradients, 39% (37) have significantly negative gradients, 28% (26) have gradients consistent with being flat, the remainder 23% (22) are considered to have unreliable gradient estimates. We find a slight trend for a more negative metallicity gradient with both increasing stellar mass and increasing star formation rate (SFR). However, given the potential redshift and size selection effects, we do not consider these trends to be significant. Indeed when we normalize the SFR of our galaxies relative to the main sequence, we do not observe any trend between the metallicity gradient and the normalized SFR. This finding is contrary to other recent studies of galaxies at similar and higher redshifts. We do, however, identify a novel trend between the metallicity gradient of a galaxy and its size. Small galaxies ((r_d < 3 kpc)) present a large spread in observed metallicity gradients (both negative and positive gradients). In contrast, we find no large galaxies (r_d > 3 kpc) with positive metallicity gradients, and overall there is less scatter in the metallicity gradient amongst the large galaxies. We suggest that these large (well-evolved) galaxies may be analogues of galaxies in the present-day Universe, which also present a common negative metallicity gradient. <P />Chapter 5 The relationship between a galaxy\'s stellar mass and its gas-phase metallicity results from the complex interplay between star formation and the inflow and outflow of gas. Since the gradient of metals in galaxies is also influenced by the same processes, it is therefore natural to contrast the metallicity gradient with the mass-metallicity relation. Here we study the interrelation of the stellar mass, central metallicity and metallicity gradient, using a sample of 72 galaxies spanning (0.13 < z < 0.84) with reliable metallicity gradient estimates. We find that typically the galaxies that fall below the mean mass-metallicity relation have flat or inverted metallicity gradients. We quantify their relationship taking full account of the covariance between the different variables and find that at fixed mass the central metallicity is anti-correlated with the metallicity gradient. We argue that this is consistent with a scenario that suppresses the central metallicity either through the inflow of metal poor gas or outflow of metal enriched gas. <P />
\nThe outlined regions mark the 57 knots in Tycho selected by the authors for velocity measurements. Magenta regions have redshifted line-of-sight velocities (moving away from us); cyan regions have blueshifted light-of-sight velocities (moving toward us). [Williams et al. 2017]The Tycho supernova remnant was first observed in the year 1572. Nearly 450 years later, astronomers have now used X-ray observations of Tycho to build the first-ever 3D map of a Type Ia supernova remnant.Signs of ExplosionsSupernova remnants are spectacular structures formed by the ejecta of stellar explosions as they expand outwards into the surrounding interstellar medium.One peculiarity of these remnants is that they often exhibit asymmetries in their appearance and motion. Is this because the ejecta are expanding into a nonuniform interstellar medium? Or was the explosion itself asymmetric? The best way we can explore this question is with detailed observations of the remnants.Histograms of the velocity in distribution of the knots in the X (green), Y (blue) and Z (red) directions (+Z is away from the observer). They show no evidence for asymmetric expansion of the knots. [Williams et al. 2017]Enter TychoTo this end, a team of scientists led by Brian Williams (Space Telescope Science Institute and NASA Goddard SFC) has worked to map out the 3D velocities of the ejecta in the Tycho supernova remnant. Tycho is a Type Ia supernova thought to be caused by the thermonuclear explosion of a white dwarf in a binary system that was destabilized by mass transfer from its companion.After 450 years of expansion, the remnant now has the morphological appearance of a roughly circular cloud of clumpy ejecta. The forward shock wave from the supernova, however, is known to have twice the velocity on one side of the shell as on the other.To better understand this asymmetry, Williams and collaborators selected a total of 57 knots in Tychos ejecta, spread out around the remnant. They then used 12 years of Chandra X-ray observations to measure both the knots proper motion in the plane of the sky and their line-of-sight velocity. These two measurements were then combined to build a full 3D map of the motion of the ejecta.3D hydrodynamical simulations of Tycho, stopped at the current epoch. These show that both initially smooth (top) and initially clumpy (bottom) ejecta models are consistent with the current observations of the morphology and dynamics of Tychos ejecta. [Adapted from Williams et al. 2017]Symmetry and ClumpsWilliams and collaborators found that the knots have total velocities that range from 2400 to 6600 km/s. Unlike the forward shock of the supernova, Tychos ejecta display no asymmetries in their motion which suggests that the explosion itself was symmetric. The more likely explanation is a density gradient in the interstellar medium, which could slow the shock wave on one side of the remnant without yet affecting the motion of the clumps of ejecta.As a final exploration, the authors attempt to address the origin of Tychos clumpiness. The fact that some of Tychos ejecta knots precede its outer edge has raised the question of whether the ejecta started out clumpy, or if they began smooth and only clumped during expansion. Williams and collaborators matched the morphological and dynamical data to simulations, demonstrating that neither scenario can be ruled out at this time.This first 3D map of a Type Ia supernova represents an important step in our ability to understand these stellar explosions. The authors suggest that well be able to expand on this map in the future with additional observations from Chandra, as well as with new data from future X-ray observatories that will be able to detect fainter emission.CitationBrian J. Williams et al 2017 ApJ 842 28. doi:10.3847/1538-4357/aa7384 <P />
