From kawabata@subaru.naoj.org Tue Oct 29 13:27:51 2002 Dear David, We will submit our next proposal for Subaru SN observation in a day. I would like you to join us again if it is fine with you. The TeX source is attached below, and its PS-file version is available at http://www.astr.tohoku.ac.jp/~kawabata/prop2.ps I am sorry, but the remaining time is short before deadline. If you have comments, please tell me within a day. Sincerely yours, Koji S. Kawabata Cc: Nomoto-sama --- % Template for Subaru proposals (as of S03A) % % If you are using LaTeX2e, you should uncomment the \documentclass and % \usepackage lines and comment the \documentstyle line. %\documentclass{article} %\usepackage{subaru} \documentstyle[subaru,epsf]{article} \begin{document} % Set this to the current Subaru semester \semester{S03A} % After submitting your proposal electronically, please insert here the % proposal ID returned by PROMS, so your electronic submission can be % matched to the hardcopies which arrive in Mitaka. \proposalid{} % % Uncomment this line if this is an Open Use Intensive Program %\intensive % % Enter your title here; it should fit on one line when printed \title{Polarimetry of Supernovae -- Probing the Origin of Asymmetric Explosions} % Enter the Principal Investigator's information here \PIfirstname {Koji} \PIinitial {S.} \PIlastname {Kawabata} \PIinstitute {Optical and Infrared Astronomy Division, National Astronomical Observatory of Japan} \PIaddress {Osawa 2-21-1, Mitaka, Tokyo 181-8588, Japan} \PIemail {koji.kawabata@nao.ac.jp} \PIphone {+81-422-34-3533} \PIfax {+81-422-34-3545} % Uncomment ONE of the following lines to indicate the scientific category %\SolarSystem %\NormalStars %\ExtrasolarPlanets %\StarandPlanetFormation \CompactObjectsandSNe %\MilkyWay %\LocalGroup %\ISM %\NearbyGalaxies %\StarburstGalaxies %\AGNandQSOActivity %\QSOAbsorptionLinesandIGM %\ClustersofGalaxies %\GravitationalLenses %\HighzGalaxies %\DeepSurveys %\LargeScaleStructure %\CosmologicalParameters %\Miscellaneous % Enter your abstract here. Please ensure it fits in the space provided. \begin{abstract} Asymmetry is an important factor in the use of supernovae as distance indicators because the luminosity can be view-angle dependent. It provides clues to the physics of supernova explosions and to the structure of circumstellar matter and hence the progenitor evolution. Existing SN polarization data suggested that {\it all} core-collapse SNe (SN II, Ib/c) are intrinsically polarized at a level of about 1\% and thus pointing to significant asymmetry. Spectropolarimetry of two nearby Type Ia supernovae (SN 2001el and SN 2002bo) have successfully been obtained both with significant detection of intrinsic polarization. Our recent success in obtaining polarimetry observations of a hypernova SN 2002ap using FOCAS proves polarimetry as a unique tool in probing the structure of supernova ejecta. We expect SUBARU+FOCAS to play a critical role in building up a database of well observed nearby supernovae with spectropolarimetry coverage. Such a database is important in understanding the complicated physical mechanisms of supernova explosions on the one hand, and assessing the significance of systematic effects in using SN Ia as distance indicators on the other. \end{abstract} % Enter name and institution of each Co-I % e.g., \CoI{I. Newton}{University of Cambridge} \begin{investigators} \CoI{K. Nomoto,~K. Maeda,~J. Deng}{\hspace*{4em}Univ. of Tokyo} \CoI{G. Kosugi,~T. Sasaki}{Subaru Telescope, NAOJ} \CoI{T. Takata,~K. Aoki}{Subaru Telescope, NAOJ} \CoI{M. Iye}{Opt.\& IR Astron. Div., NAOJ} \CoI{D. Baade}{ESO, Germany} \CoI{L. Wang}{LBNL, USA} \CoI{P. H\"oflich,~J. C. Wheeler}{Univ. of Texas, USA} \CoI{D. J. Jeffery}{New Mexico Tech, USA} \CoI{P. Mazzali}{Trieste Observatory, Italy} \end{investigators} % List all relevant publications here. \begin{publications} \normalsize Howell, D. A., H\"oflich, P., Wang, L., \& Wheeler, J. C. 2000, ApJ, 556, 320: \footnotesize{Evidence for Asphericity in a Type Ia SN 1999by} \smallskip\\ \normalsize Kawabata, K. S., Jeffery, D. J., Iye, M., Ohyama, Y., et al. 2002, ApJL, in press: \footnotesize{Optical Spectropolarimetry of SN~2002ap: A High Velocity Asymmetric Explosion} \smallskip\\ \normalsize Maeda, K., Nakamura, T., Nomoto, K., Mazzali, P. A., Patat, F., Hachisu, I. 2002, ApJ, 565, 405: \footnotesize{Explosive Nucleosynthesis in Aspherical Hypernova Explosions and Late-Time Spectra of SN 1998bw} \smallskip\\ \normalsize Mazzali, P. A., Deng, J., Maeda, K., Nomoto, K., et al. 2002, ApJ, 572, L61: \footnotesize{The Type Ic Hypernova SN 2002ap} \smallskip\\ \normalsize Wang, L., H\"oflich, P., Khokhlov, A., Wheeler, J., Baade, D., and the SINS team, ApJ, submitted, \footnotesize{The