! $Id: 5345,v 9.1 1994/08/22 15:38:04 pepsa Exp $ COVERPAGE: TITLE_1: The jet/beam - cloud interaction in PKS 2152-699 SCI_CAT: Quasars & AGN SCI_SUBCAT: Radio Galaxies PROPOSAL_FOR: GO LARGE_PROJ: KEY_PROJ: TARG_OF_OPP: REALTIME: TIME_CRIT: PI_FNAME: Robert PI_LNAME: Fosbury PI_INST: 5555 PI_COUNTRY: Germany PI_PHONE: +49 89 320 06 235 HOURS_PRI: 3.33 HOURS_PAR: 0 NUM_PRI: 1 NUM_PAR: 0 WF_PC: Y OFF_FNAME: Piero OFF_LNAME: Benvenuti OFF_TITLE: Head, ST-ECF OFF_INST: 5555 OFF_ADDR_1: ST-ECF OFF_ADDR_2: Karl-Schwarzschild Str. 2 OFF_CITY: Garching b. Muenchen OFF_ZIP: D-85748 OFF_COUNTRY: Germany OFF_PHONE: +49 89 320 06 290 ABSTRACT: LINE_1: This is a proposal to add a vital datum to an already considerable LINE_2: dataset describing the jet/beam - cloud interaction in the radio galaxy LINE_3: PKS 2152-69. The interception of a blazar (photon) beam by a small, LINE_4: gas-rich companion galaxy has produced a wealth of physical phenomena LINE_5: which we have studied from radio to X-ray wavelengths. The gas in the LINE_6: companion has become highly ionized (up to Fe9+) and the dust is LINE_7: scattering the photon beam. The full understanding of this phenomenon LINE_8: allows us to derive important properties of the photon beams and, LINE_9: possibly, particle jets which are a part of the radio-loud AGN LINE_10:phenomenon. We intend to use the WFPC2 with two ultraviolet filters LINE_11:to image the cloud in strong emission line free regions around 3000A LINE_12:and 1600A to determine the ultraviolet continuum energy distribution LINE_13:which is already known at long UV wavelengths from IUE. In the longer LINE_14:of the filters, we will measure the linear polarization in order to LINE_15:determine its wavelength dependence in conjunction with our existing LINE_16:B-band measurement. The diagnosis of the scattering mechanism is LINE_17:important for the understanding of the 'alignment effect' in high LINE_18:redshift radio galaxies. GENERAL_FORM_PROPOSERS: LNAME: FOSBURY FNAME: Robert INST: 5555 COUNTRY: Germany ESA: Y LNAME: DI SEREGO ALIGHIERI FNAME: SPERELLO INST: 6420 COUNTRY: Italy ESA: Y LNAME: COURVOISIER FNAME: THIERRY INST: 7850 COUNTRY: Switzerland ESA: Y LNAME: TADHUNTER FNAME: Clive INST: University of Sheffield COUNTRY: UK ESA: Y LNAME: BINETTE FNAME: Luc INST: 4666 COUNTRY: Canada ESA: LNAME: BEDDING FNAME: TIMOTHY INST: 5520 COUNTRY: Germany ESA: Y LNAME: Wilson FNAME: Warwick INST: 4125 COUNTRY: Australia ESA: GENERAL_FORM_ADDRESS: LNAME: Fosbury FNAME: Robert CATEGORY: PI INST: 5555 ADDR_1: ST-ECF ADDR_2: Karl-Schwarzschild Str. 2 CITY: Garching b. Muenchen ZIP: D-85748 COUNTRY: Germany PHONE: +49 89 320 06 235 TELEX: rfosbury@eso.org GENERAL_FORM_TEXT: QUESTION: 3 SECTION: 1 LINE_1: The observation consists of two parts: Linear LINE_2: polarization measurements with F300W + POLQ LINE_3: and pure imaging with F160BW. All observations LINE_4: are to be taken with WFC using 2x2 on-chip LINE_5: binning. Each filter (polarization angle) LINE_6: consists of two ~1200S exposures (each with CR-SPLIT) LINE_7: with a relative shift of 1 (unbinned) pixel (0.1") LINE_8: in both X and Y between the two parts. All the LINE_9: polarization observations should be done with LINE_10: the SAME (arbitrary) orientation. The F160BW LINE_11: pair (which have slightly longer exposures) LINE_12: should also be done with the same orientation LINE_13: although this NEED not be the same as F300W/POLQ. LINE_14: If there is no scheduling problem, it would help LINE_15: analysis to have the same orientation for ALL the LINE_16: exposures. LINE_17: NB. Following the circular by M Clampin about the LINE_18: Wood's filter, we have changed the UV filter from 160BW LINE_19: to F218W. This produces an estimated red-leak of LINE_20: less than 1% for our source and is essentially LINE_21: free