Abstract:We present Spitzer Space Telescope and Herschel Space Observatory infrared observations of the recurrent nova T Pyx during its 2011 eruption, complemented by ground-base opticalinfrared photometry. We find that the eruption has heated dust in the pre-existing nebulosity associated with T Pyx. This is most likely interstellar dust swept up by T Pyx -either during previous eruptions or by a wind -rather than the accumulation of dust produced during eruptions.
“…This agrees with the interferometric imaging (and perhaps also with the infrared emission described by Evans et al 2012). The relative contributions of the inner and outer portions of the polar lobes change systematically in time.…”
Section: Summary Of the Modelingsupporting
confidence: 78%
“…In contrast, Schaefer et al (2010) derived a mass for the matter that they identify with a single classical nova-like outburst of 1866, M ej ∼ 3 × 10 −5 M . Selvelli et al (2009) and, more recently, Evans et al (2012) have also argued that the mass of the accumulated flotsam of previous ejections may be considerably greater, perhaps a factor of order 100, than that of a single event. Evans et al (2012) based this on the infrared light curve of the 2011 event that they explain as a light echo from the previously ejected material 5 .…”
Section: Electron Density and Mass Of The Ejectamentioning
Aims. We continue our study of the physical properties of the recurrent nova T Pyx, focussing on the structure of the ejecta in the nebular stage of expansion during the 2011 outburst.
“…This agrees with the interferometric imaging (and perhaps also with the infrared emission described by Evans et al 2012). The relative contributions of the inner and outer portions of the polar lobes change systematically in time.…”
Section: Summary Of the Modelingsupporting
confidence: 78%
“…In contrast, Schaefer et al (2010) derived a mass for the matter that they identify with a single classical nova-like outburst of 1866, M ej ∼ 3 × 10 −5 M . Selvelli et al (2009) and, more recently, Evans et al (2012) have also argued that the mass of the accumulated flotsam of previous ejections may be considerably greater, perhaps a factor of order 100, than that of a single event. Evans et al (2012) based this on the infrared light curve of the 2011 event that they explain as a light echo from the previously ejected material 5 .…”
Section: Electron Density and Mass Of The Ejectamentioning
Aims. We continue our study of the physical properties of the recurrent nova T Pyx, focussing on the structure of the ejecta in the nebular stage of expansion during the 2011 outburst.
“…The observed line profiles during the optically thin stages of the expansion of T Pyx can be explained by a unified model in which the ejecta have an axial (bipolar) symmetry with the expansion directed at low inclination to the line of sight. This agrees with the interferometric imaging (and perhaps also with the infrared emission described by Evans et al (2012)). The relative contributions of the inner and outer portions of the po-lar lobes change systematically in time.…”
Section: Summary Of the Modelingsupporting
confidence: 91%
“…In contrast, Schaefer et al (2010) derived a mass for the matter that they identify with a single classical nova-like outburst of 1866, M e j ∼ 3 × 10 −5 M ⊙ . Selvelli et al (2009) and, more recently, Evans et al (2012) have also argued that the mass of the accumulated flotsam of previous ejections may be considerably greater, perhaps a factor of order 100, than that of a single event. Evans et al (2012) based this on the infrared light curve of the 2011 event that they explain as a light echo from the previously ejected material.…”
Section: Electron Density and Mass Of The Ejectamentioning
Aims. We continue our study of the physical properties of the recurrent nova T Pyx, focussing on the structure of the ejecta in the nebular stage of expansion during the 2011 outburst. Methods. The nova was observed contemporaneously with the Nordic Optical Telescope (NOT), at high resolution spectroscopic resolution (R ≈65000)
“…With multi-wavelength data collected from the 2011 outburst, we can measure key properties of the nova event, like ejected mass, and compare them with predictions from nova models. With this goal in mind, campaigns have been carried out across the entire electromagnetic spectrum, providing an exquisitely detailed picture of the 2011 nova outburst of T Pyx (Chesneau et al 2011;Kuulkers et al 2011a,b;Shore et al 2011Shore et al , 2013Evans et al 2012;Imamura & Tanabe 2012;Nelson et al 2014;Ederoclite 2013;Williams 2013;Schaefer et al 2013;Patterson et al 2013;Sokoloski et al 2013;Tofflemire et al 2013;De Gennaro Aquino et al 2014;Godon et al 2014;Surina et al 2014).…”
The recurrent nova T Pyx underwent its sixth historical outburst in 2011, and became the subject of an intensive multi-wavelength observational campaign. We analyze data from the Swift and Suzaku satellites to produce a detailed X-ray light curve augmented by epochs of spectral information. X-ray observations yield mostly non-detections in the first four months of outburst, but both a super-soft and hard X-ray component rise rapidly after Day 115. The super-soft X-ray component, attributable to the photosphere of the nuclear-burning white dwarf, is relatively cool (∼45 eV) and implies that the white dwarf in T Pyx is significantly below the Chandrasekhar mass (∼1 M ⊙ ). The late turn-on time of the super-soft component yields a large nova ejecta mass ( 10 −5 M ⊙ ), consistent with estimates at other wavelengths. The hard X-ray component is well fit by a ∼1 keV thermal plasma, and is attributed to shocks internal to the 2011 nova ejecta. The presence of a strong oxygen line in this thermal plasma on Day 194 requires a significantly super-solar abundance of oxygen and implies that the ejecta are polluted by white dwarf material. The X-ray light curve can be explained by a dualphase ejection, with a significant delay between the first and second ejection phases, and the second ejection finally released two months after outburst. A delayed ejection is consistent with optical and radio observations of T Pyx, but the physical mechanism producing such a delay remains a mystery.
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