An attempt to flesh out some of the details of what we'll observe in the first season or two.
First, the GBT pointing won't be good during the day at 3mm so we can only observe at night. Where is the sun?
| Date | Sun RA | LST @ midnight | Nighttime range (LST) |
| Sep 1 | 10:40 | 22:40 | 18:40 - 02:40 |
| Oct 1 | 12:40 | 00:40 | 20:40 - 04:40 |
| Nov 1 | 14:40 | 02:40 | 22:40 - 06:40 |
| Dec 1 | 16:40 | 04:40 | 00:40 - 08:40 |
| Jan 1 | 18:40 | 06:40 | 02:40 - 10:40 |
| Feb 1 | 30:40 | 08:40 | 04:40 - 12:40 |
| Mar 1 | 22:40 | 10:40 | 06:40 - 14:40 |
| Apr 1 | 00:40 | 12:40 | 08:40 - 16:40 |
| May 1 | 02:40 | 14:40 | 10:40 - 18:40 |
| Jun 1 | 05:40 | 16:40 | 12:40 - 20:40 |
Saturn: 10h30 or so
No brainer target once we think things are working. coordinates: 05h, +10 deg. Good for winter.
Observing Requirements
- Big mosaicked map, with a couple of passes over each 'tile'. Integration time determined by practical considerations (telescope slew speed limits, etc)
These are bright and compact but not trivially compact. 3mm observations would test dust models and complement higher frequency continuum maps (as are sensitive to colder dust than the submm). Yancy Shirley has provided a list of good targets that are well studied at other wavelengths:
GL2591 20 27 35.5 +40 01 13 B1950.0 -- early fall
S140 22 17 41.1 +63 03 42 B1950.0 -- early fall
S231 05 35 51.3 +35 44 16 B1950.0 -- winter (aka G173.49+2.42)
Observing Requirements per target
- 5'x5' map, with an hour or two total integration time, should be fine.
3. BLAST sources/High Z Galaxy fields
- Noise tests are high z galaxy fields. Might as well pick useful ones. Also-- stuff clusters. Find the brightest mm high-z source you can and use it as the center of a daisy scan, for noise tests.
- We will probably need a good submm cross-calibration. Thoughts/targets? Do we need to propose for approximately concurrent JCMT or other observations (note: JCMT deadline for the end of 05 observations, is March 31)
- Many surveys (SHADES, BLAST, IRAM, VLA, Subaru, Chandra, etc) are targeting
- Lockman Hole (10:52, +57 deg) -- ~ 20' x 20'. Good winter target.
- Subaru Deep Field South (13:24, +27 deg). Somewhat larger. Good spring target but conflicts with lockman a bit.
- Some of this can be photometry (ie mapping), some measuring already-known sources.
Observing Requirements
- To get to 15 uJy RMS (a factor of a few above the expected 3mm confusion limit) one needs 6 hours per 5' x 5' patch. Therefore a total of 100 hours per deep field (Lockman hole or Subaru).
4. SZE in Galaxy Cluster s
Fairly small maps of novel, small-scale effects are probably our niche until there is a sweeping tertiary.
- radio/x-ray "ghost" cavities-- do the massive holes in the ICM of some clusters have thermal pressure support or not? See for example Pfrommer, Ensslin, and Sarazin or McNamara et al. ... some specific targets:
- A2597 (23:25, -12:06) -- fall target
- Perseus (03:18, +41:30) aka Abell 426 -- winter target. Very strong signal expected. Also has a very bright radio galaxy in the center (3C84) so we are guaranteed some signal, and this may even help with the imaging.
Observing Requirements
- Pfrommer et al predict a few hours with GBT+Penn Array on a 5'x5' field will do Perseus. Their calculation needs to be checked in detail though.
AGNs
Cen A would make a nice image (13h, -42 deg); perhaps also Hydra A, other big jets (IC?)
| Name | ra | dec | size | notes |
| antennae | 12h | -18 | 12'x12' | any time |
| NGC 891 | 02h | +42 | 12'x12' | edge on, start of run |
| M87 =3c274 | 12:30 | +12 | 20'x20' | cool image , any time |
| cen A | 12:25 | -45 | 17'x17' | z=0.00-1, any time |
| arp 220 | 15:34 | +23 | 2'x2' | |
| hydra A | 09:18 | -12 | 2'x2' | bright; cool image; later in run |
| cyg a=3c405 | 20h | +40 | 2'.5x1'.5 | amazing image, sucky RA |
| MS0735.6+7421 | 07:41:50.2 | +74:14:51.0 | | 21 mJy in NVSS.... wait |
| Perseus=A426 | 03:19 | +41 | 6'x6' | super bright, interesting morphology; start of run |
| Herc A | 16:51 | +04 | 2'x1' | weak & steep -- see Leahy DRAGN sample also |
Rosette, Carina, etc...
from Bill Cotton:
The following look like possibilities, all a bit less than an arcmin
and in the right part of the sky.
