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ECL17 - EXPLORING THE ENERGETIC UNIVERSE 2017
Università degli Studi di Roma "La Sapienza"
Piazzale Aldo Moro 5, Roma 00185 Italia
THE FIRESHELL MODEL NOMENCLATURE:
SUBCLASS OF SHORT GAMMA-RAY BURSTS
Yerlan Aimuratov
International Center for Relativistic Astrophysics Network
Piazza della Repubblica 10, Pescara 65122 Italia
output
• motivation and review
• phenomenology as way of research
• fireshell model and subclasses
• prototype of short GRB in fireshell model
• x-ray and GeV emission
• GRB 081024B and GRB 140402A
The fireshell model nomenclature: subclass of short gamma-ray bursts
bimodal distribution (Kouveliotou+ 1993)
Motivation and review 1/34
bimodal as hardness ratio vs T90
Motivation and review 2/34
Epeak-Eiso relation (Amati 2006) for long GRBs
Epeak-Eiso relation 3/34
Epeak-Eiso relation (Zhang+ 2012) for short GRBs
Epeak-Eiso relation 4/34
output
• motivation and review
• phenomenology as way of research
• fireshell model and subclasses
• prototype of short GRB in fireshell model
• x-ray and GeV emission
• GRB 081024B and GRB 140402A
The fireshell model nomenclature: subclass of short gamma-ray bursts
Epeak-Eiso relation (Zhang+ 2012) for short GRBs
Phenomenology as way of research 5/34
Epeak-Eiso relation (Zhang+ 2012) for short GRBs
Phenomenology as way of research 5/34
Epeak-Eiso relation (Zhang+ 2012) for short GRBs
Phenomenology as way of research 5/34
output
• motivation and review
• phenomenology as way of research
• fireshell model and subclasses
• prototype of short GRB in fireshell model
• x-ray and GeV emission
• GRB 081024B and GRB 140402A
The fireshell model nomenclature: subclass of short gamma-ray bursts
fireshell model scenario
Fireshell model and subclasses 6/34
fireshell model
Fireshell model and subclasses 7/34
nomenclature of fireshell model
The fireshell model nomenclature: GRB subclasses 8/34
evolutionary scheme by fireshell model
The fireshell model nomenclature: GRB evolutionary scheme 9/34
nomenclature of fireshell model
The fireshell model nomenclature: GRB subclasses 10/34
nomenclature of fireshell model
The fireshell model nomenclature: GRB subclasses 10/34
evolutionary scenario by fireshell model
- optically thick e+/- plasma with energy
E+/-
tot forms in the gravitational collapse
into BH [1]
- the fireshell engulfs the baryons
B=MBc2/E+/-
tot left over in the process of
collapse and thermalizes with baryons
- the surface of e+/- self-accelerates to
ultra-relativistic velocities up to the
transparency and the emission of
Proper-GRB
- after transparency shell slows down
by collisions with the CircumBurst
Medium (CBM) giving rise to Prompt
emission. CBM is modeled by filling
factor R=Aeff /Avis which takes into
account filamentary structures of the
medium [2-4][10] Damour & Ruffini 1975, Phys. Ref. Letters (35) 463
[11-13] Ruffini et al. 2001, ApJ (555) L 111, L 113, L 117
The fireshell model nomenclature: GRB evolutionary scenario 11/34
short gamma-ray bursts evolution tree
Recently we proposed [5] the
existence of two families of short
GRBs, both originating from NS
mergers:
- family-1 short bursts with Eiso<1052
erg and rest-frame spectral peak
energy Epeak<2 MeV, leading to a
massive Neutron Star (NS) as the
merged core
- family-2 short bursts with Eiso>1052
erg and Epeak>2 MeV, leading to a
Black Hole as merged core. High-
energy emission is explained by
existing of accretion disk near the BH
The fireshell model nomenclature: GRB evolutionary scenario 12/34
[19] Ruffini et al. 2015 ApJ 808, 190R
output
• motivation and review
• phenomenology as way of research
• fireshell model and subclasses
• prototype of short GRB in fireshell model
• x-ray and GeV emission
• GRB 081024B and GRB 140402A
The fireshell model nomenclature: subclass of short gamma-ray bursts
GRB 090227B as prototype
Prototype of short GRB in fireshell model 13/34
GRB 090227B as prototype
Prototype of short GRB in fireshell model 14/34
GRB 090227B on Epeak-Eiso relation diagram
Prototype of short GRB in fireshell model 15/34
GRB 090227B on Epeak-Eiso relation diagram
Prototype of short GRB in fireshell model 15/34
GRB 140619B analysis
Prototype of short GRB in fireshell model 16/34
GRB 140619B analysis
Prototype of short GRB in fireshell model 17/34
GRB 140619B as S-GRB and GeV emission
Prototype of short GRB in fireshell model 18/34
output
• motivation and review
• phenomenology as way of research
• fireshell model and subclasses
• prototype of short GRB in fireshell model
• X-ray and GeV emission
• GRB 081024B and GRB 140402A
The fireshell model nomenclature: subclass of short gamma-ray bursts
x-ray and GeV emission of short GRBs
X-ray and GeV emission 19/34
x-ray and GeV emission of short GRBs
X-ray and GeV emission 19/34
x-ray and GeV emission of short GRBs
X-ray and GeV emission 19/34
x-ray and GeV emission of short GRBs
X-ray and GeV emission 19/34
nomenclature of fireshell model
The fireshell model nomenclature: GRB subclasses 20/34
short gamma-ray bursts evolution tree
Recently we proposed [5] the
existence of two families of short
GRBs, both originating from NS
mergers:
- family-1 short bursts with Eiso<1052
erg and rest-frame spectral peak
energy Epeak<2 MeV, leading to a
massive Neutron Star (NS) as the
merged core
- family-2 short bursts with Eiso>1052
erg and Epeak>2 MeV, leading to a
Black Hole as merged core. High-
energy emission is explained by
existing of accretion disk near the BH
The fireshell model nomenclature: GRB evolutionary scenario 21/34
[19] Ruffini et al. 2015 ApJ 808, 190R
output
• motivation and review
• phenomenology as way of research
• fireshell model and subclasses
• prototype of short GRB in fireshell model
• X-ray and GeV emission
• GRB 081024B and GRB 140402A
The fireshell model nomenclature: subclass of short gamma-ray bursts
GRB 140402A: time-integrated analysis
The subclass of short gamma-ray bursts: 140402A 22/34
GRB 140402A: time-integrated analysis
The subclass of short gamma-ray bursts: 140402A 23/34
GRB 140402A: time-resolved analysis (P-GRB)
The subclass of short gamma-ray bursts: 140402A 23/34
GRB 140402A: time-resolved analysis (P-GRB)
The subclass of short gamma-ray bursts: 140402A 24/34
GRB 140402A: time-resolved analysis (Prompt)
The subclass of short gamma-ray bursts: 140402A 25/34
GRB 140402A: time-resolved analysis (Prompt)
The subclass of short gamma-ray bursts: 140402A 26/34
theoretical estimation of the redshift
Figure: parameters at transparency radius
for selected values of E+/-
tot
keV
E
kT peak
obs )0.1742.335(
92.3

