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Produced by the NASA Center for Aerospace Information (CASI) I t (NASA-Td-851U3) 'ILLIPthATULL 11d; ELZAEb':AL N84 -3!234 ALUbDAMCP. S IN Tbtr ABILL C I L altb A t) 16 DBhlVEv FbU4 X-tAY UbS.: LVAIILN . ) (NASA) 33 N UC AU3/tik A01 CSCL OJb UticI dk G'/90 23130 N/SA Technical Memorandum 85103 TEMPERATURE AND ELEMENTAL ABUNDANCES IN THE ABELL CLUSTER A 576 DERIVED FROM X-RAY OBSERVATIONS .t R. Rothenflug L. Vigroux R. F. Mttshotzky S. S. Holt Oct r I ;I ,.T p:•, ^1 VEp t SEPTEMBER 1983 National Aeronautics and Space Administration 4 Goddard Space Fligil Center Gi eenbelt Maryland 20771 lift? <^$^^ U^r ., 2^^--^ ^ --- ^ qtr t . e ^7 C a Submitted to The Astrophysical Journal t 0, J 4a i e TEMPERATURE AND ELEMENTAL. ABUNDANCES IN THE AEELL BLUSTER A 576 DERIVED FROM i X-RAY OBSEPVATIONS . R.Rothenflug, L.Vigroux Service d'Astrophysique 1 t C.E.N. Saclay , 91191 Gif-sur-Yvette Cedex France and R.F.Mushotzky, S.S.Holt Laboratory for High Energy Astrophysics NASA/Goddard Space Flight Center Greenbelt, Maryland 20771 USA Received 1982, February 23 / f 4 Running title; X-Ray Spectrum of A 576 4 p.. 1' t do -0. o. 1 or X X - 2 - ORIGINAL F;' . OF POOR Q 9 i ABSTRACT We report results of Einstein Solid State Spe g trometer obser- vations of the central region of Abell 576 combined with HIM-1 spectra of the total cluster. We detected line emission due to r e Fe, Si and S from a hat (< 2.4 10 7 °K) plasma in the central region. i The temperature of the total cluster spectrum (4+11.4 10 7K) may be in conflict with the central temperature. This difference can be 3D explained either if cooling takes place in the center, or if part {{i of the measured emission is due to individual galaxies. If the 1 X-ray emission comes from the intergalactic gas only, there is some difficulty in producing all the silicon observed in the galaxies of - i A 576. ,. a 4 F Jt 1 I Subject headings: Abundances - Galaxies: clusters of - X-rays: sources X-rays: spectra t S ► V J 3 OF POW( 4j { /f I. INTRODUCTION Recant theosl*o5ti.cal work (Saraxin and Bahcall 1978; Smith, Mushotzky and Serlemitsos - S.M.S.-,3979) has stressed the importance of X-ray spectra in interpreting; the physical condition, in X-ray clusters of galaxies. In addition recent imaging results from the Einstein Observatory (White and Silk 1980 (hereafter refered to as W.S.); Branduardi-Raymont et al.1981) have pointed out the need for high quality X-ray spectra in order to unfold the X-ray spatial results. Furthermore it is only through high quality X-ray spectral measurements that the chemical abundances of the heavy elements can be determined for the intergalactic gas in clusters. The abundance of heavy elements in the intergalactic gas can place strong; constraint on galactic and cluster evolutionnary models. In the classical picture, the heavy elements have been expelled from the galaxy either by a i 5 hot wind driven by supernovae explosion (Larson 1974) or by stripping; of the interstellar gas by the ram pressure due to the motion of the galaxies in the cluster (Gunn, Gott, 1972). At later stages evaporation could be r important in removing gas. However, most of the observations have been done so far on untypical high X-ray luminosity clusters, which generally are • dynamically evolved.On the contrary we wanted to observe a typical X-ray cluster populated with normal galaxies. The cluster A 576 was selected on the basis of its galaxy content and X-ray flux which look like a "typical" Abell cluster. r^ f^ 4 - ORIGINAL r, A 0 OF POOR QUALI VV In this paper we report results of Einstein Solid State Spectrometer (SSS) observations of the central region of Abell 576 combined with HSAC-1 spectra of t4c total cluster. These results indicate, as do the imaging data of W.S. that the X-ray gas in A 576 cannot obey a D = 5/3 polytropic equation of state. We shall, tentatively, interpret this either as evi- dente for a cooling, flow in the core of A 576 similar to that in the Perseus cluster (Fabian, Nulsen, 1977; Mushotzky et al. 1981) or due to the presence of soft X-rays associa.ed with individual galaxies in the center of the cluster. We also present data on the elemental abundances in A 576 and find that Fe, S and Si have roughly half solar abundance, consistent with the Fe results for many other clusters (Mushotzky 1975). Conse- quences of this measurement for galactic evolution are presented in the last section. 