High resolution spectroscopy and BVRI photometry of Fermi J0639+0548 = Nova Mon 2012
ATel #4320; U. Munari (INAF Astr. Obs. Padova), S. Dallaporta, P. Valisa (ANS Collaboration)
on 20 Aug 2012; 21:11 UT
Credential Certification: U. Munari (ulisse.munari@oapd.inaf.it)
Subjects: Optical, Gamma Ray, Nova, Transient
The coincidence between the new gamma-ray transient Fermi J0639+0548,
discovered on June 22 by the Fermi Large Area Telescope (Cheung et al. 2012,
ATel #4224) and Nova Mon 2012 discovered by S. Fujikawa on Aug. 9.805 UT
(and announced on Aug 17 via CBET #3202) when it was emerging from the
conjunction with the Sun, has been recently pointed out by Cheung et al.
(2012, ATel #4310), who also note how this is only the third known case
(after V407 Cyg and Nova Sco 2012) of gamma-ray transient detection from
a nova by Fermi-LAT.
Soon after the announcement of its discovery was posted to the net, we begun
monitoring Nova Mon 2012 with telescopes operated by ANS Collaboration (described
by Munari et al. 2012, BaltA 21, 13). The following table summarize the BVRcIc
photometry collected so far. A BVRcIc comparison sequence was established
around Nova Mon 2012 from APASS BVgri Survey data following the
transformation equations given in Munari (2012, JAVSO tmp 206).
date and UT | V | B-V | V-Rc | V-Ic |
2012 08 16.141 | 10.009 | | | 1.758 |
2012 08 17.143 | 10.025 | 0.104 | 1.603 | 1.723 |
2012 08 19.125 | 9.985 | 0.078 | 1.590 | 1.675 |
2012 08 20.128 | 10.037 | 0.121 | 1.605 | 1.659 |
It is worth noticing that (1) the value of B-V is consistent with a limited reddening,
(2) the 0.05 mag amplitude, day to day fluctuations are larger than the total error budgets of the individual measurements (<0.01 mag), and (3) the current decline rate is very slow, consistent with the >50 days passed since the source was first detected in the gamma-rays.
We have also obtained a high resolution Echelle spectrum of Nova Mon 2012 on
August 20, 03:25 UT, with the Multi-Mode Spectrograph mounted on the 0.6m
telescope of the Schiaparelli Observatory in Varese (Italy), operating in
binned mode at a resolving power of 11,000. The integrated flux [in
erg/(cm**2 sec Ang)] and the FWHM (in km/sec) of the strongest emission
lines are:
line | flux | FWHM |
Hgamma | 3.55e-11 | 2168 |
Hbeta | 5.78e-11 | 2195 |
[OIII] 5007 | 5.89e-11 | 3035 |
NII 5680 | 1.16e-11 | 2605 |
[NII] 5755 | 2.03e-11 | 2500 |
HeI 5876 | 4.06e-11 | 2380 |
[OI] 6300 | 5.24e-12 | 2260 |
Halpha | 9.42e-10 | 2085 |
HeI 6678 | 1.39e-11 | 2200 |
HeI 7065 | 4.77e-11 | 2190 |
[OII] 7325 | 9.29e-11 | 2395 |
OI 7772 | 2.90e-11 | 2150 |
OI 8446 | 1.02e-10 | 2005 |
The emission lines generally show saddle-like profiles, with noticeable
differences among them. The large OI 8446/7772 ratio indicates
pumping by Ly-beta fluorescence. At the 11,000 resolving power of our
spectrum, the interstellar lines appear as unblended, single-component. The
0.49 Ang equivalent width of interstellar NaI 5890 corresponds to a reddening
of E(B-V)=0.30 following the calibration by Munari and Zwitter (1997, A&A
318, 269). The heliocentric velocity of interstellar NaI is +25 km/sec,
consistent with the absorption medium being centered at a distance of about
1 kpc from the Sun.