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arXiv 0707.2237astro-ph
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Ib/c型SN 2005 bf旋光分光光度计

Spectropolarimetry of the Type Ib/c SN 2005bf

J. R. Maund, J. C. Wheeler, F. Patat, D. Baade, L. Wang, P. Hoflich

摘要:

本文介绍了在MCG+00-27-005中,从3600- 8550 nm对奇特的Ib/c型SN 2005 bf的偏振光谱观测。SN于2005年4月30.9日观测到,即第一个B波段光变曲线极大值后18天,第二个B波段光变曲线极大值前6天。由光谱中的去偏振发射线确定的星际偏振度,在$p_{max}(ISP)=1.6%$和$θ(ISP)=149$ \fdg $7\pm4.0$中很大,但这可能是ISP实际值的上限。在减去ISP之后,在大的波长区域上观察到显著的偏振,指示显著程度的全局不对称性$\gtrsim 10%$。Ca Ⅱ H&K和IR三重态吸收分量的偏振度分别为3.5%和4%,He Ⅰ 5876和Fe Ⅱ吸收分量的偏振度分别为1.3%。在$Q-U$平面上观察到He I 5876线的清晰速度依赖性环结构,这表明偏离了轴对称性,并可能导致SN喷出物的聚集。观测到$\mathrm{Hα}$、$\mathrm{Hβ}$和$\mathrm{Hγ}$的弱高速分量,速度为-15000PDMATHABMV。在H $β$处观察到的低偏振度表明,对于其他巴耳末线($\sim 0.4%$高于背景偏振)观察到的偏振可能是由于分别将$\mathrm{Hα}$和$\mathrm{Hγ}$与偏振Si II和Fe II线混合。我们提出了一个模型,其中的喷流的材料,这是丰富的$\mathrm{^{56}Ni}$,已经穿透了C-O核心,但不是他的地幔。喷流的轴相对于光球的轴是倾斜的。这解释了O I 7774缺乏显著的极化,延迟激发,因此,He I的可观测性,以及He和Ca的不同几何形状。

英文摘要:

We present spectropolarimetric observations of the peculiar Type Ib/c SN 2005bf, in MCG+00-27-005, from 3600-8550Å. The SN was observed on 2005 April 30.9, 18 days after the first B-band light-curve maximum and 6 days before the second B-band light-curve maximum. The degree of the Interstellar Polarization, determined from depolarized emission lines in the spectrum, is found to be large with $p_{max}(ISP)=1.6%$ and $θ(ISP)=149$\fdg$7\pm4.0$, but this may be an upper limit on the real value of the ISP. After ISP subtraction, significant polarization is observed over large wavelength regions, indicating a significant degree of global asymmetry, $\gtrsim 10%$. Polarizations of 3.5% and 4% are observed for absorption components of Ca II H&K and IR triplet, and 1.3% for He I 5876Åand Fe II. On the $Q-U$ plane clear velocity-dependent loop structure is observed for the He I 5876Åline, suggestive of departures from an axial symmetry and possible clumping of the SN ejecta. Weak High Velocity components of $\mathrm{Hα}$, $\mathrm{Hβ}$ and $\mathrm{Hγ}$ are observed, with velocities of -15 000\kms. The low degree of polarization observed at H$β$ suggests that the polarization observed for the other Balmer lines ($\sim 0.4%$ above the background polarization) may rather be due to blending of $\mathrm{Hα}$ and $\mathrm{Hγ}$ with polarized Si II and Fe II lines, respectively. We suggest a model in which a jet of material, that is rich in $\mathrm{^{56}Ni}$, has penetrated the C-O core, but not the He mantle. The jet axis is tilted with respect to the axis of the photosphere. This accounts for the lack of significant polarization of O I 7774Å, the delayed excitation and, hence, observability of He I and, potentially, the varied geometries of He and Ca.

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