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Ohshima, Tomohito; Kato, Taichi; Pavlenko, Elena; Akazawa, Hidehiko; Imamura, Kazuyoshi; Tanabe, Kenji; de Miguel, Enrique; Stein, William; Itoh, Hiroshi; Hambsch, Franz-Josef; Dubovsky, Pavol A; Kudzej, Igor; Krajci, Thomas; Baklanov, Alex; Samsonov, Denis; Antonyuk, Oksana I; Malanushenko, Viktor; Andreev, Maksim V; Noguchi, Ryo; Ogura, Kazuyuki; Nomoto, Takashi; Ono, Rikako; Nakagawa, Shin’ichi; Taniuchi, Keisuke; Aoki, Tomoya; Kawabata, Miho; Kimura, Hitoshi; Masumoto, Kazunari; Kobayashi, Hiroshi; Matsumoto, Katsura; Shiokawa, Kazuhiko; Shugarov, Sergey Yu; Katysheva, Natalia; Voloshina, Irina; Zemko, Polina; Kasai, Kiyoshi; Ruiz, Javier; Maehara, Hiroyuki; Virnina, Natalia; Virtanen, Jani; Miller, Ian; Boitnott, Boyd; Littlefield, Colin; James, Nick; Tordai, Tamas; Robert, Fidrich; Padovan, Stefano; Miyashita, Atsushi
Publications of the Astronomical Society of Japan, 08/2014, Letnik: 66, Številka: 4Journal Article
We carried out photometric observations of the SU UMa-type dwarf nova ER UMa during 2011 and 2012, which showed the existence of persistent negative superhumps even during the superoutburst. We performed a two-dimensional period analysis of its light curves by using a method called “least absolute shrinkage and selection operator” (Lasso) and the “phase dispersion minimization” (PDM) analysis, and found that the period of negative superhumps systematically changed between a superoutburst and the next superoutburst. The trend of the period change can be interpreted as a reflection of the change of the disk radius. This change is in agreement with the one predicted by the thermal tidal instability model. The normal outburst during a supercycle showed a general trend that the rising rate to its maximum becomes slower as the next superoutburst is approaching. The change can be interpreted as the consequence of the increased gas-stream flow into the inner region of the disk as a result of the tilted disk. Some of superoutbursts were found to be triggered by a precursor normal outburst when the positive superhump appeared to develop. The positive and negative superhumps coexisted during the superoutburst. Positive superhumps were prominent only for four or five days after the supermaximum, while the signal of negative superhumps became stronger after the middle phase of the superoutburst plateau. A simple combination of the positive and negative superhumps was found to be insufficient for reproduction of the complex profile variation. We were able to detect the developing phase of positive superhumps (stage A superhumps) for the first time in ER UMa-type dwarf novae. Using the period of stage A superhumps, we obtained a mass ratio of 0.100(15), which indicates that ER UMa is on the ordinary evolutional track of cataclysmic variable stars.
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