\nA previous good encounter occurred on 2006 July 29d04h11m UT (r - Delta = +0.0003 AU, solar long. = 125.841 deg). Future encounters are predicted on 2029 July 29d01h53m (+0.0007 AU, 125.816 deg), 2042 July 29d10h48m (+0.0006 AU, 125.886 deg), 2053 July 29d05h35m (+0.0001 AU, 125.848 deg), and on 2068 July 29d02h09m UT (-0.0001 AU, 125.863 deg). <P />
\nsick infers astrophysical parameters from noisy observed spectra. Phenomena that can alter the data (e.g., redshift, continuum, instrumental broadening, outlier pixels) are modeled and simultaneously inferred with the astrophysical parameters of interest. This package relies on emcee (ascl:1303.002); it is best suited for situations where a grid of model spectra already exists, and one would like to infer model parameters given some data. <P />
\nThe included files present the numerical data of our analysis of the BM CVn photometry. The data consists of differential Johnson V-band photometry using the star HD 116010 as the comparison star. <P />The analysis has been performed using the previously published continuous period search (CPS) method, described in detail in Lehtinen et al., 2011A&A...527A.136L, Cat. J/A+A/527/A136. <P />(4 data files). <P />
\nThe observing campaign from 2016 on V694 Mon (MWC 560) (AAVSO Alert Notice 538) has been continued, but with different requirements. Photometry is no longer specifically requested on a regular basis (although ongoing observations that do not interfere with other obligations are welcome). Spectroscopy on a cadence of a week or two is requested to monitor changes in the disk outflow. Investigator Adrian Lucy writes: "Adrian Lucy and Dr. Jeno Sokoloski (Columbia University) have requested spectroscopic monitoring of the broad-absorption-line symbiotic star V694 Mon (MWC 560), as a follow-up to coordinated multi-wavelength observations obtained during its recent outburst (ATel #8653, #8832, #8957; #10281). This system is a perfect place in which to study the relationship between an accretion disk and disk winds/jets, and a high-value target for which even low-resolution spectra can be extraordinarily useful...Optical brightening in MWC 560 tends to predict higher-velocity absorption, but sometimes jumps in absorption velocity also appear during optical quiescence (e.g., Iijima 2001, ASPCS, 242, 187). If such a velocity jump occurs during photometric quiescence, it may prompt radio observations to confirm and test the proposed outflow origin for recently-discovered flat-spectrum radio emission (Lucy et al. ATel #10281)...Furthermore, volunteer spectroscopic monitoring of this system has proved useful in unpredictable ways. For example, \'amateur\' spectra obtained by Somogyi Péter in 2015 December demonstrated that the velocity of absorption was very low only a month before an optical outburst peak prompted absorption troughs up to 3000 km/s, which constrains very well the timing of the changes to the outflow to a degree that would not have been otherwise possible. Any resolution can be useful. A wavelength range that can accommodate a blueshift of at least 140 angstroms (6000 km/s) from the rest wavelengths of H-alpha at 6562 angstroms and/or H-beta at 4861 angstroms is ideal, though spectra with a smaller range can still be useful. Photometry could potentially still be useful, but will be supplementary to medium-cadence photometry being collected by the ANS collaboration." "Spectroscopy may be uploaded to the ARAS database (http://www.astrosurf.com/aras/Aras_DataBase/DataBase.htm), or sent to Adrian and Jeno directly at <lucy@astro.columbia.edu>. Finder charts with sequence may be created using the AAVSO Variable Star Plotter (https://www.aavso.org/vsp). Photometry should be submitted to the AAVSO International Database. See full Special Notice for more details. <P />
\nULIRG F01004-2237 had a strong optical flare, peaked in 2010, and the follow-up optical spectra classified this event as a TDE candidate (Tadhunter et al. 2017, Nature Astronomy). In early 2017, using archival WISE data, we discovered that its 3.4 and 4.6um fluxes have been steadily rising since 2013, increased by a factor of 3.5 and 2.6 respectively. The last epoch data from WISE on 2016-12-12 shows that F01004-2237 has reached 7.5 and 14mJy at 3.4 and 4.6um. We interpret the mid-IR LCs as infrared echoes from the earlier optical flare. We infer a convex, dust ring with a radius of 1 pc from the central heating source. Our model predicts that if this event is indeed a TDE, its mid-IR LCs should start to fade in next 5-12 months because it has already reprocessed most of the UV/optical energy from the tidal disruption. However, if this event is due to activities from an AGN, its mid-IR LCs could last over a much longer time scale. We request a total of 3.2 hours of Spitzer time to monitor the mid-IR variations in next 12 months. This will provide the critical data to confirm the nature of this transient event. <P />
\nThe African Very-long-baseline interferometry Network (AVN) is a joint project between South Africa and eight partner African countries aimed at establishing a VLBI (Very-Long-Baseline Interferometry) capable network of radio telescopes across the African continent. An existing structure that is earmarked for this project, is a 32 m diameter antenna located in Ghana that has become obsolete due to advances in telecommunication. The first phase of the conversion of this Ghana antenna into a radio astronomy telescope is to upgrade the antenna to observe at 5 GHz to 6.7 GHz frequency and then later to 18 GHz within a required performing tolerance. The surface and pointing accuracies for a radio telescope are much more stringent than that of a telecommunication antenna. The mechanical pointing accuracy of such telescopes is influenced by factors such as mechanical alignment, structural deformation, and servo drive train errors. The current research investigates the numerical simulation of the surface and pointing accuracies of the Ghana 32 m diameter radio astronomy telescope due to its structural deformation mainly influenced by gravity, wind and thermal loads. <P />
\nThe web page represents circumstances and photographs from the Moon\'s partial/penumbral eclipse from 16 September 2016 obtained from few various places in Romania (East Europe). A part of photographs give the maximum phase of the Eclipse, while another give the reddened Moon. <P />
