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A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated with SNe. (2) Demographics, attributes of possible subclass of nearby, ultra-low luminosity GRBs and their associates, nearby type Ib/c SNe. (3) Predicted range of GW strains, detection rate for GRB subclass

A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

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Page 1: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

A Subclass of GRBs as

Possible LIGO-2 Gravitational-Wave

Sources

Jay P. NorrisNASA/GSFC

(1) The prevalent belief structure:{Some, All?} GRBs associated with SNe.

(2) Demographics, attributes of possible subclass of nearby, ultra-low luminosity GRBs and their associates, nearby type Ib/c SNe.

(3) Predicted range of GW strains, detection rate for GRB subclass

Page 2: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

G

RB

98

04

25

S

N

19

98

bw

G

RB

03

03

29

S

N

20

03

dh

Only 20% of observed GRBs have associated redshifts:Some fraction of the remaining 80% may lie at higher

redshifts.

Obs’d SNzmax=1.77

Page 3: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

GRB-SN Belief Sparse Knowledge

Structure:

One very close ( 35 Mpc) ultra-low luminosity GRB, and one not so close ( 680 Mpc) subluminous GRB— Both manifest the presence of Type 1c SNe.

Constrained but open issue: The delay (in some cases)

TSN–TGRB<~ few days. Are the events simultaneous?

Detection of GW signal could depend on accurate knowledge of TSN or TGRB. Accurate TGRB is easy.

GW signal requires non-axisymmetric deformation (); Theoretical core collapses: ~ 10-4-10-2 to “unity”.

Is degree of non-axisymmetry related to GRB jet opening angle (via BH rotation)?

Page 4: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Figure 2. The detailed classification of SNe requires not only the identificationof specific features in the early spectra, but also the analysis of the line profiles,luminosity and spectral evolutions. (Cappellero & Turrato: astro-ph/0012455)

Page 5: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

E. Pianastro-ph/9910236

Revised BeppoSAXerror box forGRB 980425

Page 6: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated
Page 7: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Iwamoto et al.(1998):

Modeling yieldscore collapse for SN1998bw within +0.7/2 days of GRB 980425

22 days

40 days

12days

Page 8: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Young, Baron & Branch (1995)

Page 9: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

GRB 011211, z = 2.14 Reeves et al., Nature, 2001, 416

Blue-shifted X-ray lines ( 0.09); assume: jet 20º, ne ~ 1015

cm-3

GRB ejecta runs into SN shell at R ~ 1015 cm TGRB - TSN ~ 4 days

Page 10: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated
Page 11: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated
Page 12: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Matheson et al., GCN 2120; Stanek et al. (astro-ph/0304173)

Page 13: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Are there T0_SN T0_GRB delays?

SN 1998bw light curve has evidence for upturn (end of “UV breakout” ?), which would place T0_SN ~ few days before T0_GRB. Modeling: T = -2,+0.7 days

X-ray afterglow spectral analysis (GRB 011211) suggests 4-day hiatus, SN to GRB.

? Type 1c SNe light curves not well studied, and are known to vary in “width” by at least a factor of ~ 3:

Cannot gauge T0_SN accurately by comparison with SN 1998bw, especially given GRB afterglow photometry at faint magnitudes.

[Theory: T ~ 10s - hrs — Woosley et al., collapsars

T ~ ??? — van Putten, BH-torus ]

Page 14: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated
Page 15: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Core-collapse SN Explode Asymmetrically:

Images of 1987A (see S&T, Jan 2002, Wang & Wheeler)

Elemental asymmetries in (Wang et al. 2002)

SN remnants (1987A, Cas A)

Polarization in SNe: (Wang et al. 2001) Type 1a: <~ 0.3% Type II: ~ 1-2%, increasing with time Type 1b/c: ~ 3-7%

{GRB observed by RHESSI — Coburn & Boggs, Nature}

Some GRBs beamed into 4/[~500/2], (Frail et al. 2002)

SN Modeling — strong polar ejections

Pulsar space velocities

Some SNe are rapidly rotating at core-collapse, high T/W.

Non-axisymmetric (bar) instabilities possible, <~ unity.

Page 16: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

A Sub-Population of “Nearby” GRBs ?

BATSE subsample (~ 7%) of soft-spectrum GRBs. Defining characteristic: Very long pulses with long spectral lags (> 0.3 s).

*** Proportion increases to ~ 50% near BATSE threshold. ***

Additional Evidence for Nearby Spatial Distribution:

GRB980425/SN1998bw is canonical example, at 38

Mpc.

