! File: 2340C.PROP ! Database: PEPDB ! Date: 17-FEB-1994:05:08:43 coverpage: title_1: IMAGING AND SPECTROSCOPY IN THE CRAB NEBULA sci_cat: INTERSTELLAR MEDIUM sci_subcat: SN & SNR proposal_for: GO pi_title: DR. pi_fname: KRIS pi_lname: DAVIDSON pi_inst: MINNESOTA, UNIVERSITY OF pi_country: USA pi_phone: 612-624-5711 keywords_1: SUPERNOVA, SUPERNOVA REMNANT, CRAB NEBULA, ABUNDANCE, keywords_2: NUCLEOSYNTHESIS, MORPHOLOGY hours_pri: 12.40 num_pri: 9 wf_pc: Y foc: Y funds_amount: 140000 funds_length: 12 funds_date: JAN-91 pi_position: DR. off_fname: MERLIN off_lname: GARLID off_title: ASSISTANT DIRECTOR off_inst: UNIVERSITY OF MINNESOTA off_addr_1: 1919 UNIVERSITY AVENUE - 5TH FLOOR off_addr_2: OFFICE OF RESEARCH ADMINISTRATION off_city: ST. PAUL off_state: MN off_zip: 55104 off_country: USA off_phone: 612-624-0288 ! end of coverpage abstract: line_1: The Crab Nebula is the only young SNR (i.e., composed mainly of SN line_2: ejecta) whose condensations are resolvable by ST while also being line_3: "easily" observable in the UV. Moreover,it is now thought to represent line_4: an important SN mass range, and at the same time the Crab's chemical line_5: composition is poorly understood. V spectral data is essential for line_6: understanding the Crab, while high-spatial-resolution studies of its line_7: condensations will also be useful for producing more reliable line_8: ionization models in order to study it composition and its dynamics. line_10: We propose a detailed set of observations with the WFC, and FOC, line_11: partly to obtain useful data soon and partly to enable planning of line_12: future, more sophisticated UV spectroscopy. The WFC is to study line_13: density gradients and local structure in the condensations and also to line_14: provide accurate positions for possible future FOS work. The FOC is to line_15: make images of UV emission lines, for composition with visual- line_16: wavelength structure and also for possible future planning. ! ! end of abstract general_form_proposers: lname: KAFATOS fname: MINAS title: DR. inst: GEORGE MASON UNIVERSITY country: USA ! lname: MACALPINE fname: GORDON title: DR. mi: M inst: MICHIGAN, UNIVERSITY OF country: USA ! lname: UOMOTO fname: ALAN title: DR. inst: JOHNS HOPKINS UNIVERSITY country: USA ! lname: WILSON fname: ANDREW title: DR. mi: S inst: MARYLAND, UNIVERSITY OF country: USA ! lname: DAVIDSON fname: KRIS title: P.I. inst: MINNESOTA, UNIVERSITY OF country: USA ! lname: HENRY fname: RICHARD title: DR. mi: BC inst: OKLAHOMA, UNIVERSITY OF country: USA ! lname: FESEN fname: ROBERT title: DR. mi: A inst: DARTMOUTH COLLEGE country: USA ! lname: KIRSHNER fname: ROBERT title: DR. mi: P inst: CFA country: USA ! ! end of general_form_proposers block general_form_text: question: 3 section: 1 line_1: WFC: We will image the OIII, H-alpha, NII, and SII emission lines in 2 line_2: WFC fields in the Crab using narrow filters and about 20 m per line_3: exposure. We also plan continuum exposures in two of the fields to line_4: assess the degree of non-thermal structure associated with the thermal line_5: filaments. A third intermediate field will be done with one filter line_6: for additional coverage and astrometry. We have optimized the fields line_7: to have maximum expectation of excluding the 3 brightest stars in the line_8: region without any special