\nNot Available <P />
\nThe discovery of the physical phenomenon of Nuclear Magnetic Resonance (NMR) in 1946 gave rise to the spectroscopic technique that has become a remarkably versatile research tool. One could oversimplify NMR spectros-copy by categorizing it into the two broad applications of structure elucidation of molecules (associated with chemistry and biology) and imaging (associated with medicine). But, this certainly does not do NMR spectroscopy justice in demonstrating its general acceptance and utilization across the sciences. This manuscript is not an effort to present an exhaustive, or even partial review of NMR spectroscopy applications, but rather to provide a glimpse at the wide-ranging uses of NMR spectroscopy found within the confines of a single magnetic resonance research facility, the Stanford Magnetic Resonance Laboratory. Included here are summaries of projects involving protein structure determination, mapping of intermolecular interactions, exploring fundamental biological mechanisms, following compound cycling in the environmental, analysis of synthetic solid compounds, and microimaging of a model organism. <P />
\nPalomar-QUEST (PQ) synoptic sky survey has now been routinely processing data from driftscans in real-time. As four photometric bandpasses are utilized in nearly simultaneously, PQ is well suited to search for transient and highly variable objects. Using a series of software filters i.e. programs to select/deselect objects based on certain criteria we shorten the list of candidates from the initially flagged candidate transients. Such filters include looking for known asteroids, known variables, as well as moving, but previously uncatalogued objects based on their motion within a scan as well as between successive scans. Some software filters also deal with instrumental artifacts, edge effects, and use clustering of spurious detections around bright stars. During a typical night when we cover about 500 sq. degrees, we detect hundreds of asteroids, the primary contaminants in the search for astrophysical transients beyond our solar system. <P />Here we describe some statistics based on the software filters we employ and the nature of the objects that seem to survive the process. We also discuss the usefulness of this to amateur astronomers, projects like VOEventNet, and other synoptic sky surveys. <P />We also present an outline of the work we have started on quantifying the variability of quasars, blazars, as well as various classes of Galactic sources, by combining the large number of PQ scans with other existing data sources federated in the Virtual Observatory environment. <P />The PQ survey is partially supported by the U.S. National Science Foundation (NSF). <P />
\nNot Available <P />
\nSpacecraft operation depends upon knowledge of vehicular position and, consequently, navigational support has been required for all such systems. Technical requirements for different mission trajectories and orbits are addressed with consideration given to the various tradeoffs which may need to be considered. The broad spectrum of spacecraft are considered with emphasis upon those of greater military significance (i.e., near earth orbiting satellites). Technical requirements include, but are not limited to, accuracy; physical characteristics such as weight and volume; support requirements such as electrical power and ground support; and system integrity. Generic navigation suites for spacecraft applications are described. It is shown that operational spacecraft rely primarily upon ground-based tracking and computational centers with little or no navigational function allocated to the vehicle, while technology development efforts have been and continue to be directed primarily toward onboard navigation suites. The military significance of onboard navigators is shown to both improve spacecraft survivability and performance (accuracy). <P />
\nNot Available <P />
\nThese lectures consisted of an elementary introduction to conformal field theory, with some applications to statistical mechanical systems, and fewer to string theory. Contents: 1. Conformal theories in d dimensions 2. Conformal theories in 2 dimensions 3. The central charge and the Virasoro algebra 4. Kac determinant and unitarity 5. Identication of m = 3 with the critical Ising model 6. Free bosons and fermions 7. Free fermions on a torus 8. Free bosons on a torus 9. Affine Kac-Moody algebras and coset constructions 10. Advanced applications <P />
\nThe concept of using lunar beacon signal transmission for on-board navigation for earth satellites and near-earth spacecraft is described. The system would require powerful transmitters on the earth-side of the moon\'s surface and black box receivers with antennae and microprocessors placed on board spacecraft for autonomous navigation. Spacecraft navigation requires three position and three velocity elements to establish location coordinates. Two beacons could be soft-landed on the lunar surface at the limits of allowable separation and each would transmit a wide-beam signal with cones reaching GEO heights and be strong enough to be received by small antennae in near-earth orbit. The black box processor would perform on-board computation with one-way Doppler/range data and dynamical models. Alternatively, GEO satellites such as the GPS or TDRSS spacecraft can be used with interferometric techniques to provide decimeter-level accuracy for aircraft navigation. <P />
\nArchived and distributed through the ORNL DAAC, the Daymet data set provides gridded estimates of daily weather parameters for North America, including daily continuous surfaces of minimum and maximum temperature, precipitation occurrence and amount, humidity, shortwave radiation, snow water equivalent, and day length. The daily time step, 1 km x 1 km spatial resolution, and North American spatial extent of the data set makes it a unique and valuable contribution to scientific, research, and educational communities. The literature shows that Daymet data have been broadly applied to fields including hydrology, terrestrial vegetation growth models, carbon cycle science, and regional to large scale climate change analysis.
