A somewhat rare occurrence in the local universe is a supernova. A supernova is the end stage of a star, typically when the star gravitationally collapses due to exhausting the matter that it is fusing within it. Stars are quite the balancing act, as the energy released by the fusion of matter within restricts the gravitational attraction of the matter itself. When massive stars run out of matter to fuse, typically at the iron stage, gravity is able to compress the iron in the core into pure neutrons, with a density of that of an atomic nucleus. If this core is massive enough, it can become a black hole. Otherwise, the neutron core is compressed to the limits of neutron degeneracy pressure and can have a temperature of 100,000,000,000 Celsius. The outer shells of the star, no longer supported by fusion in the core, collapse and “bounce” off of the neutron core, causing shockwaves that result in the explosion. A white dwarf will remain.
This supernova was discovered by amateur astronomer Koichi Itagawa on 2023-05-19 17:27:10UTC. It is named SN 2023ixf. The estimated eruption time is 2023-05-18 19:49:36UTC.
Location
The supernova is located in a star-forming region in an outer spiral arm of M101. This galaxy is a target that I recently imaged, and I took some more data on the galaxy to show the location of the supernova. 90 images of 45 second exposure were taken on May 21-22, 2023 from 11:41 to 00:56 UTC-5. Figure 1.1 shows the location of the supernova, and Figure 1.2 shows the subject compared to pre-discovery. It is located at 14 3 38.56 +54 18 42.0 (J2000).
Photometry
Supernovae are extremely powerful and luminescent events. Some of them at peak can outshine their entire host galaxy. With the data I took on this subject, I used the AperturePhotometry script in PixInsight to estimate the flux and brightness. Table 2.1 shows the G-band magnitudes of local stars from GAIA DR2 and the estimated apparent magnitude of SN 2023ixf by calculating the apparent magnitude as
m + 2.5\log_{10}\frac{b}{b_{sn}}where b is the flux of the reference star, bsn is the flux of the supernova, and m is the G-band apparent magnitude of the reference star. The measured flux of the supernova was 2.57289. The average of the magnitude conversions gives the supernova an estimated G-band apparent magnitude of 11.2. The accuracy of this is unknown since I am using a green channel from a OSC camera, and the green filter is likely to not match the Johnson/Cousins filters used by professional telescopes. However, other reports of the magnitude around this time that I have read match my estimate pretty well.
StarId | RA | Dec | Catalog_Gmag | PSF_Flux_1 | Relative mag | |
SN 2023ixf | 210.910658333333 | 54.3116666666667 | 2.57289 | |||
_1609307826153070464 | 211.102293452903 | 54.653578455938 | 10.1705 | 6.200219 | 11.1254645265555 | |
_1609314938618876288 | 210.927451130937 | 54.844140289656 | 10.5602 | 4.301788 | 11.1182694618587 | |
_1609308272828044288 | 210.972673735646 | 54.6384669038205 | 10.8203 | 3.189927 | 11.0536988138402 | |
_1609321638767836288 | 210.432803601206 | 54.7384664523923 | 11.0086 | 3.294395 | 11.2769861278149 | |
_1513187969896570880 | 210.272254268827 | 53.9241118478619 | 11.2303 | 2.413923 | 11.161055484317 | |
_1609322051084697600 | 210.422496787806 | 54.7853797365819 | 11.2585 | 2.673311 | 11.3000706659911 | |
_1609296040762764672 | 210.391997068185 | 54.5950413484867 | 11.3261 | 2.313922 | 11.2109187405554 | |
_1609292256894781696 | 210.551504657823 | 54.5260337811976 | 11.6141 | 1.941964 | 11.3086498892932 | |
_1609223984094652288 | 210.957784613434 | 54.1515141425831 | 11.6509 | 1.718367 | 11.2126367619499 | |
_1609407980493607040 | 211.102190503551 | 54.844492324376 | 11.6603 | 1.741809 | 11.2367482780797 | |
_1609317515599247104 | 210.541207701838 | 54.6664517415881 | 11.6865 | 1.728897 | 11.254869754256 | |
_1609232543966385152 | 211.368446526044 | 54.1254867600814 | 11.8273 | 1.430443 | 11.1899233445035 | |
_1609250441093191808 | 211.090333466939 | 54.3228979372932 | 11.932 | 1.373125 | 11.250222138144 | |
Mean | 11.2076549220892 |
According to NED, M101 is at a distance of 17.4Mly (5.34Mpc) and has an apparent R-band magnitude of 7.76. The absolute magnitude, or the brightness of an object if viewed from a distance of 10 parsecs, is related to the apparent magnitude ma and distance in parsecs d by
m_v = m_a - 2.5\log_{10} \left(\frac{d}{10} \right) ^ 2This gives M101 an absolute magnitude of -20.88 and the supernova an absolute magnitude of -17.43. The supernova, at the time of observation, was about 3.45 magnitudes, or 24 times, dimmer than its host galaxy. With it estimated that M101 is composed of a trillion stars, one exploding star emits as much light as 40 billion stars!
Spectroscopy
Using my ALPY 600 spectroscope and ASI183MM camera, I took 140 minutes of data on this supernova on May 23, 2023, from 00:07 to 02:18 UTC-5. I used a common CFL lamp for calibration, a halogen lamp for flat correction, and the star Alkaid for instrument response correction. Figure 3.1 shows the synthetic spectra used for analysis.
Figure 3.2 shows the calibrated, flat- and response-corrected spectrum. The spectrum shows the Balmer series of hydrogen emission, classifying it as a Type-II supernova. This means that it is the result of the collapse of a massive star. A 17,000K Planck curve is included, giving an approximation to the temperature of the explosion.
Continuum removal and velocity correction reveals the emission lines, as shown in Figure 3.3. The largest spike is H-α at 656.3nm, which is present only in Type-II supernovae. Other elements of the Balmer series are prominent, as well as He-2 at 468nm. A carbon doublet is also present around 580nm. Absorption at the high end of the graph is due to tellurics. The H-β line shows what appears to be a P-Cygni profile, but it is not noticeable in the H-α line. This is due to circumstellar material being affected by the progenitor wind.
Data on the most prominent lines are given in Table 3.1. The mean of the observed velocities is 214km/s, which is pretty close to the accepted value for M101 at 243km/s. Using the FWHM of each emission line gives an average expansion velocity of 615km/s, which is in agreement with professional observations.
Element | Rest | Observed | z | Doppler Velocity | FWHM | Doppler Width |
H-α | 656.3 | 656.9 | 0.000914 | 274075.08 | 1.65 | 376509 |
H-β | 486.1 | 486.5 | 0.000823 | 246692.00 | 2.01 | 619304 |
H-γ | 434 | 434.1 | 0.000230 | 69076.60 | 2.71 | 935772 |
H-δ | 410.2 | 410.6 | 0.000975 | 292337.84 | 0.75 | 273800 |
He II | 468.5 | 468.8 | 0.000640 | 191969.56 | 2.72 | 869705 |
Mean | 0.000717 | 214830 | 1.97 | 615018 |