The expanding fireball of Nova Delphini 2013 (original) (raw)
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Acknowledgements
We acknowledge the variable star observations from the AAVSO International Database contributed by observers worldwide and used in this research. We thank O. Garde and other members of the Astronomical Ring for Access to Spectroscopy for use of their archive of Nova Del 2013 spectra. We thank G. J. Schwarz, S. N. Shore, and F. M. Walter for discussions that helped us to interpret the nova observations. This material is based upon work supported by the National Science Foundation under grant number AST-1009080. The CHARA Array is funded by the National Science Foundation through NSF grants AST 0908253 and AST 1211129, and by Georgia State University through the College of Arts and Sciences. This publication made use of data products from the Two Micron All Sky Survey, which is a joint project of the University of Massachusetts and the Infrared Processing and Analysis Center/California Institute of Technology, funded by the National Aeronautics and Space Administration and the National Science Foundation.
Author information
Authors and Affiliations
- The CHARA Array of Georgia State University, Mount Wilson Observatory, Mount Wilson, 91023, California, USA
G. H. Schaefer, T. ten Brummelaar, C. D. Farrington, N. Scott, J. Sturmann, N. Vargas, L. Sturmann & N. H. Turner - Center for High Angular Resolution Astronomy and Department of Physics and Astronomy, Georgia State University, PO Box 5060, Atlanta, Georgia 30302, USA,
D. R. Gies, B. Kloppenborg, H. A. McAlister, F. Baron & J. Jones - Laboratoire Lagrange, UMR 7293, Université de Sophia-Antipolis (UNS)–Centre National de la Recherche Scientifique (CNRS)–Observatoire de la Côte d’Azur (OCA), Boulevard de l’Observatoire, CS 34229, F-06304 Nice, Cedex 4, France,
O. Chesneau, D. Mourard, A. Meilland, N. Nardetto & P. Stee - Department of Astronomy, University of Michigan, 941 Dennison Building, Ann Arbor, Michigan 48109, USA,
J. D. Monnier, X. Che, R. M. Roettenbacher & J. Becker - National Optical Astronomy Observatory, 950 North Cherry Avenue, Tucson, 85719, Arizona, USA
S. T. Ridgway - Université de Lyon; Université Lyon 1, Observatoire de Lyon, 9 avenue Charles André, 69230 Saint Genis Laval; CNRS UMR 5574, Centre de Recherche Astrophysique de Lyon; École Normale Supérieure, 69007 Lyon, France,
I. Tallon-Bosc - Université Lyon 1, Observatoire de Lyon, 9 avenue Charles André, 69230 Saint Genis Laval,
I. Tallon-Bosc - Department of Astronomy, Yale University, New Haven, 06511, Connecticut, USA
T. Boyajian - Sydney Institute for Astronomy, School of Physics, University of Sydney, New South Wales 2006, Sydney, Australia,
V. Maestro & P. Tuthill - Research School of Astronomy and Astrophysics, Australian National University, Canberra, Australian Capital Territory 2611, Australia,
M. Ireland - Remote Sensing Division, Naval Research Laboratory, 4555 Overlook Avenue Southwest, Washington, DC 20375, USA,
E. K. Baines - Département de Physique and Centre de Recherche en Astrophysique du Québec (CRAQ), Université de Montréal, CP 6128, Succursale Centre-Ville, Montréal, Québec H3C 3J7, Canada,
N. D. Richardson - Lowell Observatory, 1400 West Mars Hill Road, Flagstaff, 86001, Arizona, USA
G. van Belle - Max Planck Institute for Astronomy (MPIA), Konigstuhl 17, 69117 Heidelberg, Germany,
K. von Braun - United States Naval Observatory, Flagstaff Station, 10391 West Naval Observatory Road, Flagstaff, Arizona 86001, USA,
R. T. Zavala - Astronomy and Astrophysics Division, Physical Research Laboratory, Navrangpura, Ahmedabad, Gujarat 380009, India,
D. P. K. Banerjee, N. M. Ashok & V. Joshi - Cahill Center for Astronomy and Astrophysics, California Institute of Technology, Pasadena, 91106, California, USA
J. Becker - Department of Astronomy, Boston University, Boston, 02215, Massachusetts, USA
P. S. Muirhead
Authors
- G. H. Schaefer
- T. ten Brummelaar
- D. R. Gies
- C. D. Farrington
- B. Kloppenborg
- O. Chesneau
- J. D. Monnier
- S. T. Ridgway
- N. Scott
- I. Tallon-Bosc
- H. A. McAlister
- T. Boyajian
- V. Maestro
- D. Mourard
- A. Meilland
- N. Nardetto
- P. Stee
- J. Sturmann
- N. Vargas
- F. Baron
- M. Ireland
- E. K. Baines
- X. Che
- J. Jones
- N. D. Richardson
- R. M. Roettenbacher
- L. Sturmann
- N. H. Turner
- P. Tuthill
- G. van Belle
- K. von Braun
- R. T. Zavala
- D. P. K. Banerjee
- N. M. Ashok
- V. Joshi
- J. Becker
- P. S. Muirhead
Contributions
