Parameters for Norris model fit to the LC of the GRB pulses. We also report the time interval (t1–t2) in which we have performed our analysis, number of time bins (n) within the time interval and the best detectors used for time-resolved spectroscopy.
| . | . | . | . | . | . | . | . | Specification of . | ||
|---|---|---|---|---|---|---|---|---|---|---|
| GRB . | Norris model parameters . | time-resolved analysis . | ||||||||
| . | ts (s) . | τ1 (s) . | τ2 (s) . | |$\chi ^2_{\rm red}\ ({\rm dof})$| . | p (s) . | w (s) . | κ . | t1, t2 (s) . | n . | Detectors used . |
| 081224 | |$-1.53_{-0.26}^{+0.34}$| | |$3.60_{-1.07}^{+0.99}$| | |$3.30_{-0.21}^{+0.27}$| | 6.80 (13) | 1.90 ± 0.10 | 7.5 ± 0.7 | 0.44 ± 0.03 | −0.5, 19.6 | 15 | n6, n7, n9, b1 |
| 090809B | |$-1.74_{-0.38}^{+0.31}$| | |$9.35_{-1.85}^{+2.59}$| | |$2.50_{-0.17}^{+0.17}$| | 5.88 (13) | 3.10 ± 0.09 | 7.4 ± 0.6 | 0.34 ± 0.02 | −4.0, 19.3 | 15 | n3, n4, n5, b0 |
| 100612A | |$-8.43_{-2.65}^{+1.61}$| | |$156.4_{-57.4}^{+137.6}$| | |$0.88_{-0.17}^{+0.14}$| | 16.8 (9) | 3.30 ± 0.06 | 6.5 ± 1.5 | 0.14 ± 0.02 | −2.0, 17.2 | 11 | n3, n4, n8, b0 |
| 100707A | |$-2.5_{-2.6}^{+3.2}\times 10^{-2}$| | |$0.37_{-0.05}^{+0.04}$| | |$7.19_{-0.16}^{+0.18}$| | 4.01 (233) | 1.60 ± 0.07 | 9.9 ± 0.28 | 0.72 ± 0.01 | −1.0, 22.6 | 18 | n4, n7, n8, b1 |
| 110721A | |$-0.62_{-0.15}^{+0.08}$| | |$1.58_{-0.46}^{+0.67}$| | |$1.59_{-0.23}^{+0.15}$| | 1.32 (229) | 0.96 ± 0.10 | 3.55 ± 0.62 | 0.45 ± 0.03 | −1.0, 10.6 | 15 | n6, n7, n9, b1 |
| |$1.75_{-0.07}^{+0.10}$| | |$0.079_{-0.053}^{+0.074}$| | |$6.75_{-0.66}^{+0.86}$| | 2.48 ± 0.12 | 8.08 ± 1.04 | 0.83 ± 0.05 | |||||
| 110817A | |$-0.62_{-0.42}^{+0.30}$| | |$1.11_{-0.66}^{+1.31}$| | |$1.76_{-0.24}^{+0.24}$| | 1.85 (8) | 0.78 ± 0.12 | 3.6 ± 0.8 | 0.49 ± 0.08 | −0.3, 7.1 | 8 | n6, n7, n9, b1 |
| 081207 | |$-8.55_{-2.21}^{+3.30}$| | |$14.14_{-6.10}^{+9.10}$| | |$50.79_{-10.22}^{+11.10}$| | 1.36 (114) | 18.25 ± 3.36 | 90 ± 21 | 0.57 ± 0.06 | −7.0, 76.0 | 20 | n1, n9, na, b1 |
| −9.64 | 304.7 | |$9.24_{-2.20}^{+3.50}$| | 43.42 ± 1.19 | 45 | 0.20 | |||||
| 090922A | |$-0.39_{-0.19}^{+0.15}$| | |$0.62_{-0.27}^{+0.38}$| | |$4.00_{-0.30}^{+0.30}$| | 6.23 (15) | 1.18 ± 0.18 | 6.4 ± 0.7 | 0.62 ± 0.05 | −4.0, 13.4 | 8 | n0, n6, n9, b1 |
| 100528A | |$-32.6_{-2.36}^{+2.36}$| | |$1262.0_{-61.1}^{+60.9}$| | |$1.29_{-0.38}^{+0.14}$| | 6.56 (21) | 7.70 ± 0.06 | 14.5 ± 3.0 | 0.09 ± 0.004 | −3.0, 21.4 | 16 | n6, n7, n9, b1 |