of emission line contamination. QUESTION: 4 SECTION: 1 LINE_1: We have obtained an extensive set of observations LINE_2: of the radio galaxy and of the HIC using ground- LINE_3: based optical and radio telescopes, IUE and Rosat LINE_4: (Tadhunter et al., 1987 and 1988, di Serego LINE_5: Alighieri et al., 1988, Fosbury et al., 1990, LINE_6: Fosbury et al. in prep, see section 2). In LINE_7: particular we have imaged the HIC in the LINE_8: continuum down to the atmospheric limit at 3250 A LINE_9: and in the H alpha and [OIII]5007 emission lines. LINE_10: We have obtained the UV spectral energy LINE_11: distribution of the cloud down to about 2500 A LINE_12: and its total Lyman alpha flux with IUE. We have LINE_13: measured the polarization of the continuum source LINE_14: in the cloud by pushing near its limits one of LINE_15: the most efficient imaging polarizers available LINE_16: (EFOSC at the 3.6m ESO telescope). We have done LINE_17: this in the B band, the only wavelength where it LINE_18: is possible from the ground since the cloud LINE_19: becomes rapidly fainter in the red and EFOSC is LINE_20: not efficient below 4000 A. Therefore we need the LINE_21: UV sensitivity of the HST both to extend the LINE_22: study of the spectral energy distribution to LINE_23: shorter wavelengths and to measure the dependence QUESTION: 4 SECTION: 2 LINE_1: of the polarization on the wavelength. We also LINE_2: need the high angular resolution of the HST to LINE_3: study the spatial distribution of the continuum LINE_4: source. We have obtained high resolution radio LINE_5: maps at 3.5 and 6.3 cm with the Australia LINE_6: Telescope, which show a radio counterpart of the LINE_7: cloud, and demonstrate that the inner radio jet LINE_8: does indeed point exactly to the cloud. The Rosat LINE_9: HRI image shows a 5-sigma source coincident with LINE_10: the cloud and at the same flux level relative to LINE_11: the X-ray nucleus as seen at radio frequencies. LINE_12: Unpublished VLBI data (SHEVE experiment, Meier, LINE_13: Reynolds, private communication) show a nuclear LINE_14: radio source elongated towards the HIC. From all LINE_15: of these data we have precise astrometry relative LINE_16: to an accurate, very high precision VLBI nucleus. QUESTION: 5 SECTION: 1 LINE_1: With a declination of (J2000) -69D 41', the source LINE_2: may be available in the CVZ. QUESTION: 6 SECTION: 1 LINE_1: The UV passband filters we use are in the list LINE_2: of recommended filters by Mark Clampin. We assume LINE_3: that the POLQ throughput will be calibrated. QUESTION: 8 SECTION: 1 LINE_1: QUESTION: 9 SECTION: 1 LINE_1: P2719: PAGB STARS IN ELLIPTICAL AND BULGE DOMINATED LINE_2: NEARBY GALAXIES (Di Serego, PI is F. Bertola). LINE_3: It is not related to this project. LINE_4: P3728:IMAGING THE HOT STELLAR CONTENT OF EARLY LINE_5: --TYPE GALAXIES (Di Serego, P.I. F. Bertola). LINE_6: It is not related to this project. LINE_7: P2498: THE NARROW AND VARIABLE EMISSION LINES LINE_8: IN NGC 4151 ( Fosbury, PI Ulrich). QUESTION: 10 SECTION: 1 LINE_1: PI and all Co-Is have adequate data analysis facilities LINE_2: at their institutes. In particular, the ST-ECF has access LINE_3: to full recalibration facilities and has extensive WFPC LINE_4: image processing experience. FIXED_TARGETS: TARGNUM: 1 NAME_1: PKS2152-69-NEB DESCR_1: E,315,316,907,922,927 POS_1: RA = 21H 57M 7.204S +/- 0.007S, POS_2: DEC = -69D 41' 15.53" +/- 0.02" EQUINOX: 2000 PM_OR_PAR: RV_OR_Z: Z = 0.028 FLUXNUM_1: 1 FLUXVAL_1: F-CONT(3000) = 3.0 +/- 0.6 E-16 FLUXNUM_2: 2 FLUXVAL_2: F-CONT(1600) = 1.3 E-16 COMMENT_1: The extent of the cloud continuum COMMENT_2: source is not known but is less COMMENT_3: than 2" square and probably highly COMMENT_4: structured. The 1600 A continuum COMMENT_5: flux assumed is a factor of 4 below COMMENT_6: the IUE