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                <value>Wolf-Rayet Stars in IC10: Probing the Massive Star Content
of the Nearest Starburst</value>
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              <param name="abstract">
                <value>IC~10 is a Local Group galaxy currently undergoing a galaxy-wide
starburst (Massey \&amp; Armandroff 1995).  Starburst galaxies have
often been suspected of having a top-heavy IMF, although the evidence
in general has been indirect (i.e., M82 according to 
Rieke et al.\ 1980).  Previous work on the evolved massive star
population of IC~10 suggested that it too might have a top-heavy
IMF as evidenced by the relatively large ratio of WC-type to WN-type
Wolf-Rayet stars. However, a newly completed
survey has detected a wealth of new Wolf-Rayet candidates
(Massey \&amp; Holmes 2003).  If these are spectroscopically confirmed
as predominately of WN-type, the IMF of this starburst system may
be normal, although the massive star population (and hence the
amount of ``burst") may be factors of 5 higher than the already 
large value previously thought.  IC~10 is the only starburst
system sufficiently close to determine the massive star population
{\it directly}, but it requires spectroscopy with Gemini-N and GMOS
to take advantage of this unique opportunity.</value>
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                  <value>Starburst galaxies are undergoing intense star formation at a
rate that is unsustainable on a Hubble time (e.g., Searle \&amp; Sargent
1972). The nearest such object is the small irregular Local Group
galaxy IC~10. Van den Bergh (2000) kindly credits the 
recognition of IC10's starburst nature to  Massey \&amp; Armandroff (1995),
who identified $\sim 20$ Wolf-Rayet stars (WRs).  WRs are the He-burning
descendents of the most massive O-type stars, and this high number in
such a small galaxy was considered quite remarkable; for comparison,
NGC~6822, another Local Group irregular of comparable absolute visual
magnitude contains only 4 WRs (Massey \&amp; Johnson 1998).  Other lines
of evidence, such as the H$\alpha$ luminosity, also argue for a starburst
nature (Hodge \&amp; Lee 1990; Youngblood \&amp; Hunter 1999; Hunter 2001). 
The galaxy is embedded in an extended H~I envelope (Huchtmeier 1979);
presumably infalling gas
fuels the burst.

The proximity of IC~10 gives us a unique opportunity
to study the effects that an intense burst has on the {\it process}
of star formation, and in particular the slope of the stellar initial mass
function (IMF).  There has long been the theoretical expectation that
the IMF would be be top-heavy in regions of intense star formation
(Larson 1986).  And, indeed such a 
claim has been made for the starburst galaxy M~82 (Rieke et al.\ 1980), 
based admittedly on fairly indirect evidence
(see Scalo 1990 and Leitherer 1998).  
However, direct measurement
of the IMF in the energetic central 
cluster (R136) of the 30 Dor giant HII region 
by Massey \&amp; Hunter (1998) found a perfectly normal IMF.

Stiil, there is evidence to suggest that IC~10 may in fact have
a top-heavy IMF.  Wolf-Rayet stars occur as two distinct types: those
of the WN class, which show the products of H-burning at their surfaces,
and those of the WC class, which show the products of He-burning at their
surfaces.    The mass range that is expected to evolve to WCs or WNs
should be a function of metallicity (due to the effect
that radiatively-driven stellar winds have on the evolution of massive stars)
but at a given metallicity the WCs will {\it on average} be descended from
more massive stars than are the WNs. (See discussion in Massey \&amp; Johnson 1998
and Massey 2003).  The WR stars found by Massey \&amp;
Armandroff (1995) were predominantly of WC type, unexpected in a galaxy
of IC~10's low metallicity (Fig.~1).  One explanation is that the IMF
is more weighted in favor of massive stars in IC~10 due to its current
starburst (Massey \&amp; Armandroff 1995; Massey \&amp; Johnson 1998).

However, another possibility exists: WNs are more difficult to detect than WCs
as their strongest emission lines are about a factor of 4 weaker than
those of WCs, and thus completeness for WNs is much harder to achieve in
any kind of a survey. (That is why the point for the Milky Way is also a bit
high in Fig.~1---the sample there is probably not complete for WNs, as 
discussed in Massey 2003).  IC10's low galactic latitude ($-3.3^\circ$)
results in a large galactic foreground reddening ($E(B-V)=0.75-0.80$, according
to Massey \&amp; Armandroff 1995) further complicating detection.
Accordingly, two years ago we proposed and were
granted time on the 4-m Mayall to conduct a deeper
imaging survey for WR stars using Mosaic and our ``optimized" interference
filters centered on WR emission lines.

Our survey has uncovered a wealth of additional candidates 
(Massey \&amp; Holmes 2003; see also Crowther et al.\ 2003). By
comparing the number of detections with those of a nearby
control field, we conclude that the total number of WRs
in IC10 might be as great as 100. If the 
majority of the new candidates are of WN-type (which might be expected if
the stronger-lined WCs have mostly all been previously detected), 
then these new candidates
could even lower the WC to WN ratio to normal---with the implication that
the IMF is also normal.  Of course, this would also imply that IC~10 is
an even more extreme starburst than previously thought!  
So far, only two of these new
candidates have been observed spectroscopically---both confirmed
as WNs.  To obtain a reasonably complete sample requires the large aperture
of Gemini and the multiplexing capability of GMOS.

\begin{figure}
\epsscale{0.85}
\plotone{N0163.01.eps}
\caption{The relative number of WC and WN stars is well correlated with
metallicity
as we would expect; the exceptions are the Milky Way, and IC~10.
The fact that the Milky Way ratio is high is easy to understand: the sample
within 2.5~kpc is probably not complete for WNs.
This figure has been adopted from Massey \&amp; Johnson 1998, with the
errors bars showing the effects of $\sqrt{N}$
statistics on the ratios.}
\end{figure}

\reference Armandroff, T. E., \&amp; Massey, P. 1995, AJ, 109, 2470
\reference Crowther, P. et al.\ 2003, A\&amp;A, 404, 483
\reference Hodge, P., \&amp; Lee, M. G. 1990, PASP, 102, 1245
\reference Huchtmeier, W. K. 1979, A\&amp;A, 75, 170
\reference Hunter, D. A.  2001, ApJ, 559, 225
\reference Larson, R.  1986, MNRAS, 218, 409
\reference Leitherer, C. 1998, in The Stellar Initial Mass Function,
ed. G. Gilmore \&amp; D. Howell, 61
\reference Massey, P. 2003, {\it ARA\&amp;A}, 15, 41
\reference Massey, P. \&amp; Holmes, S. 2002, ApJ, 580, L35
\reference Massey, P., \&amp; Hunter, D. A. 1998, ApJ, 493, 180
\reference Massey, P., \&amp; Johnson, O. 1998, ApJ, 505, 793
\reference Rieke, G. H., Lebofsky, M. J., Thompson, R. I.,
Low, F. J., \&amp; Tokunaga, A. T. 1980, ApJ, 238, 24
\reference Scalo, J. M. 1990, in Windows on Galaxies, ed. A. Renzini,
G. Gabbiano, \&amp; J. S. Gallagher, 125
\reference Searle, L., \&amp; Sargent, W. L. W. 1972, ApJ, 173, 25
\reference van den Bergh, S. 2000, The Galaxies of the Local Group
\reference Youngblood, A. J., \&amp; Hunter, D. A. 1999, ApJ, 519, 55

\begin{figure}
\epsscale{0.75}
\plotone{N0163.02.eps}
\caption{This plot shows a simulation of the detection of He~II $\lambda 4686$
with parameters typical of a weak-lined WN stars; e.g., a line width of
20\AA\ and a equivalent width of -10\AA.  The S/N per 0.9\AA (binned) pixel
is indicated.}
\end{figure}

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                  <value>NOAO PAST USE: {\bf Recent (2000-2003) allocation of time:}

{\bf 2004A-200:} The Physical Parameters of Red Supergiants:
When Massive Stars Are as Cool as They Get, 10 nights KPNO 2.1-m (5 successfully
carried out in March, 5 more scheduled in late May), plus 5 nights CTIO 1.5-m
scheduled for April.  