| . | . | . | . | . | . | . | . | Specification of . | ||
|---|---|---|---|---|---|---|---|---|---|---|
| GRB . | Norris model parameters . | time-resolved analysis . | ||||||||
| . | ts (s) . | τ1 (s) . | τ2 (s) . | |$\chi ^2_{\rm red}\ ({\rm dof})$| . | p (s) . | w (s) . | κ . | t1, t2 (s) . | n . | Detectors used . |
| 081224 | |$-1.53_{-0.26}^{+0.34}$| | |$3.60_{-1.07}^{+0.99}$| | |$3.30_{-0.21}^{+0.27}$| | 6.80 (13) | 1.90 ± 0.10 | 7.5 ± 0.7 | 0.44 ± 0.03 | −0.5, 19.6 | 15 | n6, n7, n9, b1 |
| 090809B | |$-1.74_{-0.38}^{+0.31}$| | |$9.35_{-1.85}^{+2.59}$| | |$2.50_{-0.17}^{+0.17}$| | 5.88 (13) | 3.10 ± 0.09 | 7.4 ± 0.6 | 0.34 ± 0.02 | −4.0, 19.3 | 15 | n3, n4, n5, b0 |
| 100612A | |$-8.43_{-2.65}^{+1.61}$| | |$156.4_{-57.4}^{+137.6}$| | |$0.88_{-0.17}^{+0.14}$| | 16.8 (9) | 3.30 ± 0.06 | 6.5 ± 1.5 | 0.14 ± 0.02 | −2.0, 17.2 | 11 | n3, n4, n8, b0 |
| 100707A | |$-2.5_{-2.6}^{+3.2}\times 10^{-2}$| | |$0.37_{-0.05}^{+0.04}$| | |$7.19_{-0.16}^{+0.18}$| | 4.01 (233) | 1.60 ± 0.07 | 9.9 ± 0.28 | 0.72 ± 0.01 | −1.0, 22.6 | 18 | n4, n7, n8, b1 |
| 110721A | |$-0.62_{-0.15}^{+0.08}$| | |$1.58_{-0.46}^{+0.67}$| | |$1.59_{-0.23}^{+0.15}$| | 1.32 (229) | 0.96 ± 0.10 | 3.55 ± 0.62 | 0.45 ± 0.03 | −1.0, 10.6 | 15 | n6, n7, n9, b1 |
| |$1.75_{-0.07}^{+0.10}$| | |$0.079_{-0.053}^{+0.074}$| | |$6.75_{-0.66}^{+0.86}$| | 2.48 ± 0.12 | 8.08 ± 1.04 | 0.83 ± 0.05 | |||||
| 110817A | |$-0.62_{-0.42}^{+0.30}$| | |$1.11_{-0.66}^{+1.31}$| | |$1.76_{-0.24}^{+0.24}$| | 1.85 (8) | 0.78 ± 0.12 | 3.6 ± 0.8 | 0.49 ± 0.08 | −0.3, 7.1 | 8 | n6, n7, n9, b1 |
| 081207 | |$-8.55_{-2.21}^{+3.30}$| | |$14.14_{-6.10}^{+9.10}$| | |$50.79_{-10.22}^{+11.10}$| | 1.36 (114) | 18.25 ± 3.36 | 90 ± 21 | 0.57 ± 0.06 | −7.0, 76.0 | 20 | n1, n9, na, b1 |
| −9.64 | 304.7 | |$9.24_{-2.20}^{+3.50}$| | 43.42 ± 1.19 | 45 | 0.20 | |||||
| 090922A | |$-0.39_{-0.19}^{+0.15}$| | |$0.62_{-0.27}^{+0.38}$| | |$4.00_{-0.30}^{+0.30}$| | 6.23 (15) | 1.18 ± 0.18 | 6.4 ± 0.7 | 0.62 ± 0.05 | −4.0, 13.4 | 8 | n0, n6, n9, b1 |
| 100528A | |$-32.6_{-2.36}^{+2.36}$| | |$1262.0_{-61.1}^{+60.9}$| | |$1.29_{-0.38}^{+0.14}$| | 6.56 (21) | 7.70 ± 0.06 | 14.5 ± 3.0 | 0.09 ± 0.004 | −3.0, 21.4 | 16 | n6, n7, n9, b1 |
Parameters for Norris model fit to the LC of the GRB pulses. We also report the time interval (t1–t2) in which we have performed our analysis, number of time bins (n) within the time interval and the best detectors used for time-resolved spectroscopy.
