! $Id: 5454,v 6.1 1994/07/27 18:10:55 pepsa Exp $ coverpage: title_1: ELLIPTICALS WITH KINEMATICALLY DISTINCT CORES : CYCLE 4 MEDIUM sci_cat: GALAXIES & CLUSTERS sci_subcat: NUCLEI/CORES proposal_for: GO pi_fname: MARIJN pi_lname: FRANX pi_inst: 6830 pi_country: NETHERLANDS pi_phone: (011) 31 50 634067 hours_pri: 14.54 num_pri: 16 wf_pc: Y off_fname: PIET off_lname: VAN DER KRUIT off_title: CHAIRMAN off_inst: 6830 off_addr_1: KAPTEYN ASTRONOMICAL INSTITUTE off_addr_2: P.O. BOX 800 off_city: GRONINGEN off_zip: 9700 AV off_country: NETHERLANDS off_phone: (31) 50 634053 ! end of coverpage abstract: line_1: The discovery by Franx and Illingworth of a kinematically-distinct line_2: stellar core in the nucleus of the giant radio elliptical IC 1459, and line_3: the confirmation that such components are quite common, has added a line_4: valuable diagnostic tool for understanding the structure and the formation line_5: of ellipticals. These cores are substantial (10**10 solar masses for line_6: IC 1459) and offer a valuable and unique diagnostic of the dynamical state line_7: of the nuclei of ellipticals. Further study will address their formation line_8: by investigating whether these cores could be the end result of a line_9: `starburst' event, or from the capture of a stellar companion, or even line_10: the merging of primordial subclumps. Here we propose to take advantage line_11: of the high resolution imaging of the PC to image the 16 galaxies with line_12: known kinematically distinct cores from our magnitude limited sample of line_13: 77 ellipticals. The focus of the program is the detection of stellar line_14: disks (as suggested by the spectroscopic line profile analysis) and line_15: color differences between the core region and the rest of the galaxy. line_16: If the cores have been affected by accretion of stars or gas, and star line_17: formation, then such differences are naturally expected. This program line_18: also allows us to identify the color of any jets or shells and map the line_19: dust at small radii. These data are an essential complement to our line_20: extensive ground-based spectroscopic and imaging survey. ! ! end of abstract general_form_proposers: lname: FRANX fname: MARIJN inst: 6830 country: NETHERLANDS esa: Y ! lname: ILLINGWORTH fname: GARTH inst: 1552 country: USA ! lname: FORBES fname: DUNCAN inst: 1552 country: USA ! ! end of general_form_proposers block general_form_text: question: 3 section: 1 line_1: We propose to observe all 16 ellipticals with known kinematically distinct line_2: cores from our magnitude limited sample of 77 galaxies. Several of the line_3: galaxies are of special interest. IC 1459 because it is one the most extreme line_4: examples of a galaxy with a kinematically distinct core. NGC 7626 is line_5: remarkable because it has a very irregular rotation curve(1). It is very well line_6: possible that the central parts are not fully relaxed. It will be very line_7: interesting to see whether HST detects any sharp, high contrast features in line_8: this galaxy. NGC 1439 is the intrinsically faintest galaxy in the sample, with line_9: the lowest velocity dispersion. NGC 1427 has a rotation curve that is line_10: unresolved even at subarcsecond seeing. NGC 5982 is the only galaxy which has line_11: a distinct core that has a rotation axis parallel to the major axis. All other line_12: systems rotate around the minor axis. line_13: We propose to obtain sets of images in the F555W and F814W filters. The F555W line_14: filter is chosen for this study because it provides high throughput and its PSF line_15: will be well monitored. This is important for removing a nuclear point source line_16: prior to further analysis (as was necessary for IC 1459) and if deconvolution line_17: is applied. The F814W filter provides a long wavelength base for color line_18: analysis (it is less affected by dust), the background sky is fainter (Wright line_19: 1985) and better samples the dominant stellar component. Although we expect line_20: WFPC2 to have an image quality close to specifications (i.e. 70% in 0.1''), we line_21: can still in principle gain through deconvolution techniques with imaging line_22: closer to the diffraction limit of the telescope (i.e. 80% in 0.1''). line_23: 1. Jedrzejewski Schechter 1988, ApJ, 330, L87 ! question: 4 section: 