upper limit. COMMENT_7: This is a (marginal) CVZ target. EXPOSURE_LOGSHEET: LINENUM: 1.1 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: WF2 SP_ELEMENT: F300W, POLQ PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1200S S_TO_N: 60 S_TO_N_TIME: 2400S FLUXNUM_1: 1 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 1.2-4.2 AS 1.1 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4X600 SEC EXPOSURES. LINENUM: 1.2 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: WF2 SP_ELEMENT: F300W, POLQ PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1200S S_TO_N: 60 S_TO_N_TIME: 2400S FLUXNUM_1: 1 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 1.2-4.2 AS 1.1; REQ_3: POS TARG 0.9, 0.9 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4X600 SEC EXPOSURES. LINENUM: 2.1 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: WF3 SP_ELEMENT: F300W, POLQ PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1200S S_TO_N: 60 S_TO_N_TIME: 2400S FLUXNUM_1: 1 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 1.2-4.2 AS 1.1 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4X600 SEC EXPOSURES. LINENUM: 2.2 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: WF3 SP_ELEMENT: F300W, POLQ PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1200S S_TO_N: 60 S_TO_N_TIME: 2400S FLUXNUM_1: 1 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 1.2-4.2 AS 1.1; REQ_3: POS TARG 0.9, 0.9 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4X600 SEC EXPOSURES. LINENUM: 3.1 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: WF4 SP_ELEMENT: F300W, POLQ PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1200S S_TO_N: 60 S_TO_N_TIME: 2400S FLUXNUM_1: 1 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 1.2-4.2 AS 1.1 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4X600 SEC EXPOSURES. LINENUM: 3.2 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: WF4 SP_ELEMENT: F300W, POLQ PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1200S S_TO_N: 60 S_TO_N_TIME: 2400S FLUXNUM_1: 1 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 1.2-4.2 AS 1.1; REQ_3: POS TARG 0.9, 0.9 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4X600 SEC EXPOSURES. LINENUM: 4.1 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: POLQN33 SP_ELEMENT: F300W, POLQN33 PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1200S S_TO_N: 60 S_TO_N_TIME: 2400S FLUXNUM_1: 1 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 1.2-4.2 AS 1.1 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4X600 SEC EXPOSURES. LINENUM: 4.2 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: POLQN33 SP_ELEMENT: F300W, POLQN33 PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1200S S_TO_N: 60 S_TO_N_TIME: 2400S FLUXNUM_1: 1 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 1.2-4.2 AS 1.1; REQ_3: POS TARG 0.9, 0.9 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4X600 SEC EXPOSURES. LINENUM: 5.1 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: WF2 SP_ELEMENT: F218W PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1300S S_TO_N: 16 S_TO_N_TIME: 2600S FLUXNUM_1: 2 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 5.2 AS 5.1 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4 EXPOSURES. COMMENT_4: ASSUMES WF2 BEST FOR UV. LINENUM: 5.2 TARGNAME: PKS2152-69-NEB CONFIG: WFPC2 OPMODE: IMAGE APERTURE: WF2 SP_ELEMENT: F218W PARAM_1: CR-SPLIT=0.5, PARAM_2: CR-TOLERANCE=0.0, PARAM_3: SUM=2X2, PARAM_4: ATD-GAIN=7 NUM_EXP: 1 TIME_PER_EXP: 1300S S_TO_N: 16 S_TO_N_TIME: 2600S FLUXNUM_1: 2 PRIORITY: 1 REQ_1: CYCLE 4; REQ_2: SAME ORIENT FOR 5.2 AS 5.1; REQ_3: POS TARG 0.9, 0.9 COMMENT_1: S/N CALCULATED ASSUMING FLUX FALLS COMMENT_2: ON 5 2X2 BINNED PIXELS. IT ALSO COMMENT_3: ASSUMES 4 EXPOSURES. COMMENT_4: ASSUMES WF2 BEST FOR UV. !~~~RPSS~~~,FOSBURY,5345.prop, 7-MAR-1994 05:44