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Tully-Fisher Relation (Rotation–Luminosity) Type Ia Supernovae HR diagram Cepheid Variable (Period–Luminosity) parallax redshift z = Cosmic Distance Ladder (Distance Indicators) When we measure the energy density of D-E and D-M, we need “distance” and “redshift” relation. Just after the Big Bang (CMB) L ≡ 4 π d L 2 F Gamma-Ray Bursts z = 8.2 ! z = 1.755
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Daisuke YONETOKU (Kanazawa Univ.) T. Murakami (Kanazawa Univ.),R. Tsutsui, T. Nakamura (Kyoto Univ.),K. Takahashi (Nagoya Univ.)
The Spectral Ep–Lp and Ep–Eiso Relations:
The Origin of Dispersion and Its Improvement
GRB Cosmology Project
102 known redshift samples with ( Ep, 1 sec peak flux, fluence ).Lp is calculated by 1 sec peak flux in the obs. frame.
νFν
∝ Eα
∝ Eβ
ピークエネルギー (Ep)
Briggs et al. 2000
■ Application for the GRB Cosmology■ Investigate the characteristic of GRB itself
Introduction
C.C. = 0.890d.o.f. = 100
Tully-Fisher Relation (Rotation–Luminosity)
Type Ia Supernovae
HR diagram
Cepheid Variable(Period–Luminosity)
parallaxredshift
z = 1.755
Cosmic Distance Ladder (Distance Indicators) When we measure the energy density of D-E and D-M,
we need “distance” and “redshift” relation.
Just after the Big B
ang (CM
B)
L ≡ 4πdL2 F
Gamma-Ray Bursts z = 8.2 !
z = 1.755
Calibrated Epeak-Luminosity relation52 GRBs ( z<1.755 )
Epeak(1+z) [keV]
Pea
k Lu
min
osity
[1051
erg
/sec
]
Lp = 5.93 x 1047 [ Epeak (1+z) ]1.85
5.93 x 1047 [ Epeak (1+z) ]1.85
4πFdL 2 =
Redshift
Lum
inos
ity D
ista
nce
(cm
)10
2610
2710
2810
29
0.01 0.1 1 10
Type Ia SNe New!GRB
CalibratedGRB
Hubble Diagram ( 1.8 < z < 8.2)■ GRB data (z < 1.755)■ GRB data (1.755 < z < 8.2)+ Type Ia SNe
(Ωm, ΩΛ) = (1, 0)
(0.3, 0.7)
(0, 1)
z = 8.2
ΩΛ
Cosmological Parameters (1.8 < z < 8.2 )D
ark
Ene
rgy
: ΩΛ
Matter : Ωm
( 0.24±0.10 , 0.76±0.10)(Ωm, ΩΛ) =
First Measurement of DM & DEin the early universe of z > 2.
Tsutsui, DY + (2009)
( flat universe )
Poster-094Tsutsui et al.
Origin of Data Dispersions
Peak Flux Redshift
We classified 102 GRB events into 3 groups,according to the bolometric peak flux and the redshift.
We found a redshift evolution in the Ep-Lp relation in 2 s significance, but there is no peak flux dependence.
Ep-Lp Ep-LpBrightMiddleDim
High-zMiddle-zLow-z
We systematically overestimate the peak luminosityfor higher redshift GRBs.
Rel
ativ
e P
eak
Flux
in O
bs. F
ram
e
Time Scale of Peak Flux (sec)
64msec512msec
1024msec
Redshift Evolution ?
1sec@ z=0
1sec@ z=1
1sec@ z=2
Original Ep – Lp
58 GRBs Konus & Swift
~ 3 sec
31 Konus data
2088 msec ~ 3 sec
Redefinition of the peak luminosity ( Lp,GRB )
We searched the best time scalefor the peak luminosity in the GRB frame.
Time Scale of Peak Luminosity in GRB Frame (sec)
Cor
rela
tion
Coe
ffici
ent
Lp = 1048.70 [ Ep(1+z) ]1.46
Deviation : σsys = 0.213
1sec Peak Luminosity ( measured in Obs. frame )
Cor. Coef = 0.890
Ep (1+z) [keV]
Pea
k Lu
min
osity
[erg
/sec
]
Lp = 1048.18 [ Ep(1+z) ]1.53
Deviation : σsys = 0.180
3sec Peak Luminosity (measured in GRB frame )
Cor. Coef = 0.921
Ep (1+z) [keV]
Pea
k Lu
min
osity
[erg
/sec
]
Fluence Redshift
Ep-Eiso Ep-Eiso
We found a fluence dependence in the Ep-Eiso relation in 2 s significance, but there is no redshift evolution.
Similar analysis for the Ep – Eiso relation.
BrightMiddleDim
High-zMiddle-zLow-z
■ We measured the cosmological parameters,
1.755 < z < 8.2( 0.24±0.10 , 0.76±0.10 )(Ωm, ΩΛ) =
■ We succeeded in extending the cosmic distance ladder toward z=8.2 with the Ep – Lp relation.
Redshift evolution
Peak Flux/Fluence Dependence
Ep – Lp Yes (2s C.L.) NoEp – Eiso No Yes (2s C.L.)
■ Possible origins of data dispersion
■ Using the NEW definition of “Lp,GRB (~ 3sec in GRB frame)”, we succeeded in canceling the redshift evolution, and in improving the Ep – Lp relation.
Summary