Bipolar Ejecta of Supernova 1987A} \smallskip\\ \normalsize Wang, L., Howell, A. D., H\"oflich, P., \& J. C. Wheeler, 2000, ApJ, 550, 1030: \footnotesize{Polarimetry of Core-collapse Supernovae} \smallskip\\ \normalsize Wang, L., \& Wheeler, J. C. 2002, Sky \& Telescope, 103, part no 1, 40: \footnotesize{Supernovae are not round} % \smallskip\\ \end{publications} % For each observing run, enter the instrument, number of nights requested, % lunar phase (Dark/Gray/Bright), preferred dates, acceptable % dates, and % configuration. Fractional nights are now accepted. % e.g., \run{IRCS}{1}{Bright}{Dec/early Jan}{Nov--Feb}{K grism} \begin{observingrun} %\run{}{}{}{}{}{} \run{FOCAS}{3}{Gray}{Apr/Sept}{Apr/Sept}{Gr. 300B+SY47 or L600 } % Enter the minimum acceptable number of nights to achieve your science % goals. You may leave this empty if you require your full request. \minnights{2} \end{observingrun} % Uncomment the following line if you do not want the technical reviewer % to see your target names %\hidetargets % Enter your targets here: name, RA, dec, equinox, magnitude % e.g., \target{4C~41.17}{06 50 52.10}{+41 30 30.5}{J2000.0}{$K=19.1$} \begin{targets} \target{SN2003XXXX}{00 00 00.00}{+00 00 00.0}{J2000.0}{$V<17$} \end{targets} % Explain any scheduling requests noted above. \scheduling{This is a ToO (Target of Opportunity) observation. An assignment of a half (or quarter) night is also acceptable when the target is bright enough.} %\scheduling{ToO} % Add any further instrumentation requirements, or details of your own % instrument. \instruments{Polarimetry optics are request for this program} % Please briefly describe your experience, ability, need of assistance, % etc. for making observations with Subaru % \experience{PI and some Co-Is belong to the FOCAS instrument team and have sufficient experiences of observations with the FOCAS and the Subaru telescope. We need only normal assistance by the support astronomer and by the telescope operator. Our team consists of experienced observers and theorists in analyzing and modeling polarimetry data of supernovae. } % Briefly describe your backup proposal. Please include target names so % conflicts with accepted proposals can be spotted. \backup{} % Put the Observing Method and Technical Details here. \begin{technicalinfo} We use the typical long-slit spectroscopic mode ($R\sim 600$) of the FOCAS. \begin{itemize} \item Filter: either Y47 or L600 \item Grism: 300B \item Slit width: 0.8" center/offset slit \item Readout mode: whole CCD and normal speed \item Necessary S/N: 30 \end{itemize} For spectropolarimetry, we will use the Wollaston prism and the half-wave plate. A typical observing sequence consists of four integrations at the 0, 45, 22.5 and 67.5 degs positions of the half-wave plate. \begin{itemize} \item Necessary S/N in each integration: 300 \end{itemize} Note that exposure time varies with the type and brightness of the SNe. For SN Ia before maximum and $V \sim 13$, we will target for accuracies around $\Delta P =0.1$--$0.2$ \%/pixel, whereas for SN II, Ibc, $0.2$--$0.4$ \%/pixel is enough. The total exposure time of each observation (four integrations) is approximately \[ t \simeq 10^{4} \times \frac{0.1 \mbox{ \%}}{\Delta P} \times 10^{-0.4(V-15)} \mbox{ seconds.} \] \end{technicalinfo} % If this proposal is a continuation of an accepted proposal (or a % resubmission of one which was weathered out for example), enter the % proposal ID and title here. \continuation{}{} % If these observations are intended to be part of a student's thesis, % enter the student's name and thesis title. \thesis{}{} % Enter your previous Subaru runs from the last 3 years. Enter year/month, % Proposal ID, PI name, status of data reduction, and status of publications \begin{previoususe} %\pastrun{}{}{}{}{} \pastrun{2001/3}{S00-022}{K. Nomoto}{Data reduced/analyzed}{Paper to appear in PASJ} \pastrun{2002/10-}{S02B-181}{K. Nomoto}{ToO; not yet triggered}{} \end{previoususe} % If you have more targets, please uncomment the following 3 lines and % enter them here, using the same format as above. %\begin{moretargets} %\target{}{}{}{}{} %\end{moretargets} \scijust % Enter your scientific justification here (maximum 2 pages, including % figures and additional references). SN 1987A represented a breakthrough by providing the first detailed record of the polarimetric evolution (Cropper et al. 1988, MNRAS, 231, 695; Mendez et al. 1988, ApJ, 334, 295). SN 1993J also provided a wealth of data (Trammell, Hines, and Wheeler 1993, ApJ, 414, L21). Spectropolarimetry probes the geometrical structures of the supernova (SN) debris which are closely related to the explosion mechanisms and the progenitor systems. Core-collapse SNe are found to be generally more highly