Main parameters as inferred from the spectra of SN 2015bh. The velocities are computed from the decomposition of the Hα profile.
Date . | MJD . | Phase . | Temperaturea . | Radiusb . | FWHMH α, nar . | FWHMH α, br . | vP-Cy1 . | vP-Cy2 . | LuminosityH α . | EWH αc . |
---|---|---|---|---|---|---|---|---|---|---|
. | . | (d) . | (K) . | (× 1014 cm) . | (km s−1) . | (km s−1) . | (km s−1) . | (km s−1) . | (× 1039 erg s−1) . | Å . |
20150209 | 57062.97 | −103.3 | 8600 | 1.0 (0.1) | 1500 (300) | 6000 (600) | 1000 (200) | – | 1.5 (0.6) | 400 (80) |
20150214 | 57067.07 | −99.2 | 8100 | 1.3 (0.2) | 900 (300) | 4500 (800) | 600 (400) | – | 1.5 (0.6) | 300 (70) |
20150214 | 57067.88 | −98.4 | 8300 | 1.2 (0.2) | 1000 (300) | 4800 (500) | 700 (350) | – | 1.6 (0.6) | 300 (70) |
20150311 | 57092.37 | −73.9 | 8600 | 1.5 (0.2) | 900 (300) | 3900 (400) | 700 (200) | – | 1.5 (0.6) | 300 (60) |
20150326 | 57107.95 | −58.3 | 8400 | 1.6 (0.2) | 950 (200) | 3800 (300) | 700 (200) | – | 2.3 (0.6) | 200 (50) |
20150327 | 57108.93 | −57.3 | 8600 | 1.6 (0.2) | 1200 (400) | 3700 (300) | 700 (400) | – | 2.2 (0.6) | 250 (50) |
20140424 | 57136.00 | −30.3 | 8300 | 2.0 (0.3) | 1000 (300) | 2900 (300) | 650 (300) | – | 2.0 (0.6) | 150 (30) |
20150508 | 57150.90 | −15.4 | 7100 | 2.4 (0.4) | 1400 (400) | 2600 (400) | 700 (200) | – | 1.3 (0.5) | 100 (20) |
20150516 | 57158.96 | −7.3 | 16 500 | 2.9 (0.3) | 1000 (300) | 3900 (500) | – | – | 8.5 (1.3) | 70 (20) |
20150517 | 57159.90 | −6.4 | 15 800 | 3.5 (0.3) | 1400 (200) | 2900 (300) | – | – | 11.6 (1.8) | 70 (20) |
20150520 | 57162.84 | −3.4 | 20 400 | 2.4 (0.2) | 1400 (300) | 1700 (600) | – | – | 18.1 (2.6) | 70 (20) |
20150525 | 57167.91 | 1.6 | 13 500 | 5.1 (0.6) | 1150 (300) | 2800 (300) | – | 2200 (800) | 11.1 (1.7) | 50 (10) |
20150609 | 57182.89 | 16.6 | 7900 | 11.1 (1.8) | 1200 (400) | 3000 (900) | 800 (300) | 1900 (600) | 9.8 (1.5) | 60 (10) |
20150618 | 57191.90 | 25.6 | 7300 | 11.4 (1.8) | 1100 (200) | 3900 (400) | 900 (200) | 2200 (200) | 5.9 (1.0) | 50 (10) |
FWHMblue | FWHMcore | FWHMred | vP-Cy2 | |||||||
(km s−1) | (km s−1) | (km s−1) | (km s−1) | |||||||
20151003 | 57298.78 | 132.5 | – | – | 1500 (300) | 1000 (400) | 650 (300) | 1850 (300) | 2.2 (0.6) | 900 (180) |
20151105 | 57332.04 | 165.8 | – | – | 1400 (300) | 1400 (400) | 100 (300) | – | 2.1 (0.6) | 950 (190) |
20151113 | 57339.95 | 173.7 | – | – | 1300 (300) | 1000 (400) | 800 (300) | – | 2.3 (0.6) | 1000 (200) |
20151126 | 57353.13 | 186.9 | – | – | 1300 (200) | 1300 (300) | 1000 (300) | – | 2.5 (0.6) | 1200 (240) |
20151206 | 57362.45 | 196.2 | – | – | 1200 (300) | 1300 (300) | 1100 (300) | – | 2.1 (0.6) | 1200 (240) |
20160102 | 57390.25 | 224.0 | – | – | 1250 (300) | 1400 (300) | 1100 (300) | – | 2.7 (0.6) | 1500 (300) |