{\bf Target of Opportunity:} Spectroscopy of a Newly Found Dwarf Irregular,
2 hrs kindly granted by Richard Green on the 2.1-m with GoldCam, April 2003.
The data appear in Massey, Henning, \&amp; Kraan-Korteweg, 2003, AJ, 126, 2362

\relatedwork{{\bf 2002B-218:} The Evolution and Physical Parameters of
Massive Stars at High Metallicity: O Stars in the Andromeda Galaxy", 3 nights
MMT Sept 2002.  We obtained only 0.5 nights out of 3
nights scheduled, due to weather, but published what we were able to get in
Massey \&amp; Holmes 2002, ApJ, 580, L35}

{\bf 2001A-062:} A {\it UBVR} Survey of the Magellanic Clouds, 6
nights
CTIO Curtis Schmidt April 2001: Massey 2002, ApJS 141, 81

\relatedwork{{\bf 2001B-002:} The Wolf-Rayet Content of IC10, 2 nights Mayall
4-m Sept 2001: Massey \&amp; Holmes 2002, ApJ, 580, L35}

{\bf 2001B-227:} The Red Supergiant Content of the Magellanic 
Clouds, 3 nights
CTIO 4-m Hydra, October 2001.  
Massey \&amp; Olsen 2003, AJ, 126, 2867 

{\bf 2000B-010:} A Survey of Local Group Galaxies Currently Forming Stars,
on-going survey project.  We are current with all of our data reductions,
and are completing the photometric analysis.  Some data appear in
Di Stefano et al. 2004, ApJ, in press (astroph-0306440)

{\bf 1999B-099; 2000B-070:}
Where Do Wolf-Rayet Stars Come From?
CTIO 1.5-m 5 nights October 2000; 6 nights October 1999:
Massey \&amp; Duffy 2001, ApJ 550, 713; Niemela et al. 2002,
MNRAS, 333, 347

\noindent
{\bf Recent papers (2002-2004) based upon NOAO data:}

\parindent=10pt

Massey, P., Bresolin, F., Kudritzki, R. P., Puls, J., \&amp; Pauldrach. A. W. A.
``The Effective Temperature Scale of O-type Stars as a Function of Metallicity.
I. A Sample of 20 Stars in the Magellanic Clouds", ApJ, in press (June 20 issue,
astroph/0402633)

Walborn et al.\ 2004, ``A CNO Dicomotomy Among O2 Giant Spectra in the
Magellanic Clouds", ApJ, in press (June 20 issue)

Bianchi, L., Bohlin, R., \&amp; Massey, P. 2003, ``The Ofpe/WN9 Stars in M33",
ApJ, 601, 228

Massey, P. 2003, ``The Massive Star Content of the Local Group: Implications
for Star Formation and Stellar Evolution", ARA\&amp;A, 41, 15

Di Stefano et al. 2003, ``Supersoft X-Ray Sources in M31", ApJ, submitted,
astro-ph/0306440

Massey, P., Olsen, K. A. G., \&amp; Parker, J. W. 2003, ``The Discovery of a
12th Wolf-Rayet Star in the Small Magellanic Cloud", PASP, 115, 1265
astro-ph/0308237

Massey, P., Henning, P. A., \&amp; Kraan-Korteweg, R. C. 2003, ``A
Neighboring Dwarf Irregular Galaxy Hidden By the Milky Way",
AJ 126, in press (Nov issue), astro-ph/0308080

Massey, P., \&amp; Olsen, K. A. G. 2003, ``The Evolution of Massive Stars. I.
Red Supergiants in the Magellanic Clouds", AJ, 126, 2867
astro-ph/0309272

Morrell, N. I., Ostrov, P. G., Massey, P., \&amp; Gamen, R. 2003, ``Hodge 53-47:
An Early O-type Double-lined Binary in the SMC", MNRAS, 341, 583

Massey, P., \&amp; Holmes, S. 2002 ``Wolf-Rayet Stars in IC10: Probing the Nearest
Starburst", ApJ 580, L35

Massey, P. 2002, ``A UBVR CCD Survey of the Magellanic Clouds," ApJS, 141,
81

Massey, P. 2002, ``Observational Constraints on Massive Star Evolution"
(invited review), in {\it A Massive Star Odyssey, from Main Sequence to
Supernova, IAU 212}, ed. van der Hucht, Herrero, \&amp; Esteban, 316.

Slesnick, C. L., Hillenbrand, L. A., \&amp; Massey, P. 2002, ``The Star Formation
History and Mass Function in the Double Cluster h and Chi Persei", ApJ,
576, 880

Snow, T. P., Zukowski, D., \&amp; Massey, P. 2002, ``The Intrinsic Profile of
the 4428\AA\ Diffuse Interstellar Band", ApJ 578, 877

Niemela, V. S., Massey, P., Testor, G., \&amp; Benitez, S. G. 2002, ``The Massive
Wolf-Rayet Binary WR7 in the SMC", MNRAS, 333, 347

Walborn et al. 2002, ``A Giant O2-O4 Spectral Classification
Study", AJ, 123, 2754

Bianchi et al. 2001,``The Massive Star Content of  NGC 6822. Ground-based
and {\it HST} photometry, AJ, 121, 2020.

Massey, P. \&amp; Duffy, A. S. 2001, ``A Deep Search for Wolf-Rayet Stars in
the Small Magellanic Cloud", ApJ, 550, 713.

Massey, P., DeGioia-Eastwood, K., \&amp; Waterhouse, E. 2001, ``The Progenitor
Masses of Wolf-Rayet Stars and Luminous Blue Variables Determined from
Cluster Turn-offs. II. Results from 12 Clusters in the Milky Way",
AJ, 121, 1050.

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                  <value>***EXPERIMENTAL DESIGN***:

With Gemini-N, we will obtain GMOS
multi-slit observations of $\sim 30$ of our weaker-lined
Wolf-Rayet candidates.
The size of IC10 is a good match to the 5.5 arcmin diameter masks, and
we can use a single slit mask.  {\bf Time assigned for this project
in 2003B resulted in obtaining a suitable image from which we
designed a slit mask, but the spectroscopic data was never obtained.}

For the spectroscopy we need reasonable resolution and S/N for
a solid detection/non-detection: our WR candidates
are faint ($B\sim 22-23$) and the expected emission of the strongest
line (He~II $\lambda 4686$) weak
(EWs of -10\AA; see
Table 3 of Massey \&amp; Johnson 1998 ApJ, 505, 793).  The B600 grating offers
6\AA\ resolution (with a 1-arcsec slit), which is a good match to the
width of the spectral lines (10-20\AA).  We can bin by 2 pixels both
spatially and spectrally, and as our simulation shows (Fig.~3),
we require at least a S/N of 5 per 0.9\AA (binned) pixel
for a convincing detection of such a line.  According to the
GEMINI GMOS exposure time calculator tool, we will achieve this S/N
for a $B\sim 23$ object in a 5 hr
exposure (20 x 900 sec) assuming dark skies (20 percentile) and mediocre
seeing (80 percentile), using 1-arcsec wide slits.
We will do the observation in two sets of 10x900 seconds, moving the central
wavelength of the grating by 3nm to provide continuous wavelength coverage.

As part of our survey of Local Group galaxies we also obtained imaging through
our WR filters of {\it all} the Local Group galaxies currently active in
forming stars: ten fields covering M31, 3 fields covering M33, plus single
fields covering other Local Group galaxies.  We view this IC~10 half-night
as a test run for a more extensive proposal that will help identify the
evolved massive star population (both red supergiants and WRs) in these
nearby systems.

\proprietaryperiod{18 months}


***TECHNICAL DESCRIPTION***:

Dark time is needed as our objects are faint ($B\sim 23$) and the emission
weak.  The B600 grating provides good spectral coverage and adequate
resolution, and the observations can be obtained in ``mediocre" (for
Gemini!) seeing.  As a 900-sec exposure will be photon-noise limited,
we will combine 20 of these to obtain the equivalent of a 5-hr exposure.
In the experimental design section we argue that a S/N of 5 per 0.9\AA\
spectral resolution element is needed for certain detection of emission
in our weakest-lined cases (Fig.~2), and the GMOS ETC assures us we will
achieve this with a 5-hr exposure under dark skies and 80-percentile
seeing.

We were granted Gemini-N time for this project in semester 2003B, and
we obtained excellent imaging data under good seeing conditions that
went quite deep enough to design a slitlet mask.  But the spectroscopic
observations were never made.  The mask has been cut and is ready to go;
we require only a half night (5-hr plus overhead) to complete this project.

