RECORD
RXTE Spectrum of A2319
Astrophysics · Submitted 23 Oct 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Identifying the power-law emission as Compton scattering of the radio-emitting electrons by the CMB, we obtain $B \sim0.1-0.3$ $\mu G$ for the volume-averaged magnetic field, and $\sim 4 \times 10^{-14}(R/2 Mpc)^{-3}$ erg cm$^{-3}$ for the mean energy density of the emitting electrons in the central region (radius R) of A2319.
The compiled record
The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
Open the compiled record
The abstract, sentence by sentence
The cluster of galaxies A2319 was observed in 1999 for 160 ks by the PCA and HEXTE instruments aboard the RXTE satellite. No noticeable variability is seen in the emission measured by either instrument over the 8 week observation. Fitting the RXTE data by a single thermal component we obtain $kT = 8.6 \pm 0.1$ (90% confidence limits), a low iron abundance $Z_{F_e} \sim 0.16 \pm 0.02$, and large positive residuals below 6 keV and between 15 to 30 keV. The quality of the fit is drastically improved if a second component is added. A two-temperature model yields $kT_{1} \simeq 10.1 \pm 0.6$, $kT_{2}\simeq 2.8 \pm 0.6$, and of $Z_{F_e} \sim 0.23 \pm 0.03$. An equally good fit is obtained by a combination of a primary thermal and a secondary nonthermal component, with $kT \simeq 8.9 \pm 0.6$, and power-law index $\alpha \simeq 2.4 \pm 0.3$. We have repeated the analysis by performing joint fits to both these RXTE measurements and archival ASCA data. At most 25% of the RXTE secondary component could be present in the ASCA data. Allowing for this difference, very similar results were obtained, with only somewhat different values for the temperature and power-law index in the latter model. The deduced value of $\alpha$ is consistent with the measured spectrum of extended radio emission. Identifying the power-law emission as Compton scattering of the radio-emitting electrons by the CMB, we obtain $B \sim0.1-0.3$ $\mu G$ for the volume-averaged magnetic field, and $\sim 4 \times 10^{-14}(R/2 Mpc)^{-3}$ erg cm$^{-3}$ for the mean energy density of the emitting electrons in the central region (radius R) of A2319.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The cluster of galaxies A2319 was observed in 1999 for 160 ks by the PCA and HEXTE instruments aboard the RXTE satellite. | method 0.94 | 0.84 | 0.02 | asserted 1.00 |
| s1 | No noticeable variability is seen in the emission measured by either instrument over the 8 week observation. | result 1.00 | 0.90 | 0.03 | asserted 1.00 |
| s2 | Fitting the RXTE data by a single thermal component we obtain $kT = 8.6 \pm 0.1$ (90% confidence limits), a low iron abundance $Z_{F_e} \sim 0.16 \pm 0.02$, and large positive residuals below 6 keV and between 15 to 30 keV. | result 1.00 | 0.96 | 0.09 | asserted 1.00 |
| s3 | The quality of the fit is drastically improved if a second component is added. | result 0.95 | 0.92 | 0.08 | asserted 1.00 |
| s4 | A two-temperature model yields $kT_{1} \simeq 10.1 \pm 0.6$, $kT_{2}\simeq 2.8 \pm 0.6$, and of $Z_{F_e} \sim 0.23 \pm 0.03$. | result 1.00 | 0.96 | 0.11 | asserted 1.00 |
| s5 | An equally good fit is obtained by a combination of a primary thermal and a secondary nonthermal component, with $kT \simeq 8.9 \pm 0.6$, and power-law index $\alpha \simeq 2.4 \pm 0.3$. | result 0.99 | 0.95 | 0.14 | asserted 1.00 |
| s6 | We have repeated the analysis by performing joint fits to both these RXTE measurements and archival ASCA data. | method 0.89 | 0.96 | 0.02 | asserted 1.00 |
| s7 | At most 25% of the RXTE secondary component could be present in the ASCA data. | result 0.97 | 0.88 | 0.06 | hedged possibility 0.96 |
| s8 | Allowing for this difference, very similar results were obtained, with only somewhat different values for the temperature and power-law index in the latter model. | result 0.98 | 0.94 | 0.07 | asserted 0.94 |
| s9 | The deduced value of $\alpha$ is consistent with the measured spectrum of extended radio emission. | interpretation 0.56 | 0.82 | 0.10 | hedged possibility 0.83 |
| s10 | Identifying the power-law emission as Compton scattering of the radio-emitting electrons by the CMB, we obtain $B \sim0.1-0.3$ $\mu G$ for the volume-averaged magnetic field, and $\sim 4 \times 10^{-14}(R/2 Mpc)^{-3}$ erg cm$^{-3}$ for the mean energy density of the emitting electrons in the central region (radius R) of A2319. | result 0.52 | 0.91 | 0.59 | asserted 0.88 |
What was examined, and what was not
- arXiv listing abstract v1
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
The paper
Original abstract
The cluster of galaxies A2319 was observed in 1999 for 160 ks by the PCA and HEXTE instruments aboard the RXTE satellite. No noticeable variability is seen in the emission measured by either instrument over the 8 week observation. Fitting the RXTE data by a single thermal component we obtain $kT = 8.6 \pm 0.1$ (90% confidence limits), a low iron abundance $Z_{F_e} \sim 0.16 \pm 0.02$, and large positive residuals below 6 keV and between 15 to 30 keV. The quality of the fit is drastically improved if a second component is added. A two-temperature model yields $kT_{1} \simeq 10.1 \pm 0.6$, $kT_{2}\simeq 2.8 \pm 0.6$, and of $Z_{F_e} \sim 0.23 \pm 0.03$. An equally good fit is obtained by a combination of a primary thermal and a secondary nonthermal component, with $kT \simeq 8.9 \pm 0.6$, and power-law index $\alpha \simeq 2.4 \pm 0.3$. We have repeated the analysis by performing joint fits to both these RXTE measurements and archival ASCA data. At most 25% of the RXTE secondary component could be present in the ASCA data. Allowing for this difference, very similar results were obtained, with only somewhat different values for the temperature and power-law index in the latter model. The deduced value of $\alpha$ is consistent with the measured spectrum of extended radio emission. Identifying the power-law emission as Compton scattering of the radio-emitting electrons by the CMB, we obtain $B \sim0.1-0.3$ $\mu G$ for the volume-averaged magnetic field, and $\sim 4 \times 10^{-14}(R/2 Mpc)^{-3}$ erg cm$^{-3}$ for the mean energy density of the emitting electrons in the central region (radius R) of A2319.
Human review
Discussion
Know something about this paper? Leave a comment, or highlight any passage above to comment on it.