requirement on ST orientation, but this line_9: detail is not critical to the project. line_11: FOC/48, 44" field: This is essential for imaging the brightest UV line_12: emission lines in selected parts of the Crab. (WFC readout noise is line_13: too large for this low UV surface brightness object.) The 3 most line_14: promising filamentary regions have been selected for this purpose. We line_15: will use filter F175W to detect CIII] 1908 emission and F150W to line_16: detect the sum of CIII] 1908 plus CIV 1549 and HeII 1640. (F195W is line_17: unsuitable because its visual-wavelength transmission is too high.) line_18: The exposure times are about 30 minutes each. A shorter exposure with line_19: F275W will be used to determine UV continuum for subtraction. ! question: 4 section: 1 line_1: WFC: Models suggest characteristic size scales of 0.1 to 0.4 arcsec line_2: for the thermal-gas structure, and ground-based images appear line_3: consistent with this idea. The Crab obviously cannot be done by line_4: speckle techniques. Therefore, only HST can provide images to line_5: resolve the ionization and gas-dynamical structure. Excellent line_6: measures of the filament proper motions are also attainable from the line_7: WFC images. line_8: FOC/48: We know that major spatial variations in spectra occur in the line_9: Crab, probably due to composition gradients. Bright spots in the UV line_10: carbon lines are expected to occur, and if they do occur then we need line_11: to see the UV in order to detect them for future UV and line_12: visual-wavelength spectroscopy. The FOC is the only instrument that line_13: can detect the carbon UV lines at the expected surface brightnesses. line_14: (WFC won't work for this; readout noise makes it impossible.) ! question: 5 section: 1 line_1: Since surface brightnesses of emission lines in the Crab Nebula span a line_2: very large range, S/N ratios depend on location. In general, the line_3: surface brightness is low enough to be difficult for both the WFC and line_4: the FOC. We have adjusted our exposure times to give excellent S/N line_5: and high spatial resolution on the few brightest condensations, and line_6: useful S/N on a reasonably large fraction of the Crab filaments. line_7: Spatial resolution will be S/N limited for the fainter filaments in line_8: the WFC images and for all structure in the FOC images. Refs. to line_9: fluxes in the Crab are given in (e.g.) Ann.Revs.Astron.Ap. 23, 119, line_10: Ap.J. 228, 179 (visual-wavelength) and Ap.J. 253, 696 (UV). line_11: WFC: Fairly bright filaments have apparent intensities of the order of line_12: 1.E-14 erg cm-2 s-1 arcsec-2 in each of the brightest line_13: visual-wavelength emission lines. The peak QT-factors for appropriate line_14: WFC filters are slightly less than 0.1, implying somewhat more than line_15: 100 cts/pixel in 20-minutes, for S/N = about 7. For fainter filaments line_16: the S/N-limited resolution may be degraded to 0.2 arcsec. Since we line_17: must sample several physically different emission lines, 20 minutes line_18: per field is appropriate for exploratory purposes. ! question: 5 section: 2 line_1: FOC: IUE data suggest that we can expect about 1.E-14 erg cm-2 s-1 line_2: arcsec-2 in the CIII] 1908 line (e.g.) in a bright condensation. With line_3: F175W, of the order of 360 cts per