\geminidata{pcontactnum}{1}
{\bf Principal Contact:} Philip Massey</value>
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    Program accepted for rollover into semester 05A and 
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&lt;head&gt;&lt;title&gt;Phase 1 Proposal&lt;/title&gt;&lt;/head&gt;
	&lt;body bgcolor="#FFFFFF"&gt;
&lt;!--     prolog      --&gt;
&lt;a name="prolog"&gt;&lt;/a&gt;
&lt;!--     phase1Document      --&gt;
&lt;a name="phase1Document"&gt;&lt;/a&gt;
&lt;!--     summary      --&gt;
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		&lt;table width="100%" cellspacing="10" border="0"&gt;
&lt;tr&gt;&lt;td align="center"&gt;&lt;font size="+2"&gt;&lt;b&gt;GEMINI OBSERVATORY&lt;/b&gt;&lt;/font&gt;&lt;br&gt;&lt;i&gt;&lt;font size="+1"&gt;observing time request (HTML summary)&lt;/font&gt;&lt;/i&gt;&lt;/td&gt;&lt;/tr&gt;
		&lt;/table&gt;
&lt;p&gt;
&lt;p&gt;
		&lt;table width="100%" cellspacing="5" border="0"&gt;
&lt;tr&gt;&lt;td valign="top" colspan="2"&gt;&lt;b&gt;Semester: &lt;/b&gt;2004B&lt;/td&gt;&lt;td colspan="2"&gt;&lt;b&gt;Partner reference: &lt;/b&gt;&lt;br&gt;2004B0163R1&lt;/td&gt;&lt;td&gt;&lt;b&gt;PI time requested: &lt;/b&gt;&lt;br&gt;6.0 hours&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan="2"&gt;&lt;b&gt;Gemini reference: &lt;/b&gt;&lt;br&gt;GN-2004B-Q-12&lt;/td&gt;&lt;td valign="top" colspan="2"&gt;&lt;b&gt;Partner ranking: &lt;/b&gt;6&lt;/td&gt;&lt;td&gt;&lt;b&gt;PI minimum time requested:&lt;/b&gt;&lt;br&gt;0.6 nights&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan="2"&gt;&lt;b&gt;Instruments(s): &lt;/b&gt;&lt;br&gt;GMOS North&lt;/td&gt;&lt;td colspan="2"&gt;&lt;b&gt;NTAC recommended time: &lt;/b&gt;&lt;br&gt;6.0 hours&lt;/td&gt;&lt;td&gt;&lt;b&gt;PI future time requested: &lt;/b&gt;&lt;br&gt;0.0 nights&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td valign="top" colspan="2"&gt;&lt;b&gt;Observing mode: &lt;/b&gt;queue&lt;/td&gt;&lt;td colspan="2"&gt;&lt;b&gt;NTAC minimum recommended:&lt;/b&gt;&lt;br&gt;6.0 hours&lt;/td&gt;&lt;td&gt;&lt;b&gt;PI total from all partners: &lt;/b&gt;0.0 nights&lt;br&gt;&lt;i&gt;(joint proposals)&lt;/i&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan="2"&gt;&lt;b&gt;Time awarded: &lt;/b&gt;&lt;br&gt;6.0 hours&lt;/td&gt;&lt;td&gt;&lt;b&gt;Proposal submitted to: &lt;/b&gt;United States&lt;/td&gt;&lt;/tr&gt;
		&lt;/table&gt;
&lt;!--     investigators      --&gt;
&lt;a name="investigators"&gt;&lt;/a&gt;
&lt;hr&gt;
		&lt;table cellspacing="5" width="100%" height="167" border="0"&gt;
&lt;tr&gt;&lt;td valign="top" height="38"&gt;&lt;b&gt;Title:&lt;/b&gt;&lt;/td&gt;&lt;td height="38"&gt;&lt;b&gt;Wolf-Rayet Stars in IC10: Probing the Massive Star Content
of the Nearest Starburst&lt;/b&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td&gt;&lt;b&gt;Principal Investigator:&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Philip Massey&lt;/b&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td valign="top"&gt;&lt;b&gt;PI institution:&lt;/b&gt;&lt;/td&gt;&lt;td&gt;Lowell Observatory, 1400 W. Mars Hill Rd,Flagstaff, AZ  86001,USA&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td&gt;&lt;b&gt;PI status:&lt;/b&gt;&lt;/td&gt;&lt;td&gt;PhD/Doctorate&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td valign="top"&gt;&lt;b&gt;PI phone / fax / e-mail:&lt;/b&gt;&lt;/td&gt;&lt;td&gt;928-233-3264  / (928) 774-6296  / Phil.Massey@lowell.edu &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td&gt;&lt;b&gt;Principal Contact:&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Philip Massey&lt;/b&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td valign="top"&gt;&lt;b&gt;PC institution:&lt;/b&gt;&lt;/td&gt;&lt;td&gt;Lowell Observatory&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td valign="top"&gt;&lt;b&gt;PC phone / fax / e-mail:&lt;/b&gt;&lt;/td&gt;&lt;td&gt;928-233-3264  / (928) 774-6296  / Phil.Massey@lowell.edu &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td valign="top"&gt;&lt;b&gt;Co-investigators:&lt;/b&gt;&lt;/td&gt;&lt;td&gt;Shadrian Holmes: Univ of Texas, sholmes@astro.as.utexas.edu &lt;/td&gt;&lt;/tr&gt;
		&lt;/table&gt;
&lt;!--     abstract      --&gt;
&lt;a name="abstract"&gt;&lt;/a&gt;
&lt;hr&gt;
&lt;h3&gt;&lt;/h3&gt;
&lt;b&gt;Abstract:&lt;/b&gt;
&lt;i&gt;IC~10 is a Local Group galaxy currently undergoing a galaxy-wide
starburst (Massey \&amp;amp; Armandroff 1995).  Starburst galaxies have
often been suspected of having a top-heavy IMF, although the evidence
in general has been indirect (i.e., M82 according to 
Rieke et al.\ 1980).  Previous work on the evolved massive star
population of IC~10 suggested that it too might have a top-heavy
IMF as evidenced by the relatively large ratio of WC-type to WN-type
Wolf-Rayet stars. However, a newly completed
survey has detected a wealth of new Wolf-Rayet candidates
(Massey \&amp;amp; Holmes 2003).  If these are spectroscopically confirmed
as predominately of WN-type, the IMF of this starburst system may
be normal, although the massive star population (and hence the
amount of ``burst&amp;quot;) may be factors of 5 higher than the already 
large value previously thought.  IC~10 is the only starburst
system sufficiently close to determine the massive star population
{\it directly}, but it requires spectroscopy with Gemini-N and GMOS
to take advantage of this unique opportunity.
&lt;/i&gt;
&lt;!--     scienceJustification      --&gt;
&lt;a name="scienceJustification"&gt;&lt;/a&gt;
&lt;hr&gt;
&lt;h3&gt;Science Justification&lt;/h3&gt;
Starburst galaxies are undergoing intense star formation at a
rate that is unsustainable on a Hubble time (e.g., Searle \&amp;amp; Sargent
1972). The nearest such object is the small irregular Local Group
galaxy IC~10. Van den Bergh (2000) kindly credits the 
recognition of IC10's starburst nature to  Massey \&amp;amp; Armandroff (1995),
who identified $\sim 20$ Wolf-Rayet stars (WRs).  WRs are the He-burning
descendents of the most massive O-type stars, and this high number in
such a small galaxy was considered quite remarkable; for comparison,
NGC~6822, another Local Group irregular of comparable absolute visual
magnitude contains only 4 WRs (Massey \&amp;amp; Johnson 1998).  Other lines
of evidence, such as the H$\alpha$ luminosity, also argue for a starburst
nature (Hodge \&amp;amp; Lee 1990; Youngblood \&amp;amp; Hunter 1999; Hunter 2001). 
The galaxy is embedded in an extended H~I envelope (Huchtmeier 1979);
presumably infalling gas
fuels the burst.
&lt;p&gt;
The proximity of IC~10 gives us a unique opportunity
to study the effects that an intense burst has on the {\it process}
of star formation, and in particular the slope of the stellar initial mass
function (IMF).  There has long been the theoretical expectation that
the IMF would be be top-heavy in regions of intense star formation
(Larson 1986).  And, indeed such a 
claim has been made for the starburst galaxy M~82 (Rieke et al.\ 1980), 
based admittedly on fairly indirect evidence
(see Scalo 1990 and Leitherer 1998).  
However, direct measurement
of the IMF in the energetic central 
cluster (R136) of the 30 Dor giant HII region 
by Massey \&amp;amp; Hunter (1998) found a perfectly normal IMF.
&lt;p&gt;
Stiil, there is evidence to suggest that IC~10 may in fact have
a top-heavy IMF.  Wolf-Rayet stars occur as two distinct types: those
of the WN class, which show the products of H-burning at their surfaces,
and those of the WC class, which show the products of He-burning at their
surfaces.    The mass range that is expected to evolve to WCs or WNs
should be a function of metallicity (due to the effect
that radiatively-driven stellar winds have on the evolution of massive stars)
but at a given metallicity the WCs will {\it on average} be descended from
more massive stars than are the WNs. (See discussion in Massey \&amp;amp; Johnson 1998
and Massey 2003).  The WR stars found by Massey \&amp;amp;
Armandroff (1995) were predominantly of WC type, unexpected in a galaxy
of IC~10's low metallicity (Fig.~1).  One explanation is that the IMF
is more weighted in favor of massive stars in IC~10 due to its current
starburst (Massey \&amp;amp; Armandroff 1995; Massey \&amp;amp; Johnson 1998).
&lt;p&gt;
However, another possibility exists: WNs are more difficult to detect than WCs
as their strongest emission lines are about a factor of 4 weaker than
those of WCs, and thus completeness for WNs is much harder to achieve in
any kind of a survey. (That is why the point for the Milky Way is also a bit
high in Fig.~1---the sample there is probably not complete for WNs, as 
discussed in Massey 2003).  IC10's low galactic latitude ($-3.3^\circ$)
results in a large galactic foreground reddening ($E(B-V)=0.75-0.80$, according
to Massey \&amp;amp; Armandroff 1995) further complicating detection.
Accordingly, two years ago we proposed and were
granted time on the 4-m Mayall to conduct a deeper
imaging survey for WR stars using Mosaic and our ``optimized&amp;quot; interference
filters centered on WR emission lines.
&lt;p&gt;
Our survey has uncovered a wealth of additional candidates 
(Massey \&amp;amp; Holmes 2003; see also Crowther et al.\ 2003). By
comparing the number of detections with those of a nearby
control field, we conclude that the total number of WRs
in IC10 might be as great as 100. If the 
majority of the new candidates are of WN-type (which might be expected if
the stronger-lined WCs have mostly all been previously detected), 
then these new candidates
could even lower the WC to WN ratio to normal---with the implication that
the IMF is also normal.  Of course, this would also imply that IC~10 is
an even more extreme starburst than previously thought!  
So far, only two of these new
candidates have been observed spectroscopically---both confirmed
as WNs.  To obtain a reasonably complete sample requires the large aperture
of Gemini and the multiplexing capability of GMOS.
&lt;p&gt;
\begin{figure}
\epsscale{0.85}
\plotone{N0163.01.eps}
\caption{The relative number of WC and WN stars is well correlated with
metallicity
as we would expect; the exceptions are the Milky Way, and IC~10.
The fact that the Milky Way ratio is high is easy to understand: the sample
within 2.5~kpc is probably not complete for WNs.
This figure has been adopted from Massey \&amp;amp; Johnson 1998, with the
errors bars showing the effects of $\sqrt{N}$
statistics on the ratios.}
\end{figure}
&lt;p&gt;
\reference Armandroff, T. E., \&amp;amp; Massey, P. 1995, AJ, 109, 2470
\reference Crowther, P. et al.\ 2003, A\&amp;amp;A, 404, 483
\reference Hodge, P., \&amp;amp; Lee, M. G. 1990, PASP, 102, 1245
\reference Huchtmeier, W. K. 1979, A\&amp;amp;A, 75, 170
\reference Hunter, D. A.  2001, ApJ, 559, 225
\reference Larson, R.  1986, MNRAS, 218, 409
\reference Leitherer, C. 1998, in The Stellar Initial Mass Function,
ed. G. Gilmore \&amp;amp; D. Howell, 61
\reference Massey, P. 2003, {\it ARA\&amp;amp;A}, 15, 41
\reference Massey, P. \&amp;amp; Holmes, S. 2002, ApJ, 580, L35
\reference Massey, P., \&amp;amp; Hunter, D. A. 1998, ApJ, 493, 180
\reference Massey, P., \&amp;amp; Johnson, O. 1998, ApJ, 505, 793
\reference Rieke, G. H., Lebofsky, M. J., Thompson, R. I.,
Low, F. J., \&amp;amp; Tokunaga, A. T. 1980, ApJ, 238, 24
\reference Scalo, J. M. 1990, in Windows on Galaxies, ed. A. Renzini,
G. Gabbiano, \&amp;amp; J. S. Gallagher, 125
\reference Searle, L., \&amp;amp; Sargent, W. L. W. 1972, ApJ, 173, 25
\reference van den Bergh, S. 2000, The Galaxies of the Local Group
\reference Youngblood, A. J., \&amp;amp; Hunter, D. A. 1999, ApJ, 519, 55
&lt;p&gt;
\begin{figure}
\epsscale{0.75}
\plotone{N0163.02.eps}
\caption{This plot shows a simulation of the detection of He~II $\lambda 4686$
with parameters typical of a weak-lined WN stars; e.g., a line width of
20\AA\ and a equivalent width of -10\AA.  The S/N per 0.9\AA (binned) pixel
is indicated.}
\end{figure}
&lt;p&gt;
\clearpage
&lt;p&gt;

