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Peremennye Zvezdy (Variable Stars) 44, No. 12, 2024
Received 6 December; accepted 12
December.
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Article in PDF |
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DOI: 10.24412/2221-0474-2024-44-139-147
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- M.V.Lomonosov Moscow State University, Sternberg
Astronomical Institute, Universitetskii pr.13, 119234 Moscow,
Russia
- National Research Center "Kurchatov Institute",
123182 Moscow, Russia
- Lebedev Physical Institute, Russian
Academy of Sciences, 119333 Moscow, Russia
Type II Supernovae are the result of explosions of massive stars
(
) that retained their hydrogen envelopes (e.g.
Smartt et al. 2009). Among these objects, the most frequent ones
are type II-P SNe, which have nearly constant brightness for a
time interval of
days after maximum (Anderson et al.
2014, Smith et al. 2011). The length of the plateau phase and
luminosity at the plateau exhibit significant diversity, which is
related to the physical parameters of the exploding stars (e.g.
Litvinova and Nadezhin 1985). It is important to expand the sample
of well-studied type II SNe also because SNe II have been
established as useful independent distance indicators (Hamuy &
Pinto 2002).
We present photometry of two type II-P SNe: SN 2012ch and SN
2012fs, for which very few data have been reported, although they
were quite bright at maximum.
SN2012ch was discovered in unfiltered Catalina Sky Survey (CSS)
images obtained on May 17.38 UT. The position of the transient was
(J2000); the offset from the center of the host galaxy was
West,
South, and its brightness, 16
4
(Drake et al. 2012). A spectrum of the object was obtained on May
18 with the F.L. Whipple Observatory's 1.5-m telescope, it showed
that the object was a type II-P supernova before maximum light. A
good fit was found to the spectra of SN II-P 1999em at 4 days
before maximum, and the velocity of H
absorption was
measured as 14200 km s
(Marion 2012). The host galaxy is
WISEA J150602.64+412535.3 at
, according to the
NASA/IPAC Extragalactic Database (NED)1.
SN2012fs was discovered by the Italian Supernovae Search Project
(ISSP) at brightness about 16
5 on two unfiltered CCD images,
taken with the 0.28-m telescope of the Col Druscié Observatory
on Oct. 7.960 UT. The new object was located at
(J2000), which
is 6
West and 1
North of the nucleus of the galaxy
IC35 (Dimai 2012).
An optical spectrum of SN2012fs, obtained on Oct. 9 with the New
Technology Telescope, showed that SN2012fs was a type II-P
supernova, the best fit was to the spectrum of SN2004et within a
few days from explosion (Inserra et al. 2012).
Two spectra of SN2012fs were presented by Lin et al. (2024),
they appear typical of SNe II-P; the explosion date was estimated
as JD2456199 (Sept. 29).
Photometric CCD observations of SNe 2012ch and 2012fs
in the
bands
were
performed with the 60-cm telescope of the Crimean Astronomical
Station of Sternberg Astronomical Institute (SAI CAS).
Images of SN2012fs were also obtained at the
70-cm telescope in Moscow, SN2012ch was
observed on one epoch at the 50-cm telescope of SAI CAS.
The unfiltered observations with MASTER telescopes (Lipunov et
al., 2010) were carried out at Tunka, Amur, and Kislovodsk sites.
The standard image reductions and photometry were made using
IRAF2. Photometric
measurements of the SNe 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 galaxies
obtained at the SAI CAS 60-cm telescope two years after discovery
of the SNe.
The images of SNe 2012ch and 2012fs and local standard stars are
presented in Figs. 1, 2. The stars for SN2012ch were calibrated
using APASS3 and
PanSTARRS4databases, the
magnitides were converted to the
Johnson-Cousins
magnitudes using relations from Jester et
al. (2005) and Kostov & Bonev (2018).
The comparison stars for SN2012fs were calibrated using
observations of Landolt standards. The magnitudes of local
standard stars are reported in Tables 1, 2. The errors are
presented in parentheses in both tables.
Table 1.
Magnitudes of local standard stars for SN2012ch
| Star |
 |
 |
 |
 |
| 1 |
15.40 (0.02) |
14.77 (0.01) |
14.40 (0.01) |
14.06 (0.01) |
| 2 |
15.94 (0.02) |
15.31 (0.02) |
14.97 (0.02) |
14.62 (0.02) |
| 3 |
17.55 (0.04) |
16.35 (0.03) |
15.63 (0.02) |
15.07 (0.02) |
| 4 |
16.53 (0.02) |
15.22 (0.02) |
14.40 (0.03) |
13.79 (0.02) |
| 5 |
17.99 (0.04) |
16.98 (0.03) |
16.38 (0.03) |
15.86 (0.03) |
Table 2.
