2016AJ....152..102B


Query : 2016AJ....152..102B

2016AJ....152..102B - Astron. J., 152, 102-102 (2016/October-0)

Interpreting flux from broadband photometry.

BROWN P.J., BREEVELD A., ROMING P.W.A. and SIEGEL M.

Abstract (from CDS):

We discuss the transformation of observed photometry into flux for the creation of spectral energy distributions (SED) and the computation of bolometric luminosities. We do this in the context of supernova studies, particularly as observed with the Swift spacecraft, but the concepts and techniques should be applicable to many other types of sources and wavelength regimes. Traditional methods of converting observed magnitudes to flux densities are not very accurate when applied to UV photometry. Common methods for extinction and the integration of pseudo-bolometric fluxes can also lead to inaccurate results. The sources of inaccuracy, though, also apply to other wavelengths. Because of the complicated nature of translating broadband photometry into monochromatic flux densities, comparison between observed photometry and a spectroscopic model is best done by forward modeling the spectrum into the count rates or magnitudes of the observations. We recommend that integrated flux measurements be made using a spectrum or SED which is consistent with the multi-band photometry rather than converting individual photometric measurements to flux densities, linearly interpolating between the points, and integrating. We also highlight some specific areas where the UV flux can be mischaracterized.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

Journal keyword(s): instrumentation: photometers - methods: data analysis - methods: observational - standards - supernovae: general - techniques: photometric - techniques: photometric

VizieR on-line data: <Available at CDS (J/AJ/152/102): table1.dat>

Simbad objects: 24

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Number of rows : 24
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* S And No* 00 42 43.12368 +41 16 03.2124           ~ 190 2
2 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
3 SN 2007ke SN* 02 54 23.90 +41 34 16.3     18.5     SNIb 41 1
4 SN 2007Y SN* 03 02 35.92 -22 53 50.1     17.5     SNIb 135 1
5 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
6 SN 2012Z SN* 03 22 05.39641 -15 23 14.9390           SNIax 142 1
7 SN 1992A SN* 03 36 27.41 -34 57 31.4   12.56 12.50     SNIa 409 1
8 SN 1999em SN* 04 41 27.04 -02 51 45.2   13.79 13.7     SNIIP 727 1
9 SN 2006jc SN* 09 17 20.78 +41 54 32.7     13.8     SNIbn 380 1
10 SN 2010jl SN* 09 42 53.33 +09 29 41.8           SNIIn 350 1
11 SN 2014J SN* 09 55 42.12 +69 40 25.9           SNIa-norm 456 1
12 SN 2012aw SN* 10 43 53.735 +11 40 17.63       15   SNIIP 252 1
13 SN 2006bp SN* 11 53 55.74 +52 21 09.4 14.5 15.8 14.7     SNIIP 191 1
14 SN 2011by SN* 11 55 45.56 +55 19 33.8   12.97 12.95     SNIa-norm 109 1
15 SN 2008es SN* 11 56 49.13 +54 27 25.7           SNIIL 122 1
16 SN 2008aw SN* 13 04 14.11 -10 19 12.9     15.9     SNII 34 1
17 SN 2005cs SN* 13 29 53.37 +47 10 28.2   14.5       SNIIP 450 1
18 SN 1994I SN* 13 29 54.072 +47 11 30.50     12.9     SNIc 645 1
19 SN 2011dh SN* 13 30 05.10555 +47 10 10.9227           SNIIb 445 1
20 SN 2011fe SN* 14 03 05.711 +54 16 25.22   10.12 10.06     SNIa-norm 747 1
21 SN 2007af SN* 14 22 21.03 -00 23 37.6     15.4     SNIa 185 1
22 SN 2011de SN* 15 43 53.25 +67 45 42.5           SNIa(N) 16 1
23 * alf Lyr dS* 18 36 56.33635 +38 47 01.2802 0.03 0.03 0.03 0.07 0.10 A0V 2787 1
24 ASASSN -15lh ev 22 02 15.4 -61 39 34           ~ 187 1

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