20160305 | 57452.89 | 286.6 | – | – | 1300 (200) | 1500 (300) | 1100 (200) | – | 2.2 (0.6) | 1500 (300) |
Date . | MJD . | Phase . | Temperaturea . | Radiusb . | FWHMH α, nar . | FWHMH α, br . | vP-Cy1 . | vP-Cy2 . | LuminosityH α . | EWH αc . |
---|---|---|---|---|---|---|---|---|---|---|
. | . | (d) . | (K) . | (× 1014 cm) . | (km s−1) . | (km s−1) . | (km s−1) . | (km s−1) . | (× 1039 erg s−1) . | Å . |
20150209 | 57062.97 | −103.3 | 8600 | 1.0 (0.1) | 1500 (300) | 6000 (600) | 1000 (200) | – | 1.5 (0.6) | 400 (80) |
20150214 | 57067.07 | −99.2 | 8100 | 1.3 (0.2) | 900 (300) | 4500 (800) | 600 (400) | – | 1.5 (0.6) | 300 (70) |
20150214 | 57067.88 | −98.4 | 8300 | 1.2 (0.2) | 1000 (300) | 4800 (500) | 700 (350) | – | 1.6 (0.6) | 300 (70) |
20150311 | 57092.37 | −73.9 | 8600 | 1.5 (0.2) | 900 (300) | 3900 (400) | 700 (200) | – | 1.5 (0.6) | 300 (60) |
20150326 | 57107.95 | −58.3 | 8400 | 1.6 (0.2) | 950 (200) | 3800 (300) | 700 (200) | – | 2.3 (0.6) | 200 (50) |
20150327 | 57108.93 | −57.3 | 8600 | 1.6 (0.2) | 1200 (400) | 3700 (300) | 700 (400) | – | 2.2 (0.6) | 250 (50) |
20140424 | 57136.00 | −30.3 | 8300 | 2.0 (0.3) | 1000 (300) | 2900 (300) | 650 (300) | – | 2.0 (0.6) | 150 (30) |
20150508 | 57150.90 | −15.4 | 7100 | 2.4 (0.4) | 1400 (400) | 2600 (400) | 700 (200) | – | 1.3 (0.5) | 100 (20) |
20150516 | 57158.96 | −7.3 | 16 500 | 2.9 (0.3) | 1000 (300) | 3900 (500) | – | – | 8.5 (1.3) | 70 (20) |
20150517 | 57159.90 | −6.4 | 15 800 | 3.5 (0.3) | 1400 (200) | 2900 (300) | – | – | 11.6 (1.8) | 70 (20) |
20150520 | 57162.84 | −3.4 | 20 400 | 2.4 (0.2) | 1400 (300) | 1700 (600) | – | – | 18.1 (2.6) | 70 (20) |
20150525 | 57167.91 | 1.6 | 13 500 | 5.1 (0.6) | 1150 (300) | 2800 (300) | – | 2200 (800) | 11.1 (1.7) | 50 (10) |
20150609 | 57182.89 | 16.6 | 7900 | 11.1 (1.8) | 1200 (400) | 3000 (900) | 800 (300) | 1900 (600) | 9.8 (1.5) | 60 (10) |
20150618 | 57191.90 | 25.6 | 7300 | 11.4 (1.8) | 1100 (200) | 3900 (400) | 900 (200) | 2200 (200) | 5.9 (1.0) | 50 (10) |
FWHMblue | FWHMcore | FWHMred | vP-Cy2 | |||||||
(km s−1) | (km s−1) | (km s−1) | (km s−1) | |||||||
20151003 | 57298.78 | 132.5 | – | – | 1500 (300) | 1000 (400) | 650 (300) | 1850 (300) | 2.2 (0.6) | 900 (180) |
20151105 | 57332.04 | 165.8 | – | – | 1400 (300) | 1400 (400) | 100 (300) | – | 2.1 (0.6) | 950 (190) |
20151113 | 57339.95 | 173.7 | – | – | 1300 (300) | 1000 (400) | 800 (300) | – | 2.3 (0.6) | 1000 (200) |
20151126 | 57353.13 | 186.9 | – | – | 1300 (200) | 1300 (300) | 1000 (300) | – | 2.5 (0.6) | 1200 (240) |
20151206 | 57362.45 | 196.2 | – | – | 1200 (300) | 1300 (300) | 1100 (300) | – | 2.1 (0.6) | 1200 (240) |
20160102 | 57390.25 | 224.0 | – | – | 1250 (300) | 1400 (300) | 1100 (300) | – | 2.7 (0.6) | 1500 (300) |
20160305 | 57452.89 | 286.6 | – | – | 1300 (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.