&lt;h4&gt;Attachments:&lt;/h4&gt;
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&lt;tr&gt;&lt;td&gt;Science Justification&lt;/td&gt;&lt;td&gt;scijust.ps&lt;/td&gt;&lt;td&gt;PS&lt;/td&gt;&lt;/tr&gt;
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&lt;!--     technicalJustification      --&gt;
&lt;a name="technicalJustification"&gt;&lt;/a&gt;
&lt;hr&gt;
&lt;h3&gt;Technical Justification&lt;/h3&gt;
***EXPERIMENTAL DESIGN***:
&lt;p&gt;
With Gemini-N, we will obtain GMOS
multi-slit observations of $\sim 30$ of our weaker-lined
Wolf-Rayet candidates.
The size of IC10 is a good match to the 5.5 arcmin diameter masks, and
we can use a single slit mask.  {\bf Time assigned for this project
in 2003B resulted in obtaining a suitable image from which we
designed a slit mask, but the spectroscopic data was never obtained.}
&lt;p&gt;
For the spectroscopy we need reasonable resolution and S/N for
a solid detection/non-detection: our WR candidates
are faint ($B\sim 22-23$) and the expected emission of the strongest
line (He~II $\lambda 4686$) weak
(EWs of -10\AA; see
Table 3 of Massey \&amp;amp; Johnson 1998 ApJ, 505, 793).  The B600 grating offers
6\AA\ resolution (with a 1-arcsec slit), which is a good match to the
width of the spectral lines (10-20\AA).  We can bin by 2 pixels both
spatially and spectrally, and as our simulation shows (Fig.~3),
we require at least a S/N of 5 per 0.9\AA (binned) pixel
for a convincing detection of such a line.  According to the
GEMINI GMOS exposure time calculator tool, we will achieve this S/N
for a $B\sim 23$ object in a 5 hr
exposure (20 x 900 sec) assuming dark skies (20 percentile) and mediocre
seeing (80 percentile), using 1-arcsec wide slits.
We will do the observation in two sets of 10x900 seconds, moving the central
wavelength of the grating by 3nm to provide continuous wavelength coverage.
&lt;p&gt;
As part of our survey of Local Group galaxies we also obtained imaging through
our WR filters of {\it all} the Local Group galaxies currently active in
forming stars: ten fields covering M31, 3 fields covering M33, plus single
fields covering other Local Group galaxies.  We view this IC~10 half-night
as a test run for a more extensive proposal that will help identify the
evolved massive star population (both red supergiants and WRs) in these
nearby systems.
&lt;p&gt;
\proprietaryperiod{18 months}
&lt;p&gt;