11. DATA ANALYSIS AND INSTRUMENT DESCRIPTION i ^ s r The SSS consists of a cryogenically cooled Si(Li) detector at the a focus of the Einstein Observatory X-ray telescope. It has a 3' radius circular beam with roughly uniform response across the field. The detector and telescope combination is sensitive in the 0.5 - 4.5 keV band with N 160 eV FWHM energy resolution approximately independent of energy. A more complete description of the instrumentation may be found in Holt et al. (1979). The SSS observatioi:s of the central region of A 576 were obtained in a ^,, 15,000 second exposure in September 1979 resulting, in .v 4000 source counts. Of this total number, the contribution of the 8th mag K star in the field of view is estimated to be far less than 10% (Vaiana et al. 1981). ORIG INAL PA,,^^`Z y OF P4OR QUALI The SSS spectra have been fit to the model of an isothermal Ras i.: collisional equilibrium. Two models of such a gas have been used, one, that jt is due to Raymond and Smith, R-S, (1977) has been described in detail before (Holt, 1979). The other model referred to as X-R (Rothenflua, Arnaud, 1983) was developed at Saclay, mainly based on the compilation of atomic data listed in Kato (1976). The main difference between these two models lies in the ionization balance. The R-S model is based primarily on .- ionization cross sections of Summers (1974) while the K-R model is based on the cross sections of Lotz (1967) (see appendix and also Schnopper et al., 1982). The net result is that the maximum of equilibrium abundance is shifted to higher temperatures for the R-S model in comparison with the K-12 model. This shift is most noticeable for the least ionized species (e.g. Fe XVII or re XVIII). For helium like and hydrogen like ions the differences are small. The HERO-1 experiment A-2 a instrumentation has been described in detail by Rothschild et al. (1978). Previous HEAO-1 observations of A 576 have been reported by Pravdo et al. (1580) who used a summed rate combina- tion, R15, in their analysis. In this paper we have used the results of ,.. 4 a long; pointing at A 576 which occurred on day 297 of 1978. c t This exposure of 8600 seconds resulted in,- 6500 source counts in the 2 - 20 keV band. The major origin of uncertainty in the data is not due to photon counting; statistics or uncertainty in the internal backfround, but is due; to ,intrinsic fluctuations in the diffuse X-ray background. i a. The A-2-experiment on HFAO-1 was a collaborative effort led by E.Boldt of GSFC and G.Garmire of CIT, W th collaborators at GSFC, CIT, JPL, and UCB. s - g - ORIGINAL PAOM-. ;1- OF POOH QUAi,1V Mo RESULTS . The SSS spectrum was well fit by either the R-S or K-R model with a A reduction in 2 of 1H compared to a simple thermal breamsstrahlung fit (Figure 1). For the addition of A additional parameters, the reduction T2 in is significant at greater than the 90% confidence level. The best f1t temperature is 1.6 keV (:;3) (90% confidence errors) with roughly half solar abundances of Fe, Si and S (see Table 1 and Figure 2). As seen in Table 1, there is no significant difference found for the temperature or the abundance determinations between the R-S and K-R models. The best fit absorption of 1.1 x 1021 at/rm2 is consistent with the G x 10`0 at/cm2 derived from 21 cm data (Neiles, 1975). The best fait emission integral, ne 2V, is 6,6 x 1066 .h 5o cm . rt The HEAO-1 experiment A-2 data with a larger angular resolution of 3 0 x 1.5 0 were fit to a simple thermal model (Figure 3). The best fit . temperature was K= 3.5 +3- 1 : 02, keV (90% confidence).
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