\nNot Available <P />
\nNot Available <P />
\nNot Available <P />
\nNot Available <P />
\nNot Available <P />
\nChapter 2: As part of the Bluedisk survey we analyse the radial gas-phase metallicity profiles of 50 late-type galaxies. We compare the metallicity profiles of a sample of HI-rich galaxies against a control sample of HI-\'normal\' galaxies. We find the metallicity gradient of a galaxy to be strongly correlated with its HI mass fraction {M}{HI}) / {M}_{\\ast}). We note that some galaxies exhibit a steeper metallicity profile in the outer disc than in the inner disc. These galaxies are found in both the HI-rich and control samples. This contradicts a previous indication that these outer drops are exclusive to HI-rich galaxies. These effects are not driven by bars, although we do find some indication that barred galaxies have flatter metallicity profiles. By applying a simple analytical model we are able to account for the variety of metallicity profiles that the two samples present. The success of this model implies that the metallicity in these isolated galaxies may be in a local equilibrium, regulated by star formation. This insight could provide an explanation of the observed local mass-metallicity relation. <P />Chapter 3 We present a method to recover the gas-phase metallicity gradients from integral field spectroscopic (IFS) observations of barely resolved galaxies. We take a forward modelling approach and compare our models to the observed spatial distribution of emission line fluxes, accounting for the degrading effects of seeing and spatial binning. The method is flexible and is not limited to particular emission lines or instruments. We test the model through comparison to synthetic observations and use downgraded observations of nearby galaxies to validate this work. As a proof of concept we also apply the model to real IFS observations of high-redshift galaxies. From our testing we show that the inferred metallicity gradients and central metallicities are fairly insensitive to the assumptions made in the model and that they are reliably recovered for galaxies with sizes approximately equal to the half width at half maximum of the point-spread function. However, we also find that the presence of star forming clumps can significantly complicate the interpretation of metallicity gradients in moderately resolved high-redshift galaxies. Therefore we emphasize that care should be taken when comparing nearby well-resolved observations to high-redshift observations of partially resolved galaxies. <P />Chapter 4 We present gas-phase metallicity gradients for 94 star-forming galaxies between (0.08 < z < 0.84). We find a negative median metallicity gradient of (-0.043^{+0.009}_{-0.007}, dex/kpc)/span>, i.e. on average we find the centres of these galaxies to be more metal-rich than their outskirts. However, there is significant scatter underlying this and we find that 10% (9) galaxies have significantly positive metallicity gradients, 39% (37) have significantly negative gradients, 28% (26) have gradients consistent with being flat, the remainder 23% (22) are considered to have unreliable gradient estimates. We find a slight trend for a more negative metallicity gradient with both increasing stellar mass and increasing star formation rate (SFR). However, given the potential redshift and size selection effects, we do not consider these trends to be significant. Indeed when we normalize the SFR of our galaxies relative to the main sequence, we do not observe any trend between the metallicity gradient and the normalized SFR. This finding is contrary to other recent studies of galaxies at similar and higher redshifts. We do, however, identify a novel trend between the metallicity gradient of a galaxy and its size. Small galaxies ((r_d < 3 kpc)) present a large spread in observed metallicity gradients (both negative and positive gradients). In contrast, we find no large galaxies (r_d > 3 kpc) with positive metallicity gradients, and overall there is less scatter in the metallicity gradient amongst the large galaxies. We suggest that these large (well-evolved) galaxies may be analogues of galaxies in the present-day Universe, which also present a common negative metallicity gradient. <P />Chapter 5 The relationship between a galaxy\'s stellar mass and its gas-phase metallicity results from the complex interplay between star formation and the inflow and outflow of gas. Since the gradient of metals in galaxies is also influenced by the same processes, it is therefore natural to contrast the metallicity gradient with the mass-metallicity relation. Here we study the interrelation of the stellar mass, central metallicity and metallicity gradient, using a sample of 72 galaxies spanning (0.13 < z < 0.84) with reliable metallicity gradient estimates. We find that typically the galaxies that fall below the mean mass-metallicity relation have flat or inverted metallicity gradients. We quantify their relationship taking full account of the covariance between the different variables and find that at fixed mass the central metallicity is anti-correlated with the metallicity gradient. We argue that this is consistent with a scenario that suppresses the central metallicity either through the inflow of metal poor gas or outflow of metal enriched gas. <P />