***TECHNICAL DESCRIPTION***:
&lt;p&gt;
Dark time is needed as our objects are faint ($B\sim 23$) and the emission
weak.  The B600 grating provides good spectral coverage and adequate
resolution, and the observations can be obtained in ``mediocre&amp;quot; (for
Gemini!) seeing.  As a 900-sec exposure will be photon-noise limited,
we will combine 20 of these to obtain the equivalent of a 5-hr exposure.
In the experimental design section we argue that a S/N of 5 per 0.9\AA\
spectral resolution element is needed for certain detection of emission
in our weakest-lined cases (Fig.~2), and the GMOS ETC assures us we will
achieve this with a 5-hr exposure under dark skies and 80-percentile
seeing.
&lt;p&gt;
We were granted Gemini-N time for this project in semester 2003B, and
we obtained excellent imaging data under good seeing conditions that
went quite deep enough to design a slitlet mask.  But the spectroscopic
observations were never made.  The mask has been cut and is ready to go;
we require only a half night (5-hr plus overhead) to complete this project.
&lt;p&gt;
\geminidata{pcontactnum}{1}
{\bf Principal Contact:} Philip Massey

&lt;h4&gt;Attachments:&lt;/h4&gt;
		&lt;table width="100%" border="1"&gt;
&lt;tr bgcolor="#4AA02C"&gt;&lt;td&gt;&lt;b&gt;Name&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Source&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Type&lt;/b&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td&gt;Technical Justification&lt;/td&gt;&lt;td&gt;runinfo.ps&lt;/td&gt;&lt;td&gt;PS&lt;/td&gt;&lt;/tr&gt;
		&lt;/table&gt;
&lt;!--     observationDetails      --&gt;
&lt;a name="observationDetails"&gt;&lt;/a&gt;
&lt;hr&gt;
&lt;h3&gt;Observation Details&lt;/h3&gt;
		&lt;table width="100%" border="1"&gt;
&lt;tr bgcolor="#4AA02C"&gt;&lt;td valign="top"&gt;&lt;b&gt;Observation&lt;/b&gt;&lt;/td&gt;&lt;td valign="top"&gt;&lt;b&gt;RA&lt;/b&gt;&lt;/td&gt;&lt;td valign="top"&gt;&lt;b&gt;Dec&lt;/b&gt;&lt;/td&gt;&lt;td valign="top"&gt;&lt;b&gt;Brightness&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Total Time&lt;/b&gt;&lt;br&gt;&lt;i&gt;(including overheads)&lt;/i&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td&gt;&lt;b&gt;IC10&lt;/b&gt;&lt;/td&gt;&lt;td&gt;00:20:24.5&lt;/td&gt;&lt;td&gt;+59:17:30&lt;/td&gt;&lt;td&gt;23&lt;/td&gt;&lt;td&gt;300.0 minutes&lt;/td&gt;&lt;/tr&gt;&lt;tr&gt;&lt;td&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&lt;b&gt;pwfs1001_1&lt;/b&gt; (wfs)&lt;/td&gt;&lt;td&gt;0:20:21.228&lt;/td&gt;&lt;td&gt;59:12:10.81&lt;/td&gt;&lt;td&gt;9.70 R&lt;/td&gt;&lt;td&gt;separation 5.34&lt;/td&gt;&lt;/tr&gt;&lt;tr&gt;&lt;td&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&lt;b&gt;pwfs1001_2&lt;/b&gt; (wfs)&lt;/td&gt;&lt;td&gt;0:20:16.052&lt;/td&gt;&lt;td&gt;59:23:14.13&lt;/td&gt;&lt;td&gt;11.20 R&lt;/td&gt;&lt;td&gt;separation 5.84&lt;/td&gt;&lt;/tr&gt;&lt;tr&gt;&lt;td&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&lt;b&gt;iwfs1001_1&lt;/b&gt; (oiwfs)&lt;/td&gt;&lt;td&gt;0:20:40.051&lt;/td&gt;&lt;td&gt;59:14:30.62&lt;/td&gt;&lt;td&gt;10.60 R&lt;/td&gt;&lt;td&gt;separation 3.59&lt;/td&gt;&lt;/tr&gt;&lt;tr&gt;&lt;td colspan="2"&gt;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&amp;#160;&lt;a href="#observingConditions"&gt;observing conditions:&lt;/a&gt; Global Default&lt;/td&gt;&lt;td colspan="3"&gt;&lt;a href="#resources"&gt;resources:&lt;/a&gt; GMOS North&lt;/td&gt;&lt;/tr&gt;
		&lt;/table&gt;
&lt;!--     resources      --&gt;
&lt;a name="resources"&gt;&lt;/a&gt;
&lt;p&gt;
&lt;b&gt;Resources&lt;/b&gt;
&lt;ul&gt;&lt;li&gt;Gemini North&lt;ul&gt;&lt;li&gt;GMOS North (GMOS North)&lt;ul&gt;&lt;li&gt;Focal Plane Unit&lt;ul&gt;&lt;li&gt;Custom Mask&lt;/ul&gt;&lt;li&gt;Disperser&lt;ul&gt;&lt;li&gt;B600_G5303&lt;/ul&gt;&lt;/ul&gt;&lt;/ul&gt;&lt;/ul&gt;
&lt;!--     observingConditions      --&gt;
&lt;a name="observingConditions"&gt;&lt;/a&gt;
&lt;p&gt;
&lt;b&gt;Observing Conditions&lt;/b&gt;
		&lt;table width="100%" border="1"&gt;
&lt;tr bgcolor="#4AA02C"&gt;&lt;td&gt;&lt;b&gt;Name&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Image Quality&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Sky Background&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Water Vapor&lt;/b&gt;&lt;/td&gt;&lt;td&gt;&lt;b&gt;Cloud Cover&lt;/b&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td&gt;Global Default&lt;/td&gt;&lt;td&gt;85%&lt;/td&gt;&lt;td&gt;20%&lt;/td&gt;&lt;td&gt;Any&lt;/td&gt;&lt;td&gt;70%&lt;/td&gt;&lt;/tr&gt;
		&lt;/table&gt;
&lt;!--     schedulingInformation      --&gt;
&lt;a name="schedulingInformation"&gt;&lt;/a&gt;
&lt;p&gt;
&lt;b&gt;Scheduling Information:&lt;/b&gt;
&lt;p&gt;
&lt;b&gt;Synchronous dates: &lt;/b&gt;
&lt;p&gt;
&lt;b&gt;Optimal dates: &lt;/b&gt;
2004/8/1-2004/11/30
&lt;br&gt;
&lt;b&gt;Reason: &lt;/b&gt;

&lt;p&gt;
&lt;b&gt;Impossible dates: &lt;/b&gt;
2005/1/1-2005/1/31
&lt;br&gt;
&lt;b&gt;Reason: &lt;/b&gt;
None
&lt;!--     allocationCommitteeComments      --&gt;
&lt;a name="allocationCommitteeComments"&gt;&lt;/a&gt;
&lt;hr&gt;
&lt;h3&gt;Allocation Committee Comments&lt;/h3&gt;
&lt;h4&gt;NTAC Comment&lt;/h4&gt;
Comments from PI:
None

&lt;h4&gt;ITAC Comment&lt;/h4&gt;

    Program accepted for rollover into semester 05A and 
05B if not completed in 04B.
&lt;p&gt;

&lt;h4&gt;Gemini Comment&lt;/h4&gt;

&lt;p&gt;

&lt;!--     additionalInformation      --&gt;
&lt;a name="additionalInformation"&gt;&lt;/a&gt;
&lt;hr&gt;
&lt;h3&gt;Additional Information&lt;/h3&gt;
&lt;!--     keywords      --&gt;
&lt;a name="keywords"&gt;&lt;/a&gt;
&lt;br&gt;
&lt;b&gt;Keyword Category: &lt;/b&gt;
Galactic
&lt;p&gt;
&lt;b&gt;Keywords: &lt;/b&gt;
Massive stars, Wolf-Rayet stars
&lt;!--     publications      --&gt;
&lt;a name="publications"&gt;&lt;/a&gt;
&lt;p&gt;
&lt;b&gt;Publications:&lt;/b&gt;
&lt;ul&gt;&lt;li&gt;NOAO PAST USE: {\bf Recent (2000-2003) allocation of time:}

{\bf 2004A-200:} The Physical Parameters of Red Supergiants:
When Massive Stars Are as Cool as They Get, 10 nights KPNO 2.1-m (5 successfully
carried out in March, 5 more scheduled in late May), plus 5 nights CTIO 1.5-m
scheduled for April.  

