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public:bggrbinfo [2019/02/16 01:02] bruce [Synchrotron Emission Mechanism Theory (Encoded information in self-absorption frequency)] |
public:bggrbinfo [2023/09/12 12:04] (current) bruce [X-rays] |
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^GRB^Comment^ | ^GRB^Comment^ | ||
|080319b| **Prototype? | |080319b| **Prototype? | ||
- | |11025A|**Prototype? | + | |110205A|**Prototype? |
|130427A|Largest E_ISO ever measured; 5.65e54 | |130427A|Largest E_ISO ever measured; 5.65e54 | ||
|130603B| - short, Bright burst| | |130603B| - short, Bright burst| | ||
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|160625B|**Prototype? | |160625B|**Prototype? | ||
|GW170817| Short-GRB observed in LIGO/VIRGO, confirming for the first time NS inspiral model| | |GW170817| Short-GRB observed in LIGO/VIRGO, confirming for the first time NS inspiral model| | ||
- | |190114C| brightest LAT event ever; detected by MAGIC at > 300 GeV GCN 23701; z=0.425| | + | |190114C| brightest LAT event ever; detected by MAGIC at > 300 GeV GCN 23701, intepreted as evidence for IC in GRB (Veres, P. 2019 Nature 575,459); z=0.425| |
===== Z>6 list of GRB ===== | ===== Z>6 list of GRB ===== | ||
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*general-grb> | *general-grb> | ||
+ | |||
+ | *general-grb> | ||
+ | |||
+ | ===== Fundamentals - GRBs are beamed - The Inverse Compton Catastrophe ===== | ||
+ | |||
+ | |||
+ | There is a lot to this. There is an old standard radio astro thing called the Inverse Compton Catastrophe - that is that if Tb > 1e12K, a radio source , given equipartition of particle and mag energy, will radiate all its energy away in the X-rays in days, because so many electrons will be upscattered, | ||
+ | |||
+ | The paper Readhead 94, ApJ 426,51 " | ||
+ | |||
+ | He also notes that there are brightness temp.s estimated by variability time - because the timescale for the e- to "poop out" is a function of Tb. This drops rapidly with Tb = 1e11K; intra-day variability implies Tb ~ 1e12k at high radio freq; ~ 1e13k at low. Tb measured by interferometer is limited by the resolution; vblty time I think is more sensitive or allows higher. | ||
+ | |||
+ | Conclusion: Very high Tb will scatter electrons to very high energies, and the vblty time scale will be very, very short, and requires constant energy injection. | ||
+ | |||
+ | I think there is another issue of pair production opacity, I did not see it in that paper. | ||
+ | |||
+ | keywords: Inverse Compton Catastrophe, | ||
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GRBs are often modeled as Band Functions - high-E and low-E power laws, but high-E is > 100 keV (for Fermi to observe) | GRBs are often modeled as Band Functions - high-E and low-E power laws, but high-E is > 100 keV (for Fermi to observe) | ||
+ | |||
+ | |||
+ | Here is four years of GBM data BEST FIT N(E) slopes, a, such that log slopes = 1+a. NOTE that the figure is labeled " | ||
+ | |||
+ | {{: | ||
+ | |||
+ | |||
+ | |||
+ | |||
Nava, L et al. 2010 arXiv: 1004.1410 http:// | Nava, L et al. 2010 arXiv: 1004.1410 http:// | ||
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=== Alternative Classifications to the Short vs. Long Classification Scheme: === | === Alternative Classifications to the Short vs. Long Classification Scheme: === | ||
+ | |||
+ | At the GRB50 meeting there was a lot of talk of long GRBs apparently with Knovae, longs with no SNe, etc. So the distinction is not that clear. | ||
+ | |||
+ | Here is a Girlanda paper asking if they are so different: https:// | ||
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To understand the various spectral components and the theoretical slopes, please see the section on [[public: | To understand the various spectral components and the theoretical slopes, please see the section on [[public: | ||
- | GRB 110205A: http:// | + | ==== GRB 110205A |
+ | |||
+ | GRB 110205A was a 200 s duration GRB from z=2.2 that has really good data. | ||
+ | |||
+ | http:// | ||
+ | |||
+ | ==== GROND Prompt Measurement (but long delayed) ==== | ||
+ | |||
+ | Eliot+13 | ||
+ | |||
+ | Listen to this incredibly useful summary from abstract, "Only in a handful of cases has it been possible obtain simultaneous coverage of the prompt emission in a multi-wavelength regime (gamma-ray to optical), as a result of: observing the field by chance prior to the GRB (e.g. 080319B/ | ||
+ | |||
+ | |||
+ | ==== Other Papers ==== | ||
+ | |||
+ | |||
