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Long Duration High Energy Transients Long Duration High Energy Transients

Long Duration High Energy Transients - PowerPoint Presentation

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Long Duration High Energy Transients - PPT Presentation

S R Kulkarni An interlude compactness problem From saris talk circa 2000 Energy We measure F10 6 ergcm 2 Cosmological D 10 28 cm E 4 D 2 F 10 51 erg ID: 511808

relativistic amp 100 energy amp relativistic energy 100 object duration long erg eph 1000 data motion time lithwick 1015 disruption triggers

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Slide1

Long Duration High Energy Transients

S. R. KulkarniSlide2

An interlude – compactness problemSlide3

From sari’s talk (circa 2000)Slide4

Energy

We measure F~10

-6

erg/cm

2

Cosmological: D ~ 10

28

cm

E =

4

D

2

F ~ 10

51

ergSlide5
Slide6

Temporal Variability

dT<1s, T~100

N=T/dT>100Slide7

Implications of short timescale

dt=R/c

R/cSlide8

dT ~ 1ms

R < 3•10

7

cm

E ~ 10

51

ergs

10

57

photons

high photon density

(many above 500 keV).

Optical depth

T

n R~

10

15>>1

Inconsistent with the non thermal spectrum!

COMPACTNESS PROBLEM

g + g

 e+ + e

-

Spectrum:

Optically thin

Size & Energy:

Optically thick

? Paradox ?Slide9

A

C

B

D

R

R

R

~1/

Relativistic

Time-Scales

t

B

-t

A

~ R (1-

) / c ~ R/2

2

c

t

C

-t

A

~ R(1-

cos )/c ~ R/2

2

c

t

D

-t

A

~

/cSlide10

Due to Relativistic Motion

R =

g

2

c dT

E

ph

(emitted) = E

ph

(obs) /

g

t

gg

=

g

-(4+2a)

n

s

T

R ~ 10

15

/g

4+2a (Goodman; Paczynski; Krolik & Pier; Fenimore; Woods & Loeb; Piran & Shemi; Lithwick & RS 01)

g

> 100

The Solution:

Relativistic MotionSlide11

Relativistic Motion

(Lithwick & RS 2001)Slide12

References

F. J.

Virigili

et al. 2013 (

ApJ

778)

A. J.

Levan

et al. 2013 (

astroph

)Slide13

GRB091024A

z

=1.09Slide14
Slide15
Slide16
Slide17
Slide18

Lorentz Factor -

g

Einstein theory of relativity

g

measures how close to the speed of light an object is moving.

Determines how slowly time evolves

Determines the beaming angle

Examples:

g=3

v=95% c

g=10

v=99.5% c

g=100

v=99.995% c

g=1000 v=99.99995% c

Speed of light

GRBsSlide19

Nuclear sources?Slide20

Need a long lived engine

Collapsar

model: What determines the duration of the engine?

Tidal Disruption Event

Long duration nicely explained

Magnetar

powered?Slide21

Tidal Disruption Flare?Slide22

Movie!Slide23

Grand OverviewSlide24

Observational difficulties

Most GRB missions work on “triggers” – spikes of emission

Such events are best seen in “imaging triggers”

But satellite must be pointed to the same piece of sky for 1000

s

(not the case with Swift)

I wonder how well has the BAT data been analyzed for such objects (or for that matter WFC data)Slide25

Tests

Does the object coincide with the nucleus?

Is there a 1998bw-like supernova associated with the object?

What is the total energy loss? (relative to say 10

52

erg)