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Uncertainties beyond 10-100TeV of Gamma ray & CR phenomena : 「QG effects on the detection method etc.」 by T. Kifune
10-100 TeV 以上の ガンマ線には 通常・従来の検出方法を 適用できない The usual / conventional method of detecting gamma rays can not be applied to gamma rays beyond 10 -100 Tev .
Some comments ………. • Relative Delay time = -5.5 ±10.9 ±10.3 [sec TeV-1] HESS Beijing 2011, Bolmont et al. PKS 2155-304, z=0.116, d = 1.4×109 [ly] = 4.2×1016 [light sec]
M > 2.1×1027 eV = 0.6 Mplanck
• Modified p-E relation
• Systematic errors
emission time within (1-10) second Emission size within 1010-11 cm
2
3
42222
cM
EcmEcP
)10TeV1
E1(c)
Mc
E1(c
dP
dEv 16
2
]c/eV[102.1G2
hcMM 228
PL
Some comments ………. • Relative Delay time = -5.5 ±10.9 ±10.3 [sec TeV-1] HESS Beijing 2011, Bolmont et al. PKS 2155-304, z=0.116, d = 1.4×109 [ly] = 4.2×1016 [light sec]
M > 2.1×1027 eV = 0.6 Mplanck
• Modified p-E relation
• Systematic errors
emission time within (1-10) second Emission size within 1010-11 cm
2
3
42222
cM
EcmEcP
)10TeV1
E1(c)
Mc
E1(c
dP
dEv 16
2
]c/eV[102.1G2
hcMM 228
PL
OPERA Oscillation Project with Emulsion-tRacking Apparatus, CERN CNGS1
d = 7.3×107cm=2.4×10 -3 sec Delay time = 60.7 ±6.9 ±7.4 [nsec] (v –c)/ c = (2.4 ±0.28 ±0.30) ×10 -5
相対論(量子重力理論)の高精度検証
宇宙の構成物の大きさ・質量・密度 長さ:大きさ L
質量 M
原子
惑星 隕石
人間
細菌
分子
銀河
恒星
-30 -20 -10 0 10 20 30
30
-30
0
Log L[m]
Log M[kg]
ブラックホール
電子
コンプトン波長
λ = h/MC
シュワルツシルト半径
R = GM/c2
中性子星
陽子
Planck mass
臨界密度 ρc = 3H02/(8πG)
= 2×10-26[kg/m3]
Log E [eV] 1012 1020 1028 Mc2
Quantum gravity ?
不確定性原理
paticles GUT Super Symmetry cosmos
Quantum Gravity effect on VHE gamma ray astrophysics
1.Propagation 2.Emission 3.Detection
Effect on propagation speed : ● systematic error ??
● higher gamma ray energy ……..
Effects on astrophysical reactions :
yes /no type test/observation
γ + ε (EBL) e++e-
e + ε (EBL) e+ γ
absorption
A : atmospheric nucleus γ + A e++e- + A
e + A e+ γ + A
Inverse Compton
Cascade, Air shower process
Interaction with atmosphere
γ + ε (EBL) e++e- Absorption
Pair creation k0 – ε p+ + p- K0 + ε E+ + E-
Momentum / energy conservation
Energy / momentum of EBL photon
?? term of ξ K2/Mplanck ??
Effect of
ε≄0 for the process to proceed
γ + ε (EBL) e++e- (absorption)
Energy : K0 +ε = E1 + E2 momentum : k0 – ε = p1 + p2 k0 - ε =K0(1+ξK/M)
0.5 - ε p1 = E1 (1-me
2/E12
+ξE1/M)0.5
p2 = E2 (1-me2/E2
2 +ξE2/M)
0.5
Threshold energy, phase volume, …..