1 line_1: The use of the imaging capabilities of HST is a logical and important component line_2: of a broadly-based observational program involving ground-based long-slit line_3: spectra and ground-based images of ellipticals with kinematically-distinct line_4: cores. Both the spectroscopic and the imaging results suggest that these line_5: distinct nuclear subcomponents are unresolved from the ground in typical line_6: 1-2'' seeing. The cores of ellipticals are known to be at best marginally line_7: resolved from the ground, with a few notable exceptions (see e.g., ref. 1). If line_8: compact star clusters or black-holes are significant in these cores, the small line_9: gains in resolution possible at Hawaii and other sites will not be decisive in line_10: establishing the structure of the nuclei on scales <0.2''. The results by line_11: Lauer et al (ref. 2,3,4) have shown convincingly that PC imaging can do line_12: significantly better than any ground-based facilities. The images requested line_13: here will complement the available ground-based multicolor CCD surface line_14: photometry by allowing comparison of the core structure and properties with line_15: those at larger radii. Furthermore, the early `discovery' spectroscopic line_16: observations have been supplemented by a set of higher S/N long-slit spectra line_17: taken with the highest practical ground-based spatial resolution (1'' with line_18: 0.3-0.6'' pixels) at a variety of position angles. These data have been line_19: acquired both in the Northern and Southern hemispheres, at CTIO and Lick. line_20: The use of the imaging capabilities of HST is a logical and important component line_21: Ideally one would like high spatial resolution spectroscopic observations from line_22: HST. This is impractical without a good imaging capacity and without a line_23: long-slit spectrograph on HST; the FOS integrations required would be ! question: 4 section: 2 line_1: prohibitively long. The best approach is the compromise one of high resolution line_2: HST images, combined with ground-based kinematical mapping and overlapping with line_3: ground-based images that define the large-scale (r > 5-10'') structure. line_4: 1. Kormendy 1985, ApJ, 292, L9 line_5: 2. Lauer, et al 1991, ApJ, 369, L41 line_6: 3. Lauer, et al 1992a, AJ, 103, 703 line_7: 4. Lauer, et al 1992b, AJ, 104, 552 ! question: 5 section: 1 line_1: ! question: 6 section: 1 line_1: ! ! ! question: 8 section: 1 line_1: ! question: 9 section: 1 line_1: The PI (MF) and Co-I (GDI) have been involved in several previous HST programs. line_2: They include: line_4: 2684 (The Medium Deep Survey), GDI. line_5: 4664 (Nearby Nuclei Snapshot Survey), GDI. line_6: 3551 (Ellipticals with Kinematically Distinct Nuclei), GDI and MF. line_7: 2227 and 3905 (The Extra-Galactic Distance Scale), GDI. line_9: The most directly related program is 3551 from cycle 2. This was a single color line_10: (F555W) PC imaging project of seven galaxies with kinematically distinct cores. line_11: In our paper (Illingworth, Forbes Franx 1993, in preparation) we report that IC line_12: 1459 reveals an unresolved point source (V 18.5mag), a cusp to the central line_13: starlight profile (with a slope similar to that found for M87) and a small line_14: scale dust lane that appears to reach into the very nucleus and may thus be line_15: associated with material that fuels the nuclear activity. Reduction and line_16: analysis of the other six galaxies are in progress. Although this data contains line_17: much useful information on small scales, it provides no color information which line_18: is the main focus of this proposal. The data requested here will also benefit line_19: from the improved optics allowing more subtle features, than present in IC line_20: 1459, to be revealed. line_22: Program 4664 involved short, single color (F555W) exposures of nearby SO and line_23: spiral nuclei. Although it is related in general aim (to probe the nuclear ! question: 9 section: 2 line_1: region of galaxies unavailable to ground-based observations) this program can line_2: not address the specific areas that can be tackled with the multi-color data line_3: requested in this proposal. line_5: Publications include: line_6: Illingworth, Forbes Franx 1993, in preparation (June 93). line_7: Forbes et al. 1993, IAU 