arcsec2 will be obtained in a line_4: 30-minute exposure. But the non-thermal continuum background will be line_5: comparable; therefore the S/N ratio in one arcsec2 would be 10-15 if line_6: continuum subtraction (based on F275W exposure) were perfect. So a line_7: realistic S/N in the net CIII]-emission image is between 5 and 10 for line_8: 1 arcsec2, which will therefore be the effective resolution for the line_9: assumed emission brightness. A few condensations may be considerably line_10: brighter. ! question: 7 section: 1 line_1: A WFC image of the Crab will contain structure across most of the WFC line_2: field, and is more complicated than an image even of a cluster of line_3: localized objects. Moreover, the intersection of radial velocities in line_4: the Crab within the available WFC narrow emission-line filter bands line_5: will create additional complexity in the data analysis. Image line_6: resolution will be position-dependent (because it is S/N-limited in line_7: some of the filaments). The FOC images will not be quite as line_8: complicated, but will have to be linearly combined in order to produce line_9: separate CIII], (CIV+HeII), and UV-continuum maps of the localized FOC line_10: fields. line_11: Davidson, Uomoto, Fesen, and Wilson will concentrate on data line_12: reduction. Using the WFC images, emission-line surface brightnesses line_13: will be measured at high resolution, leading to estimates of local line_14: column thickness and densities of ions as functions of location within line_15: individual condensations. Astrometry will be done on stars in the WFC line_16: fields and precise locations of gaseous condensations will be line_17: determined -- both for future spectroscopy and also to measure the line_18: nebular expansion rate. ! question: 7 section: 2 line_1: The FOC ultraviolet images will allow maps of (CIV + HeII) and CIII] line_2: emission-line brightnesses to be made. These will be compared with line_3: ground-based visual-wavelength spectroscopy of the same regions. If line_4: UV-bright spots are discovered in the FOC images, ground-based spectra line_5: of those locations will be obtained using, for example, the line_6: McGraw-Hill 2.4-m telescope. line_8: Henry, MacAlpine, Kafatos and Kirshner will concentrate on the line_9: spectroscopic implications of the FOC data. MacAlpine's line_10: photoionization codes will be used to produce realistic models of line_11: thermal condensations, taking local morphology indicated in the WFC line_12: images into account. ! !end of general form text general_form_address: lname: DAVIDSON fname: KRIS title: DR. category: PI inst: UNIVERSITY OF MINNESOTA addr_1: 116 CHRUCH ST. S.E. city: MINNEAPOLIS state: MN zip: 55455 country: USA ! ! end of general_form_address records fixed_targets: targnum: 1 name_1: NGC1952-WFCC1 name_2: CRAB-NEBULA name_3: M1 descr_1: INTERSTELLAR MEDIUM; SUPERNOVA REMNANT; descr_2: CENTRAL FIELD pos_1: RA= 05H 34M 32.72S +/- 0.07S, pos_2: DEC=+22D 01' 04.00" +/- 1" equinox: 2000 rv_or_z: V=0 comment_1: EMISSION LINES SPAN +/- 1500 KM/S comment_2: IN RADIAL VELOCITY IN EACH PART comment_3: OF FIELD. SURFACE BRIGHTNESS comment_4: SPANS A LARGE RANGE OF VALUES. comment_5: FLUXES QUOTED HERE REFER comment_6: TO A TYPICAL MODERATE FILAMENT. fluxnum_1: 1 fluxval_1: SURF(V) = 21 +/- 2 fluxnum_2: 2 fluxval_2: SURF-LINE(5007) = 1.0 +/- 1.0 E-14 fluxnum_3: 3 fluxval_3: SURF-LINE(6563) = 1.0 +/- 1.0 E-14 fluxnum_4: 4 fluxval_4: SURF-LINE(6583) = 1.0 +/- 1.0 E-15 fluxnum_5: 5 fluxval_5: SURF-LINE(6724) = 0.7 +/- 0.7 E-15 fluxnum_6: 6 fluxval_6: SURF-LINE(3727) = 5.0 +/- 5.0 E-15 fluxnum_7: 7 fluxval_7: W-LINE(5007) = 1.0 +/- 0.0 fluxnum_8: 8 fluxval_8: W-LINE(6563) = 1.0 +/- 0.0 fluxnum_9: 9 fluxval_9: W-LINE(6583) = 1.0 +/- 0.0 fluxnum_10: 10 fluxval_10: W-LINE(6724) = 1.0 +/- 0.0 ! targnum: 2 name_1: NGC1952-WFCS1 name_2: CRAB-NEBULA name_3: M1 descr_1: INTERSTELLAR MEDIUM; SUPERNOVA REMNANT; descr_2: SOUTH-1 FIELD pos_1: RA= 05H 34M 33.44S +/- 0.07S, pos_2: DEC=+22D 00' 12.00" +/- 1" equinox: 2000 rv_or_z: V=0 comment_1: EMISSION LINES SPAN +/- 1500 KM/S comment_2: IN RADIAL VELOCITY IN EACH PART comment_3: OF FIELD. SURFACE BRIGHTNESS comment_4: SPANS A LARGE RANGE OF VALUES. comment_5: FLUXES QUOTED HERE REFER comment_6: TO A TYPICAL MODERATE FILAMENT. fluxnum_1: 1 fluxval_1: SURF(V) = 21 +/- 2 fluxnum_2: 2 fluxval_2: SURF-LINE(5007) = 1.0 +/- 1.0 E-14 fluxnum_3: 3 fluxval_3: SURF-LINE(6563) = 1.0 +/- 1.0 E-14 fluxnum_4: 4 fluxval_4: SURF-LINE(6583) = 1.0 +/- 1.0 E-15 fluxnum_5: 5 fluxval_5: SURF-LINE(6724) = 0.7 +/- 0.7 E-15 fluxnum_6: 6 fluxval_6: SURF-LINE(3727) = 5.0 +/- 5.0 E-15 fluxnum_7: 7 fluxval_7: W-LINE(5007) = 1.0 +/- 0.0 fluxnum_8: 8 fluxval_8: W-LINE(6563) = 1.0 +/- 0.0 fluxnum_9: 9 fluxval_9: W-LINE(6583) = 1.0 +/- 0.0 fluxnum_10: 10 fluxval_10: W-LINE(6724) = 1.0 +/- 0.0 ! targnum: 3 name_1: NGC1952-WFCN1 name_2: CRAB-NEBULA name_3: M1 descr_1: INTERSTELLAR MEDIUM; SUPERNOVA REMNANT; descr_2: NORTH-1 FIELD pos_1: RA= 05H 34M 28.84S +/- 0.07S, pos_2: DEC=+22D 02' 44.00" +/- 1" equinox: 2000 rv_or_z: V=0 comment_1: EMISSION LINES SPAN +/- 1500 KM/S comment_2: IN RADIAL VELOCITY IN EACH PART comment_3: OF FIELD. SURFACE BRIGHTNESS comment_4: SPANS A LARGE RANGE OF VALUES. comment_5: FLUXES QUOTED HERE REFER comment_6: TO A TYPICAL MODERATE FILAMENT. fluxnum_1: 1 fluxval_1: SURF(V) = 21 +/- 2 fluxnum_2: 2 fluxval_2: SURF-LINE(5007) = 1.0 +/- 1.0 E-14 fluxnum_3: 3 fluxval_3: SURF-LINE(6563) = 1.0 +/- 1.0 E-14 fluxnum_4: 4 fluxval_4: SURF-LINE(6583) = 1.0 +/- 1.0 E-15 fluxnum_5: 5 fluxval_5: SURF-LINE(6724) = 0.7 +/- 0.7 E-15 fluxnum_6: 6 fluxval_6: SURF-LINE(3727) = 5.0 +/- 5.0 E-15 fluxnum_7: 7 fluxval_7: W-LINE(5007) = 1.0 +/- 0.0 fluxnum_8: 8 fluxval_8: W-LINE(6563) = 1.0 +/- 0.0 fluxnum_9: 9 fluxval_9: W-LINE(6583) = 1.0 +/- 0.0 fluxnum_10: 10 fluxval_10: W-LINE(6724) = 1.0 +/- 0.0 ! targnum: 4 name_1: NGC1952-FOC01 name_2: CRAB-NEBULA name_3: M1 descr_1: INTERSTELLAR MEDIUM; SUPERNOVA REMNANT; descr_2: NORTH LOOP pos_1: RA= 05H 34M 32.80S +/- 0.07S, pos_2: DEC=+22D 02' 11.00" +/- 1" equinox: 2000 rv_or_z: V=0 fluxnum_1: 1 fluxval_1: SURF(V) = 21.1 +/- 0.8 fluxnum_2: 2 fluxval_2: SURF-LINE(1908) = 1.0 +/- 0.8 E-14 fluxnum_3: 3 fluxval_3: SURF-LINE(1548) = 1.0 +/- 0.8 E-14 fluxnum_4: 4 fluxval_4: SURF-CONT(1800) = 0.6 +/- 0.3 E-17 fluxnum_5: 5 fluxval_5: W-LINE(1908) = 1.0 +/- 0.0 fluxnum_6: 6 fluxval_6: W-LINE(1548) = 1.0 +/- 0.0 ! targnum: 5 name_1: NGC1952-FOC02 name_2: CRAB-NEBULA name_3: M1 descr_1: INTERSTELLAR MEDIUM; SUPERNOVA REMNANT; descr_2: BRIGHT FILAMENT WSW pos_1: RA= 05H 34M 29.70S +/- 0.07S, pos_2: DEC=+22D 00' 35.00" +/- 1" equinox: 2000 rv_or_z: V=0 fluxnum_1: 1 fluxval_1: SURF(V) = 19.8 +/- 0.5 fluxnum_2: 2 fluxval_2: SURF-LINE(1908) = 1.0 +/- 0.8 E-14 fluxnum_3: 3 fluxval_3: SURF-LINE(1548) = 1.0 +/- 0.8 E-14 fluxnum_4: 4 fluxval_4: SURF-CONT(1800) = 2.0 +/- 0.8 E-17 fluxnum_5: 5 fluxval_5: W-LINE(1908) = 1.0 +/- 0.0 fluxnum_6: 6 fluxval_6: W-LINE(1548) = 1.0 +/- 0.0 ! targnum: 6 name_1: NGC1952-FOC03 name_2: CRAB-NEBULA name_3: M1 descr_1: INTERSTELLAR MEDIUM; SUPERNOVA REMNANT; descr_2: BRIGHT FILAMENT SE pos_1: RA= 05H 34M 34.20S +/- 0.07S, pos_2: DEC=+21D 59' 50.00" +/- 1" equinox: 2000 rv_or_z: V=0 fluxnum_1: 1 fluxval_1: SURF(V) = 20.5 +/- 0.6 fluxnum_2: 2 fluxval_2: SURF-LINE(1908) = 1.0 +/- 0.8 E-14 fluxnum_3: 3 fluxval_3: SURF-LINE(1548) = 1.0 +/- 0.8 E-14 fluxnum_4: 4 fluxval_4: SURF-CONT(1800) = 1.1 +/- 0.5 E-17 fluxnum_5: 5 fluxval_5: W-LINE(1908) = 1.0 +/- 0.0 fluxnum_6: 6 fluxval_6: W-LINE(1548) = 1.0 +/- 0.0 ! ! end of fixed targets ! No solar system records found ! No generic target records found exposure_logsheet: linenum: 11.000 sequence_1: DEFINE sequence_2: WFCC1 targname: NGC1952-WFCC1 config: WFC opmode: IMAGE aperture: ALL sp_element: # num_exp: 1 time_per_exp: 1M s_to_n: # fluxnum_1: # priority: # param_1: PRE-FLASH=YES, param_2: CR-SPLIT=NO req_1: POS TARG 0,0 ! linenum: 12.000 sequence_1: DEFINE sequence_2: WFCS1 targname: NGC1952-WFCS1 config: WFC opmode: IMAGE aperture: ALL sp_element: # num_exp: 1 time_per_exp: 1M s_to_n: # fluxnum_1: # priority: # param_1: PRE-FLASH=YES, param_2: CR-SPLIT=NO req_1: POS TARG 0,0 ! linenum: 13.000 sequence_1: DEFINE sequence_2: WFCN1 targname: NGC1952-WFCN1 config: WFC opmode: IMAGE aperture: ALL sp_element: # num_exp: 1 time_per_exp: 1M s_to_n: # fluxnum_1: # priority: # param_1: PRE-FLASH=YES, param_2: CR-SPLIT=NO req_1: POS TARG 0,0 ! linenum: 14.000 sequence_1: DEFINE sequence_2: FOC01 targname: NGC1952-FOC01 config: FOC/48 opmode: IMAGE aperture: 512X1024 sp_element: # num_exp: 1 time_per_exp: 1M s_to_n: # fluxnum_1: # priority: # param_1: PIXEL=50X25 ! linenum: 15.000 sequence_1: DEFINE sequence_2: FOC02 targname: NGC1952-FOC02 config: FOC/48 opmode: IMAGE aperture: 512X1024 sp_element: # num_exp: 1 time_per_exp: 1M s_to_n: # fluxnum_1: # priority: # param_1: PIXEL=50X25 ! linenum: 16.000 sequence_1: DEFINE sequence_2: FOC03 targname: NGC1952-FOC03 config: FOC/48 opmode: IMAGE aperture: 512X1024 sp_element: # num_exp: 1 time_per_exp: 1M s_to_n: # fluxnum_1: # priority: # param_1: PIXEL=50X25 ! linenum: 111.000 sequence_1: USE WFCC1 sp_element: F664N time_per_exp: X15 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4, fluxnum_3: 5 priority: 3 ! linenum: 112.000 sequence_1: USE WFCC1 sp_element: F656N time_per_exp: X15 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4 priority: 3 ! linenum: 114.000 sequence_1: USE WFCC1 sp_element: F502N time_per_exp: X15 s_to_n: 7 fluxnum_1: 2 priority: 3 ! linenum: 121.000 sequence_1: USE WFCS1 sp_element: F664N time_per_exp: X30 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4, fluxnum_3: 5 priority: 2 ! linenum: 122.000 sequence_1: USE WFCS1 sp_element: F656N time_per_exp: X24 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4 priority: 2 ! linenum: 123.000 sequence_1: USE WFCS1 sp_element: F547M time_per_exp: X20 s_to_n: 7 fluxnum_1: 1 priority: 2 comment_1: S/N IS FOR 1 PIXEL WITH comment_2: SURF(V)=21, CRAB AVERAGE. comment_3: CONTINUUM