Table 3.

Main parameters as inferred from the spectra of SN 2015bh. The velocities are computed from the decomposition of the Hα profile.

DateMJDPhaseTemperatureaRadiusbFWHMH α, narFWHMH α, brvP-Cy1vP-Cy2LuminosityH αEWH αc
(d)(K)(× 1014 cm)(km s−1)(km s−1)(km s−1)(km s−1)(× 1039 erg s−1)Å
2015020957062.97−103.386001.0 (0.1)1500 (300)6000 (600)1000 (200)1.5 (0.6)400 (80)
2015021457067.07−99.281001.3 (0.2)900 (300)4500 (800)600 (400)1.5 (0.6)300 (70)
2015021457067.88−98.483001.2 (0.2)1000 (300)4800 (500)700 (350)1.6 (0.6)300 (70)
2015031157092.37−73.986001.5 (0.2)900 (300)3900 (400)700 (200)1.5 (0.6)300 (60)
2015032657107.95−58.384001.6 (0.2)950 (200)3800 (300)700 (200)2.3 (0.6)200 (50)
2015032757108.93−57.386001.6 (0.2)1200 (400)3700 (300)700 (400)2.2 (0.6)250 (50)
2014042457136.00−30.383002.0 (0.3)1000 (300)2900 (300)650 (300)2.0 (0.6)150 (30)
2015050857150.90−15.471002.4 (0.4)1400 (400)2600 (400)700 (200)1.3 (0.5)100 (20)
2015051657158.96−7.316 5002.9 (0.3)1000 (300)3900 (500)8.5 (1.3)70 (20)
2015051757159.90−6.415 8003.5 (0.3)1400 (200)2900 (300)11.6 (1.8)70 (20)
2015052057162.84−3.420 4002.4 (0.2)1400 (300)1700 (600)18.1 (2.6)70 (20)
2015052557167.911.613 5005.1 (0.6)1150 (300)2800 (300)2200 (800)11.1 (1.7)50 (10)
2015060957182.8916.6790011.1 (1.8)1200 (400)3000 (900)800 (300)1900 (600)9.8 (1.5)60 (10)
2015061857191.9025.6730011.4 (1.8)1100 (200)3900 (400)900 (200)2200 (200)5.9 (1.0)50 (10)
FWHMblueFWHMcoreFWHMredvP-Cy2
(km s−1)(km s−1)(km s−1)(km s−1)
2015100357298.78132.51500 (300)1000 (400)650 (300)1850 (300)2.2 (0.6)900 (180)
2015110557332.04165.81400 (300)1400 (400)100 (300)2.1 (0.6)950 (190)
2015111357339.95173.71300 (300)1000 (400)800 (300)2.3 (0.6)1000 (200)
2015112657353.13186.91300 (200)1300 (300)1000 (300)2.5 (0.6)1200 (240)
2015120657362.45196.21200 (300)1300 (300)1100 (300)2.1 (0.6)1200 (240)
2016010257390.25224.01250 (300)1400 (300)1100 (300)2.7 (0.6)1500 (300)
2016030557452.89286.61300 (200)1500 (300)1100 (200)2.2 (0.6)1500 (300)
DateMJDPhaseTemperatureaRadiusbFWHMH α, narFWHMH α, brvP-Cy1vP-Cy2LuminosityH αEWH αc
(d)(K)(× 1014 cm)(km s−1)(km s−1)(km s−1)(km s−1)(× 1039 erg s−1)Å
2015020957062.97−103.386001.0 (0.1)1500 (300)6000 (600)1000 (200)1.5 (0.6)400 (80)
2015021457067.07−99.281001.3 (0.2)900 (300)4500 (800)600 (400)1.5 (0.6)300 (70)
2015021457067.88−98.483001.2 (0.2)1000 (300)4800 (500)700 (350)1.6 (0.6)300 (70)
2015031157092.37−73.986001.5 (0.2)900 (300)3900 (400)700 (200)1.5 (0.6)300 (60)
2015032657107.95−58.384001.6 (0.2)950 (200)3800 (300)700 (200)2.3 (0.6)200 (50)
2015032757108.93−57.386001.6 (0.2)1200 (400)3700 (300)700 (400)2.2 (0.6)250 (50)
2014042457136.00−30.383002.0 (0.3)1000 (300)2900 (300)650 (300)2.0 (0.6)150 (30)
2015050857150.90−15.471002.4 (0.4)1400 (400)2600 (400)700 (200)1.3 (0.5)100 (20)
2015051657158.96−7.316 5002.9 (0.3)1000 (300)3900 (500)8.5 (1.3)70 (20)
2015051757159.90−6.415 8003.5 (0.3)1400 (200)2900 (300)11.6 (1.8)70 (20)
2015052057162.84−3.420 4002.4 (0.2)1400 (300)1700 (600)18.1 (2.6)70 (20)
2015052557167.911.613 5005.1 (0.6)1150 (300)2800 (300)2200 (800)11.1 (1.7)50 (10)
2015060957182.8916.6790011.1 (1.8)1200 (400)3000 (900)800 (300)1900 (600)9.8 (1.5)60 (10)
2015061857191.9025.6730011.4 (1.8)1100 (200)3900 (400)900 (200)2200 (200)5.9 (1.0)50 (10)
FWHMblueFWHMcoreFWHMredvP-Cy2
(km s−1)(km s−1)(km s−1)(km s−1)
2015100357298.78132.51500 (300)1000 (400)650 (300)1850 (300)2.2 (0.6)900 (180)
2015110557332.04165.81400 (300)1400 (400)100 (300)2.1 (0.6)950 (190)
2015111357339.95173.71300 (300)1000 (400)800 (300)2.3 (0.6)1000 (200)
2015112657353.13186.91300 (200)1300 (300)1000 (300)2.5 (0.6)1200 (240)
2015120657362.45196.21200 (300)1300 (300)1100 (300)2.1 (0.6)1200 (240)
2016010257390.25224.01250 (300)1400 (300)1100 (300)2.7 (0.6)1500 (300)
2016030557452.89286.61300 (200)1500 (300)1100 (200)2.2 (0.6)1500 (300)