Magnitudes of local standard stars for SN2012fs
| Star |
 |
 |
 |
 |
| 1 |
14.51 (0.04) |
13.75 (0.01) |
13.31 (0.01) |
12.93 (0.01) |
| 2 |
16.11 (0.04) |
15.39 (0.02) |
14.95 (0.02) |
14.56 (0.01) |
| 3 |
17.76 (0.04) |
16.73 (0.02) |
16.13 (0.01) |
15.64 (0.04) |
| 4 |
17.61 (0.04) |
16.75 (0.01) |
16.31 (0.02) |
15.81 (0.05) |
Table 3.
photometry of SN2012ch
JD 2456000 |
 |
 |
 |
 |
Tel. |
| 071.17 |
|
|
15.80 (0.05) |
|
M40 |
| 076.27 |
|
|
15.73 (0.06) |
|
M40 |
| 101.13 |
|
|
15.85 (0.05) |
|
M40 |
| 154.36 |
|
16.63 (0.04) |
16.01 (0.03) |
|
C60 |
| 156.29 |
|
16.56 (0.04) |
16.04 (0.04) |
|
C50 |
| 166.32 |
18.20 (0.10) |
16.90 (0.03) |
16.21 (0.03) |
15.70 (0.07) |
C60 |
| 167.39 |
|
16.97 (0.03) |
16.24 (0.03) |
15.80 (0.08) |
C60 |
| 170.25 |
18.40 (0.10) |
16.97 (0.03) |
16.30 (0.03) |
15.87 (0.06) |
C60 |
| 171.33 |
|
17.06 (0.06) |
16.33 (0.03) |
15.93 (0.10) |
C60 |
| 174.34 |
|
17.14 (0.03) |
16.47 (0.03) |
|
C60 |
| 176.33 |
18.62 (0.17) |
17.31 (0.04) |
16.54 (0.03) |
16.04 (0.07) |
C60 |
| 177.36 |
|
17.32 (0.04) |
16.60 (0.03) |
16.09 (0.10) |
C60 |
Table 4.
photometry of SN2012fs
JD 2456000 |
 |
 |
 |
 |
Tel. |
| 206.09 |
|
|
17.48 (0.08) |
|
M40 |
| 216.16 |
|
|
17.49 (0.06) |
|
M40 |
| 217.26 |
|
|
17.55 (0.04) |
|
M40 |
| 236.32 |
19.10 (0.10) |
18.05 (0.04) |
17.55 (0.04) |
17.27 (0.15) |
C60 |
| 237.32 |
19.02 (0.18) |
18.08 (0.05) |
17.60 (0.06) |
|
C60 |
| 240.30 |
19.15 (0.16) |
18.05 (0.04) |
17.61 (0.05) |
17.37 (0.26) |
C60 |
| 241.31 |
19.14 (0.13) |
18.06 (0.03) |
17.62 (0.03) |
17.32 (0.20) |
C60 |
| 243.32 |
19.18 (0.14) |
18.09 (0.04) |
17.60 (0.04) |
|
C60 |
| 244.31 |
|
18.10 (0.04) |
17.60 (0.04) |
17.26 (0.15) |
C60 |
| 245.27 |
|
18.05 (0.06) |
17.59 (0.04) |
|
C60 |
| 249.32 |
19.42 (0.08) |
18.15 (0.06) |
17.62 (0.04) |
17.40 (0.11) |
C60 |
| 250.32 |
19.25 (0.13) |
18.06 (0.04) |
17.58 (0.04) |
17.22 (0.10) |
C60 |
| 252.27 |
19.27 (0.13) |
18.17 (0.05) |
17.66 (0.04) |
17.28 (0.10) |
C60 |
| 254.23 |
19.28 (0.18) |
18.27 (0.06) |
17.63 (0.05) |
17.16 (0.11) |
C60 |
| 281.24 |
|
|
17.40 (0.20) |
|
M70 |
The magnitude estimates of the SNe on unfiltered MASTER images
were made using the
-band magnitudes of local standards.
The photometry is presented in Tables 3, 4, the identification of
telescopes is given by codes: M70 is the 70-cm reflector in
Moscow; M40 are the 40-cm MASTER telescopes; C60 is the 60-cm
telescope of the SAI CAS; C50 is the 50-cm telescope of the SAI
CAS.
 |
Fig. 1.
SN 2012ch and local standard stars. |
 |
Fig. 2.
SN 2012fs and local standard stars. |
The light curves for SNe 2012ch and 2012fs are presented in Figs.
3, 4, they appear typical of SNe II-P. For SN2012ch, the
discovery magnitudes and comparison to our early data allow us to
conclude that the end of brightness increase and start of the
plateau phase occurred at about JD2456067. The description of
the classification spectrum by Marion et al. (2012) and comparison
to the data for SN1999em (Elmhamidi et al. 2003, Leonard et al.
2002) permit us to estimate that the explosion occurred in the
time interval JD2456054-2456058, assuming that the rise of
luminosity was similar for SNe 2012ch and 1999em.
The rise time
10 days is within the range of this quantity
for SNe II-P according to Gall et al. (2015). The data from
continuous monitoring with the C60 telescope shows that, in this
time interval, SN2012ch exhibited a fast brightness decline
after the plateau. We estimate that the end of the plateau
occurred at about JD2456150, and the length of the plateau was
93 days, which is a typical value for SNe II-P.
 |
Fig. 3.