NGC2346 J 07 09 41 -00 48 56 size ~54" NVSS nothing obvious
NGC2371 J 07 25 34.7 +29 29 25.6 size ~44" NVSS ~ 60 mJy
NGC2392 J 07 29 10.77 +20 54 42.5 size ~48" NVSS ~ 300 mJy
The last one, the Eskimo Nebula, is the strongest at 20 cm.
Primary calibrators
- weak planets like uranus & neptune??
- Uranus: sep 2005 (22:30, -09 deg; 3.7'' diam). essentially the same in feb 06. Brightness temp ~100 K.
- Neptune: sep 2005 (21h , -16 deg; 2.3'' diam). ditto. temp ~ 100 K.
- SMA Calibrator list -- unclear absolute scale, but many sources, incl. 3mm fluxes, and date of obs
- SMA Primary Calibrator online modeller -- includes uranus, neptune, some asteroids (for which GBT might need special ephemerides) -- http://sma1.sma.hawaii.edu/planetvis.html
Secondary calibrators, pointing calibrators and general "bright pointlike targets"
- IRAM 30m pointing calibrators (mostly 3mm)
- Valid 3mm pointing calibrators from Jim Condon's "calfind2" program. These sources are known to be compact and have very good positions. The 90 GHz flux densities are extrapolated, sometimes from below 40 GHz, and may not be reliable.
- Here is a list of 3mm measurements of AGN and quasars from the NRAO 12-m, due to Holdaway, Owen, & Rupen
- Ultra-compact HII regions will have flattish spectra from the radio, with dust just starting to contribute at 3mm, and few arcsecond sizes. A good catalog is that of
Kurtz, Churchwell, and Wood
- Michelle Caler's writeup of BLAST calibrators is attached below
- selected wmap sources -- these are bright and often not terribly extended, and are a reasonable sample of first things to look at. Since many are somewhat extended they are not good for determining pointing offsets. It would be sensible to cross-correlate this list-- reliably bright-- with the Condon list-- reliably compact-- these are our perfect pointing sources and secondary flux calibrators.
- (13jan06) I have now done this-- here is the Condon and Yin 3mm calibrators correlated with WMAP detections list. The radius for a positive coincidence was taken as 15 arcseconds; positions listed are from Condon and Yin which has 0.5" accuracy.
- Here are the brightest few sources (by their WMAP 90 GHz fluxes-- these are actually ALL the WMAP 90 GHz detections)
0808-0751 08:08:15.54 -07:51:09.886 90.00 1.31 121.60 90.00 1.20 0.60
2139+1423 21:39:01.31 +14:23:35.991 90.00 0.54 38.10 90.00 1.50 0.80
0646+4451 06:46:32.03 +44:51:16.590 90.00 1.31 98.90 90.00 1.70 0.80
1512-0905 15:12:50.53 -09:05:59.829 90.00 0.72 130.90 90.00 1.70 0.70
1829+4844 18:29:31.78 +48:44:46.161 90.00 0.78 85.90 90.00 1.70 0.40
2331-1556 23:31:38.65 -15:56:57.009 90.00 0.60 16.50 90.00 1.90 0.60
2134-0153 21:34:10.31 -01:53:17.238 90.00 0.66 36.50 90.00 2.00 0.60
1159+2914 11:59:31.83 +29:14:43.826 90.00 1.07 151.80 90.00 2.10 0.60
1753+2848 17:53:42.47 +28:48:04.939 90.00 0.60 91.90 90.00 2.20 0.70
0457-2324 04:57:03.18 -23:24:52.020 90.00 1.01 75.20 90.00 2.70 0.60
0136+4751 01:36:58.59 +47:51:29.100 90.00 0.95 53.20 90.00 2.90 0.70
0927+3902 09:27:03.01 +39:02:20.851 90.00 2.03 128.40 90.00 3.10 0.80
2232+1143 22:32:36.41 +11:43:50.904 90.00 1.49 25.20 90.00 3.10 0.70
1337-1257 13:37:39.78 -12:57:24.693 90.00 4.17 152.00 90.00 3.70 0.70
NOTE: 1337-1257 is a z=0.5 QSO with a nearby (possibly coincident) xray source. NVSS image is pointlike
0423-0120 04:23:15.80 -01:20:33.065 90.00 1.73 65.80 90.00 3.90 1.00
1635+3808 16:35:15.49 +38:08:04.500 90.00 1.25 107.20 90.00 4.20 0.70
NOTE: 1635+3808 is a z=1.8 QSO. NVSS image is pointlike
2253+1608 22:53:57.75 +16:08:53.560 90.00 10.20 23.70 90.00 5.90 0.90
- Jan 2008 -- I attached the OVRO/BIMA/CARMA database of 90 GHz fluxes as a function of time to the bottom of this page.
-- BrianMason - 17 Mar 2005
Revision r1.26 - 07 Jul 2008 - 14:58 GMT - BrianMason Parents: WebHome
|
Content copyright © 1999-2007 by the contributing authors. All material on this collaboration platform is the property of the contributing authors.
|
| |