| . | . | . | . | . | . | . | . | Specification of . | ||
|---|---|---|---|---|---|---|---|---|---|---|
| GRB . | Norris model parameters . | time-resolved analysis . | ||||||||
| . | ts (s) . | τ1 (s) . | τ2 (s) . | |$\chi ^2_{\rm red}\ ({\rm dof})$| . | p (s) . | w (s) . | κ . | t1, t2 (s) . | n . | Detectors used . |
| 081224 | |$-1.53_{-0.26}^{+0.34}$| | |$3.60_{-1.07}^{+0.99}$| | |$3.30_{-0.21}^{+0.27}$| | 6.80 (13) | 1.90 ± 0.10 | 7.5 ± 0.7 | 0.44 ± 0.03 | −0.5, 19.6 | 15 | n6, n7, n9, b1 |
| 090809B | |$-1.74_{-0.38}^{+0.31}$| | |$9.35_{-1.85}^{+2.59}$| | |$2.50_{-0.17}^{+0.17}$| | 5.88 (13) | 3.10 ± 0.09 | 7.4 ± 0.6 | 0.34 ± 0.02 | −4.0, 19.3 | 15 | n3, n4, n5, b0 |
| 100612A | |$-8.43_{-2.65}^{+1.61}$| | |$156.4_{-57.4}^{+137.6}$| | |$0.88_{-0.17}^{+0.14}$| | 16.8 (9) | 3.30 ± 0.06 | 6.5 ± 1.5 | 0.14 ± 0.02 | −2.0, 17.2 | 11 | n3, n4, n8, b0 |
| 100707A | |$-2.5_{-2.6}^{+3.2}\times 10^{-2}$| | |$0.37_{-0.05}^{+0.04}$| | |$7.19_{-0.16}^{+0.18}$| | 4.01 (233) | 1.60 ± 0.07 | 9.9 ± 0.28 | 0.72 ± 0.01 | −1.0, 22.6 | 18 | n4, n7, n8, b1 |
| 110721A | |$-0.62_{-0.15}^{+0.08}$| | |$1.58_{-0.46}^{+0.67}$| | |$1.59_{-0.23}^{+0.15}$| | 1.32 (229) | 0.96 ± 0.10 | 3.55 ± 0.62 | 0.45 ± 0.03 | −1.0, 10.6 | 15 | n6, n7, n9, b1 |
| |$1.75_{-0.07}^{+0.10}$| | |$0.079_{-0.053}^{+0.074}$| | |$6.75_{-0.66}^{+0.86}$| | 2.48 ± 0.12 | 8.08 ± 1.04 | 0.83 ± 0.05 | |||||
| 110817A | |$-0.62_{-0.42}^{+0.30}$| | |$1.11_{-0.66}^{+1.31}$| | |$1.76_{-0.24}^{+0.24}$| | 1.85 (8) | 0.78 ± 0.12 | 3.6 ± 0.8 | 0.49 ± 0.08 | −0.3, 7.1 | 8 | n6, n7, n9, b1 |
| 081207 | |$-8.55_{-2.21}^{+3.30}$| | |$14.14_{-6.10}^{+9.10}$| | |$50.79_{-10.22}^{+11.10}$| | 1.36 (114) | 18.25 ± 3.36 | 90 ± 21 | 0.57 ± 0.06 | −7.0, 76.0 | 20 | n1, n9, na, b1 |
| −9.64 | 304.7 | |$9.24_{-2.20}^{+3.50}$| | 43.42 ± 1.19 | 45 | 0.20 | |||||
| 090922A | |$-0.39_{-0.19}^{+0.15}$| | |$0.62_{-0.27}^{+0.38}$| | |$4.00_{-0.30}^{+0.30}$| | 6.23 (15) | 1.18 ± 0.18 | 6.4 ± 0.7 | 0.62 ± 0.05 | −4.0, 13.4 | 8 | n0, n6, n9, b1 |
| 100528A | |$-32.6_{-2.36}^{+2.36}$| | |$1262.0_{-61.1}^{+60.9}$| | |$1.29_{-0.38}^{+0.14}$| | 6.56 (21) | 7.70 ± 0.06 | 14.5 ± 3.0 | 0.09 ± 0.004 | −3.0, 21.4 | 16 | n6, n7, n9, b1 |
