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arXiv 2102.04104astro-ph.SR
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ASASSN-18 aan:一颗轨道周期为3.6小时的旋转SU UMa型激变变星和一颗晚G型副星

ASASSN-18aan: An Eclipsing SU UMa-type Cataclysmic Variable with a 3.6-hour Orbital Period and a Late G-type Secondary Star

Yasuyuki Wakamatsu, John R. Thorstensen, Naoto Kojiguchi, Keisuke Isogai, Mariko Kimura, Ryuhei Ohnishi, Taichi Kato, Hiroshi Itoh, Yuki Sugiura, Sho Sumiya, Ha… 展开作者

Yasuyuki Wakamatsu, John R. Thorstensen, Naoto Kojiguchi, Keisuke Isogai, Mariko Kimura, Ryuhei Ohnishi, Taichi Kato, Hiroshi Itoh, Yuki Sugiura, Sho Sumiya, Hanami Matsumoto, Daiki Ito, Kengo Nikai, Hiroshi Akitaya, Chihiro Ishioka, Kohei Oide, Takahiro Kanai, Yoshinori Uzawa, Yumiko Oasa, Tamás Tordai, Tonny Vanmunster, Sergey Yu. Shugarov, Masayuki Yamanaka, Mahito Sasada, Kengo Takagi, Yuki Nishinaka, Yuina Yamazaki, Ikki Otsubo, Tatsuya Nakaoka, Katsuhiro L. Murata, Ryou Ohsawa, Masahiro Morita, Makoto Ichiki, Sjoerd Dufoer, Masanori Mizutani, Takashi Horiuchi, Miyako Tozuka, Masaki Takayama, Tomohito Ohshima, Tomoki Saito, Pavol A. Dubovsky, Geoff Stone, Ian Miller, Daisaku Nogami

摘要:

本文报道了食SU UMa型矮新星ASASSN-18 aan的光度和光谱观测结果。我们观测到2018年的超级爆发,亮度为2.3等,发现轨道周期($P_{\rm orb}$)为0.149454(3)d,或3.59 hr。这是周期间隔的长度,确定ASASSN-18 aan是少数长$P_{\rm orb}$ SU UMa型矮新星之一。估算的质量比($q=M_2/M_1 = 0.278(1)$)与3:1共振的潮汐不稳定上限几乎相同。从日食观测中我们发现,在超爆发开始时的吸积盘可能达到3:1的共振半径,说明ASASSN-18 aan的超爆发是由潮汐不稳定性引起的。考虑到长$P_{\rm orb}$ WZ Sge型矮新星的情况,我们认为在潮汐截断半径处的潮汐耗散足以在相对高的$q$系统(如SU UMa型矮新星)中诱导类SU UMa行为,但这在低$q$系统(如WZ Sge型矮新星)中不再有效。该系统的不寻常的性质延伸到第二颗恒星,我们发现它的光谱类型为G9,远早于轨道周期的典型值,第二颗恒星的质量$M_2$约为0.18 M $_{\odot}$,小于轨道周期和第二颗恒星光谱类型的预期值。我们还看到了在次级光谱中钠丰度增加的迹象。在少量其他CV和相关对象中可以看到异常热的二次曲线。这些系统显然经历了显着的核演化开始之前的质量转移。在ASASSN-18 aan的情况下,这显然导致了比通常在系统的$P_{\rm orb}$中发现的质量比更低,这可能是在这个相对较长的时期内发生超级爆发的原因。

英文摘要:

We report photometric and spectroscopic observations of the eclipsing SU UMa-type dwarf nova ASASSN-18aan. We observed the 2018 superoutburst with 2.3 mag brightening and found the orbital period ($P_{\rm orb}$) to be 0.149454(3) d, or 3.59 hr. This is longward of the period gap, establishing ASASSN-18aan as one of a small number of long-$P_{\rm orb}$ SU UMa-type dwarf novae. The estimated mass ratio, ($q=M_2/M_1 = 0.278(1)$), is almost identical to the upper limit of tidal instability by the 3:1 resonance. From eclipses, we found that the accretion disk at the onset of the superoutburst may reach the 3:1 resonance radius, suggesting that the superoutburst of ASASSN-18aan results from the tidal instability. Considering the case of long-$P_{\rm orb}$ WZ Sge-type dwarf novae, we suggest that the tidal dissipation at the tidal truncation radius is enough to induce SU UMa-like behavior in relatively high-$q$ systems such as SU UMa-type dwarf novae, but that this is no longer effective in low-$q$ systems such as WZ Sge-type dwarf novae. The unusual nature of the system extends to the secondary star, for which we find a spectral type of G9, much earlier than typical for the orbital period, and a secondary mass $M_2$ of around 0.18 M$_{\odot}$, smaller than expected for the orbital period and the secondary's spectral type. We also see indications of enhanced sodium abundance in the secondary's spectrum. Anomalously hot secondaries are seen in a modest number of other CVs and related objects. These systems evidently underwent significant nuclear evolution before the onset of mass transfer. In the case of ASASSN-18aan, this apparently resulted in a mass ratio lower than typically found at the system's $P_{\rm orb}$, which may account for the occurrence of a superoutburst at this relatively long period.

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