Main parameters as inferred from the spectra of SN 2015bh. The velocities are computed from the decomposition of the Hα profile.
Date . | MJD . | Phase . | Temperaturea . | Radiusb . | FWHMH α, nar . | FWHMH α, br . | vP-Cy1 . | vP-Cy2 . | LuminosityH α . | EWH αc . |
---|---|---|---|---|---|---|---|---|---|---|
. | . | (d) . | (K) . | (× 1014 cm) . | (km s−1) . | (km s−1) . | (km s−1) . | (km s−1) . | (× 1039 erg s−1) . | Å . |
20150209 | 57062.97 | −103.3 | 8600 | 1.0 (0.1) | 1500 (300) | 6000 (600) | 1000 (200) | – | 1.5 (0.6) | 400 (80) |
20150214 | 57067.07 | −99.2 | 8100 | 1.3 (0.2) | 900 (300) | 4500 (800) | 600 (400) | – | 1.5 (0.6) | 300 (70) |
20150214 | 57067.88 | −98.4 | 8300 | 1.2 (0.2) | 1000 (300) | 4800 (500) | 700 (350) | – | 1.6 (0.6) | 300 (70) |
20150311 | 57092.37 | −73.9 | 8600 | 1.5 (0.2) | 900 (300) | 3900 (400) | 700 (200) | – | 1.5 (0.6) | 300 (60) |
20150326 | 57107.95 | −58.3 | 8400 | 1.6 (0.2) | 950 (200) | 3800 (300) | 700 (200) | – | 2.3 (0.6) | 200 (50) |
20150327 | 57108.93 | −57.3 | 8600 | 1.6 (0.2) | 1200 (400) | 3700 (300) | 700 (400) | – | 2.2 (0.6) | 250 (50) |
20140424 | 57136.00 | −30.3 | 8300 | 2.0 (0.3) | 1000 (300) | 2900 (300) | 650 (300) | – | 2.0 (0.6) | 150 (30) |
20150508 | 57150.90 | −15.4 | 7100 | 2.4 (0.4) | 1400 (400) | 2600 (400) | 700 (200) | – | 1.3 (0.5) | 100 (20) |
20150516 | 57158.96 | −7.3 | 16 500 | 2.9 (0.3) | 1000 (300) | 3900 (500) | – | – | 8.5 (1.3) | 70 (20) |
20150517 | 57159.90 | −6.4 | 15 800 | 3.5 (0.3) | 1400 (200) | 2900 (300) | – | – | 11.6 (1.8) | 70 (20) |
20150520 | 57162.84 | −3.4 | 20 400 | 2.4 (0.2) | 1400 (300) | 1700 (600) | – | – | 18.1 (2.6) | 70 (20) |
20150525 | 57167.91 | 1.6 | 13 500 | 5.1 (0.6) | 1150 (300) | 2800 (300) | – | 2200 (800) | 11.1 (1.7) | 50 (10) |
20150609 | 57182.89 | 16.6 | 7900 | 11.1 (1.8) | 1200 (400) | 3000 (900) | 800 (300) | 1900 (600) | 9.8 (1.5) | 60 (10) |
20150618 | 57191.90 | 25.6 | 7300 | 11.4 (1.8) | 1100 (200) | 3900 (400) | 900 (200) | 2200 (200) | 5.9 (1.0) | 50 (10) |
FWHMblue | FWHMcore | FWHMred | vP-Cy2 | |||||||
(km s−1) | (km s−1) | (km s−1) | (km s−1) | |||||||
20151003 | 57298.78 | 132.5 | – | – | 1500 (300) | 1000 (400) | 650 (300) | 1850 (300) | 2.2 (0.6) | 900 (180) |
20151105 | 57332.04 | 165.8 | – | – | 1400 (300) | 1400 (400) | 100 (300) | – | 2.1 (0.6) | 950 (190) |
20151113 | 57339.95 | 173.7 | – | – | 1300 (300) | 1000 (400) | 800 (300) | – | 2.3 (0.6) | 1000 (200) |
20151126 | 57353.13 | 186.9 | – | – | 1300 (200) | 1300 (300) | 1000 (300) | – | 2.5 (0.6) | 1200 (240) |
20151206 | 57362.45 | 196.2 | – | – | 1200 (300) | 1300 (300) | 1100 (300) | – | 2.1 (0.6) | 1200 (240) |
20160102 | 57390.25 | 224.0 | – | – | 1250 (300) | 1400 (300) | 1100 (300) | – | 2.7 (0.6) | 1500 (300) |
20160305 | 57452.89 | 286.6 | – | – | 1300 (200) | 1500 (300) | 1100 (200) | – | 2.2 (0.6) | 1500 (300) |