{\bf Target of Opportunity:} Spectroscopy of a Newly Found Dwarf Irregular,
2 hrs kindly granted by Richard Green on the 2.1-m with GoldCam, April 2003.
The data appear in Massey, Henning, \&amp; Kraan-Korteweg, 2003, AJ, 126, 2362

\relatedwork{{\bf 2002B-218:} The Evolution and Physical Parameters of
Massive Stars at High Metallicity: O Stars in the Andromeda Galaxy", 3 nights
MMT Sept 2002.  We obtained only 0.5 nights out of 3
nights scheduled, due to weather, but published what we were able to get in
Massey \&amp; Holmes 2002, ApJ, 580, L35}

{\bf 2001A-062:} A {\it UBVR} Survey of the Magellanic Clouds, 6
nights
CTIO Curtis Schmidt April 2001: Massey 2002, ApJS 141, 81

\relatedwork{{\bf 2001B-002:} The Wolf-Rayet Content of IC10, 2 nights Mayall
4-m Sept 2001: Massey \&amp; Holmes 2002, ApJ, 580, L35}

{\bf 2001B-227:} The Red Supergiant Content of the Magellanic 
Clouds, 3 nights
CTIO 4-m Hydra, October 2001.  
Massey \&amp; Olsen 2003, AJ, 126, 2867 

{\bf 2000B-010:} A Survey of Local Group Galaxies Currently Forming Stars,
on-going survey project.  We are current with all of our data reductions,
and are completing the photometric analysis.  Some data appear in
Di Stefano et al. 2004, ApJ, in press (astroph-0306440)

{\bf 1999B-099; 2000B-070:}
Where Do Wolf-Rayet Stars Come From?
CTIO 1.5-m 5 nights October 2000; 6 nights October 1999:
Massey \&amp; Duffy 2001, ApJ 550, 713; Niemela et al. 2002,
MNRAS, 333, 347

\noindent
{\bf Recent papers (2002-2004) based upon NOAO data:}

\parindent=10pt

Massey, P., Bresolin, F., Kudritzki, R. P., Puls, J., \&amp; Pauldrach. A. W. A.
``The Effective Temperature Scale of O-type Stars as a Function of Metallicity.
I. A Sample of 20 Stars in the Magellanic Clouds", ApJ, in press (June 20 issue,
astroph/0402633)

Walborn et al.\ 2004, ``A CNO Dicomotomy Among O2 Giant Spectra in the
Magellanic Clouds", ApJ, in press (June 20 issue)

Bianchi, L., Bohlin, R., \&amp; Massey, P. 2003, ``The Ofpe/WN9 Stars in M33",
ApJ, 601, 228

Massey, P. 2003, ``The Massive Star Content of the Local Group: Implications
for Star Formation and Stellar Evolution", ARA\&amp;A, 41, 15

Di Stefano et al. 2003, ``Supersoft X-Ray Sources in M31", ApJ, submitted,
astro-ph/0306440

Massey, P., Olsen, K. A. G., \&amp; Parker, J. W. 2003, ``The Discovery of a
12th Wolf-Rayet Star in the Small Magellanic Cloud", PASP, 115, 1265
astro-ph/0308237

Massey, P., Henning, P. A., \&amp; Kraan-Korteweg, R. C. 2003, ``A
Neighboring Dwarf Irregular Galaxy Hidden By the Milky Way",
AJ 126, in press (Nov issue), astro-ph/0308080

Massey, P., \&amp; Olsen, K. A. G. 2003, ``The Evolution of Massive Stars. I.
Red Supergiants in the Magellanic Clouds", AJ, 126, 2867
astro-ph/0309272

Morrell, N. I., Ostrov, P. G., Massey, P., \&amp; Gamen, R. 2003, ``Hodge 53-47:
An Early O-type Double-lined Binary in the SMC", MNRAS, 341, 583

Massey, P., \&amp; Holmes, S. 2002 ``Wolf-Rayet Stars in IC10: Probing the Nearest
Starburst", ApJ 580, L35

Massey, P. 2002, ``A UBVR CCD Survey of the Magellanic Clouds," ApJS, 141,
81

Massey, P. 2002, ``Observational Constraints on Massive Star Evolution"
(invited review), in {\it A Massive Star Odyssey, from Main Sequence to
Supernova, IAU 212}, ed. van der Hucht, Herrero, \&amp; Esteban, 316.

Slesnick, C. L., Hillenbrand, L. A., \&amp; Massey, P. 2002, ``The Star Formation
History and Mass Function in the Double Cluster h and Chi Persei", ApJ,
576, 880

Snow, T. P., Zukowski, D., \&amp; Massey, P. 2002, ``The Intrinsic Profile of
the 4428\AA\ Diffuse Interstellar Band", ApJ 578, 877

Niemela, V. S., Massey, P., Testor, G., \&amp; Benitez, S. G. 2002, ``The Massive
Wolf-Rayet Binary WR7 in the SMC", MNRAS, 333, 347

Walborn et al. 2002, ``A Giant O2-O4 Spectral Classification
Study", AJ, 123, 2754

Bianchi et al. 2001,``The Massive Star Content of  NGC 6822. Ground-based
and {\it HST} photometry, AJ, 121, 2020.

Massey, P. \&amp; Duffy, A. S. 2001, ``A Deep Search for Wolf-Rayet Stars in
the Small Magellanic Cloud", ApJ, 550, 713.

Massey, P., DeGioia-Eastwood, K., \&amp; Waterhouse, E. 2001, ``The Progenitor
Masses of Wolf-Rayet Stars and Luminous Blue Variables Determined from
Cluster Turn-offs. II. Results from 12 Clusters in the Milky Way",
AJ, 121, 1050.