IS comment_4: BRIGHTER THAN SURF(V)=21 IN comment_5: PARTS OF FIELD. ! linenum: 124.000 sequence_1: USE WFCS1 sp_element: F502N time_per_exp: X30 s_to_n: 7 fluxnum_1: 2 priority: 2 ! linenum: 125.000 sequence_1: USE WFCS1 sp_element: F658N time_per_exp: X30 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4 priority: 2 ! linenum: 126.000 sequence_1: USE WFCS1 sp_element: F673N time_per_exp: X30 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4, fluxnum_3: 5 priority: 2 ! linenum: 131.000 sequence_1: USE WFCN1 sp_element: F664N time_per_exp: X20 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4, fluxnum_3: 5 priority: 1 ! linenum: 132.000 sequence_1: USE WFCN1 sp_element: F656N time_per_exp: X20 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4 priority: 1 req_1: SAME POS FOR 132-136 AS 131 ! linenum: 133.000 sequence_1: USE WFCN1 sp_element: F547M time_per_exp: X15 s_to_n: 7 fluxnum_1: 1 priority: 2 ! linenum: 134.000 sequence_1: USE WFCN1 sp_element: F502N time_per_exp: X20 s_to_n: 7 fluxnum_1: 2 priority: 1 ! linenum: 135.000 sequence_1: USE WFCN1 sp_element: F658N time_per_exp: X20 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4 priority: 1 ! linenum: 136.000 sequence_1: USE WFCN1 sp_element: F673N time_per_exp: X20 s_to_n: 7 fluxnum_1: 3, fluxnum_2: 4, fluxnum_3: 5 priority: 2 ! linenum: 141.000 sequence_1: USE FOC01 sp_element: F175W time_per_exp: X30 s_to_n: 12 fluxnum_1: 4 priority: 3 comment_1: S/N IS PER SQ ARCSEC FOR comment_2: EMISSION LINE IMAGE AFTER comment_3: CONTINUUM SUBTRACTION. ! linenum: 142.000 sequence_1: USE FOC01 sp_element: F150W time_per_exp: X30 s_to_n: 12 fluxnum_1: 3 priority: 3 comment_1: S/N IS PER SQ ARCSEC FOR comment_2: EMISSION LINE IMAGE AFTER comment_3: CONTINUUM SUBTRACTION. ! linenum: 143.000 sequence_1: USE FOC01 sp_element: F275W time_per_exp: X10 s_to_n: 15 fluxnum_1: 4 priority: 3 comment_1: S/N IS FOR 1 SQ ARCSEC, comment_2: NEEDED FOR SUBTRACTION IN comment_3: LINE EMISSION IMAGES. ! linenum: 151.000 sequence_1: USE FOC02 sp_element: F175W time_per_exp: X30 s_to_n: 12 fluxnum_1: 4 priority: 2 comment_1: S/N IS PER SQ ARCSEC FOR comment_2: EMISSION LINE IMAGE AFTER comment_3: CONTINUUM SUBTRACTION. ! linenum: 152.000 sequence_1: USE FOC02 sp_element: F150W time_per_exp: X30 s_to_n: 12 fluxnum_1: 3 priority: 2 comment_1: S/N IS PER SQ ARCSEC FOR comment_2: EMISSION LINE IMAGE AFTER comment_3: CONTINUUM SUBTRACTION. ! linenum: 153.000 sequence_1: USE FOC02 sp_element: F275W time_per_exp: X10 s_to_n: 25 fluxnum_1: 4 priority: 2 comment_1: S/N IS FOR 1 SQ ARCSEC, comment_2: NEEDED FOR SUBTRACTION IN comment_3: LINE EMISSION IMAGES. ! linenum: 161.000 sequence_1: USE FOC03 sp_element: F175W time_per_exp: X30 s_to_n: 12 fluxnum_1: 4 priority: 1 comment_1: S/N IS PER SQ ARCSEC FOR comment_2: EMISSION LINE IMAGE AFTER comment_3: CONTINUUM SUBTRACTION. ! linenum: 162.000 sequence_1: USE FOC03 sp_element: F150W time_per_exp: X30 s_to_n: 12 fluxnum_1: 3 priority: 1 comment_1: S/N IS PER SQ ARCSEC FOR comment_2: EMISSION LINE IMAGE AFTER comment_3: CONTINUUM SUBTRACTION. ! linenum: 163.000 sequence_1: USE FOC03 sp_element: F275W time_per_exp: X10 s_to_n: 20 fluxnum_1: 4 priority: 1 comment_1: S/N IS FOR 1 SQ ARCSEC, comment_2: NEEDED FOR SUBTRACTION IN comment_3: LINE EMISSION IMAGES. ! ! end of exposure logsheet ! No scan data records found