The light curves of SN2012ch. Dots are
observations with the C60 and C50 telescopes; triangles are data
from the MASTER telescopes; circles are magnitude estimates at the
discovery. |
 |
Fig. 4.
The light curves of SN2012fs. Dots are
observations with the C60 and M70 telescopes; triangles are data
from the MASTER telescopes; circles are the discovery magnitude
and estimates by amateurs, reported in CBET No. 3278. |
The data for SN2012fs indicate that all our observations were
obtained at the plateau phase. The discovery magnitude and other
estimates by amateurs show very large scatter, up to 2
. We
suppose that this is the result of difficulty of measuring the SN
near the nucleus of the galaxy, in the region of high background
surface brightness. The explosion epoch can be estimated only
using the data on SN spectra. The results of Inserra et al. (2012)
suggests the explosion date about JD2456200 (Sept. 30), while
Lin et al. (2024) determined that the explosion occurred on
JD2456199 (Sept. 29). Both estimates are in a good agreement,
and we accept JD2456199.5 as an explosion epoch. SN2012fs was
discovered on Oct. 7.96 (JD2456208.46), but out first images
were obtained 2 days earlier, on JD2456206.09, and at that time,
the SN has already reached the plateau. The rise time from these
data is about 6
5, which is also within the range of this
quantity for SNe II-P according to Gall et al. (2015).
Unfortunately, we have no data after the phase
80 days and
cannot determine the length of the plateau.
The color curves for SNe 2012ch and 2012fs are presented in
Fig. 6, they are compared to those for type II-P SNe 1999em,
2004et, 2012aw, and 2017eaw (Elmhamidi et al. 2003; Maguire et al.
2010; Bose et al. 2013; Tsvetkov et al. 2018; Buta & Keel 2019).
 |
Fig. 5.
The color curves of SNe 2012ch and 2012fs,
and their comparison to those for four SNe II-P. |
The color curves for the SNe from the comparison sample were
corrected for extinction, the values were taken from the papers
cited above. All four color curves show similar behavior, with
constant reddening during the displayed time interval. The
comparison shows that the colors of SN2012fs clearly demonstrate
a significant color excess, while it is negligible for SN2012ch.
We estimate the color excess for SN2012fs as
, while the Galactic extinction for the
host galaxy is
from the NED. We conclude that
small extinction in the host galaxy,
, is
also present. For SN2012ch, the Galactic extinction is
(NED), and the extinction in the host galaxy is
negligible.
The distances to the host galaxies of SNe 2012ch and 2012fs were
calculated from their redshifts, corrected for the motion relative
to the cosmic microwave background (NED), using
km
s
Mpc
. The resulting distance moduli are
for SN2012ch and
for SN2012fs. Using the distances
and extinction derived above, we obtain the absolute magnitudes of
the SNe at the plateau stage:
for SN2012ch,
for SN2012fs. The mean maximum absolute magnitude
in the
band for SNe II, according to Anderson et al. (2014),
is
. The color curves presented in
Fig. 6 show that the mean color index
at the start of the
plateau stage for SNe II-P is about
, so the mean maximum
magnitude in the
band is
. We
conclude that the maximum luminosity of the SNe 2012ch and 2012fs
is very close to the mean value for this class of objects.
Our study of the two type II-P SNe, 2012ch and 2012fs, shows that
these objects present quite typical photometric behavior, although
our data are quite sparse and do not cover all important stages of
their evolution.
The data for SN2012ch allows us to determine such important
parameters as the length of the plateau and luminosity on the
plateau. We attempted modelling the light curves with the STELLA
code that incorporates implicit hydrodynamics coupled to a
time-dependent multi-group non-equilibrium radiative transfer
(Blinnikov et al. 1998, 2000, 2006; Baklanov et al. 2005).
The explosion is initiated by energy release at the center of the
pre-supernova. A neutron star with mass 1.55
forms in
the center. We varied main parameters of the model: mass
and radius
of the pre-supernova, explosion
energy
, and mass of synthesized
Ni
; we calculated a grid of models searching for better fit to
the observed light curves. The light curves and photospheric
velocity for the optimal model are presented in Fig. 6. The
parameters of this model are:
,
,
,
erg. The single velocity
estimate for SN2012ch is based on blueshift of H
absorption (Marion 2012). Dessart and Hillier (2005) showed that,
at that phase, the photospheric velocity was about 1.5 times lower
than the H
velocity, so the agreement between our model
and observations is satisfactory. The derived model parameters are
quite typical of type II-P supernovae.
 |
Fig. 6.
The light curves and photospheric
velocity of the optimal model (curves) for SN2012ch compared to
observations (dots). |
Acknowledgments. The work of D. Tsvetkov on data reduction
and analysis and work of P. Baklanov on modelling supernova light
curves with the STELLA code were supported by RSF grant No.
24-12-00141.
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