Log N—Log Fp has ~ -3/2 slope: cosmology

unimportant. Tendency towards Supergalactic Plane, similar to

SN Ib/c; long-lag GRB and nearby galaxy sky

distributions similar.

Implications: Detected sample, d <~ 100 Mpc. Ultra-

low luminosity (<~ 1048 ergs s-1). Rate: RGRB ~ ¼ RSN

Ib/c

*** Could be LIGO II sources: ~ 4 yr-1 within 50 Mpc

***

(see ApJ 2002, 579, 386)

Page 17: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

> 300 keV

: blue100-300 keV: green 50- 100 keV: yellow 25- 50 keV: red

“Typical” long-lag GRB, detected by BATSE.

Page 18: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

HETE-2 time profile for GRB 030329, 5-120 keV

Page 19: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated
Page 20: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

A Main Sequence “HR Diagram for Gamma-Ray Bursts”

L53 ≈ 1.1 (lag/0.01 s)-1.15

970228

000131

991216

030329Prediction:

Woosley & MacFadyen (1999), Ioka & Nakamura (2001), others predicted subclass of numerous, nearby GRBs: low luminosity, soft-spectrum, long-lag.Properties attributed to: (1) large jet opening angle & (2) low ~ 2-5.

Page 21: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

M. J. Hudson (1993)

7200 km/s100 Mpcz = 0.024

Page 22: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Virgo

980425971208

Page 23: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

SNe Ib/Ic : 62 detected 1954-2001.75,

(> 2/3 since 1998.0)

With 85% at distances < 100 Mpc.

Only ~10% of “nearby” SNe are detected.

Page 24: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

RGRB (< 100 Mpc) ~ 30 yr-1 ~ ¼ RSNIb/c

Page 25: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Fryer, Holz & Hughes

(2002);

Blondin, Mezzacappa & DeMarino (2003) :

Bar instabilities likely

( ~ unity).

Assuming 100 cycles,

f ~ 200-800 Hz,

source < 50 Mpc

h/Hz ~ 1.3 10-23

Expect ~ 4 long-lag

GRBs yr-1 (< 50

Mpc),

and we know when

they occur.

50 Mpc

680 Mpc

Page 26: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Summary

Very good evidence that high-mass, highly energetic core-

collapse SNe are associated with GRBs — one nearby, a

few cosmologically distant examples of such associations.

Evidence indicates that these SNe and GRB events are

asymmetric ( high T/W). Are SN and GRB simultaneous?

Long-lag, soft-spectrum, apparently nearby, ultra low-

luminosity GRBs are numerous (~ 50%) near BATSE

threshold.

RGRB (<100 Mpc) ~ 30/yr ~ ¼ RSNIb/c.

A few yr-1 detectable by LIGO II.

Swift should see a larger fraction of “long-lag” GRBs than

BATSE.

Many chances to find the associated SNe and GW

signals !!!

Page 27: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

The End

Page 28: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

G.M. Harry et al.

Page 29: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

jet varies, view varies, view varies,

~ 2–20. outside jet cone. inside profiled jet.

Lmin

Lmax

Beaming Fraction Viewing angle Profiled jet

4 Ld ~ constant, Special Relativity: L() reflects ():

L-1. Lorentz contraction 30 < () < 1000

& Doppler boost (jet fastest on axis)

All three models realize broad observed, butnarrow actual Luminosity and Energy distributions.

v,max v,min

jet

L ~ const.across jet

Page 30: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated
Page 31: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated
Page 32: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

GRB “Pulse Paradigm”

GRBs : LGRBs : Lpeakpeak vs. vs. GRBs : LGRBs : Lpeakpeak vs. vs.

Page 33: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

GRBs : LGRBs : Lpeakpeak vs. vs. GRBs : LGRBs : Lpeakpeak vs. vs.

CCFLag

Time

Page 34: A Subclass of GRBs as Possible LIGO-2 Gravitational-Wave Sources Jay P. Norris NASA/GSFC (1) The prevalent belief structure: {Some, All?} GRBs associated

Possible Confirmation Approaches

(1) Untriggered BATSE bursts: For Fp < 0.25 ph cm-2

s-1 long-lag bursts predominate. But, larger localization errors; ID’ing as bona fide GRBs is problematic.

(2) ~ 400-500 additional triggered BATSE bursts.

(3) Cross-correlation of nearby matter distribution (d < 100 Mpc) and GRB positions (M. Hudson).

(4) Extrapolation of SNe light curves to T0,

comparison with GRB times and positions (J. Bonnell).

(5) Swift