aWe consider a conservative uncertainty in the temperature of about ± 500 K.

bWe have propagated the uncertainties from the Stefan–Boltzmann equation.

cWe consider a conservative uncertainty in the EW of about 20 per cent of the measurements.

Table 3.

Main parameters as inferred from the spectra of SN 2015bh. The velocities are computed from the decomposition of the Hα profile.

DateMJDPhaseTemperatureaRadiusbFWHMH α, narFWHMH α, brvP-Cy1vP-Cy2LuminosityH αEWH αc
(d)(K)(× 1014 cm)(km s−1)(km s−1)(km s−1)(km s−1)(× 1039 erg s−1)Å
2015020957062.97−103.386001.0 (0.1)1500 (300)6000 (600)1000 (200)1.5 (0.6)400 (80)
2015021457067.07−99.281001.3 (0.2)900 (300)4500 (800)600 (400)1.5 (0.6)300 (70)
2015021457067.88−98.483001.2 (0.2)1000 (300)4800 (500)700 (350)1.6 (0.6)300 (70)
2015031157092.37−73.986001.5 (0.2)900 (300)3900 (400)700 (200)1.5 (0.6)300 (60)
2015032657107.95−58.384001.6 (0.2)950 (200)3800 (300)700 (200)2.3 (0.6)200 (50)
2015032757108.93−57.386001.6 (0.2)1200 (400)3700 (300)700 (400)2.2 (0.6)250 (50)
2014042457136.00−30.383002.0 (0.3)1000 (300)2900 (300)650 (300)2.0 (0.6)150 (30)
2015050857150.90−15.471002.4 (0.4)1400 (400)2600 (400)700 (200)1.3 (0.5)100 (20)
2015051657158.96−7.316 5002.9 (0.3)1000 (300)3900 (500)8.5 (1.3)70 (20)
2015051757159.90−6.415 8003.5 (0.3)1400 (200)2900 (300)11.6 (1.8)70 (20)
2015052057162.84−3.420 4002.4 (0.2)1400 (300)1700 (600)18.1 (2.6)70 (20)
2015052557167.911.613 5005.1 (0.6)1150 (300)2800 (300)2200 (800)11.1 (1.7)50 (10)
2015060957182.8916.6790011.1 (1.8)1200 (400)3000 (900)800 (300)1900 (600)9.8 (1.5)60 (10)
2015061857191.9025.6730011.4 (1.8)1100 (200)3900 (400)900 (200)2200 (200)5.9 (1.0)50 (10)
FWHMblueFWHMcoreFWHMredvP-Cy2
(km s−1)(km s−1)(km s−1)(km s−1)
2015100357298.78132.51500 (300)1000 (400)650 (300)1850 (300)2.2 (0.6)900 (180)
2015110557332.04165.81400 (300)1400 (400)100 (300)2.1 (0.6)950 (190)
2015111357339.95173.71300 (300)1000 (400)800 (300)2.3 (0.6)1000 (200)
2015112657353.13186.91300 (200)1300 (300)1000 (300)2.5 (0.6)1200 (240)
2015120657362.45196.21200 (300)1300 (300)1100 (300)2.1 (0.6)1200 (240)
2016010257390.25224.01250 (300)1400 (300)1100 (300)2.7 (0.6)1500 (300)
