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Although spectroscopy is available for which will lead toto thethe determination of early-stage observations are mlsslngmissing several SNe lala around maximum light,light, thethe totaltotal mass of radioactiveradioactive 56CO56Co pro­pro- and an unambiguous classification is we still entirely lack bolometric lumi­lumi- duced. Regularly spaced spectra of a thenthen impossible.impossible. However, therethere are nosities and regular spectral observa­observa- number of objects will clarify whether all about 70 SNe older than 10 years ac­ac- tionstions beyond 150150 days. It is not clear, inin thethe documented differences are real or cessible fromfrom La Silla, whwhichich are can­can- fact,fact, how wide among various objects due only toto thethe uneven spacing of the didates for detection. Although many are thethe differences suggested both by available information. IfIf thisthis variety rep­rep- difficulties arise when one tries toto locatelocate spectra (Branch et al. 1988) and by light resentsresents differences inin thethe envelopes of thethe very faint candidates insideinside thethe pa­pa- curves (Barbon(Barbon 1980) and how theythey cor­cor- thesethese SNe, itit isis not clear how this relatesrelates rentrent galaxy, even a small number of relaterelate with other parameters. This could toto thethe characteristics of thethe progenitor successes would constitute milestones be a problem forfor thethe frequentfrequent use of stars. inin thethe understanding of thethe evolution of such objects as standard candles un­un- Beside thethe regularlyregularly spaced observa­observa- young SNR. lessless such differences can be accounted tionstions of newly discovered SNe, a special The collaboration with CTIO, with for and calibrated in a systematic way. effort will be devoted toto thethe identifica­identifica- whom important coordinated observa­observa- For thethe lessless luminousluminous and rarerrarer Type IbI b titionon and eventual observation of "very tions have been obtained on SN 19871987A,A, SNe, thethe observational status isis at pre­pre- old" supernovae. There exists, in fact, and with thethe Asiago Observatory, forfor thethe sent even worse. Few objects have opti­opti- an observational gap between thethe latestlatest early stages of thethe SNe visible also from cal light curves, and bolometric informa­informa- stages of SNe, which can be placed at thethe northern hemisphere, should also tiontion isis completely lacking.lacking. Even thethe early about 2 years after thethe lightlight maximum, ensure both a better temporal and spec­spec- spectral evolution isis poorly known (be­(be- and the youngest SNRs, whose ages tral coverage. cause of sparse observations). Because are of the order of a few centuries. The the conditions in the envelope have not optical detection of SN 195701957 D inin MM8383 been clarified, since neither a spectros­spectros- (TurattoFuratto et al., 1989; Long et al., 1989) copic temperature nor a thermal equilib­equilib- and of SN 1885A inin M31M 31 (Fesen et al., References rium calculation have been derived, the 1989) indicatesindicates that itit isis possible to get Barbon, R.: 1980, in SNt,SNI, Proceedings of the actual mass of oxygen has not been precious information on the interrnedi­intermedi- Texas Workshop on Type Il supernovae, determined to within a factor of 10, pre­pre- ate agageses even with the presently avail­avail- ed. J.J.C.C. Wheeler (University of Texas, Au­Au- venting an accurate determination of the able instrurnentation.instrumentation. In particular, the stin), p. 16. mass range of possible progenitors and spectrum of the 30-year-old SN 195701957 D Barbon, R., Cappellaro, E., Turatto, M.: 1989, their contribution to the chemical evolu­evolu- inin M83 shows broad [0111][OIII] 4959, 5007 Astron. Astrophys. Suppt.Suppl. 81, 421. tion of galaxies. lines with asymmetric profiles and a ve­ve- Branch, D., Drucker, W., Jeffery, D.: 1988, Astron. J. 330, L 117.11 7. The heterogeneous class of Type 11II locity of the maximum emission of ap­ap- Fesen, R.A., Hamilton, A.J.S., Saken, J.J.M.:M.: SNe represent another interesting field proximately -650 km/s relative to the 1989, Astrophys.ASlfOphys. J.341,J. 341, L55. of investigation. In particular, we will try rest velocity. This could be due to the Turatto, M., Cappellaro, E., Danziger, I.J.: to understand if different shapes exist presence of dust filling the line-forming 1989, The Messenger 56, 36. also in the bolometric light curves and to region analogous to the situation found Long, K.S., Blair, W.W.P.,P., Krzeminski, W.: determine their total energy budget, in SN 19871987A.A. For this SN, unfortunately, 1989, Astrophys. J. 340, L25. PROFILE OF A KEY PROGRAMME Optical Follow-up Identifications of Hard X-Ray1X-Rayl Soft