\parindent=0pt&lt;/ul&gt;
&lt;!--     pastAllocations      --&gt;
&lt;a name="pastAllocations"&gt;&lt;/a&gt;
&lt;!--     proposalContents      --&gt;
&lt;a name="proposalContents"&gt;&lt;/a&gt;
&lt;hr&gt;
&lt;h2&gt;Proposal Contents&lt;/h2&gt;
&lt;a href="#summary"&gt;Summary&lt;/a&gt;
&lt;br&gt;
&lt;a href="#investigators"&gt;Investigators&lt;/a&gt;
&lt;br&gt;
&lt;a href="#abstract"&gt;Abstract&lt;/a&gt;
&lt;br&gt;
&lt;a href="#scienceJustification"&gt;Science Justification&lt;/a&gt;
&lt;br&gt;
&lt;a href="#technicalJustification"&gt;Technical Justification&lt;/a&gt;
&lt;br&gt;
&lt;a href="#observationDetails"&gt;Observation Details&lt;/a&gt;
&lt;br&gt;
&lt;a href="#allocationCommitteeComments"&gt;Allocation Committee Comments&lt;/a&gt;
&lt;br&gt;
&lt;a href="#additionalInformation"&gt;Additional Information&lt;/a&gt;
&lt;br&gt;
&lt;!--     coda      --&gt;
&lt;a name="coda"&gt;&lt;/a&gt;
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          <param name="disperserOrder" value="1"/>
          <param name="fpuMode" value="Custom Mask"/>
          <param name="fpu" value="Custom Mask"/>
          <param name="fpuCustomMask" value="GN2004BQ012-01"/>
          <param name="filter" value="None"/>
          <param name="ccdXBinning" value="1"/>
          <param name="ccdYBinning" value="2"/>
          <param name="port" value="side-looking"/>
          <param name="posAngleMode" value="Set Value"/>
          <param name="posAngle" value="180"/>
          <param name="stageMode" value="Follow in XY"/>
          <param name="dtaXOffset" value="0"/>
          <param name="builtinROI" value="Full Frame Readout"/>
          <param name="useNS" value="false"/>
        </paramset>
      </container>
      <container version="2002-06" kind="obsComp" key="667d7170-9069-41ed-a8f2-8c061599d3bf" type="Info" subtype="note" name="Note">
        <paramset name="Note" kind="dataObj">
          <param name="title" value="MOS observation"/>
          <param name="NoteText">
            <value>
MOS observation for GN2004BQ012-01.  The observations are being done with
a rotator angle of 180 degrees, the same as for the pre-imaging data.  The
sequence will consist of 5 exposures of 1800 sec each with the B600 grating centered
at 525nm, followed by 5 exposures of 1800 sec each with the grating dithered
to 500nm.  </value>
          </param>
        </paramset>
      </container>
      <container version="2002-06" kind="seqComp" key="a8e984f1-d8ac-438a-83a4-b1ee4f5acc8d" type="Iterator" subtype="base" name="Sequence">
        <paramset name="Sequence" kind="dataObj"/>
        <container version="2002-06" kind="seqComp" key="9aec7161-9e87-4615-9b37-b2391e418c18" type="DataProc" subtype="DataProc" name="Data Processing">
          <paramset name="Data Processing" kind="dataObj">
            <paramset name="nodes"/>
            <paramset name="edges"/>
          </paramset>
        </container>
        <container version="2002-06" kind="seqComp" key="3a391169-0d2e-47fe-a8eb-8b5d271ac7ea" type="Iterator" subtype="GMOS" name="GMOS-N Sequence">
          <paramset name="GMOS-N Sequence" kind="dataObj">
            <param name="disperserLambda">
              <value sequence="0">525.0</value>
              <value sequence="1">520.0</value>
            </param>
          </paramset>
          <container version="2002-06" kind="seqComp" key="dd302702-d6fa-40d2-9bbc-a1669cc26b16" type="Observer" subtype="observe" name="Observe">
            <paramset name="Observe" kind="dataObj">
              <param name="repeatCount" value="5"/>
              <param name="uid" value="10c02266-565e-4ffe-903a-9ddb6db5ca8e"/>
            </paramset>
          </container>
          <container version="2002-06" kind="seqComp" key="1710de6b-5a6b-499c-b68d-b75cf17b2968" type="Observer" subtype="GemFlat" name="Flat/Arc">
            <paramset name="Flat/Arc" kind="dataObj">
              <param name="repeatCount" value="1"/>
              <param name="uid" value="32e453f6-91d4-4129-81bc-a2d33f190713"/>
              <param name="coadds" value="1"/>
              <param name="exposureTime" value="2.0"/>
              <param name="lamp" value="Quartz Halogen"/>
              <param name="shutter" value="Closed"/>
              <param name="filter" value="GMOS balance"/>
              <param name="diffuser" value="IR"/>
            </paramset>
          </container>
        </container>
      </container>
    </container>
    <container version="2002-06" kind="observation" key="b8a6b3ed-1d3c-4953-93a2-bfc84c0e3b8b" type="Observation" subtype="basic" name="GN-2004B-Q-12-6">
      <paramset name="Observation" kind="dataObj">
        <param name="title" value="Baseline Twilight for GN2004BQ012-01"/>
        <param name="priority" value="High"/>
        <param name="status" value="Phase 2"/>
        <param name="dataStatus" value="No Data"/>
        <param name="totalUsedTime" units="seconds" value="0.0"/>
      </paramset>
      <container version="2002-06" kind="obsComp" key="22a333d2-903e-4c31-bdef-a09427c90419" type="Scheduling" subtype="conditions" name="Observing Conditions">
        <paramset name="Observing Conditions" kind="dataObj">
          <param name="CloudCover" value="70%"/>
          <param name="ImageQuality" value="70%"/>
          <param name="SkyBackground" value="20%/Darkest"/>
          <param name="WaterVapor" value="Any"/>
        </paramset>
      </container>
      <container version="2002-06" kind="obsComp" key="03c30dd2-9756-42f1-8b9d-ab58a4b7050d" type="Telescope" subtype="targetEnv" name="Targets">
        <paramset name="Targets" kind="dataObj">
          <paramset name="posList">
            <paramset name="Base">
              <param name="name" value="twilight"/>
              <param name="system" value="J2000"/>
              <param name="epoch" units="years" value="2000.0"/>
              <param name="brightness" value=""/>
              <param name="c1" value="00:00:00.00"/>
              <param name="c2" value="00:00:00.0"/>
              <param name="pm1" units="milli-arcsecs/year" value="0.0"/>
              <param name="pm2" units="milli-arcsecs/year" value="0.0"/>
              <param name="parallax" units="arcsecs" value="0.0"/>
              <param name="rv" units="km/sec" value="0.0"/>
              <param name="wavelength" units="angstroms" value="-1.0"/>
            </paramset>
          </paramset>
        </paramset>
      </container>
      <container version="2003-06" kind="obsComp" key="6871c7b1-8c63-4018-8b11-81e0c99be15b" type="Instrument" subtype="GMOS" name="GMOS-N">
        <paramset name="GMOS-N" kind="dataObj">
          <param name="exposureTime" value="30.0"/>
          <param name="posAngle" value="180"/>
          <param name="coadds" value="1"/>
          <param name="adc" value="No Correction"/>
          <param name="ampCount" value="Three"/>
          <param name="gainChoice" value="Low"/>
          <param name="ampReadMode" value="Slow"/>
          <param name="disperser" value="B600_G5303"/>
          <param name="disperserLambda" value="525.0"/>
          <param name="disperserOrder" value="1"/>
          <param name="fpuMode" value="Custom Mask"/>
          <param name="fpu" value="Custom Mask"/>
          <param name="fpuCustomMask" value="GN2004BQ012-01"/>
          <param name="filter" value="None"/>
          <param name="ccdXBinning" value="1"/>
          <param name="ccdYBinning" value="2"/>
          <param name="port" value="side-looking"/>
          <param name="posAngleMode" value="Set Value"/>
          <param name="posAngle" value="180"/>
          <param name="stageMode" value="Follow in XY"/>
          <param name="dtaXOffset" value="0"/>
          <param name="builtinROI" value="Full Frame Readout"/>
          <param name="useNS" value="false"/>
        </paramset>
      </container>
      <container version="2002-06" kind="obsComp" key="9e39db75-f578-43ee-8500-9daf72cc2224" type="Info" subtype="note" name="Note">
        <paramset name="Note" kind="dataObj">
          <param name="title" value="Twilight exposure"/>
          <param name="NoteText">
            <value>This is the placeholder for the baseline twilight exposure through mask
GN2004BQ012-01</value>
          </param>
        </paramset>
      </container>
      <container version="2002-06" kind="seqComp" key="0a46081d-4585-486c-b0a9-9f9b17b418ac" type="Iterator" subtype="base" name="Sequence">
        <paramset name="Sequence" kind="dataObj"/>
        <container version="2002-06" kind="seqComp" key="5903c4aa-cebb-4abe-8256-a4719b354238" type="DataProc" subtype="DataProc" name="Data Processing">
          <paramset name="Data Processing" kind="dataObj">
            <paramset name="nodes"/>
            <paramset name="edges"/>
          </paramset>
        </container>
        <container version="2002-06" kind="seqComp" key="bd1184a4-5adf-4de4-bc99-a072648c8e4b" type="Observer" subtype="observe" name="Observe">
          <paramset name="Observe" kind="dataObj">
            <param name="repeatCount" value="1"/>
            <param name="uid" value="51fb4da0-5f60-4a62-8aef-98cad5f3f508"/>
          </paramset>
        </container>
      </container>
    </container>
    <container version="2002-06" kind="observation" key="707f0909-ecd3-4209-9468-a8ee3b9512b8" type="Observation" subtype="basic" name="GN-2004B-Q-12-7">
      <paramset name="Observation" kind="dataObj">
        <param name="title" value="Baseline comp for GN2004BQ012-01"/>
        <param name="priority" value="High"/>
        <param name="status" value="Phase 2"/>
        <param name="dataStatus" value="No Data"/>
        <param name="totalUsedTime" units="seconds" value="0.0"/>
      </paramset>
      <container version="2002-06" kind="obsComp" key="e41e341b-252e-460f-aa38-86eed6370431" type="Scheduling" subtype="conditions" name="Observing Conditions">
