IMAGER: Expected results from UV dust observations of M101 M. E. Danowski1, T. A. Cook1, K. D. Gordon2, S. Chakrabarti1 1Department of Astronomy and Center for Space Physics, Boston University; 2 Space Telescope Science Institute Background The Interstellar Medium Absorption Gradient Experiment Rocket (IMAGER) will probe the correlation between ultraviolet dust extinction, and the metallicity and radiation environment in M101. Evidence from studies of starburst galaxies (Englebracht et al. 2008) indicate that active, high-mass star formation modifies the UV dust extinction curve, demonstrated by the lack of a 2175 Å bump. With photometry from IMAGER, we measure the apparent strength of the 2175Å bump, the UV continuum, and the far-UV rise− the spectral features which probe the nature of dust formation and processing in these areas near massive star formation. With four 400Å-wide bandpasses, IMAGER is sensitive to these UV extinction features and will utilize M101 as a laboratory for studying dust in HII regions. M101 is nearly face-on, has large angular extent, contains many well studied HII regions, and has a steep metallicity gradient, log(O/H)+12 = 7.4 8.8 (Kennicutt et al. 2003). RUV1 RUV2 RUV3 RUV4 Our data, when combined with infrared data from Spitzer, the DIRTY radiative transfer model, and models of stellar evolution, will allow us to examine the changes seen in the UV extinction curve and the IR emission features as a function of metallicity and radiation field hardness. This study will directly impact our understanding of the nature of dust and our ability to accurately account for the effects of dust on observations at all redshifts. Experiment Dichroics Detector Secondary Mirror Results RUV4 RUV3 RUV2 Electronics Tertiary OAP Fold Mirror Primary Mirror Figure 3 (Top Left): Color-color plot of expected IMAGER data from idealized dichroics. The lines are for different combinations of PEGASE stellar evolutionary synthesis (Fioc & RoccaVolmerange 1998), and DIRTY (radiative transfer) models. The large angle between trajectories for these models combined with the age dependency ensures that any point can be unambigulously assigned to a given dust model. Figure 4 (Top Right) A similar color-color plot, but for GALEX & u-band data. The smaller trajectory angle makes it difficult to clearly determine the type of dust. Figure 5 (Bottom Left): Color-color plot from expected IMAGER data with system response. Figure 6 (Bottom Right) Simulated IMAGER Observations with superimposed Hα-selected circular apertures. RUV1 Star Tracker Fold Mirror R R MCP U U Detec V V 2 3 tor R1 R 1 focal U U 6 9 plane V V 0 5 Beam Fold 01 04 from Mirror 1 2 Å Å Tertiary 3401 0 2 IMAGER DESIGN 0 0 9 4 Telescope f/12.29 Ritchey-Chretien Å Å 5 0 00Primary Mirror 0.5 meter, AlMgF2 coated for high reflectance 1 in UVÅ 2 Å 6 8 0 tolerances Field of View 30 arcminutes, fits M101 with pointing and 0alignment 0 0 Å Å Dichroic Bandpasses Four from three dichroic beamsplitters (see Figure 2) One on 2175 Å bump, one on FUV rise Two on UV continuum Detector Photon-counting microchannel plate z-stack detector wedge-and-strip with four anodes from Photek Photocathode CsTe, QE ~10-15% across observed wavelengths Electronics Refurbished previously flown sounding rocket electronics Resolution 9 arcseconds including pointing & alignment error, and detector resolution Figure 1 (Top): Simulated IMAGER Observations with nominal flight/observing time t=389s, 6 arcsecond resolution, and expected dichroic and detector response. Figure 2 (Bottom) Measured extinction curves (Gordon et al. 2003). Normalized IMAGER response curves to illustrate sensitivities of IMAGER bands to dust features. Analysis All IMAGER data will be calibrated for sensitivity, bandpass, and resolution at Boston University. Using this information, we reduce raw data and perform aperture photometry on the HII regions in the four IMAGER ultraviolet bands. HII regions are visually identified by correlating the UV images with Hα (van Zee et al. 1998). We measure the flux within a circular aperture of 12 arc seconds at each HII region. We also calculate and correct for the sky background. To examine the strength of the 2175Å feature and the FUV rise, we generate color-color plots and compare these to curves calculated from models of stellar evolution, taking into account our system response and radiative transfer effects. We then compare the strength of these features at a given galactic location and compare to the local galactic properties. Local dust content and aromatic feature strength are measured from Spitzer, radiation field hardness is measured from line ratios, and the metallicity is also available from measured emission lines. We will compare galactic environment (metallicity and radiation hardness) on a pixel-to-pixel scale with the observations to determine the relationship of the dust properties to the environment. Observations with the Spitzer Space Telescope have revealed that the strength of the aromatic features (PAH features) correlates better with radiation field hardness, a tracer of processing due to massive star formation, than it does with metallicity, a tracer unaffected until a threshold of radiation hardness. We will examine if this correlation extends to the UV– Are the UV extinction features best correlated with the aromatic features and radiation hardness, or are they better correlated with the metallicity? If, as we expect, the 2175Å feature traces the aromatic/PAH features, we would anticipate the central region of M101 (radius of a few arcminutes) to all have the same strength 2175Å bump; past this ‘threshold radius’ the strength of the bump should decrease rapidly. However, if the strength of this feature is better correlated with metallicity, which strongly varies from the galactic center to the outer edges, then we would expect the strongest 2175Å features to lie in the center of the galaxy, at the nucleus, and then decline outwards. Some dust grain models suggest that the 2175Å bump and the aromatic features are carried by the same material (Li & Draine 2002). Observations from IMAGER will provide an excellent probe of this hypothesis. References Fioc, M., & Rocca-Volmerange, B. 1997, A&A, 326, 950 Gordon, K.D., Clayton, G.C., Misselt, K.A., Landolt, A.U., & Wolff, M.J. 2003, ApJ, 594, 279 Gordon, K.D., Engelbracht, C.W., Rieke, G.H., Misselt, K.A, Smith, J.-D.T., Kennicutt, Jr., R.C. 2008, 682, 336 Kennicutt, Jr., R.C., Bresolin, F., & Garnett, D.R. 2003, ApJ, 591, 80 Li, A. & Draine, B.T. 2002, ApJ, 576, 762 van Zee, L., Salzer, J.J., Haynes, M.P., O’Donoghue, A.A., & Balonek, T.J. 1998, AJ, 116, 2805 Acknowledgments IMAGER is a NASA sounding rocket experiment set to launch in 2011. This work is supported by NASA grant NNX09AE23G.