\nThe outlined regions mark the 57 knots in Tycho selected by the authors for velocity measurements. Magenta regions have redshifted line-of-sight velocities (moving away from us); cyan regions have blueshifted light-of-sight velocities (moving toward us). [Williams et al. 2017]The Tycho supernova remnant was first observed in the year 1572. Nearly 450 years later, astronomers have now used X-ray observations of Tycho to build the first-ever 3D map of a Type Ia supernova remnant.Signs of ExplosionsSupernova remnants are spectacular structures formed by the ejecta of stellar explosions as they expand outwards into the surrounding interstellar medium.One peculiarity of these remnants is that they often exhibit asymmetries in their appearance and motion. Is this because the ejecta are expanding into a nonuniform interstellar medium? Or was the explosion itself asymmetric? The best way we can explore this question is with detailed observations of the remnants.Histograms of the velocity in distribution of the knots in the X (green), Y (blue) and Z (red) directions (+Z is away from the observer). They show no evidence for asymmetric expansion of the knots. [Williams et al. 2017]Enter TychoTo this end, a team of scientists led by Brian Williams (Space Telescope Science Institute and NASA Goddard SFC) has worked to map out the 3D velocities of the ejecta in the Tycho supernova remnant. Tycho is a Type Ia supernova thought to be caused by the thermonuclear explosion of a white dwarf in a binary system that was destabilized by mass transfer from its companion.After 450 years of expansion, the remnant now has the morphological appearance of a roughly circular cloud of clumpy ejecta. The forward shock wave from the supernova, however, is known to have twice the velocity on one side of the shell as on the other.To better understand this asymmetry, Williams and collaborators selected a total of 57 knots in Tychos ejecta, spread out around the remnant. They then used 12 years of Chandra X-ray observations to measure both the knots proper motion in the plane of the sky and their line-of-sight velocity. These two measurements were then combined to build a full 3D map of the motion of the ejecta.3D hydrodynamical simulations of Tycho, stopped at the current epoch. These show that both initially smooth (top) and initially clumpy (bottom) ejecta models are consistent with the current observations of the morphology and dynamics of Tychos ejecta. [Adapted from Williams et al. 2017]Symmetry and ClumpsWilliams and collaborators found that the knots have total velocities that range from 2400 to 6600 km/s. Unlike the forward shock of the supernova, Tychos ejecta display no asymmetries in their motion which suggests that the explosion itself was symmetric. The more likely explanation is a density gradient in the interstellar medium, which could slow the shock wave on one side of the remnant without yet affecting the motion of the clumps of ejecta.As a final exploration, the authors attempt to address the origin of Tychos clumpiness. The fact that some of Tychos ejecta knots precede its outer edge has raised the question of whether the ejecta started out clumpy, or if they began smooth and only clumped during expansion. Williams and collaborators matched the morphological and dynamical data to simulations, demonstrating that neither scenario can be ruled out at this time.This first 3D map of a Type Ia supernova represents an important step in our ability to understand these stellar explosions. The authors suggest that well be able to expand on this map in the future with additional observations from Chandra, as well as with new data from future X-ray observatories that will be able to detect fainter emission.CitationBrian J. Williams et al 2017 ApJ 842 28. doi:10.3847/1538-4357/aa7384 <P />
\nA previous good encounter occurred on 2006 July 29d04h11m UT (r - Delta = +0.0003 AU, solar long. = 125.841 deg). Future encounters are predicted on 2029 July 29d01h53m (+0.0007 AU, 125.816 deg), 2042 July 29d10h48m (+0.0006 AU, 125.886 deg), 2053 July 29d05h35m (+0.0001 AU, 125.848 deg), and on 2068 July 29d02h09m UT (-0.0001 AU, 125.863 deg). <P />
\nsick infers astrophysical parameters from noisy observed spectra. Phenomena that can alter the data (e.g., redshift, continuum, instrumental broadening, outlier pixels) are modeled and simultaneously inferred with the astrophysical parameters of interest. This package relies on emcee (ascl:1303.002); it is best suited for situations where a grid of model spectra already exists, and one would like to infer model parameters given some data. <P />
\nThe included files present the numerical data of our analysis of the BM CVn photometry. The data consists of differential Johnson V-band photometry using the star HD 116010 as the comparison star. <P />The analysis has been performed using the previously published continuous period search (CPS) method, described in detail in Lehtinen et al., 2011A&A...527A.136L, Cat. J/A+A/527/A136. <P />(4 data files). <P />
\nThe observing campaign from 2016 on V694 Mon (MWC 560) (AAVSO Alert Notice 538) has been continued, but with different requirements. Photometry is no longer specifically requested on a regular basis (although ongoing observations that do not interfere with other obligations are welcome). Spectroscopy on a cadence of a week or two is requested to monitor changes in the disk outflow. Investigator Adrian Lucy writes: "Adrian Lucy and Dr. Jeno Sokoloski (Columbia University) have requested spectroscopic monitoring of the broad-absorption-line symbiotic star V694 Mon (MWC 560), as a follow-up to coordinated multi-wavelength observations obtained during its recent outburst (ATel #8653, #8832, #8957; #10281). This system is a perfect place in which to study the relationship between an accretion disk and disk winds/jets, and a high-value target for which even low-resolution spectra can be extraordinarily useful...Optical brightening in MWC 560 tends to predict higher-velocity absorption, but sometimes jumps in absorption