Date . | MJD . | Phase . | Temperaturea . | Radiusb . | FWHMH α, nar . | FWHMH α, br . | vP-Cy1 . | vP-Cy2 . | LuminosityH α . | EWH αc . |
---|---|---|---|---|---|---|---|---|---|---|
. | . | (d) . | (K) . | (× 1014 cm) . | (km s−1) . | (km s−1) . | (km s−1) . | (km s−1) . | (× 1039 erg s−1) . | Å . |
20150209 | 57062.97 | −103.3 | 8600 | 1.0 (0.1) | 1500 (300) | 6000 (600) | 1000 (200) | – | 1.5 (0.6) | 400 (80) |
20150214 | 57067.07 | −99.2 | 8100 | 1.3 (0.2) | 900 (300) | 4500 (800) | 600 (400) | – | 1.5 (0.6) | 300 (70) |
20150214 | 57067.88 | −98.4 | 8300 | 1.2 (0.2) | 1000 (300) | 4800 (500) | 700 (350) | – | 1.6 (0.6) | 300 (70) |
20150311 | 57092.37 | −73.9 | 8600 | 1.5 (0.2) | 900 (300) | 3900 (400) | 700 (200) | – | 1.5 (0.6) | 300 (60) |
20150326 | 57107.95 | −58.3 | 8400 | 1.6 (0.2) | 950 (200) | 3800 (300) | 700 (200) | – | 2.3 (0.6) | 200 (50) |
20150327 | 57108.93 | −57.3 | 8600 | 1.6 (0.2) | 1200 (400) | 3700 (300) | 700 (400) | – | 2.2 (0.6) | 250 (50) |
20140424 | 57136.00 | −30.3 | 8300 | 2.0 (0.3) | 1000 (300) | 2900 (300) | 650 (300) | – | 2.0 (0.6) | 150 (30) |
20150508 | 57150.90 | −15.4 | 7100 | 2.4 (0.4) | 1400 (400) | 2600 (400) | 700 (200) | – | 1.3 (0.5) | 100 (20) |
20150516 | 57158.96 | −7.3 | 16 500 | 2.9 (0.3) | 1000 (300) | 3900 (500) | – | – | 8.5 (1.3) | 70 (20) |
20150517 | 57159.90 | −6.4 | 15 800 | 3.5 (0.3) | 1400 (200) | 2900 (300) | – | – | 11.6 (1.8) | 70 (20) |
20150520 | 57162.84 | −3.4 | 20 400 | 2.4 (0.2) | 1400 (300) | 1700 (600) | – | – | 18.1 (2.6) | 70 (20) |
20150525 | 57167.91 | 1.6 | 13 500 | 5.1 (0.6) | 1150 (300) | 2800 (300) | – | 2200 (800) | 11.1 (1.7) | 50 (10) |
20150609 | 57182.89 | 16.6 | 7900 | 11.1 (1.8) | 1200 (400) | 3000 (900) | 800 (300) | 1900 (600) | 9.8 (1.5) | 60 (10) |
20150618 | 57191.90 | 25.6 | 7300 | 11.4 (1.8) | 1100 (200) | 3900 (400) | 900 (200) | 2200 (200) | 5.9 (1.0) | 50 (10) |
FWHMblue | FWHMcore | FWHMred | vP-Cy2 | |||||||
(km s−1) | (km s−1) | (km s−1) | (km s−1) | |||||||
20151003 | 57298.78 | 132.5 | – | – | 1500 (300) | 1000 (400) | 650 (300) | 1850 (300) | 2.2 (0.6) | 900 (180) |
20151105 | 57332.04 | 165.8 | – | – | 1400 (300) | 1400 (400) | 100 (300) | – | 2.1 (0.6) | 950 (190) |
20151113 | 57339.95 | 173.7 | – | – | 1300 (300) | 1000 (400) | 800 (300) | – | 2.3 (0.6) | 1000 (200) |
20151126 | 57353.13 | 186.9 | – | – | 1300 (200) | 1300 (300) | 1000 (300) | – | 2.5 (0.6) | 1200 (240) |
20151206 | 57362.45 | 196.2 | – | – | 1200 (300) | 1300 (300) | 1100 (300) | – | 2.1 (0.6) | 1200 (240) |
20160102 | 57390.25 | 224.0 | – | – | 1250 (300) | 1400 (300) | 1100 (300) | – | 2.7 (0.6) | 1500 (300) |
20160305 | 57452.89 | 286.6 | – | – | 1300 (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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