LHC and Astroparticle Physics — The Next High Energy Frontier · The Next High Energy Frontier...
Transcript of LHC and Astroparticle Physics — The Next High Energy Frontier · The Next High Energy Frontier...
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LHC and Astroparticle Physics
— The Next High Energy Frontier
Tao Han
University of Wisconsin – Madison
TeV Particle Astrophysics II
(August 30, 2006)
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LHC and Astroparticle Physics
— The Next High Energy Frontier
Tao Han
University of Wisconsin – Madison
TeV Particle Astrophysics II
(August 30, 2006)
Introduction to the Next HE Frontier
Physics Beyond the Standard Model
In the LHC Era
High-Energy Astroparticle Physics
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The Next High Energy Frontier
The Large Hadron Collider:
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The Next High Energy Frontier
The Large Hadron Collider:
• New threshold for new physics:√
Spp = 14 TeV, sparton = x1x2Spp
⇒ Mnew =√
sparton ∼ 0.2√
Spp ∼ 3 TeV.
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The Next High Energy Frontier
The Large Hadron Collider:
• New threshold for new physics:√
Spp = 14 TeV, sparton = x1x2Spp
⇒ Mnew =√
sparton ∼ 0.2√
Spp ∼ 3 TeV.
• Multiple channels, broad physics reach:qq′, gg, qg, bb → colored; Q = 0,±1; J = 0,1,2 states;
γγ, WW, WZ, ZZ → IW = 0,1,2; Q = 0,±1,±2; J = 0,1,2 states.
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The Next High Energy Frontier
The Large Hadron Collider:
• New threshold for new physics:√
Spp = 14 TeV, sparton = x1x2Spp
⇒ Mnew =√
sparton ∼ 0.2√
Spp ∼ 3 TeV.
• Multiple channels, broad physics reach:qq′, gg, qg, bb → colored; Q = 0,±1; J = 0,1,2 states;
γγ, WW, WZ, ZZ → IW = 0,1,2; Q = 0,±1,±2; J = 0,1,2 states.
• Higher luminosity, higher event rate:
L = 1033 − 1034 cm−2s−1 ⇒ 104 − 105 pb−1/yr.
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HE cosmic Rays by Nature’s Accelerators
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HE cosmic Rays by Nature’s Accelerators
• Cosmic rays have historically led to new particle discoveries.
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HE cosmic Rays by Nature’s Accelerators
• Cosmic rays have historically led to new particle discoveries.
• The observed high energy events extend to
Elab ≈ 1011 GeV ⇒ Ecm =√
2mNElab ≈ 500 TeV.
beyond the GZK cutoff; higher than the conceivable collider energies.
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HE cosmic Rays by Nature’s Accelerators
• Cosmic rays have historically led to new particle discoveries.
• The observed high energy events extend to
Elab ≈ 1011 GeV ⇒ Ecm =√
2mNElab ≈ 500 TeV.
beyond the GZK cutoff; higher than the conceivable collider energies.
• Variety of incoming particles:
γ, p, heavy nuclei, ν′s...
but the components not precisely known.
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HE cosmic Rays by Nature’s Accelerators
• Cosmic rays have historically led to new particle discoveries.
• The observed high energy events extend to
Elab ≈ 1011 GeV ⇒ Ecm =√
2mNElab ≈ 500 TeV.
beyond the GZK cutoff; higher than the conceivable collider energies.
• Variety of incoming particles:
γ, p, heavy nuclei, ν′s...
but the components not precisely known.
• Main drawback:The flux (or the luminosity) falls rapidly faster than E−3.
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Physics Beyond the Standard Model
The Highly successful SM:
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Physics Beyond the Standard Model
The Highly successful SM:
• SU(3)C ⊗ SU(2)L ⊗ U(1)Y ⇒ SU(3)C ⊗ U(1)em
Experimentally tested to 0.1%!
150 160 170 180 190 200m t [GeV]
80.2
80.3
80.4
80.5
80.6
MW
[GeV
]
direct (1 σ)
indirect (1 σ)
all (90% CL)
MH [GeV]10
020
040
080
0
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Physics Beyond the Standard Model
The Highly successful SM:
• SU(3)C ⊗ SU(2)L ⊗ U(1)Y ⇒ SU(3)C ⊗ U(1)em
Experimentally tested to 0.1%!