velocity also appear during optical quiescence (e.g., Iijima 2001, ASPCS, 242, 187). If such a velocity jump occurs during photometric quiescence, it may prompt radio observations to confirm and test the proposed outflow origin for recently-discovered flat-spectrum radio emission (Lucy et al. ATel #10281)...Furthermore, volunteer spectroscopic monitoring of this system has proved useful in unpredictable ways. For example, \'amateur\' spectra obtained by Somogyi Péter in 2015 December demonstrated that the velocity of absorption was very low only a month before an optical outburst peak prompted absorption troughs up to 3000 km/s, which constrains very well the timing of the changes to the outflow to a degree that would not have been otherwise possible. Any resolution can be useful. A wavelength range that can accommodate a blueshift of at least 140 angstroms (6000 km/s) from the rest wavelengths of H-alpha at 6562 angstroms and/or H-beta at 4861 angstroms is ideal, though spectra with a smaller range can still be useful. Photometry could potentially still be useful, but will be supplementary to medium-cadence photometry being collected by the ANS collaboration." "Spectroscopy may be uploaded to the ARAS database (http://www.astrosurf.com/aras/Aras_DataBase/DataBase.htm), or sent to Adrian and Jeno directly at <lucy@astro.columbia.edu>. Finder charts with sequence may be created using the AAVSO Variable Star Plotter (https://www.aavso.org/vsp). Photometry should be submitted to the AAVSO International Database. See full Special Notice for more details. <P />
\nULIRG F01004-2237 had a strong optical flare, peaked in 2010, and the follow-up optical spectra classified this event as a TDE candidate (Tadhunter et al. 2017, Nature Astronomy). In early 2017, using archival WISE data, we discovered that its 3.4 and 4.6um fluxes have been steadily rising since 2013, increased by a factor of 3.5 and 2.6 respectively. The last epoch data from WISE on 2016-12-12 shows that F01004-2237 has reached 7.5 and 14mJy at 3.4 and 4.6um. We interpret the mid-IR LCs as infrared echoes from the earlier optical flare. We infer a convex, dust ring with a radius of 1 pc from the central heating source. Our model predicts that if this event is indeed a TDE, its mid-IR LCs should start to fade in next 5-12 months because it has already reprocessed most of the UV/optical energy from the tidal disruption. However, if this event is due to activities from an AGN, its mid-IR LCs could last over a much longer time scale. We request a total of 3.2 hours of Spitzer time to monitor the mid-IR variations in next 12 months. This will provide the critical data to confirm the nature of this transient event. <P />
\nThe African Very-long-baseline interferometry Network (AVN) is a joint project between South Africa and eight partner African countries aimed at establishing a VLBI (Very-Long-Baseline Interferometry) capable network of radio telescopes across the African continent. An existing structure that is earmarked for this project, is a 32 m diameter antenna located in Ghana that has become obsolete due to advances in telecommunication. The first phase of the conversion of this Ghana antenna into a radio astronomy telescope is to upgrade the antenna to observe at 5 GHz to 6.7 GHz frequency and then later to 18 GHz within a required performing tolerance. The surface and pointing accuracies for a radio telescope are much more stringent than that of a telecommunication antenna. The mechanical pointing accuracy of such telescopes is influenced by factors such as mechanical alignment, structural deformation, and servo drive train errors. The current research investigates the numerical simulation of the surface and pointing accuracies of the Ghana 32 m diameter radio astronomy telescope due to its structural deformation mainly influenced by gravity, wind and thermal loads. <P />
\nThe web page represents circumstances and photographs from the Moon\'s partial/penumbral eclipse from 16 September 2016 obtained from few various places in Romania (East Europe). A part of photographs give the maximum phase of the Eclipse, while another give the reddened Moon. <P />
\nNot Available <P />
\nThe discovery of the physical phenomenon of Nuclear Magnetic Resonance (NMR) in 1946 gave rise to the spectroscopic technique that has become a remarkably versatile research tool. One could oversimplify NMR spectros-copy by categorizing it into the two broad applications of structure elucidation of molecules (associated with chemistry and biology) and imaging (associated with medicine). But, this certainly does not do NMR spectroscopy justice in demonstrating its general acceptance and utilization across the sciences. This manuscript is not an effort to present an exhaustive, or even partial review of NMR spectroscopy applications, but rather to provide a glimpse at the wide-ranging uses of NMR spectroscopy found within the confines of a single magnetic resonance research facility, the Stanford Magnetic Resonance Laboratory. Included here are summaries of projects involving protein structure determination, mapping of intermolecular interactions, exploring fundamental biological mechanisms, following compound cycling in the environmental, analysis of synthetic solid compounds, and microimaging of a model organism. <P />