ε≄0 for the process to proceed
Relativistic approximation QG modification
γ + ε (EBL) e++e-
M2
EEKm
EE2
K2
2
2
2
1
2
02
e
21
0
K0 - ε + ξK02/(2M)
= p1 + p2 - p1 θ12/2 - p2 θ2
2/2 < p1 + p2 < E1+ E2 – Km
2/(2E1E2) +ξ(E1
2+E12)/(2M)
Perpendicular component
1012 1013 1014 1015 1016
1
0.1
0.01
K0 (eV)
ε0 (
eV
)
ε0 K0 = me2
prohibited
0.001
(1)
(1) (2) (2) (3) (3)
all
M2
EEKm
EE2
K2
2
2
2
1
2
02
e
21
0
M
)a1(a2Km
)a1(aK
14
2
02
e
0
左辺 > 右辺第1項
左辺 > 右辺第2項
右辺第1項 ≈ 右辺第2項
0
1
K
Ea
0
10
0
2
K
EK
K
Ea1
threshold
prohibition /suppression of large K0
characteristic energy “asymmetric parameter “a
characteristic /critical energies
eV10)M
m( 23/1
4
e
c
eV10)Mm(K 133/12ec
eV10eV1
)M(K 142/1*
x
Infra Red
10-100 TeV
1
0.5
K0
a Allowed prohibited
0
me2/ ε0
Q R
(8ε0M)1/ 2
(4ε0M)1/ 2
[case I]
[case II]
P
γ + ε (EBL) e++e-
Inverse Compton
scattering
Energy : E0 + ε = E + K
momentum : p0 - ε = p + k
e + ε (EBL) e+ γ
M
)b1(bEm
)b1(E2
b2
M2
KEEm
EE2
K2
2
02
e
0
222
02
e
0
b=K/E0
1
0.5
E0
b
Allowed
Prohibited
0 (8ε0M)
1/ 2
Q
me2/ (4ε0)
P
R
e + ε (EBL) e+ γ
e + ε (EBL) e+ γ
M
)b1(bEm
)b1(E2
b2
M2
KEEm
EE2
K2
2
02
e
0
222
02
e
0
b=K/E0
Mm
E21
1)
m
E(4K
m
E4E
E4m
E4K
2
e
3
0
2
e
o
2
e
2
0
0
0
2
e
0
IC/synchrotron radiation
1
E0
Q
(8 ε0 M)1/2
Allowed
Prohibited
0
0.5
(me2 M/2 )1/3
me2/(4 ε0)
b
P
R
e + ε (EBL) e+ γ synchrotron radiation
Effects on interaction/process
• Prohibition of reaction
• Suppression
• Asymmetric energy partition
for final particles
(εM)1/2
(me2M)1/3
γ + ε (EBL) e- + e+
M
KAmK4
2
2
e0
0a=E1/K0
A=1/(a(1-a))
AM2Km4
A0
2
e
Asymmetric energy partition
4
e
32
0
m
M2A
M2
K
M4Km4
A0
2
e
Left > 1 st or 2 nd term of right side
1 st ¥ge 2 nd term of right side
3
13
0
2
e
3
0 )10
K(4.0
Mm
KA 2/3
13
0
2
e
3
0 )10
K(9.0
Mm
K2A
From Rene Ong’s talk
e-e+ pair creation bremsstrahlung
momentum : k - ε = p1 + p2
γ + γb (EBL) e++e-
M2
EEKm
EE2
Kq
2
2
2
1
2
02
e
21
0
γ + A e++e- + A
momentum : k = p1 + p2 + Δq
ε Δq k
ε = Δq
Gamma ray proton
1
0.5
K0
a Allowed prohibited
0
me2/ ε0
Q R
(8ε0M)1/ 2
(4ε0M)1/ 2
[case I]
[case II]
P
γ + ε (EBL) e++e-
Asymmetric pairs
Detection altitude
!?
M2
EEEKm
E
Km
EE
)EK(KmK2
2
A
2
2
2
1
2
02
A
A
02
e
21
A00
A0
γ + A e++e- + A
momentum : k = p1 + p2 + pA
The case of all particles are
relativistic
k ε -> Δq
E1 K0 or E2 K0 or EA K0
favored
● Slow development of EAS Penetrating deeper to the bottom of atmosphere ● High altitudes -- sea level ? At least, it is necessary to compare the results at different altitudes
● Proton-like shower……. muon content ? width, concentration …….
Gamma-ray initiated Extensive Air Shower ?
Adding some words onto a slide from Rene Ong’s
Crimea
Not muon poor !?
Time variable Recently detected by Fermi
summary • Extragalactic gamma ray of 1014 – 1015 eV We badly need
clear evidence for quantum gravity effect gamma rays from nearby galaxies CR physics • Suppression of IC, synchrotron radiation for E0 > 10
13 – 1014 eV
SSC model lepton/hadron model.. ..
• Detection method ? Are we driving a right vehicle along the paved road / right road ? toward the destination we are heading for ? • Many other effects ……….. • Prospect for gamma ray astronomy/CR physics will be dramatically changed