2016030557452.89286.61300 (200)1500 (300)1100 (200)2.2 (0.6)1500 (300)
DateMJDPhaseTemperatureaRadiusbFWHMH α, narFWHMH α, brvP-Cy1vP-Cy2LuminosityH αEWH αc
(d)(K)(× 1014 cm)(km s−1)(km s−1)(km s−1)(km s−1)(× 1039 erg s−1)Å
2015020957062.97−103.386001.0 (0.1)1500 (300)6000 (600)1000 (200)1.5 (0.6)400 (80)
2015021457067.07−99.281001.3 (0.2)900 (300)4500 (800)600 (400)1.5 (0.6)300 (70)
2015021457067.88−98.483001.2 (0.2)1000 (300)4800 (500)700 (350)1.6 (0.6)300 (70)
2015031157092.37−73.986001.5 (0.2)900 (300)3900 (400)700 (200)1.5 (0.6)300 (60)
2015032657107.95−58.384001.6 (0.2)950 (200)3800 (300)700 (200)2.3 (0.6)200 (50)
2015032757108.93−57.386001.6 (0.2)1200 (400)3700 (300)700 (400)2.2 (0.6)250 (50)
2014042457136.00−30.383002.0 (0.3)1000 (300)2900 (300)650 (300)2.0 (0.6)150 (30)
2015050857150.90−15.471002.4 (0.4)1400 (400)2600 (400)700 (200)1.3 (0.5)100 (20)
2015051657158.96−7.316 5002.9 (0.3)1000 (300)3900 (500)8.5 (1.3)70 (20)
2015051757159.90−6.415 8003.5 (0.3)1400 (200)2900 (300)11.6 (1.8)70 (20)
2015052057162.84−3.420 4002.4 (0.2)1400 (300)1700 (600)18.1 (2.6)70 (20)
2015052557167.911.613 5005.1 (0.6)1150 (300)2800 (300)2200 (800)11.1 (1.7)50 (10)
2015060957182.8916.6790011.1 (1.8)1200 (400)3000 (900)800 (300)1900 (600)9.8 (1.5)60 (10)
2015061857191.9025.6730011.4 (1.8)1100 (200)3900 (400)900 (200)2200 (200)5.9 (1.0)50 (10)
FWHMblueFWHMcoreFWHMredvP-Cy2
(km s−1)(km s−1)(km s−1)(km s−1)
2015100357298.78132.51500 (300)1000 (400)650 (300)1850 (300)2.2 (0.6)900 (180)
2015110557332.04165.81400 (300)1400 (400)100 (300)2.1 (0.6)950 (190)
2015111357339.95173.71300 (300)1000 (400)800 (300)2.3 (0.6)1000 (200)
2015112657353.13186.91300 (200)1300 (300)1000 (300)2.5 (0.6)1200 (240)
2015120657362.45196.21200 (300)1300 (300)1100 (300)2.1 (0.6)1200 (240)
2016010257390.25224.01250 (300)1400 (300)1100 (300)2.7 (0.6)1500 (300)
2016030557452.89286.61300 (200)1500 (300)1100 (200)2.2 (0.6)1500 (300)

aWe consider a conservative uncertainty in the temperature of about ± 500 K.

bWe have propagated the uncertainties from the Stefan–Boltzmann equation.

cWe consider a conservative uncertainty in the EW of about 20 per cent of the measurements.

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