150 160 170 180 190 200m t [GeV]
80.2
80.3
80.4
80.5
80.6
MW
[GeV
]
direct (1 σ)
indirect (1 σ)
all (90% CL)
MH [GeV]10
020
040
080
0Triumph for the HEP theory and experiments!
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Higgs boson (or alike) must exist !
• Mass generation for all elementary particles
• SM renormalizability
• Partial wave unitarity mH < O(TeV)
• Indirect experimental indication mH <∼ 200 GeV
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Higgs boson (or alike) must exist !
• Mass generation for all elementary particles
• SM renormalizability
• Partial wave unitarity mH < O(TeV)
• Indirect experimental indication mH <∼ 200 GeV
A light Higgs boson is highly expected!
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Light Higgs boson is sick !
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Light Higgs boson is sick !
Quantum corrections drag m2h to ultra-violet modes ∼ Λ2.
(a) (c)(b)
t
W,B
h
hh h h
h h
tc
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Light Higgs boson is sick !
Quantum corrections drag m2h to ultra-violet modes ∼ Λ2.
(a) (c)(b)
t
W,B
h
hh h h
h h
tc
m2H = m2
H0 − 3
8π2y2t Λ
2 +1
16π2g2Λ2 +
1
16π2λ2Λ2
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Light Higgs boson is sick !
Quantum corrections drag m2h to ultra-violet modes ∼ Λ2.
(a) (c)(b)
t
W,B
h
hh h h
h h
tc
m2H = m2
H0 − 3
8π2y2t Λ
2 +1
16π2g2Λ2 +
1
16π2λ2Λ2
(200 GeV)2 = m2H0 +
[
−(2 TeV)2 + (700 GeV)2 + (500 GeV)2]
(
Λ
10 TeV
)2
.
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Light Higgs boson is sick !
Quantum corrections drag m2h to ultra-violet modes ∼ Λ2.
(a) (c)(b)
t
W,B
h
hh h h
h h
tc
m2H = m2
H0 − 3
8π2y2t Λ
2 +1
16π2g2Λ2 +
1
16π2λ2Λ2
(200 GeV)2 = m2H0 +
[
−(2 TeV)2 + (700 GeV)2 + (500 GeV)2]
(
Λ
10 TeV
)2
.
• If Λ ∼ Mpl, then 1030-digits cancellation (Anthropic principle)!
• Naturalness: less than 90% cancellation on m2h ⇒ Λ <∼ 3 TeV.
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Light Higgs boson is sick !
Quantum corrections drag m2h to ultra-violet modes ∼ Λ2.
(a) (c)(b)
t
W,B
h
hh h h
h h
tc
m2H = m2
H0 − 3
8π2y2t Λ
2 +1
16π2g2Λ2 +
1
16π2λ2Λ2
(200 GeV)2 = m2H0 +
[
−(2 TeV)2 + (700 GeV)2 + (500 GeV)2]
(
Λ
10 TeV
)2
.
• If Λ ∼ Mpl, then 1030-digits cancellation (Anthropic principle)!
• Naturalness: less than 90% cancellation on m2h ⇒ Λ <∼ 3 TeV.
Other New Physics must show up at TeV scale!
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1. Symmetry/Cancellation at work?
• Super-symmetry (SUSY) (symmetry between opposite spin & statistics)
Natural cancellations: t versus t
W versus W
H versus H
Hd versus Hu,
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1. Symmetry/Cancellation at work?
• Super-symmetry (SUSY) (symmetry between opposite spin & statistics)
Natural cancellations: t versus t
W versus W
H versus H
Hd versus Hu,
∆m2H ∼ (M2
SUSY − M2SM)
λ2f
16π2ln
(
Λ
MSUSY
)
.
Weak scale SUSY is natural if MSUSY ∼ O (1 TeV).
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1. Symmetry/Cancellation at work?
• Super-symmetry (SUSY) (symmetry between opposite spin & statistics)
Natural cancellations: t versus t
W versus W
H versus H
Hd versus Hu,
∆m2H ∼ (M2
SUSY − M2SM)
λ2f
16π2ln
(
Λ
MSUSY
)
.
Weak scale SUSY is natural if MSUSY ∼ O (1 TeV).
• The Little Higgs idea – Strongly interacting dynamics:
An alternative way to keep H light (naturally).
Again, predicting new states:
W±, Z, B ↔ W±H , ZH , BH; t ↔ T ; H ↔ Φ.
(cancellation among same spin states!)
