Best-fitting source PSD model parameters for the joint fit of a smoothly double bending power-law model (equation 3) to the three longest observations: 0725200301, 0725200101 and 0311190101. The first column, (1), gives the energy range, the second column, (2), the high-frequency PSD bend, the third column, (3), the medium-frequency PSD index, the fourth column, (4), the high-frequency PSD index, the fifth column, (5), the PSD normalization, and finally the sixth, seventh and eighth column, (6,7 and 8), the constant Poisson noise levels for the three observations, respectively. Note that during the fit, αl and fl are fixed to the values 0 and 10−8 Hz, respectively.
| (1) . | (2) . | (3) . | (4) . | (5) . | (6) . | (7) . | (8) . |
|---|---|---|---|---|---|---|---|
| Energy range . | fh × 10−5 . | αm . | αh . | A . | c1 . | c2 . | c3 . |
| (keV) . | (Hz) . | . | . | (Hz−1) . | (Hz−1) . | (Hz−1) . | (Hz−1) . |
| 0.5–10 | |$6.71^{+1.31}_{-0.97}$| | |$0.51^{+0.30}_{-0.19}$| | |$1.99^{+0.17}_{-0.06}$| | |$79.64^{+5.96}_{-3.73}$| | |$0.29^{+0.13}_{-0.06}$| | |$0.24^{+0.18}_{-0.05}$| | |$0.37^{+0.19}_{-0.05}$| |
| 0.5–2 | |$6.05^{+1.89}_{-1.06}$| | |$0.32^{+0.48}_{-0.24}$| | |$2.21^{+0.22}_{-0.10}$| | |$41.23^{+7.43}_{-5.06}$| | |$0.67^{+0.99}_{-0.12}$| | |$0.55^{+1.06}_{-0.33}$| | |$0.86^{+1.11}_{-0.12}$| |
| 2–4 | |$4.93^{+1.92}_{-1.39}$| | |$0.75^{+0.67}_{-0.39}$| | |$1.86^{+0.25}_{-0.12}$| | |$243.01^{+10.04}_{-9.39}$| | |$0.95^{+0.96}_{-0.26}$| | |$0.77^{+1.01}_{-0.31}$| | |$1.21^{+1.12}_{-0.45}$| |
| 4–10 | |$4.26^{+2.08}_{-\,{\rm -\!-}}$| | |$0.83^{+0.74}_{-0.42}$| | |$1.78^{+0.34}_{-0.22}$| | |$689.64^{+15.98}_{-12.34}$| | |$1.47^{+1.10}_{-0.12}$| | |$1.22^{+1.07}_{-0.11}$| | |$1.80^{+1.23}_{-0.15}$| |
| (1) . | (2) . | (3) . | (4) . | (5) . | (6) . | (7) . | (8) . |
|---|---|---|---|---|---|---|---|
| Energy range . | fh × 10−5 . | αm . | αh . | A . | c1 . | c2 . | c3 . |
| (keV) . | (Hz) . | . | . | (Hz−1) . | (Hz−1) . | (Hz−1) . | (Hz−1) . |
| 0.5–10 | |$6.71^{+1.31}_{-0.97}$| | |$0.51^{+0.30}_{-0.19}$| | |$1.99^{+0.17}_{-0.06}$| | |$79.64^{+5.96}_{-3.73}$| | |$0.29^{+0.13}_{-0.06}$| | |$0.24^{+0.18}_{-0.05}$| | |$0.37^{+0.19}_{-0.05}$| |
| 0.5–2 | |$6.05^{+1.89}_{-1.06}$| | |$0.32^{+0.48}_{-0.24}$| | |$2.21^{+0.22}_{-0.10}$| | |$41.23^{+7.43}_{-5.06}$| | |$0.67^{+0.99}_{-0.12}$| | |$0.55^{+1.06}_{-0.33}$| | |$0.86^{+1.11}_{-0.12}$| |
| 2–4 | |$4.93^{+1.92}_{-1.39}$| | |$0.75^{+0.67}_{-0.39}$| | |$1.86^{+0.25}_{-0.12}$| | |$243.01^{+10.04}_{-9.39}$| | |$0.95^{+0.96}_{-0.26}$| | |$0.77^{+1.01}_{-0.31}$| | |$1.21^{+1.12}_{-0.45}$| |
| 4–10 | |$4.26^{+2.08}_{-\,{\rm -\!-}}$| | |$0.83^{+0.74}_{-0.42}$| | |$1.78^{+0.34}_{-0.22}$| | |$689.64^{+15.98}_{-12.34}$| | |$1.47^{+1.10}_{-0.12}$| | |$1.22^{+1.07}_{-0.11}$| | |$1.80^{+1.23}_{-0.15}$| |
Best-fitting source PSD model parameters for the joint fit of a smoothly double bending power-law model (equation 3) to the three longest observations: 0725200301, 0725200101 and 0311190101. The first column, (1), gives the energy range, the second column, (2), the high-frequency PSD bend, the third column, (3), the medium-frequency PSD index, the fourth column, (4), the high-frequency PSD index, the fifth column, (5), the PSD normalization, and finally the sixth, seventh and eighth column, (6,7 and 8), the constant Poisson noise levels for the three observations, respectively. Note that during the fit, αl and fl are fixed to the values 0 and 10−8 Hz, respectively.