Observations with the CHARA Array were originally proposed by B.K. and D.R.G. Modelling and interpreting the angular expansion curve and asymmetries were done by G.H.S., D.R.G., B.K., T.t.B., O.C., I.T.-B. and S.T.R. The CHARA data were reduced by T.t.B., J.D.M., O.C., I.T.-B., D.M., V.M., C.D.F., N.S. and G.H.S. The observations were planned and conducted by C.D.F., N.S., N.V., B.K., D.R.G., T.B., G.H.S., D.M., A.M., N.N., P.S., M.I., V.M., P.T., J.J., N.D.R., R.M.R., G.v.B., K.v.B. and R.T.Z. Observational setup and technical support were provided by J.S., L.S., N.H.T. and X.C. Administrative oversight and access to CHARA were provided by H.A.M. and T.t.B. Reconstructing and interpreting the nova images were done by G.H.S., F.B., J.D.M. and B.K. Infrared magnitudes derived from CHARA data were computed by N.S. and G.H.S. Infrared spectra were taken and reduced by D.P.K.B., N.M.A., V.J., P.S.M., J.B. and analysed by D.R.G. All authors discussed the results and commented on the manuscript.
Corresponding author
Correspondence toG. H. Schaefer.
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Extended data figures and tables
Extended Data Figure 1 Integrated emission line to continuum flux ratios measured from infrared spectroscopy.
The squares represent the H-band ratios while the diamonds represent the K′-band ratios. The rise in the emission line flux is consistent with an increasing contribution from optically thin emission. The down turn in the curve during the last measurement is probably caused by a rising contribution of the continuum owing to the formation of dust.
Extended Data Figure 2 Closure phases measured with MIRC on ut 2013 August 21.
The measurements are plotted against the length of the maximum baseline (B) for the group of three telescopes that were used to form the closure phase. The non-zero closure phases indicate an asymmetry in the light distribution that is not point symmetric. The colours of the symbols are used to differentiate the measurements from each grouping of three telescopes in the array. The closure phases are measured in eight wavelength channels. Error bars represent 1_σ_ measurement uncertainties.
Extended Data Figure 3 Example of MIRC observations obtained on ut 2013 August 21.
The light is dispersed over eight wavelength channels in the H-band. a, Coverage of the interferometric baselines projected on the plane of the sky in right ascension (RA) and declination (Dec.) in units of spatial frequencies (u = B x /λ, v = B y /λ). b, Squared, normalized visibility amplitude measurements, colour-coded to match the baselines on the left. The solid line shows the best-fitting uniform disk model. The small black dots show the best-fitting uniform ellipse model. Error bars represent 1_σ_ measurement uncertainties.
Extended Data Figure 4 Interferometric visibilities of Nova Del 2013 measured with the CHARA Array.
The red line shows the best-fitting model for a uniformly bright, circular disk. The time since the explosion (in days) is indicated in the upper right corner of each panel. The measurements were obtained with the CLASSIC, CLIMB, and MIRC beam combiners (see Extended Table 1). Error bars represent 1_σ_ measurement uncertainties.
Extended Data Figure 5 Time evolution of the two-component model of Nova Del 2013.
The model consists of a circular core surrounded by a halo ring. The expansion rate and size ratio were determined by minimizing _χ_2 across all of the nights while allowing the flux ratio to vary night by night. In plotting the images, we used the flux ratio measured directly for the first three nights, the linear fit plotted in Fig. 3 of the main paper for t = 4–27 days, and our measurement that the ring contributes an average of 68% of the light on the last five nights (dust emission in the outer layers). Each panel is 12 mas on a side. We scaled the model flux by the infrared magnitude measured on each night to show how the surface brightness changes. The time since the explosion (in days) is indicated in each panel. Intensity refers to the flux per unit area.
Extended Data Table 1 Journal of observations and angular diameters measurements of Nova Del 2013
Extended Data Table 2 Uniform ellipse models of Nova Del 2013
Extended Data Table 3 Infrared magnitudes of Nova Del 2013
Extended Data Table 4 Effective bandwidth of the CLASSIC/CLIMB observations
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Schaefer, G., Brummelaar, T., Gies, D. et al. The expanding fireball of Nova Delphini 2013.Nature 515, 234–236 (2014). https://doi.org/10.1038/nature13834
- Received: 13 May 2014
- Accepted: 03 September 2014
- Published: 26 October 2014
- Issue date: 13 November 2014
- DOI: https://doi.org/10.1038/nature13834