| . | . | . | . | . | . | . | . | Specification of . | ||
|---|---|---|---|---|---|---|---|---|---|---|
| GRB . | Norris model parameters . | time-resolved analysis . | ||||||||
| . | ts (s) . | τ1 (s) . | τ2 (s) . | |$\chi ^2_{\rm red}\ ({\rm dof})$| . | p (s) . | w (s) . | κ . | t1, t2 (s) . | n . | Detectors used . |
| 081224 | |$-1.53_{-0.26}^{+0.34}$| | |$3.60_{-1.07}^{+0.99}$| | |$3.30_{-0.21}^{+0.27}$| | 6.80 (13) | 1.90 ± 0.10 | 7.5 ± 0.7 | 0.44 ± 0.03 | −0.5, 19.6 | 15 | n6, n7, n9, b1 |
| 090809B | |$-1.74_{-0.38}^{+0.31}$| | |$9.35_{-1.85}^{+2.59}$| | |$2.50_{-0.17}^{+0.17}$| | 5.88 (13) | 3.10 ± 0.09 | 7.4 ± 0.6 | 0.34 ± 0.02 | −4.0, 19.3 | 15 | n3, n4, n5, b0 |
| 100612A | |$-8.43_{-2.65}^{+1.61}$| | |$156.4_{-57.4}^{+137.6}$| | |$0.88_{-0.17}^{+0.14}$| | 16.8 (9) | 3.30 ± 0.06 | 6.5 ± 1.5 | 0.14 ± 0.02 | −2.0, 17.2 | 11 | n3, n4, n8, b0 |
| 100707A | |$-2.5_{-2.6}^{+3.2}\times 10^{-2}$| | |$0.37_{-0.05}^{+0.04}$| | |$7.19_{-0.16}^{+0.18}$| | 4.01 (233) | 1.60 ± 0.07 | 9.9 ± 0.28 | 0.72 ± 0.01 | −1.0, 22.6 | 18 | n4, n7, n8, b1 |
| 110721A | |$-0.62_{-0.15}^{+0.08}$| | |$1.58_{-0.46}^{+0.67}$| | |$1.59_{-0.23}^{+0.15}$| | 1.32 (229) | 0.96 ± 0.10 | 3.55 ± 0.62 | 0.45 ± 0.03 | −1.0, 10.6 | 15 | n6, n7, n9, b1 |
| |$1.75_{-0.07}^{+0.10}$| | |$0.079_{-0.053}^{+0.074}$| | |$6.75_{-0.66}^{+0.86}$| | 2.48 ± 0.12 | 8.08 ± 1.04 | 0.83 ± 0.05 | |||||
| 110817A | |$-0.62_{-0.42}^{+0.30}$| | |$1.11_{-0.66}^{+1.31}$| | |$1.76_{-0.24}^{+0.24}$| | 1.85 (8) | 0.78 ± 0.12 | 3.6 ± 0.8 | 0.49 ± 0.08 | −0.3, 7.1 | 8 | n6, n7, n9, b1 |
| 081207 | |$-8.55_{-2.21}^{+3.30}$| | |$14.14_{-6.10}^{+9.10}$| | |$50.79_{-10.22}^{+11.10}$| | 1.36 (114) | 18.25 ± 3.36 | 90 ± 21 | 0.57 ± 0.06 | −7.0, 76.0 | 20 | n1, n9, na, b1 |
| −9.64 | 304.7 | |$9.24_{-2.20}^{+3.50}$| | 43.42 ± 1.19 | 45 | 0.20 | |||||
| 090922A | |$-0.39_{-0.19}^{+0.15}$| | |$0.62_{-0.27}^{+0.38}$| | |$4.00_{-0.30}^{+0.30}$| | 6.23 (15) | 1.18 ± 0.18 | 6.4 ± 0.7 | 0.62 ± 0.05 | −4.0, 13.4 | 8 | n0, n6, n9, b1 |
| 100528A | |$-32.6_{-2.36}^{+2.36}$| | |$1262.0_{-61.1}^{+60.9}$| | |$1.29_{-0.38}^{+0.14}$| | 6.56 (21) | 7.70 ± 0.06 | 14.5 ± 3.0 | 0.09 ± 0.004 | −3.0, 21.4 | 16 | n6, n7, n9, b1 |
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