The subclass of short gamma-ray bursts: 140402A 27/34
  52.511 
obs
theor
obstheor
kT
kT
zkTzkT
 
 





 1000
10
)1/(10000
)1/(1
90
902
1
4
EdEEN
EdEEN
F
z
t
dE
z
z
liso 
N(E) – photon spectrum
E – energy channel
[13] Ruffini et al. 2001 ApJ 555, L113 [19] Ruffini et al. 2015 ApJ 808, 190 [9] Muccino et al. 2013 ApJ 763, 125
)%1654(
)1/(4
)1/(4
2
2



 
 tot
BB
tottotl
GRBPBBl
tot
ee
GRBP
S
S
ztFd
ztFd
E
E


Output of the fitting provides us with following parameters:
- energy and time intervals
- energy fluxes
- Epeak
theoretical estimation of the redshift
The procedure:
- using the simulation and varying the values of E+/-
tot and B during the selection we found
the best fit to energy ratio of P-GRB and T90.
- peak energy Epeak is used for derivation of observed temperature kTobs
- simulation provided with fireshell temperature at transparency kTtheor by using which
redshift z was calculated
- by using redshift the isotropic energy was calculated
Redshift was estimated as z=5.52+/-0.93 and correspondingly Eiso = 4.7x1052 erg and B = 3.6x10-5
 BEtot
ee
,







 
theor
iso
GRBP
kT
E
E
, 





 z
kT
kT
obs
theor
1
 
 





