Peremennye Zvezdy (Variable Stars) 43, No. 4, 2023 Received 11 May; accepted 23 May. |
Article in PDF |
DOI: 10.24412/2221-0474-2023-43-27-32
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M.V. Lomonosov Moscow State University, Sternberg Astronomical Institute, Universitetskii pr. 13, 119234. Moscow, Russia
Photometric observations of SN2019tua, spanning
350 days of its evolution, show a linear light curve with a rate
of brightness decline slower than for most SNe II-L. The maximum
absolute magnitude of SN2019tua,
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Explosions of high-mass stars (
) with hydrogen
envelopes due to the gravitational collapse of their cores are
classified as type II Supernovae (SNe). Barbon et al. (1979)
proposed to divide SNe II into two major groups: SNe II-P, which
have nearly constant luminosity for a time interval of
days after maximum, and SNe II-L, which are characterized by
linear decline (in magnitudes) after maximum. When more data had
become available, objects with intermediate parameters between SNe
II-P and II-L were also found, and it was supposed that these
classes presented the utmost cases of a continuous distribution
(Anderson et al., 2014).
Explosions of two or more SNe in the same parent galaxy, which are called Supernova siblings, present special interest due to possibilities of exploring some characteristics of the host galaxies and testing distance estimation methods using SNe.
SN2019tua (ATLAS19zjt, Gaia19ezc) in the galaxy UGC11860 was
discovered by ATLAS on 2019-10-31.33 UT at
. The Supernova was offset by 2
3
South, 7
3 East from the center of its host galaxy, and was
located at
, 2000.0 (Srivastav et al., 2019).
Spectra of SN2019tua were obtained on 2019-11-01.38 UT at the
Faulkes Telescope North, the best fit was found to SNe II at early
phases. The expansion velocity was found to be about 17000 km
s from the H
absorption and from the HeI 5876 Å line (Burke at al., 2019).
SN 2019tua is the second SN outburst in UGC 11860: five years earlier, SN ASASSN-14dq was discovered in this galaxy. ASASSN-14dq was a transitional event between the type II-P and type II-L SNe (Singh et al., 2018; Valenti et al., 2016).
The nearly simultaneous outbursts of two SNe are surprising
because UGC11860 is a low-luminosity type Sdm dwarf galaxy, its
luminosity being only
(Singh et al.,
2018). Using the mean values of SN frequency from Li et al.
(2011), we can estimate the SN II rate for this galaxy as
SN in 1300 years. Of course, the real time interval between the
explosions of two SNe is unknown, but still we consider this a
very rare event.
We obtained images of SN2019tua in the band with the 70-cm
telescope in Moscow on 2019-11-21.6 UT. The observations with
MASTER telescopes (Lipunov et al., 2010) were carried out at
Tunka, Amur, SAAO. and OAFA sites. Unfiltered images were obtained
on 5 epochs, from 2019-11-28 to 2019-12-21. Photometric monitoring
at the 60-cm RC600 telescope of the Caucasus Mountain Observatory
of Sternberg Astronomical Institute (Berdnikov et al., 2020), in
the
bands, was performed between 2020-07-03 and 2020-11-09.
The standard image reductions and photometry were performed using
IRAF1. Photometric
measurements of the SN were made relative to local standard stars
using PSF fitting with the IRAF DAOPHOT package. The galaxy
background was subtracted using images of the host galaxy obtained
at the RC600 telescope on 2022-05-30, when the SN had faded. The
magnitudes of the local standard stars were taken from Singh et
al. (2018). The unfiltered MASTER images were calibrated using the
-band magnitudes of local standards. The photometry is
presented in Table 1, the identification of telescopes is given by
the following codes: M70, the 70-cm reflector in Moscow; M40,
40-cm MASTER telescopes; K60, the 60-cm RC600 telescope of the
Caucasus Mountain Observatory.