polarized than thermonuclear SNe (SN Ia) (Wang et al. 1996, ApJ, 467, 435; 2001, ApJ, 550, 1030; Howell et al. 2001, ApJ, 556, 302). A peculiar, subluminous SN Ia was found to be polarized at 1\% level (Howell et al. 2001). The recent FOCAS observations of the hypernova SN 2002ap shows that polarimetry can provide unique information on the structure of a supernova ejecta (Kawabata et al. 2002, ApJ, in press). In particular, we have identified a high velocity component which may be associated with a jet produced during the supernova explosion. The database of supernova polarimetry however are still sparse, these earlier results should be considered preliminary. It is the goal of this proposal to obtain a data set that is of sufficient quantity and quality to address many of the critical issues on the physics of supernova explosions and the use of them as standard candles for probing the dark energy content of the universe. {\bf 1. Thermonuclear Explosions (Type Ia)} Type Ia SNe are crucial for determining cosmological distance scales and the dynamics of the Universe. Significant asymmetries would mean the luminosity to be dependent on the viewer aspect angle which could make a SN less reliable as a distance calibrator. Polarization data are therefore of fundamental importance as a self-consistency check for SNe as distance calibrators, and to understand the remaining 10\% luminosity scatter of stretch-corrected SNe Ia to determine H$_0$ and the dark energy content. Our collaborator have observed successfully three pre-maximum SN Ia (SN 2001V, SN 2001el and SN 2002bo) using the ESO+VLT. All three SNe are polarized before optical maximum. The polarization of SN 2001el diminished post-maximum. Most SN Ia have small polarization. The polarization can be modeled and gives clues to the physics of the deflegation of the white dwarf (Wang, Wheeler, \& H\"oflich 1997, ApJ, 476, L27). The observations will be used to test SN Ia models based on a close binary system involving a white dwarf (WD) and a main sequence, subgiant or red giant star as the progenitor of SN Ia. According to recent calculations of Marietta, Burrows, and Fryxell (ApJS, 128, 615, 2000) the impact of the SN ejecta with the secondary star creates a hole in the SN debris with an angular size of $\sim 30^{\circ}$ in the ejecta which corresponds to 7\%-12\% of the ejecta's surface. Such a hole, if it exists, is expected to produce average polarizations of around 1\%. A low observed degree of polarization therefore implies that either the hole is very close to the line of sight (in front of or behind the WD), or the models have to be modified. The spectral profiles would also be tests for such models when viewed at different angles. Asymmetry probes also the complicated explosion mechanisms of SN Ia. Recently, Livne (ApJL, 527, 97, 1999) pointed out that the deflagration/detonation transition may be aspherical. Polarimetry will provide the necessary guidance for these and many other complicated models. It thus seems that the low observed degree of polarization of SN Ia in previous studies is by no means a final answer to polarimetry properties of this group of SNe. These data are important for using SN Ia as distance calibrators. To test the effect of asymmetry on the luminosity of SN Ia, SNe in the smooth Hubble flow are required, which are usually too faint for small telescopes but can be comfortably observed by SUBARU telescope. Polarimetry will be combined with photometric data to study the effect of asymmetry on distance calibrations using SN Ia. Time evolution is critical. We would like to know at which phase an SN Ia shows lower degrees of polarization so that it can be a 'better' calibrator. {\it We require the large aperture of the SUBARU to make careful measurements of the polarization of more SN Ia to determine their origin and whether asymmetry could affect distance estimates.} {\bf 2. Core-collapse Supernovae} Earlier studies are suggestive that core-collapse SNe show higher polarizations for events with smaller envelope mass and that the polarization increases with time as we see to greater depth in a single event. (Wang et al. 2001, ApJ, 550, 1035; Leonard et al. 2001, ApJ, 553, 8611). This suggests that the core collapse process may be intrinsically asymmetric and that the asymmetry is damped by an extensive envelope. The data on Type Ic SN 1997X showed strong polarization, well in excess of 1 \%. This is an especially exciting observation because SN 1997X must have occurred in a nearly naked, non-degenerate, carbon/oxygen core. There is little mass to diffuse an asymmetrical explosion and render it more spherical. There is thus the tantalizing expectation that in SN 1997X we may be seeing the direct effects of a strongly