 1000
10
)1/(10000
)1/(1
90
902
1
4
EdEEN
EdEEN
F
z
t
dE
z
z
liso 
The subclass of short gamma-ray bursts: 140402A 28/34
[13] Ruffini et al. 2001 ApJ 555, L113 [19] Ruffini et al. 2015 ApJ 808, 190 [9] Muccino et al. 2013 ApJ 763, 125
GRB 081024B
The subclass of short gamma-ray bursts: 081024B 29/34
GRB 081024B
The subclass of short gamma-ray bursts: 081024B 30/34
Consistency with observation
isoGRBP
iso
EE
z
B
ergE
)%2650()%2650(
)82.112.3(
10)8.26.4(
10)00.164.2(
5
52






[9] Muccino et al. 2013 ApJ 763, 125 [7] Zhang et al. 2012 ApJ 750, 88 [8] Calderone et al. 2015 MNRAS 448, 403
The subclass of short gamma-ray bursts: 081024B 31/34
GRB 140402A and subclass of S-GRBs
The fireshell model nomenclature: GRB subclasses 32/34
Figure: Epeak-Eiso relation and Family-2 short bursts [5]
[20] Ruffini et al. 2016 ApJ 832, 136 [7] Zhang et al. 2012 ApJ 750, 88 [8] Calderone et al. 2015 MNRAS 448, 403
GeV emission for subclass of S-GRBs
The fireshell model nomenclature: GRB subclasses 33/34
[21] Aimuratov et al. 2017 ApJ 844, 83 [22] Ruffini & Wheeler 1969
GeV emission for subclass of S-GRBs
The fireshell model nomenclature: GRB subclasses 33/34
[21] Aimuratov et al. 2017 ApJ 844, 83 [22] Ruffini & Wheeler 1969
x-ray afterglow upperlimits for short GRBs
The fireshell model nomenclature: GRB subclasses 34/34
[21] Aimuratov et al. 2017 ApJ 844, 83
conclusion
• We implemented a detailed analysis of the sources GRB 081024B and GRB
140402A within the fireshell model
• It was found that not all Short GRBs are able to produce GeV emission and its
production is supposed to be associated with accretion of the remnant mass onto
a Black Hole with an output being a relativistic jet
• The absence of an XRT detection after a short burst is not surprising.
Only in case of Swift-BAT triggering, quick response of Swift-XRT will provide us
with precise location and x-ray spectra and corresponding analysis could be done.
• Otherwise the method within the fireshell model can give a good redshift
estimation. we have derived for 081024B and 140402A respectively the redshift
z=3.12 and z=5.52, its isotropic energy Eiso=2.64x1052 and Eiso=4.7x1052 erg, and
baryon load B=4.6x10-5 andB=3.6x10-5.
• That makes possible to cross-check the ideas of phenomenological classification.
The fireshell model nomenclature: GRB evolutionary scheme
EXPLORING THE ENERGETIC UNIVERSE
Thank You for Attention!
The Fireshell Model Nomenclature:
Subclass of Short Gamma-Ray Bursts
Yerlan Aimuratov
evolutionary scheme by fireshell model
The fireshell model nomenclature: GRB evolutionary scheme 16/31
bimodal distribution (Kouveliotou+ 1993)
Bimodal distribution 2/31
Epeak-Eiso relation (Zhang+ 2012) for short GRBs
Epeak-Eiso relation 11/31
other phenomenological distributions
(Margutti+ 2013; Dainotti+ 2008; Bernardini+ 2012)
Other phenomenological distributions 12/31
other phenomenological distributions
(Margutti+ 2013; Dainotti+ 2008; Bernardini+ 2012)
Other phenomenological distributions 13/31
other phenomenological distributions
Other phenomenological distributions 14/31