| (1) . | (2) . | (3) . | (4) . | (5) . | (6) . | (7) . | (8) . |
|---|---|---|---|---|---|---|---|
| Energy range . | fh × 10−5 . | αm . | αh . | A . | c1 . | c2 . | c3 . |
| (keV) . | (Hz) . | . | . | (Hz−1) . | (Hz−1) . | (Hz−1) . | (Hz−1) . |
| 0.5–10 | |$6.71^{+1.31}_{-0.97}$| | |$0.51^{+0.30}_{-0.19}$| | |$1.99^{+0.17}_{-0.06}$| | |$79.64^{+5.96}_{-3.73}$| | |$0.29^{+0.13}_{-0.06}$| | |$0.24^{+0.18}_{-0.05}$| | |$0.37^{+0.19}_{-0.05}$| |
| 0.5–2 | |$6.05^{+1.89}_{-1.06}$| | |$0.32^{+0.48}_{-0.24}$| | |$2.21^{+0.22}_{-0.10}$| | |$41.23^{+7.43}_{-5.06}$| | |$0.67^{+0.99}_{-0.12}$| | |$0.55^{+1.06}_{-0.33}$| | |$0.86^{+1.11}_{-0.12}$| |
| 2–4 | |$4.93^{+1.92}_{-1.39}$| | |$0.75^{+0.67}_{-0.39}$| | |$1.86^{+0.25}_{-0.12}$| | |$243.01^{+10.04}_{-9.39}$| | |$0.95^{+0.96}_{-0.26}$| | |$0.77^{+1.01}_{-0.31}$| | |$1.21^{+1.12}_{-0.45}$| |
| 4–10 | |$4.26^{+2.08}_{-\,{\rm -\!-}}$| | |$0.83^{+0.74}_{-0.42}$| | |$1.78^{+0.34}_{-0.22}$| | |$689.64^{+15.98}_{-12.34}$| | |$1.47^{+1.10}_{-0.12}$| | |$1.22^{+1.07}_{-0.11}$| | |$1.80^{+1.23}_{-0.15}$| |
| (1) . | (2) . | (3) . | (4) . | (5) . | (6) . | (7) . | (8) . |
|---|---|---|---|---|---|---|---|
| Energy range . | fh × 10−5 . | αm . | αh . | A . | c1 . | c2 . | c3 . |
| (keV) . | (Hz) . | . | . | (Hz−1) . | (Hz−1) . | (Hz−1) . | (Hz−1) . |
| 0.5–10 | |$6.71^{+1.31}_{-0.97}$| | |$0.51^{+0.30}_{-0.19}$| | |$1.99^{+0.17}_{-0.06}$| | |$79.64^{+5.96}_{-3.73}$| | |$0.29^{+0.13}_{-0.06}$| | |$0.24^{+0.18}_{-0.05}$| | |$0.37^{+0.19}_{-0.05}$| |
| 0.5–2 | |$6.05^{+1.89}_{-1.06}$| | |$0.32^{+0.48}_{-0.24}$| | |$2.21^{+0.22}_{-0.10}$| | |$41.23^{+7.43}_{-5.06}$| | |$0.67^{+0.99}_{-0.12}$| | |$0.55^{+1.06}_{-0.33}$| | |$0.86^{+1.11}_{-0.12}$| |
| 2–4 | |$4.93^{+1.92}_{-1.39}$| | |$0.75^{+0.67}_{-0.39}$| | |$1.86^{+0.25}_{-0.12}$| | |$243.01^{+10.04}_{-9.39}$| | |$0.95^{+0.96}_{-0.26}$| | |$0.77^{+1.01}_{-0.31}$| | |$1.21^{+1.12}_{-0.45}$| |
| 4–10 | |$4.26^{+2.08}_{-\,{\rm -\!-}}$| | |$0.83^{+0.74}_{-0.42}$| | |$1.78^{+0.34}_{-0.22}$| | |$689.64^{+15.98}_{-12.34}$| | |$1.47^{+1.10}_{-0.12}$| | |$1.22^{+1.07}_{-0.11}$| | |$1.80^{+1.23}_{-0.15}$| |
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