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首页> 外文期刊>Astronomy and astrophysics >The outer regions of the giant Virgo galaxy M?87 Kinematic separation of stellar halo and intracluster light
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The outer regions of the giant Virgo galaxy M?87 Kinematic separation of stellar halo and intracluster light

机译:巨大的处女座星系M?87的外部区域是恒星晕和群内光的运动学分离

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Aims. We present a spectroscopic study of a sample of 287 planetary nebulas (PNs) around the brightest cluster galaxy (BCG) M?87 in Virgo A, of which 211 are located between 40 kpc and 150 kpc from the galaxy centre. With these data we can distinguish the stellar halo from the co-spatial intracluster light (ICL) and study both components separately. Methods. We obtained PN velocities with a high resolution FLAMES/VLT survey targeting eight fields in a total area of ~0.4 deg2. We identified PNs from their narrow and symmetric redshifted λ5007 ? [OIII] emission line, the presence of the second λ4959 ? [OIII] emission line, and the absence of significant continuum. We implement a robust technique to measure the halo velocity dispersion from the projected phase-space to identify PNs associated with the M?87 halo and ICL. Using photometric magnitudes, we construct PN luminosity functions (PNLFs), which are complete down to m5007 = 28.8. Results. The velocity distribution of the spectroscopically confirmed PNs is bimodal, containing a narrow component centred on the systemic velocity of the BCG and an off-centred broader component, which we identify as halo and ICL, respectively. We find that 243 PNs are part of the velocity distribution of the M?87 halo, while the remaining subsample of 44 PNs are intracluster PNs (ICPNs). Halo and ICPNs have different spatial distributions: the number density of halo PNs follow the galaxy’s surface brightness profile, whereas the ICPNs are characterised by a shallower power-law profile, IICL ∝ Rγ with γ in the range [?0.34, ?0.04 ]. No evidence is found for an asymmetry in the halo and ICPN density distributions when the NW and SE fields are studied separately. A study of the composite PN number density profile confirms the superposition of different PN populations associated with the M?87 halo and the ICL, characterised by different PN specific numbers α. We derive αhalo = 1.06 × 10-8NPN L⊙,bol-1 and αICL = 2.72 × 10-8NPN L⊙,bol-1, respectively. The M?87 halo PNLF has fewer bright PNs and a steeper slope towards faint magnitudes than the ICPNLF, and both are steeper than the standard PNLF for the M?31 bulge. Moreover, the ICPNLF has a dip at ~1?1.5 mag fainter than the bright cut-off, reminiscent of the PNLFs of systems with extended star formation history, such as M?33 or the Magellanic clouds. Conclusions. The BCG halo of M?87 and the Virgo ICL are dynamically distinct components with different density profiles and velocity distributions. Moreover, the different α-parameter values and PNLF shapes of the halo and ICL indicate distinct parent stellar populations, consistent with the existence of a gradient towards bluer colours at large radii. These results reflect the hierarchical build-up of the Virgo cluster.
机译:目的我们对在处女座A最亮的星系星系(BCG)M?87周围的287个行星状星云(PN)进行光谱研究,其中211个位于距银河系中心40 kpc至150 kpc之间。利用这些数据,我们可以将星光晕与同空间簇内光(ICL)区别开来,并分别研究这两个分量。方法。我们通过高分辨率FLAMES / VLT测量获得了PN速度,该FLAMES / VLT测量针对总面积约为0.4 deg2的八个场。我们从窄且对称的红移λ5007?中识别出PN。 [OIII]发射线,第二个λ4959的存在? [OIII]发射谱线,并且没有明显的连续谱。我们采用了一种强大的技术来测量投影相空间中的光晕速度色散,以识别与M?87光晕和ICL相关的PN。使用光度大小,我们构造了PN发光度函数(PNLF),该函数直到m5007 = 28.8为止都是完整的。结果。光谱确认的PNs的速度分布是双峰的,包含一个以BCG的系统速度为中心的窄分量和一个偏心的较宽分量,我们分别将其标识为光晕和ICL。我们发现243个PN是M?87光晕速度分布的一部分,而其余44个PN的子样本是簇内PN(ICPN)。晕和ICPN具有不同的空间分布:晕PN的数量密度遵循星系的表面亮度分布,而ICPN的特征是具有较浅的幂律分布IICL ∝Rγ,其中γ的范围为[?0.34,?0.04]。当分别研究NW和SE场时,没有发现晕圈和ICPN密度分布不​​对称的证据。对复合PN数密度分布图的研究证实了与M?87光环和ICL相关的不同PN种群的叠加,其特征是不同的PN比数α。我们分别得出αhalo= 1.06×10-8NPNL⊙,bol-1和αICL= 2.72×10-8NPNL⊙,bol-1。与ICPNLF相比,M?87晕PNLF的亮PN更少,朝微弱幅度的斜率也比ICPNLF陡,并且都比M?31凸起的标准PNLF陡。此外,ICPNLF比明亮的截止点低约1?1.5 mag,这使人联想起具有延长恒星形成历史的系统(如M?33或麦哲伦星云)的PNLF。结论。 M?87的BCG光晕和处女座ICL是动态不同的组件,具有不同的密度分布和速度分布。此外,晕圈和ICL的不同α参数值和PNLF形状表示不同的母体恒星种群,这与大半径处朝向蓝色的梯度存在有关。这些结果反映了处女座集群的层次结构。

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