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Aimuratov ecl 17

  • 1. ECL17 - EXPLORING THE ENERGETIC UNIVERSE 2017 Università degli Studi di Roma "La Sapienza" Piazzale Aldo Moro 5, Roma 00185 Italia THE FIRESHELL MODEL NOMENCLATURE: SUBCLASS OF SHORT GAMMA-RAY BURSTS Yerlan Aimuratov International Center for Relativistic Astrophysics Network Piazza della Repubblica 10, Pescara 65122 Italia
  • 2. output • motivation and review • phenomenology as way of research • fireshell model and subclasses • prototype of short GRB in fireshell model • x-ray and GeV emission • GRB 081024B and GRB 140402A The fireshell model nomenclature: subclass of short gamma-ray bursts
  • 3. bimodal distribution (Kouveliotou+ 1993) Motivation and review 1/34
  • 4. bimodal as hardness ratio vs T90 Motivation and review 2/34
  • 5. Epeak-Eiso relation (Amati 2006) for long GRBs Epeak-Eiso relation 3/34
  • 6. Epeak-Eiso relation (Zhang+ 2012) for short GRBs Epeak-Eiso relation 4/34
  • 7. output • motivation and review • phenomenology as way of research • fireshell model and subclasses • prototype of short GRB in fireshell model • x-ray and GeV emission • GRB 081024B and GRB 140402A The fireshell model nomenclature: subclass of short gamma-ray bursts
  • 8. Epeak-Eiso relation (Zhang+ 2012) for short GRBs Phenomenology as way of research 5/34
  • 9. Epeak-Eiso relation (Zhang+ 2012) for short GRBs Phenomenology as way of research 5/34
  • 10. Epeak-Eiso relation (Zhang+ 2012) for short GRBs Phenomenology as way of research 5/34
  • 11. output • motivation and review • phenomenology as way of research • fireshell model and subclasses • prototype of short GRB in fireshell model • x-ray and GeV emission • GRB 081024B and GRB 140402A The fireshell model nomenclature: subclass of short gamma-ray bursts
  • 12. fireshell model scenario Fireshell model and subclasses 6/34
  • 13. fireshell model Fireshell model and subclasses 7/34
  • 14. nomenclature of fireshell model The fireshell model nomenclature: GRB subclasses 8/34
  • 15. evolutionary scheme by fireshell model The fireshell model nomenclature: GRB evolutionary scheme 9/34
  • 16. nomenclature of fireshell model The fireshell model nomenclature: GRB subclasses 10/34
  • 17. nomenclature of fireshell model The fireshell model nomenclature: GRB subclasses 10/34
  • 18. evolutionary scenario by fireshell model - optically thick e+/- plasma with energy E+/- tot forms in the gravitational collapse into BH [1] - the fireshell engulfs the baryons B=MBc2/E+/- tot left over in the process of collapse and thermalizes with baryons - the surface of e+/- self-accelerates to ultra-relativistic velocities up to the transparency and the emission of Proper-GRB - after transparency shell slows down by collisions with the CircumBurst Medium (CBM) giving rise to Prompt emission. CBM is modeled by filling factor R=Aeff /Avis which takes into account filamentary structures of the medium [2-4][10] Damour & Ruffini 1975, Phys. Ref. Letters (35) 463 [11-13] Ruffini et al. 2001, ApJ (555) L 111, L 113, L 117 The fireshell model nomenclature: GRB evolutionary scenario 11/34
  • 19. short gamma-ray bursts evolution tree Recently we proposed [5] the existence of two families of short GRBs, both originating from NS mergers: - family-1 short bursts with Eiso<1052 erg and rest-frame spectral peak energy Epeak<2 MeV, leading to a massive Neutron Star (NS) as the merged core - family-2 short bursts with Eiso>1052 erg and Epeak>2 MeV, leading to a Black Hole as merged core. High- energy emission is explained by existing of accretion disk near the BH The fireshell model nomenclature: GRB evolutionary scenario 12/34 [19] Ruffini et al. 2015 ApJ 808, 190R