JD![]() |
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Tel. |
8809.10 | 15.41 | 0.05 | M70 | ||||||
8815.96 | 15.40 | 0.03 | M40 | ||||||
8816.29 | 15.43 | 0.04 | M40 | ||||||
8817.00 | 15.44 | 0.04 | M40 | ||||||
8817.06 | 15.43 | 0.05 | M40 | ||||||
8838.97 | 15.91 | 0.02 | M40 | ||||||
9033.50 | 19.27 | 0.06 | 18.32 | 0.03 | 18.02 | 0.03 | K60 | ||
9047.48 | 20.10 | 0.07 | 19.55 | 0.04 | 18.52 | 0.03 | 18.16 | 0.04 | K60 |
9050.47 | 20.15 | 0.08 | 19.51 | 0.05 | 18.48 | 0.04 | 18.17 | 0.04 | K60 |
9057.44 | 20.25 | 0.07 | 19.55 | 0.07 | 18.52 | 0.04 | 18.16 | 0.05 | K60 |
9058.46 | 20.44 | 0.06 | 19.57 | 0.04 | 18.53 | 0.02 | 18.26 | 0.03 | K60 |
9067.44 | 19.82 | 0.06 | 18.66 | 0.03 | 18.46 | 0.04 | K60 | ||
9079.51 | 20.74 | 0.06 | 19.94 | 0.05 | 18.78 | 0.03 | 18.63 | 0.07 | K60 |
9085.39 | 19.90 | 0.08 | 18.79 | 0.04 | 18.66 | 0.07 | K60 | ||
9103.29 | 20.36 | 0.06 | 19.09 | 0.06 | 19.12 | 0.06 | K60 | ||
9116.24 | 20.88 | 0.05 | 19.44 | 0.03 | 19.32 | 0.07 | K60 | ||
9129.39 | 19.47 | 0.06 | K60 | ||||||
9146.27 | 21.20 | 0.10 | 19.93 | 0.05 | K60 | ||||
9163.31 | 20.27 | 0.04 | K60 |
The light curves of SN2019tua are presented in Fig. 1, we also plotted
the magnitudes in Gaia -band2and the discovery magnitude from ATLAS (Srivastav et al., 2019).
The maximum light was reached on about JD2458812 with
. After maximum, the brightness decline was
nearly linear, with a rate 0.013 magday
in the
band.
Gaia
magnitudes demonstrated nearly the same rate, 0.015
magday
. During the time interval of our continuous
monitoring (JD24589033-34589163), the rate of decline was 0.015
and 0.017 magday
in the
and
bands, respectively.
Thus, the linear phase of photometric evolution continued for
about 350 days.
The absolute -band light curve of SN2019tua is presented in
Fig. 2, it is compared with the light curve of ASASSN-14dq, which
occurred in the same galaxy UGC11860, and with five SNe II-L:
1998S, 2014G, ASASSN-15nx, 2016gsd, 2020mmz (Fassia et al., 2000,
Bose et al., 2016, Bose et al., 2018, Reynolds et al., 2019,
Tsvetkov et al., 2022).
We plotted the magnitudes from Singh et al. (2018) for ASASSN-14dq, and also an upper limit from images obtained at the MASTER Tunka telescope on 2014-07-01.66 UT, 7 days before discovery.
We accept the distance modulus for UGC11860 from
Singh et al. (2018). We consider the extinction in the host galaxy
to be negligible for both SNe, because the interstellar lines of
NaI were not detected in the published spectra (Singh et al.,
2018; Burke et al.. 2019). We also note that both SNe occurred at
similar projected distances from the center of the host galaxy:
1.9 and 1.7 kpc for ASASSN-14dq and 2019tua, respectively. The
projected distance between the sites of the two SNe is 2.4 kpc.
We applied to both SNe only the galactic extinction
according to Schlafly and Finkbeiner (2011). The
distances and extinctions for the SNe from the comparison sample
were adopted from the references above.
The maximum luminosities of SN ASASSN-14dq and SN 2019tua are
similar, with SN2019tua only 03 brighter. The shape of the
light curves is different. ASASSN-14dq shows typical photometric
evolution for a transitional event between types II-P and II-L:
three phases with different rates of decline. The light curve of
SN2019tua exhibits monotonous decline. The comparison with the
light curves of five SNe II-L shows that the decline rate of
SN2019tua is quite slow, at phase
300 days it is brighter
than other SNe from the sample. Only SN2016gsd has similar
luminosity at that epoch, but at maximim it was 1
7 brighter
than SN2019tua. We also note that most SNe II-L and transitional
objects show changes of decline rate, while for SN2019tua it is
quite monotonous. The absolute magnitude
for SN2019tua is very close to the
mean value for SNe II-L according to Richardson et al. (2014).
The comparison of two type II SNe that occurred in the galaxy
UGC11860 reveals that they had quite different luminosity
evolution, although their maximum absolute magnitudes were quite
close to each other. Singh et al. (2018) applied the SCM method to
ASASSN-14dq to estimate the distance for the host galaxy, the
result was close to that derived from the galaxy redshift. We
cannot apply the same method to SN2019tua to verify its
precision because of different nature of the light curve and
insufficient set of observational data. Singh et al. (2018) did
not reveal any peculiarity of the dwarf galaxy UGC11860, we
suppose that the nearly simultaneous outbursts of two SNe were
rare occasional events.
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Fig. 2.
The absolute |
Acknowledgements. This study was performed using the
equipment purchased through the funds of the Development Program
of the Moscow State University. The work was supported by the
Scientific and Educational School of the Moscow State University
"Fundamental and Applied Space Research".
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