\nPalomar-QUEST (PQ) synoptic sky survey has now been routinely processing data from driftscans in real-time. As four photometric bandpasses are utilized in nearly simultaneously, PQ is well suited to search for transient and highly variable objects. Using a series of software filters i.e. programs to select/deselect objects based on certain criteria we shorten the list of candidates from the initially flagged candidate transients. Such filters include looking for known asteroids, known variables, as well as moving, but previously uncatalogued objects based on their motion within a scan as well as between successive scans. Some software filters also deal with instrumental artifacts, edge effects, and use clustering of spurious detections around bright stars. During a typical night when we cover about 500 sq. degrees, we detect hundreds of asteroids, the primary contaminants in the search for astrophysical transients beyond our solar system. <P />Here we describe some statistics based on the software filters we employ and the nature of the objects that seem to survive the process. We also discuss the usefulness of this to amateur astronomers, projects like VOEventNet, and other synoptic sky surveys. <P />We also present an outline of the work we have started on quantifying the variability of quasars, blazars, as well as various classes of Galactic sources, by combining the large number of PQ scans with other existing data sources federated in the Virtual Observatory environment. <P />The PQ survey is partially supported by the U.S. National Science Foundation (NSF). <P />
\nNot Available <P />
\nSpacecraft operation depends upon knowledge of vehicular position and, consequently, navigational support has been required for all such systems. Technical requirements for different mission trajectories and orbits are addressed with consideration given to the various tradeoffs which may need to be considered. The broad spectrum of spacecraft are considered with emphasis upon those of greater military significance (i.e., near earth orbiting satellites). Technical requirements include, but are not limited to, accuracy; physical characteristics such as weight and volume; support requirements such as electrical power and ground support; and system integrity. Generic navigation suites for spacecraft applications are described. It is shown that operational spacecraft rely primarily upon ground-based tracking and computational centers with little or no navigational function allocated to the vehicle, while technology development efforts have been and continue to be directed primarily toward onboard navigation suites. The military significance of onboard navigators is shown to both improve spacecraft survivability and performance (accuracy). <P />
\nNot Available <P />
\nThese lectures consisted of an elementary introduction to conformal field theory, with some applications to statistical mechanical systems, and fewer to string theory. Contents: 1. Conformal theories in d dimensions 2. Conformal theories in 2 dimensions 3. The central charge and the Virasoro algebra 4. Kac determinant and unitarity 5. Identication of m = 3 with the critical Ising model 6. Free bosons and fermions 7. Free fermions on a torus 8. Free bosons on a torus 9. Affine Kac-Moody algebras and coset constructions 10. Advanced applications <P />
\nThe concept of using lunar beacon signal transmission for on-board navigation for earth satellites and near-earth spacecraft is described. The system would require powerful transmitters on the earth-side of the moon\'s surface and black box receivers with antennae and microprocessors placed on board spacecraft for autonomous navigation. Spacecraft navigation requires three position and three velocity elements to establish location coordinates. Two beacons could be soft-landed on the lunar surface at the limits of allowable separation and each would transmit a wide-beam signal with cones reaching GEO heights and be strong enough to be received by small antennae in near-earth orbit. The black box processor would perform on-board computation with one-way Doppler/range data and dynamical models. Alternatively, GEO satellites such as the GPS or TDRSS spacecraft can be used with interferometric techniques to provide decimeter-level accuracy for aircraft navigation. <P />
\nArchived and distributed through the ORNL DAAC, the Daymet data set provides gridded estimates of daily weather parameters for North America, including daily continuous surfaces of minimum and maximum temperature, precipitation occurrence and amount, humidity, shortwave radiation, snow water equivalent, and day length. The daily time step, 1 km x 1 km spatial resolution, and North American spatial extent of the data set makes it a unique and valuable contribution to scientific, research, and educational communities. The literature shows that Daymet data have been broadly applied to fields including hydrology, terrestrial vegetation growth models, carbon cycle science, and regional to large scale climate change analysis.
\nRecently Pomme et al. (Solar Phys 292:162, 2017) did an analysis of 36Cl radioactive decay data from measurements at the Physikalisch-Technische Bundesanstalt (PTB), in order to verify the claims by Sturrock and collaborators of an influence on beta-decay rates measured at Brookhaven National Lab (BNL) due to the rotation-induced modulation of the solar neutrino flux. Their analysis excluded any sinusoidal modulations in the frequency range from 0.2 to 20/year. We carry out an independent analysis of the same PTB and BNL data, using the generalized Lomb–Scargle periodogram to look for any statistically significant peaks in the range from 0 to 14 per year, and by evaluating the significance of every peak using multiple methods. Our results for the PTB data are in agreement with those by Pomme et al. For BNL data, we do find peaks at some of the same frequencies as Sturrock et al., but the significance is much lower. All our analysis codes and datasets have been made publicly available.