+ | This oddly short little paper gives a kind of list of " | ||
- | Other Papers: | ||
BIggest collected study of prompt is Kopac+13 http:// | BIggest collected study of prompt is Kopac+13 http:// | ||
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This paper http:// | This paper http:// | ||
+ | |||
+ | Later, however, [[public: | ||
+ | |||
+ | |||
+ | ===== ulGRBs - Ultralong GRBs ===== | ||
+ | |||
+ | GRB 111209a had a duratino of at least 7 hours. It had been proposed as a magneter powered SNe. The debate rages on as to whether or not UlGRBs are the tail of lGRBs or a separate class. | ||
+ | |||
+ | Boer+15 https:// | ||
+ | |||
+ | |||
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There is also a very brief section mapping observations to theory. This is important in measurement of the BLF. | There is also a very brief section mapping observations to theory. This is important in measurement of the BLF. | ||
- | == Correlations (possibly with z) == | ||
- | The Amati, Ghirlanda, and Yonetoku relations are the most famous. | + | ====== high-z GRB ====== |
- | + | ||
- | Kocevski11: | + | |
- | + | ||
- | Shahmoradi& | + | |
- | + | ||
- | And again, http:// | + | |
- | + | ||
- | + | ||
- | ''' | + | |
- | + | ||
- | The paper above is supposedly based on the exhaustive analysis of Margutti, R. 12+ arXiv: | + | |
- | == high-z GRB == | ||
Photo-z analysis suggests z~9.4 for GRB 090429B --- http:// | Photo-z analysis suggests z~9.4 for GRB 090429B --- http:// | ||
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Ellis& | Ellis& | ||
- | == HECR_associated_with_GRB == | + | ====== HECR_associated_with_GRB ====== |
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Spectra: | Spectra: | ||
Mostly GRB have BAND function spectra, which can only sort-of be explained by a synchrotron emission mechanism. However, optical never quite fits these predictions. **ELIMINATED: | Mostly GRB have BAND function spectra, which can only sort-of be explained by a synchrotron emission mechanism. However, optical never quite fits these predictions. **ELIMINATED: | ||
+ | |||
+ | |||
+ | ===== Emission Time Evolution ===== | ||
+ | |||
+ | Of course prompt may be dominant in early emission but there could be evolution and phases of emission. | ||
+ | |||
+ | Lots of GRB are dominated by Reverse Shock, especially in the optical, rather than forward shock. This is most noticeable by smooth and round light curve structure, rather than spiky 980123b like light curve structure. | ||
+ | |||
+ | IN GRB 160625B. Nat Astron 2, 69–75 (2018). https:// | ||
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{{: | {{: | ||
+ | |||
+ | ===== Inverse Compton Emission ===== | ||
+ | |||
+ | |||
+ | This paper, on IC in prompt GRB emission, | ||
+ | https:// | ||
+ | abstract ends with " | ||
+ | |||
+ | The paper says that big BLF <=> adiabatic expansion dominant cooling of e-s, <=> hard LE photon spectrum <=> Observable IC. | ||
+ | |||
+ | NOTE: IC NOT YET OBSERVED IN PROMPT - 190114C MAGIC ~ 1 TeV gammas intepreted as evidence for IC in GRB, but in AFTERGLOW (Veres, P. 2019 Nature 575, | ||
+ | |||
+ | What are the prospects for observing prompt IC? What are the response times of Hess and Magic and Hawc? Apparently, Magic, HESS responds to GCNs, as I believe do all atmospheric cerenkov telescopes. | ||
+ | |||
+ | HAWC - water cherenkov, not steered, so can measure prompt! FOV ~ 15% of sky (https:// | ||
+ | |||
+ | MAGIC - steered UV/ | ||
+ | |||
+ | HESS - Stereoscopic UV/opt in Namibia, steered, one set of teles has 3.2 deg, one 5.0 deg on sky. | ||
===== Other components, multiple components, etc. ===== | ===== Other components, multiple components, etc. ===== | ||
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- | ===== Cosmology Theory with GRB ===== | + | ====== Cosmology Theory with GRB ====== |
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The paper above is supposedly based on the exhaustive analysis of Margutti, R. 12+ arXiv: | The paper above is supposedly based on the exhaustive analysis of Margutti, R. 12+ arXiv: | ||
+ | |||
+ | |||
+ | == Correlations (possibly with z) == | ||
+ | |||
+ | The Amati, Ghirlanda, and Yonetoku relations are the most famous. | ||
+ | |||
+ | Kocevski11: | ||
+ | |||
+ | Shahmoradi& | ||
+ | |||
+ | And again, http:// | ||
+ | |||
+ | |||
+ | ''' | ||
+ | |||
+ | This is one of my favorite papers because it took a " | ||
+ | |||
+ | The paper above is supposedly based on the exhaustive analysis of Margutti, R. 12+ arXiv: |