158, Very High Angular Resolution Imaging, in press. line_8: Forbes, Illingworth Franx 1993, in preparation (July 93). line_9: Griffiths et al. 1993, Science with the HST, in press. line_11: There have also been various abstracts published from talks and posters at AAS line_12: meetings. ! question: 10 section: 1 line_1: Most of the data reduction will be carried out at Lick Observatory. line_2: Lick Observatory has a strong foundation for image processing of large line_3: HST images (via the Medium Deep Survey key project and WFPC IDT). The line_4: department has a powerful host SUN 4/280 system with high performance line_5: peripherals. Both GDI and DAF have UCSC-supplied SUN workstations, line_6: which will draw upon the departmental resources. Several staff are line_7: available to support the systems and system software development. line_8: There is also a pool of ten or more graduate students, some of whom line_9: have University Fellowships, who work intensively with optical imaging line_10: and spectroscopy. S. Faber, an WFPC IDT team member, is on the Lick line_11: faculty, and will be a source of the IDT team's valuable early line_12: experience in processing WFPC data. GDI also has access to the 3 m and line_13: 1 m telescopes on Mt. Hamilton, and to the Keck 10m. line_15: MF, previously a Hubble Fellow, is now a full Professor at the Kapteyn line_16: Astronomical Institute. This position includes summer salary, and some line_17: research funding. The Kapteyn Institute is involved in several HST GO line_18: programs. ! !end of general form text general_form_address: lname: FRANX fname: MARIJN category: PI inst: 6830 addr_1: KAPTEYN ASTRONOMICAL INSTITUTE addr_2: P.O. BOX 800 city: GRONINGEN zip: 9700 AV country: NETHERLANDS phone: (011) 31 50 634067 telex: FRANX@ASTRO.RUG.NL ! lname: category: CON ! ! end of general_form_address records fixed_targets: targnum: 1 name_1: IC1459 descr_1: E,303 pos_1: RA= 22H57M10.47S +/- 0.1S, pos_2: DEC=-36D27'45.2 " +/- 1.0", pos_3: PLATE-ID=05XU equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.1 +/- 1 ! targnum: 2 name_1: NGC1427 descr_1: E,303 pos_1: RA= 03H42M19.50S +/- 0.1S, pos_2: DEC=-35D23'32.7 " +/- 1.0" equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER ! targnum: 3 name_1: NGC1439 descr_1: E,303 pos_1: RA= 03H44M49.86S +/- 0.1S, pos_2: DEC=-21D55'13.8" +/- 1.0" equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=16.0 +/- 1 ! targnum: 4 name_1: NGC1700 descr_1: E,303 pos_1: RA= 04H56M56.21S +/- 0.1S, pos_2: DEC=-04D51'56.5" +/- 1.0", pos_3: PLATE-ID=04MX equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.5 +/- 1 ! targnum: 5 name_1: NGC3608 descr_1: E,303 pos_1: RA= 11H16M58.95S +/- 0.1S, pos_2: DEC= 18D08'54.9 " +/- 1.0", pos_3: PLATE-ID=01TO equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=16.2 +/- 1 ! targnum: 6 name_1: NGC4278 descr_1: E,303 pos_1: RA= 12H20M06.86S +/- 0.1S, pos_2: DEC= 29D16'50.3" +/- 1.0", pos_3: PLATE-ID=00DJ equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.4 +/- 1 ! targnum: 7 name_1: NGC4365 descr_1: E,303 pos_1: RA= 12H24M28.30S +/- 0.1S, pos_2: DEC= 7D19'03.4" +/- 1.0", pos_3: PLATE-ID=01UQ equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.9 +/- 1 ! targnum: 8 name_1: NGC4406 descr_1: E,303 pos_1: RA= 12H26M11.78S +/- 0.1S, pos_2: DEC= 12D56'46.3" +/- 1.0", pos_3: PLATE-ID=00IY equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.7 +/- 1 ! targnum: 10 name_1: NGC4494 descr_1: E,303 pos_1: RA= 12H31M24.09S +/- 0.1S, pos_2: DEC= 25D46'28.9" +/- 1.0" equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.6 +/- 1 ! targnum: 11 name_1: NGC4552 descr_1: E,303 pos_1: RA= 12H35M39.83S +/- 0.1S, pos_2: DEC= 12D33'22.8" +/- 1.0", pos_3: PLATE-ID=00IY equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.0 +/- 1 ! targnum: 12 name_1: NGC4589 descr_1: E,303 pos_1: RA= 12H37M24.89S +/- 0.1S, pos_2: DEC= 74D11'30.9" +/- 1.0" equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=16.3 +/- 1 ! targnum: 13 name_1: NGC5322 descr_1: E,303 pos_1: RA= 13H49M15.45S +/- 0.1S, pos_2: DEC= 60D11'25.9" +/- 1.0", pos_3: PLATE-ID=01R0 equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.8 +/- 1 ! targnum: 14 name_1: NGC5813 descr_1: E,303 pos_1: RA= 15H01M11.18S +/- 0.1S, pos_2: DEC= 01D42'07.1" +/- 1.0" equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=16.0 +/- 1 ! targnum: 15 name_1: NGC5982 descr_1: E,303 pos_1: RA= 15H38M39.94S +/- 0.1S, pos_2: DEC= 59D21'21.6" +/- 1.0" equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=15.9 +/- 1 ! targnum: 16 name_1: NGC7626 descr_1: E,303 pos_1: RA= 23H20M42.55S +/- 0.1S, pos_2: DEC= 08D13'01.0" +/- 1.0" equinox: J2000 comment_1: FLUX IS SURFACE BRIGHTNESS AT 1 comment_2: ARCSEC DISTANCE FROM CENTER comment_3: SURFACE BRIGHTNESS (MUCH) HIGHER comment_4: AT CENTER fluxnum_1: 1 fluxval_1: SURF(R)=16.6 +/- 1 ! ! end of fixed targets ! No solar system records found ! No generic target records found exposure_logsheet: linenum: 1.000 targname: IC1459 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: CYCLE 4 / 1-16.1; req_2: GROUP 1-1.1 NO GAP ! linenum: 1.100 targname: IC1459 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 1.1 AS 1.0 ! linenum: 2.000 targname: NGC1427 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 4 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 2-2.1 NO GAP ! linenum: 2.100 targname: NGC1427 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 2.1 AS 2.0 ! linenum: 3.000 targname: NGC1439 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 6 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 3-3.1 NO GAP ! linenum: 3.100 targname: NGC1439 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 3.1 AS 3.0 ! linenum: 4.000 targname: NGC1700 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 5 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 4-4.1 NO GAP ! linenum: 4.100 targname: NGC1700 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 4.1 AS 4.0 ! linenum: 5.000 targname: NGC3608 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 5-5.1 NO GAP ! linenum: 5.100 targname: NGC3608 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 5.1 AS 5.0 ! linenum: 6.000 targname: NGC4278 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 6-6.1 NO GAP ! linenum: 6.100 targname: NGC4278 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 6.1 AS 6.0 ! linenum: 7.000 targname: NGC4365 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 7-7.1 NO GAP ! linenum: 7.100 targname: NGC4365 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 7.1 AS 7.0 ! linenum: 8.000 targname: NGC4406 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 8-8.1 NO GAP ! linenum: 8.100 targname: NGC4406 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 8.1 AS 8.0 ! linenum: 10.000 targname: NGC4494 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 10-10.1 NO GAP ! linenum: 10.100 targname: NGC4494 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 10.1 AS 10.0 ! linenum: 11.000 targname: NGC4552 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 11-11.1 NO GAP ! linenum: 11.100 targname: NGC4552 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 11.1 AS 11.0 ! linenum: 12.000 targname: NGC4589 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 12-12.1 NO GAP ! linenum: 12.100 targname: NGC4589 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 12.1 AS 12.0 ! linenum: 13.000 targname: NGC5322 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 3 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 13-13.1 NO GAP ! linenum: 13.100 targname: NGC5322 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 13.1 AS 13.0 ! linenum: 14.000 targname: NGC5813 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 14-14.1 NO GAP ! linenum: 14.100 targname: NGC5813 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 14.1 AS 14.0 ! linenum: 15.000 targname: NGC5982 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 7 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 15-15.1 NO GAP ! linenum: 15.100 targname: NGC5982 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 15.1 AS 15.0 ! linenum: 16.000 targname: NGC7626 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F555W num_exp: 1 time_per_exp: 1000S fluxnum_1: 1 priority: 2 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: GROUP 16-16.1 NO GAP ! linenum: 16.100 targname: NGC7626 config: WFPC2 opmode: IMAGE aperture: PC1 sp_element: F814W num_exp: 1 time_per_exp: 500S fluxnum_1: 1 priority: 1 param_1: CR-SPLIT=0.5 param_2: CR-TOLERANCE=0.1 param_3: ATD-GAIN=7 req_1: SAME POS FOR 16.1 AS 16.0 ! ! end of exposure logsheet ! 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