        <paramset name="Observing Conditions" kind="dataObj">
          <param name="CloudCover" value="70%"/>
          <param name="ImageQuality" value="70%"/>
          <param name="SkyBackground" value="20%/Darkest"/>
          <param name="WaterVapor" value="Any"/>
        </paramset>
      </container>
      <container version="2002-06" kind="obsComp" key="6216b2d8-f2aa-4c61-99e7-8f1893bf7c8e" type="Telescope" subtype="targetEnv" name="Targets">
        <paramset name="Targets" kind="dataObj">
          <paramset name="posList">
            <paramset name="Base">
              <param name="name" value="Baseline comp"/>
              <param name="system" value="J2000"/>
              <param name="epoch" units="years" value="2000.0"/>
              <param name="brightness" value=""/>
              <param name="c1" value="00:00:00.00"/>
              <param name="c2" value="00:00:00.0"/>
              <param name="pm1" units="milli-arcsecs/year" value="0.0"/>
              <param name="pm2" units="milli-arcsecs/year" value="0.0"/>
              <param name="parallax" units="arcsecs" value="0.0"/>
              <param name="rv" units="km/sec" value="0.0"/>
              <param name="wavelength" units="angstroms" value="-1.0"/>
            </paramset>
          </paramset>
        </paramset>
      </container>
      <container version="2003-06" kind="obsComp" key="4cd3761e-1bec-4ccd-bf40-b793db6d544b" type="Instrument" subtype="GMOS" name="GMOS-N">
        <paramset name="GMOS-N" kind="dataObj">
          <param name="exposureTime" value="30.0"/>
          <param name="posAngle" value="180"/>
          <param name="coadds" value="1"/>
          <param name="adc" value="No Correction"/>
          <param name="ampCount" value="Three"/>
          <param name="gainChoice" value="Low"/>
          <param name="ampReadMode" value="Slow"/>
          <param name="disperser" value="B600_G5303"/>
          <param name="disperserLambda" value="525.0"/>
          <param name="disperserOrder" value="1"/>
          <param name="fpuMode" value="Custom Mask"/>
          <param name="fpu" value="Custom Mask"/>
          <param name="fpuCustomMask" value="GN2004BQ012-01"/>
          <param name="filter" value="None"/>
          <param name="ccdXBinning" value="1"/>
          <param name="ccdYBinning" value="2"/>
          <param name="port" value="side-looking"/>
          <param name="posAngleMode" value="Set Value"/>
          <param name="posAngle" value="180"/>
          <param name="stageMode" value="Do Not Follow"/>
          <param name="dtaXOffset" value="0"/>
          <param name="builtinROI" value="Full Frame Readout"/>
          <param name="useNS" value="false"/>
        </paramset>
      </container>
      <container version="2002-06" kind="obsComp" key="16f1bc01-950c-4c18-a99c-952f42954f82" type="Info" subtype="note" name="Note">
        <paramset name="Note" kind="dataObj">
          <param name="title" value="Daytime CuAr exposures"/>
          <param name="NoteText">
            <value>This is the placehold for the baseline CuAr exposures obtained with a center of
525nm and 500nm.</value>
          </param>
        </paramset>
      </container>
      <container version="2002-06" kind="seqComp" key="fd8ab927-00a7-46d0-8afc-b4356f35ddd3" type="Iterator" subtype="base" name="Sequence">
        <paramset name="Sequence" kind="dataObj"/>
        <container version="2002-06" kind="seqComp" key="518eb1c9-a922-49a4-a88e-8f8abb4b8df6" type="DataProc" subtype="DataProc" name="Data Processing">
          <paramset name="Data Processing" kind="dataObj">
            <paramset name="nodes"/>
            <paramset name="edges"/>
          </paramset>
        </container>
        <container version="2002-06" kind="seqComp" key="6ed47f4d-015b-4a67-900e-b09efc13d026" type="Iterator" subtype="GMOS" name="GMOS-N Sequence">
          <paramset name="GMOS-N Sequence" kind="dataObj">
            <param name="disperserLambda">
              <value sequence="0">525.0</value>
              <value sequence="1">520.0</value>
            </param>
          </paramset>
          <container version="2002-06" kind="seqComp" key="cff33c21-c117-4062-8954-b7de9a03e580" type="Observer" subtype="GemFlat" name="Flat/Arc">
            <paramset name="Flat/Arc" kind="dataObj">
              <param name="repeatCount" value="1"/>
              <param name="uid" value="101753fc-54f0-407a-8927-947ec627a451"/>
              <param name="coadds" value="1"/>
              <param name="exposureTime" value="30.0"/>
              <param name="lamp" value="CuAr arc"/>
              <param name="shutter" value="Closed"/>
              <param name="filter" value="none"/>
              <param name="diffuser" value="IR"/>
            </paramset>
          </container>
        </container>
      </container>
    </container>
    <container version="2002-06" kind="observation" key="2f64abec-7ced-4b15-ace3-b2daac7f05a8" type="Observation" subtype="basic" name="GN-2004B-Q-12-8">
      <paramset name="Observation" kind="dataObj">
        <param name="title" value="Baseline Mask image GN2004BQ012-01"/>
        <param name="priority" value="High"/>
        <param name="status" value="Phase 2"/>
        <param name="dataStatus" value="No Data"/>
        <param name="totalUsedTime" units="seconds" value="0.0"/>
      </paramset>
      <container version="2002-06" kind="obsComp" key="00c71275-995b-449c-9e8e-9356f2c4f119" type="Scheduling" subtype="conditions" name="Observing Conditions">
        <paramset name="Observing Conditions" kind="dataObj">
          <param name="CloudCover" value="70%"/>
          <param name="ImageQuality" value="70%"/>
          <param name="SkyBackground" value="20%/Darkest"/>
          <param name="WaterVapor" value="Any"/>
        </paramset>
      </container>
      <container version="2002-06" kind="obsComp" key="c831c01a-a587-4036-8774-a9b6aaa73069" type="Telescope" subtype="targetEnv" name="Targets">
        <paramset name="Targets" kind="dataObj">
          <paramset name="posList">
            <paramset name="Base">
              <param name="name" value="Baseline Mask"/>
              <param name="system" value="J2000"/>
              <param name="epoch" units="years" value="2000.0"/>
              <param name="brightness" value=""/>
              <param name="c1" value="00:00:00.00"/>
              <param name="c2" value="00:00:00.0"/>
              <param name="pm1" units="milli-arcsecs/year" value="0.0"/>
              <param name="pm2" units="milli-arcsecs/year" value="0.0"/>
              <param name="parallax" units="arcsecs" value="0.0"/>
              <param name="rv" units="km/sec" value="0.0"/>
              <param name="wavelength" units="angstroms" value="-1.0"/>
            </paramset>
          </paramset>
        </paramset>
      </container>
      <container version="2003-06" kind="obsComp" key="75403840-99c3-4746-ba16-bb8fb316b7c7" type="Instrument" subtype="GMOS" name="GMOS-N">
        <paramset name="GMOS-N" kind="dataObj">
          <param name="exposureTime" value="4.0"/>
          <param name="posAngle" value="180"/>
          <param name="coadds" value="1"/>
          <param name="adc" value="No Correction"/>
          <param name="ampCount" value="Three"/>
          <param name="gainChoice" value="Low"/>
          <param name="ampReadMode" value="Slow"/>
          <param name="disperser" value="Mirror"/>
          <param name="fpuMode" value="Custom Mask"/>
          <param name="fpu" value="Custom Mask"/>
          <param name="fpuCustomMask" value="GN2004BQ012-01"/>
          <param name="filter" value="r_G0303"/>
          <param name="ccdXBinning" value="1"/>
          <param name="ccdYBinning" value="1"/>
          <param name="port" value="side-looking"/>
          <param name="posAngleMode" value="Set Value"/>
          <param name="posAngle" value="180"/>
          <param name="stageMode" value="Do Not Follow"/>
          <param name="dtaXOffset" value="0"/>
          <param name="builtinROI" value="Full Frame Readout"/>
          <param name="useNS" value="false"/>
        </paramset>
      </container>
      <container version="2002-06" kind="obsComp" key="2899968e-a869-4eaf-ae78-9750367fa3a0" type="Info" subtype="note" name="Note">
        <paramset name="Note" kind="dataObj">
          <param name="title" value="Mask image"/>
          <param name="NoteText" value="This is the baseline mask image for GN2004BQ012-01"/>
        </paramset>
      </container>
      <container version="2002-06" kind="seqComp" key="3b6309f0-6249-4fb0-a844-87e8dc8ba653" type="Iterator" subtype="base" name="Sequence">
        <paramset name="Sequence" kind="dataObj"/>
        <container version="2002-06" kind="seqComp" key="ae050c0a-f4ff-4c7a-8e71-bb268a328c9c" type="DataProc" subtype="DataProc" name="Data Processing">
          <paramset name="Data Processing" kind="dataObj">
            <paramset name="nodes"/>
            <paramset name="edges"/>
          </paramset>
        </container>
        <container version="2002-06" kind="seqComp" key="296426d3-16e2-487e-9e20-98327a434ad6" type="Observer" subtype="GemFlat" name="Flat/Arc">
          <paramset name="Flat/Arc" kind="dataObj">
            <param name="repeatCount" value="3"/>
            <param name="uid" value="28446b52-4c52-44e4-8166-be150b591893"/>
            <param name="coadds" value="1"/>
            <param name="exposureTime" value="4.0"/>
            <param name="lamp" value="Quartz Halogen"/>
            <param name="shutter" value="Closed"/>
            <param name="filter" value="ND4.0"/>
            <param name="diffuser" value="IR"/>
          </paramset>
        </container>
      </container>
    </container>
  </container>
</document>