  • 20. output • motivation and review • phenomenology as way of research • fireshell model and subclasses • prototype of short GRB in fireshell model • x-ray and GeV emission • GRB 081024B and GRB 140402A The fireshell model nomenclature: subclass of short gamma-ray bursts
  • 21. GRB 090227B as prototype Prototype of short GRB in fireshell model 13/34
  • 22. GRB 090227B as prototype Prototype of short GRB in fireshell model 14/34
  • 23. GRB 090227B on Epeak-Eiso relation diagram Prototype of short GRB in fireshell model 15/34
  • 24. GRB 090227B on Epeak-Eiso relation diagram Prototype of short GRB in fireshell model 15/34
  • 25. GRB 140619B analysis Prototype of short GRB in fireshell model 16/34
  • 26. GRB 140619B analysis Prototype of short GRB in fireshell model 17/34
  • 27. GRB 140619B as S-GRB and GeV emission Prototype of short GRB in fireshell model 18/34
  • 28. output • motivation and review • phenomenology as way of research • fireshell model and subclasses • prototype of short GRB in fireshell model • X-ray and GeV emission • GRB 081024B and GRB 140402A The fireshell model nomenclature: subclass of short gamma-ray bursts
  • 29. x-ray and GeV emission of short GRBs X-ray and GeV emission 19/34
  • 30. x-ray and GeV emission of short GRBs X-ray and GeV emission 19/34
  • 31. x-ray and GeV emission of short GRBs X-ray and GeV emission 19/34
  • 32. x-ray and GeV emission of short GRBs X-ray and GeV emission 19/34
  • 33. nomenclature of fireshell model The fireshell model nomenclature: GRB subclasses 20/34
  • 34. short gamma-ray bursts evolution tree Recently we proposed [5] the existence of two families of short GRBs, both originating from NS mergers: - family-1 short bursts with Eiso<1052 erg and rest-frame spectral peak energy Epeak<2 MeV, leading to a massive Neutron Star (NS) as the merged core - family-2 short bursts with Eiso>1052 erg and Epeak>2 MeV, leading to a Black Hole as merged core. High- energy emission is explained by existing of accretion disk near the BH The fireshell model nomenclature: GRB evolutionary scenario 21/34 [19] Ruffini et al. 2015 ApJ 808, 190R
  • 35. output • motivation and review • phenomenology as way of research • fireshell model and subclasses • prototype of short GRB in fireshell model • X-ray and GeV emission • GRB 081024B and GRB 140402A The fireshell model nomenclature: subclass of short gamma-ray bursts
  • 36. GRB 140402A: time-integrated analysis The subclass of short gamma-ray bursts: 140402A 22/34
  • 37. GRB 140402A: time-integrated analysis The subclass of short gamma-ray bursts: 140402A 23/34
  • 38. GRB 140402A: time-resolved analysis (P-GRB) The subclass of short gamma-ray bursts: 140402A 23/34
  • 39. GRB 140402A: time-resolved analysis (P-GRB) The subclass of short gamma-ray bursts: 140402A 24/34
  • 40. GRB 140402A: time-resolved analysis (Prompt) The subclass of short gamma-ray bursts: 140402A 25/34
  • 41. GRB 140402A: time-resolved analysis (Prompt) The subclass of short gamma-ray bursts: 140402A 26/34
  • 42. theoretical estimation of the redshift Figure: parameters at transparency radius for selected values of E+/- tot keV E kT peak obs )0.1742.335( 92.3  The subclass of short gamma-ray bursts: 140402A 27/34   52.511  obs theor obstheor kT kT zkTzkT           1000 10 )1/(10000 )1/(1 90 902 1 4 EdEEN EdEEN F z t dE z z liso  N(E) – photon spectrum E – energy channel [13] Ruffini et al. 2001 ApJ 555, L113 [19] Ruffini et al. 2015 ApJ 808, 190 [9] Muccino et al. 2013 ApJ 763, 125 )%1654( )1/(4 )1/(4 2 2       tot BB tottotl GRBPBBl tot ee GRBP S S ztFd ztFd E E   Output of the fitting provides us with following parameters: - energy and time intervals - energy fluxes - Epeak
