Infrared Observations of Novae with Subaru/COMICS and Gemini/T- ReCS Sakon, I., Sako, S., Shimonishi, T., Onaka, T. (Univ. of Tokyo) Takahashi, H. (Gunma.

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Infrared Observations of Novae with Subaru/COMICS and Gemini/T- ReCS Sakon, I., Sako, S., Shimonishi, T., Onaka, T. (Univ. of Tokyo) Takahashi, H. (Gunma Observatory) Yamashita, T., Fujiyoshi, T. (NAOJ) Rodomski, J. (Gemini Observatory)

Infrared Observations of Novae Mid-infrared Imaging and Spectroscopic monitoring observations of Galactic dust forming novae  unique laboratories to study the process of dust formation and to understand the mass-loss history of the CO white dwarves from the chemical point of view Infrared Spectral Evolution of CO Novae and ONeMg Novae -Hot ejecta gas is initially seen as an expanding photosphere or “fireball” -When the expanding material becomes optically thin, free-free and line emission dominate 1). CO Novae; - Thermonuclear runaway (TNR) on the surface of relatively low-mass CO white dwarves (e.g., M WD <1.1M ☉ ) -Dust formation after the free-free phase is reported for several CO novae [e.g., V2362 CYGNI (Lynch et al. 2008), V705 Cas (Evans et al. 1997), etc.] - Complicated dust compositions (both Silicates and Carbonaceous dust) 2). ONeMg Novae; - Thermonuclear runaway (TNR) on the surface of relatively higher-mass ONeMg white dwarves (e.g., M WD >1.1M ☉ ) - coronal emission-lines phase comes after the free-free phase - No or little evidence of dust formation (cf., V1974 CYGNI; Woodward et al ) chemical evolution of the Nova ejecta over various physical phases is not fully understood

V1280 Scorpii -Discovered on 2007 Feb 4.86 by Y. Nakamura and Y. Sakurai (Yamaoka et al. 2007) - d = 1.6±0.4 kpc (Chesneau et al. 2008) -Dust formation occurred at d~23days after discovery (Das et al. 2007) VLTI/AMBER and MIDI observations between t=23 d and 145 d (Chesneau et al. 2008) -An apparent linear expansion rate for the dust shell; 0.35±0.03mas day -1 -Expansion velocity of the nova ejecta; 500±100 km/s -Dust production rate; 2-8x10 -9 M sun day -1 (a probable peak in production at t=36-46 days) -The amount of dust in the shell; 2.2x10 -7 M sun Late-epoch Observations of Dust Forming Nova V1280Sco - July 7, 2007 (epoch ~150 days) Subaru/COMICS; N-band spectroscopy (  m) N- & Q-band photometry (8.8  m, 11.7  m, 18.8  m, 24.5  m) Kanata/TRISPEC (June 26, 2007; epoch ~140 days); Ks-band photometry (2.15  m) - September 8, 2009 (epoch ~940 days) AKARI/IRC; near-infrared spectroscopy (2.5-5  m) - August 1, 2010 (epoch ~1270 days) Gemini-S/TReCS; N-band spectroscopy (  m) N- & Q-band photometry (7.8  m, 9.7  m, 11.7  m,18.8  m, 24.5  m) Gunma (Aug 26, 2010; epoch ~1300 days); J, H, Ks-band photometry (1.24, 1.66, 2.15  m)

Infrared Spectral Energy Distribution of V1280Sco at ~150 days with Subaru/COMICS Possible Silicate Absorption Feature at ~10  m

15 (a) Near-Infrared spectrum of V1280 Sco on the epoch 940 days after the discovery normalized to the continuum obtained with Infrared Camera (IRC) onboard AKARI. A PAH 3.3  m feature with a strong redwing in  m was recognized. (b) Near-infrared spectrum of Galactic ISM as an example of typical spectrum of PAH features with a normal inter-band ratios among 3.3, 3.4 and 3.5  m features obtained with AKARI/IRC. Near Infrared Spectrum of V1280Sco at ~940 days with AKARI/IRC

Results of N- & Q-band imaging observations of V1280 Sco at t=~1270 days with Gemini-S/TReCS Example; Qa band data of V1280Sco and HD Intrinsic profile of the dust emission; 3D-Elliptical Gaussian  ; position angle for the major-axis  a ; semi-major axis radius  b ; semi-minor axis radius  bb aa The best-fit 3D-Elliptical Gaussian parameters Band (  m)  (deg)  a (“)  b (“) Si ± ±0.02 Si ± ±0.02 Si ± ±0.02 Qa ± ±0.03 Qb ± ±  m Non-spherical distribution of dust emission Effective size of the dust shell; 7.2x10 10 k (~500AU)  Much smaller than the size of the expanding Ejecta Shell with 500km/s at t~1300d; 2x10 13 km