\nThe NASA Astrophysics Data System (ADS) is used daily by researchers and curators as a discovery platform for the Astronomy literature. Over the past several years, the ADS has been adding to the breadth and depth of its contents. Scholarly astronomy articles are now indexed as full-text documents, allowing for complete and accurate literature searches. High-level data products, data links, and software used in refereed astronomy papers are now also being ingested and indexed in our database. All the search functionality exposed in the new ADS interface is also available via its API, which we are continuing to develop and enhance. In this talk I will describe the current system, our current roadmap, and solicit input from the community regarding what additional data, services, and discovery capabilities the ADS should support.
\nChanges: improved installation mechanism for Julia spelling fixes in README.MD
\nNow the surface of Mars is a waterless desert, over which storms rage, raising sand and dust to a height of tens of kilometers. Under modern conditions, open bodies of water cannot exist on Mars. And water on the planet is contained either in the soil layer as permafrost, or in the form of open ice and snow; a very small amount of water is present in gaseous form in the atmosphere. The large reservoirs of water ice on Mars are the polar caps. Studies of Mars by spacecraft have shown that there is a huge amount of ice, and possibly liquid water, under the surface layer at a shallow depth. Analysis of the collected data allowed us to come to the conclusion that liquid water existed in significant quantities on the surface of Mars several billion years ago. That is, in the past, Mars had a full-fledged hydrosphere and a rather powerful atmosphere with a pressure near the surface of more than 0.4 bar. Later, the planet\'s climate changed. It lost much of its atmosphere and water, turning into a cold world. On the surface of Mars, there are numerous winding valleys with a long length, reminiscent of the dried-up channels of terrestrial rivers. A significant portion of the water that once flowed along currently dry riverbeds must now be under the surface of the planet. It is also possible that some channels are the result of the action of not liquid water, but a mixture of mud, ice and steam that flow only episodically. It is possible that the meandering valleys formed moving masses of glaciers. There is every reason to believe that there is still a lot of water on Mars, and it still exists in the form of permafrost. A perspective image of the Echus Chasma region suggests that liquid water was present on this part of the Martian surface up to a billion years ago. Later, the planet cooled down, the lakes froze, and glaciers formed, which \'cut\' the Kasei Valles with their streams.
\nIn the next few years, several new astronomical instruments are planned to be launched on Earth and in space. Each of these devices is very expensive! But many countries allocate large amounts of money for this, and plan to receive more and more recent data about the surrounding universe. Telescopes are devices for observing distant objects. The very first working telescope was created in 1608 by the Dutch optician Hans Lippersgei. The creation of the telescope was also attributed to such masters as another Dutch eyeglass maker from Middelburg, Zachary Janssen, and Jacob Mathews from the city of Alkmaar. These earliest telescopes consisted of a convex lens as an objective and a concave lens that served as an eyepiece. In 1609, Galileo Galilei significantly improved the design of the telescope, achieving a 30-fold increase in the original images. With its help, Galileo performed the first survey of the heavenly bodies. Therefore, even now, the creation of astronomical instruments, whose characteristics significantly improve previous examples of telescope construction, is considered extremely important in astronomical research. The Hubble telescope was the first to provide interesting information about the features of images of the most distant galaxies. They are significantly different from those formed relatively recently. One of the world\'s largest ground-based telescopes, the Giant Magellan Telescope, is under construction. It is being built in Chile and its gradual commissioning will begin in 2024. Segments of seven monolithic mirrors, with a diameter of 8.4 m each, create an optical surface with an equivalent diameter of 24.5 m. Larger will be the 30-meter telescope, which is planned to be built on the island of Hawaii, next to the two 9-meter Keck reflectors at the Mauna Kea observatory. The mirror surface of this telescope will consist of almost five hundred hexagonal segments and will reach a diameter of 30 m. It is expected to be tested in 2027. In 2014, the European Southern Observatory started the construction of the Extremely Large Telescope. In 2025, it is planned to become the most powerful optical astronomical instrument in the world, with an equivalent diameter of its mirror surface of 39 m.
\nThe portable Raspberry Pi computing platform with the power of Linux yields an exciting exploratory tool for beginning scientific computing. Science and Computing with Raspberry Pi takes the reader through explorations in a variety of computing exercises with the physical sciences. The book guides the user through: configuring your Raspberry Pi and Linux operating system; understanding the software requirements while using the Pi for scientific computing; computing exercises in physics, astronomy, chaos theory, and machine learning.
\nA forecast for New Zealand\'s changing climate and why it matters to our everyday lives A warmer world will change more than just our weather patterns. It will change the look of the land around us, what grows and lives on it - including us. Drawing on climate models that can travel to ice ages and hothouses of the deep past, Professor James Renwick untangles how we know exactly what the future holds and why it matters to our everyday lives. He looks at New Zealand\'s more frequent natural disasters, warming and increasingly acidic waters, the creep of rising sea levels, and the ways that the changing weather will affect our agriculture, lifestyle, food security and economy.Arresting, galvanizing and clear-sighted, Under the Weather is a picture of a miraculous planet in danger, a stock-take on what it means for this small country, and a reminder that the shape of our future is up to us.\'--Publisher description.
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