  • 43. theoretical estimation of the redshift The procedure: - using the simulation and varying the values of E+/- tot and B during the selection we found the best fit to energy ratio of P-GRB and T90. - peak energy Epeak is used for derivation of observed temperature kTobs - simulation provided with fireshell temperature at transparency kTtheor by using which redshift z was calculated - by using redshift the isotropic energy was calculated Redshift was estimated as z=5.52+/-0.93 and correspondingly Eiso = 4.7x1052 erg and B = 3.6x10-5  BEtot ee ,          theor iso GRBP kT E E ,        z kT kT obs theor 1           1000 10 )1/(10000 )1/(1 90 902 1 4 EdEEN EdEEN F z t dE z z liso  The subclass of short gamma-ray bursts: 140402A 28/34 [13] Ruffini et al. 2001 ApJ 555, L113 [19] Ruffini et al. 2015 ApJ 808, 190 [9] Muccino et al. 2013 ApJ 763, 125
  • 44. GRB 081024B The subclass of short gamma-ray bursts: 081024B 29/34
  • 45. GRB 081024B The subclass of short gamma-ray bursts: 081024B 30/34
  • 46. Consistency with observation isoGRBP iso EE z B ergE )%2650()%2650( )82.112.3( 10)8.26.4( 10)00.164.2( 5 52       [9] Muccino et al. 2013 ApJ 763, 125 [7] Zhang et al. 2012 ApJ 750, 88 [8] Calderone et al. 2015 MNRAS 448, 403 The subclass of short gamma-ray bursts: 081024B 31/34
  • 47. GRB 140402A and subclass of S-GRBs The fireshell model nomenclature: GRB subclasses 32/34 Figure: Epeak-Eiso relation and Family-2 short bursts [5] [20] Ruffini et al. 2016 ApJ 832, 136 [7] Zhang et al. 2012 ApJ 750, 88 [8] Calderone et al. 2015 MNRAS 448, 403
  • 48. GeV emission for subclass of S-GRBs The fireshell model nomenclature: GRB subclasses 33/34 [21] Aimuratov et al. 2017 ApJ 844, 83 [22] Ruffini & Wheeler 1969
  • 49. GeV emission for subclass of S-GRBs The fireshell model nomenclature: GRB subclasses 33/34 [21] Aimuratov et al. 2017 ApJ 844, 83 [22] Ruffini & Wheeler 1969
  • 50. x-ray afterglow upperlimits for short GRBs The fireshell model nomenclature: GRB subclasses 34/34 [21] Aimuratov et al. 2017 ApJ 844, 83
  • 51. conclusion • We implemented a detailed analysis of the sources GRB 081024B and GRB 140402A within the fireshell model • It was found that not all Short GRBs are able to produce GeV emission and its production is supposed to be associated with accretion of the remnant mass onto a Black Hole with an output being a relativistic jet • The absence of an XRT detection after a short burst is not surprising. Only in case of Swift-BAT triggering, quick response of Swift-XRT will provide us with precise location and x-ray spectra and corresponding analysis could be done. • Otherwise the method within the fireshell model can give a good redshift estimation. we have derived for 081024B and 140402A respectively the redshift z=3.12 and z=5.52, its isotropic energy Eiso=2.64x1052 and Eiso=4.7x1052 erg, and baryon load B=4.6x10-5 andB=3.6x10-5. • That makes possible to cross-check the ideas of phenomenological classification. The fireshell model nomenclature: GRB evolutionary scheme
  • 52. EXPLORING THE ENERGETIC UNIVERSE Thank You for Attention! The Fireshell Model Nomenclature: Subclass of Short Gamma-Ray Bursts Yerlan Aimuratov
  • 53. evolutionary scheme by fireshell model The fireshell model nomenclature: GRB evolutionary scheme 16/31
  • 54.
  • 55.
  • 56.
  • 57.
  • 58.
  • 59. bimodal distribution (Kouveliotou+ 1993) Bimodal distribution 2/31
  • 60. Epeak-Eiso relation (Zhang+ 2012) for short GRBs Epeak-Eiso relation 11/31
  • 61. other phenomenological distributions (Margutti+ 2013; Dainotti+ 2008; Bernardini+ 2012) Other phenomenological distributions 12/31
  • 62. other phenomenological distributions (Margutti+ 2013; Dainotti+ 2008; Bernardini+ 2012) Other phenomenological distributions 13/31
  • 63. other phenomenological distributions Other phenomenological distributions 14/31