Spectral Decomposition of model fit to the Infrared Continuum Spectrum of V1280Sco at ~1300 days obtained with Gemini-S/TReCS Amorphous Carbon; 485±5 (K), 1.54x10 -7 Msun Astronomical Silicate; 185±5 (K), 1.90x10 -6 Msun

Mid-Infrared Spectral Features over the Infrared Continuum modeled with amorphous carbon and astronomical silicate Features at ~8.1  m, ~8.7  m, ~11.35  m; Hydrogenated Amorphous Carbons (HACs), NH2-rocks (Grishko & Duley 2002)  similar to those found in V704 Cas 1993 (Evans et al. 1997, 2005) A Broad Feature at ~10.1  m; amorphous silicate Features at ~9.2  m, ~9.8  m, ~10.7  m, ~11.4  m; Possible contributions of forsterite, enstatite and diopside (Molster et al. 2002)

Interpretations; IR observations of V1280Sco -Near- to mid-infrared (1-25  m) spectrum at t = ~1270 day with Gemini-S/TReCS is well reproduced by Emission from warm (T~185±5K) astronomical silicate dust of 1.9x10 -6 M sun and hot (T~485±5 K) amorphous carbon dust of 1.5x10 -7 M sun  presence of both carbonaceous dust and (pre-existing?) silicate dust  the emitting regions of both components are confined within ~500AU (within an expanding dust shell; 0.35mas/day). -Strong 18-  m /10-  m silicate band ratio  presence of lower temperature astronomical silicate dust (T~185K) of 1.9x10 -6 M sun ?  Possible annealing effect? (evolution of circumstellar silicate) (Nuth & Hecht 1990) (consistent with the possible presence of crystalline silicate band emission.) -Detection of 3.3  m feature with strong red-wing in AKARI/IRC NIR spectrum at t = ~940 days -Detection of 8.1, 8.7 and  m features in the spectrum of of V1280 Sco at t=~1270 days with Gemini-S/TReCS  Formation of Hydrogenated Amorphous Carbons (HACs) in the nova ejecta -Presence of silicate absorption in the N-band Low-resolution spectrum of V1280Sco at t = ~150 days with Subaru/COMICS -CO gas absorption in the AKARI/IRC near-infrared spectrum of V1280Sco at t=~940 days  presence of rich circumstellar medium around the white dwarf

Summary Mid-infrared Imaging and Spectroscopic monitoring of Galactic dust forming novae  unique laboratories to study the process of dust formation and to understand the mass-loss history of the CO white dwarves from the chemical point of view - Late epoch observations t>1000 days are important to examine the chemical evolution of dust grains formed around novae in harsh UV radiation environment -High spatial resolution achieved by 8-10m class telescopes in the mid-infrared is indispensable to resolve the dust shell structures at those late epochs Excellent Performance of Gemini-S/TReCS, not just in N-band, but also in Q-band Subaru/COMICS; Useful N-band, Q-band Spectroscopic capability with slit viewer  crucial to examine the distribution of each dust component by means of the spectral decomposition of the spatially resolved spectra Whole sky coverage achieved by Subaru/COMICS and Gemini-S/TReCS - Strong advantages in the chemical understanding of dust formation around evolved stars - Good collaboration with Space Infrared missions (AKARI, SPICA, etc.) - Observations of time varying phenomena with a timescale of several years; (novae, Wolf-Rayet +O-type binary stars, nearby supernovae, optical transients etc.) - Continuous multi-epoch observations are indispensable

Hydrogenated Amorphous Carbons (HACs) (Duley & Williams et al. 1990) -contain PAH-like units weakly bounded by van der Waals forces -consist of a mixture of aromatic hydrocarbons dominated by sp 2 bonds which can produce the polycyclic ring and aliphatic hydrocarbons including sp 1 bonds (like in acetylene) and sp 3 bonds (like in methane). The “aromatic” to “aliphatic” ratio in HACs can be modified by the irradiance of UV fields. Polycyclic Aromatic hydrocarbons (PAHs) (Allamandola et al. 1989) 3.3  m feature; aromatic C-H stretch mode 3.4  m feature; aliphatic C-H stretch mode Near infrared spectrum of NGC1333 with UKIRT (Joblin et al. 1996)