y-Ray Sources Discovered by the "SIGMA" Telescope G. F,F. BIGNAMI, P.A. CARAVEO, S. MEREGHETTI, lstitutoIstituto Fisica Cosmica, Milano, Italy J. PAUL, A. GOLDWURM, L. VIGROUX, Service d'Astrophysique, CEA Saclay, France P. MANDROU, G. VEDRENNE, J. P. ROQUES, CERS, Toulouse, France The aim of this programme is to The SIGMA telescope (constructed by 11005- 5-10 1o6 6 sec. pointed observations of search for the optical counterparts of two French groups at CEA/SaclayCENSaclay and the 3-axis stabilized telescope. hard X-raylsoftX-ray/soft y-ray sources (including CESR Toulouse) aboard the Soviet After the mandatory outgassing y-ray bursts and transient events) dis-dis­ GRANAT satellite represents the first period of the various SIGMA subsys-subsys­ covered by the SIGMA telescope (suc-(suc­ breakthrough in one of the last unex-unex­ tems, more than two months of in-flight cessfully launched on December 1, plored wavelength regions in as-as­ operations were required both to com-com­ 1989), also exploiting the soft X-ray data tronomy. Launched on December 1, plete the telescope adjustment (a quite of the all sky survey to be performed 1989, it consists of a gamma camera/ difficult task, taking into account the 131 by the ROSAT satellite (launched(Iaunched on coded mask telescope system (see photomultiplier tubes of the gamma May 31, 1990). Fig. I)1) separated by 2.5 m, with imaging camera, the on-board calibration sour-sour­ It will be the first time that coordina-coordina­ capability yielding a source localization ces and the active shielding device), and tion between on-going high-energy accuracy of 2' within a field of view of to evaluate the background along the space missions, such as SIGMA and 4034c; 3 x 40 4c; 7 and a sensitivity inin thethe orbit. This is now stabilized on a rather ROSAT, and ground-based telescopes millicrabmilliCrab region. The energy range goes constant value of 440 counts/sec, which isis implementedimplemented on a programmed long-long­ fromfrom 35 keV toto 1.3 MeV, and operations, compares favourably with thethe one com-com­ termterm basis. planned for twotwo years, will be based on puted on thethe ground of 320 counts/sec, 16 inging aa rapidrapid coordinationcoordination withwith ground·ground- basedbased oplicaloptical observations.observations. ItIt isis worthworth nolingnoting thatthat tMthe rectangutarrectangular telescopetelescope fleldfield ofof viewview fealuresfeatures aa centralcentral area,area, inin whichwhich thethe telescopetelescope isis atat itsits maximum,maximum, surroundedsurrounded byby aa widewide fieldfield ofof decreas­decreas- inging sensitivitysensitivity (the(the half·sensitivityhalf-sensitivity boundaryboundary isis aa 1096x1O? 6 x 119411 ? 4 rectangle)rectangle) withinwithin whichwhich sourcessources cancan stillstill bebe posi­posi- tionedtioned withinwithin aa fewfew arcminutes.arcminutes. InInparallel parallelto tothe the SIGMASlGMA higherhigherenergy energy observations,observations, thethe well~knownwell-known ROSATROSAT missionmission willwill workwork inin thethe softsoft (.1-2(.I -2 keV)keV) X-rayX-ray domain,domain, performingperformingfirst first aasky sky sur­sur- veyvey andand thenthen aa sequeneesequence ofof pointedpointed observations.observations. TheTheproposers proposersof of thisthis ESOESO KeyKey ProgrammeProgramme havehave organizedorganized aa eol­col- laborationlaborationbetween betweenthe the twotwo missionsmissionsfor for exploilingexploiting thethe ROSATROSAT surveysurvey daladata onon thethe basisbasis ofof thethe SIGMASlGMA results.results. ThisThis shouldshould resultresult inin anan improvementimprovement ofof bothboth sourcesource positioningpositioning andand knowledgeknowledge ofof spectralspectral Shape,shape, renderingrendering muehmuch moremore intereslinginteresting andand meaningrulmeaningful thethe searchsearch FiglX8rlgure I;I: The1neSIGMA SIUIVIHcoded coaeamask. maSK. AA patternpattern ofor 4949)( x 53SY absorbingaosoro~ngelementselements (1.5 (7.3an cm tungsten)rungsrenl forfor thethe opticaJoptical counterpart.counterpart.Based Basedon on thethe isis arrangedarranged inin aa URAURA (Uniformly(Uniformly RedundantRedundant Amry),Array), eacheach elementelementis is 9.49.4x x 9.49.4 mm.mm. proposer'sproposer's experieneeexperiencein in opticaloptical studiesstudies ofof ylX-rayyiX-ray sources,sources, thethe additionaddition ofof lhethe ROSATROSAT datadata willwill bebe erucialcrucial 10to thethe successsuccess ofof !histhis profectproject especiallyespecially farfor thethe consideringconsideringthe the eurrentcurrent highhigh levellevel ofof s0­so- themthem havehave aJreadyalready beenbeen observed.observed. searchsearch farfor anan opticaloptical idefltiflcationidentification ofof larlar activity.activity. AtAt thethe endend
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