asymmetric explosion. SN polarimetry is still an under-cultivated field which promises rich and interesting scientific returns, and surprises. The hypernova SN~2002ap serves as a nice example as shown in Figure 1. The degree of polarization is nearly 1\%, which is among the average values for SN II events. The polarizations and their time evolution will allow us to study the geometry of different chemical layers. The positive detection of polarization features across spectral lines implies that the ejecta are asymmetric. In particular, the data are suggestive of a high velocity jet material. \begin{figure} \begin{flushleft} \epsfysize=9cm \epsfbox{sn02apb.eps} \caption{FOCAS spectropolarimetry of SN 2002ap} \end{flushleft} \end{figure} Many questions can be asked of these canonical events. Is the progenitor in a binary system ? Is the asymmetry due to external circumstellar material or is it from deep inside the stellar core ? If the origin of the asymmetry is from near the stellar center and the symmetry axis is constant, as is consistent with the observed polarimetry evolution, the central engine for the explosion must be highly aspherical and co-aligned so that the asymmetry can still influence the outermost part of the ejecta. We need SUBARU data to follow a number of core-collapse events to late times to determine if the polarization anti-correlates with envelope mass and luminosity and how it varies with time. The SUBARU data will help to establish whether or not the the core-collapse process is intrinsically strongly asymmetric and the nature of the asymmetry, eg, jet-like. This program aims to make use of the SUBARU telescope to obtain high quality spectropolarimetric data on 3-6 SNe brighter than V=16 mag. Because the current data are sparse and every new SN adds to our understanding of SN asymmetry, we will observe all types of SNe that are available. We will observe Type Ia SNe down to a noise level $\sim$ 0.2\%, with a spectral coverage from 4100 to 8600 \AA. To probe core collapse, it is important to monitor asymmetries as the SN fades and the photosphere recedes, so these events need to be followed to faint epochs, outside the reach of 4-m telescopes. The data will be used to study both the properties of the SNe and of the interstellar dust in the host galaxies of the SNe. Some immediate applications include: {\bf (a)} Polarimetry data base. With this data we will expand the statistical base, the time coverage, and the quality of the data. We will attempt to test our hypothesis that Type Ib/c are systematically more polarized than Type II. We will attempt to study the geometry of the ejecta and correlate it with the observed luminosity. The data will be used to isolate different mechanisms to produce polarization and to constrain physical mechanisms of core collapses. We will seek to determine the frequency, amplitude and cause of the polarization of Type Ia, and determine the effect of asymmetry on the luminosity of an SN Ia. {\bf (b)} Models. We will explore multi-dimensional physical models of thermonuclear explosions in Type Ia and core collapse in Type II and Ib/c to understand the origin and nature of asymmetries. Some asymmetry is expected in the turbulent burning of a white dwarf in a Type Ia, but large polarizations may require an external influence such as a companion or an accretion disk. We will be able to test dynamical models of core collapse that generate jets to determine the degree of fundamental asymmetry in the explosion necessary to imprint a certain polarization in the homologously expanding ejecta. We will also compute multi-dimensional radiative transfer to determine the predicted polarization spectrum to compare to the observations. {\bf (c)} Dust properties. This program yields the wavelength dependence of the degree of polarization of the ISM as a by-product. The ISM data gives the wavelength of the maximum polarization which is a sensitive diagnostic of the reddening coefficient $R_V\ =\ A_V/E(B-V)$. Our preliminary result is that the reddening coefficient is different for the host galaxy of every SN and the result can deviate substantially from the canonical value of $R_{V}=3.1$. We will continue a systematic study of the interstellar polarization. {\it The large aperture of SUBARU provides the almost unique means to lead the small sample of SNe with spectropolarimetry out of statistical meaninglessness. This concerns especially studies of individual spectral features, which are crucial for all types of SNe and would be wiped out by strong binning, and the follow-up into advanced stages of core-collapse SNe, when the inner layers of the progenitor become accessible and so come closer to the zone of origin of the asymmetry. } \end{document}