TeV scale new dynamics needed associated with a symmetry.
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2. Low fundamental scale?
• With the help of Extra-dimensions, low-scale gravity/string theories
resolve the large hierarchy:
ADD:
tyi
x
SM
planck brane
gravity
Randall-Sundrum
Mply0
m ey0Mpl
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2. Low fundamental scale?
• With the help of Extra-dimensions, low-scale gravity/string theories
resolve the large hierarchy:
ADD:
tyi
x
SM
planck brane
gravity
Randall-Sundrum
Mply0
m ey0MplMn+2
S ∼ M2PL/Rn −→ O(1 TeV2).
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Consequently,
For R−1 <∼ E <∼ MS, march into extra-dimensions:
Kaluza-Klein (KK) states: M2n ∼ n2
k/R2;
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Consequently,
For R−1 <∼ E <∼ MS, march into extra-dimensions:
Kaluza-Klein (KK) states: M2n ∼ n2
k/R2;
For E >∼ MS, R−1, stringy effects:
String resonances: M2 ∼ nsM2S ;
Winding modes: M2n ∼ n2
wR2M4S .
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Consequently,
For R−1 <∼ E <∼ MS, march into extra-dimensions:
Kaluza-Klein (KK) states: M2n ∼ n2
k/R2;
For E >∼ MS, R−1, stringy effects:
String resonances: M2 ∼ nsM2S ;
Winding modes: M2n ∼ n2
wR2M4S .
Or other quantum gravity effects ...
⇒ testing the geometry of the extrad-dimensions!
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Consequently,
For R−1 <∼ E <∼ MS, march into extra-dimensions:
Kaluza-Klein (KK) states: M2n ∼ n2
k/R2;
For E >∼ MS, R−1, stringy effects:
String resonances: M2 ∼ nsM2S ;
Winding modes: M2n ∼ n2
wR2M4S .
Or other quantum gravity effects ...
⇒ testing the geometry of the extrad-dimensions!
For E ≫ MS, semi-classical gravity:
TeV-Scale Black Holes:
σ ≈ π r2bh,
rbh =1√
πMD
MBH
MD
8Γ(
n+32
)
n + 2
1n+1
→ MBH/M2pl in 4d
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Unification of forces ?
Do the forces E & M/Weak/Strong all unify into a single force ?
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Unification of forces ?
Do the forces E & M/Weak/Strong all unify into a single force ?
YES if there is a TeV scale new physics threshold !
0
10
20
30
40
50
60
10 10 10 10 10 10 10 10 2 4 6 8 10 12 14 16
1/α i
µ(GeV)
1
1/α
2
1/α
3
1/α
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Unification of forces ?
Do the forces E & M/Weak/Strong all unify into a single force ?
YES if there is a TeV scale new physics threshold !
0
10
20
30
40
50
60
10 10 10 10 10 10 10 10 2 4 6 8 10 12 14 16
1/α i
µ(GeV)
1
1/α
2
1/α
3
1/α
Motivation is strong for physics BSM at the TeV scale.
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Unification of forces ?
Do the forces E & M/Weak/Strong all unify into a single force ?
YES if there is a TeV scale new physics threshold !
0
10
20
30
40
50
60
10 10 10 10 10 10 10 10 2 4 6 8 10 12 14 16
1/α i
µ(GeV)
1
1/α
2
1/α
3
1/α
Motivation is strong for physics BSM at the TeV scale.
(skip extensions of gauge, SUSY; ν masse and mixing ...)
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We are entering a “data-rich” era:
B-factories (SLAC, KEK): test CP violation;
Neutrino Oscillation Experiments: Neutrino masses and mixing;
µ-magnetic moment: g − 2;
neutron/electron electric-dipole-moments ...
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We are entering a “data-rich” era:
B-factories (SLAC, KEK): test CP violation;
Neutrino Oscillation Experiments: Neutrino masses and mixing;
µ-magnetic moment: g − 2;
neutron/electron electric-dipole-moments ...
Cosmological observations: Dark matter, mν, and dark energy ...
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We are entering a “data-rich” era:
B-factories (SLAC, KEK): test CP violation;
Neutrino Oscillation Experiments: Neutrino masses and mixing;
µ-magnetic moment: g − 2;
neutron/electron electric-dipole-moments ...
Cosmological observations: Dark matter, mν, and dark energy ...
Astroparticle physics experiments:
Cosmic rays, neutrinos, dark matter, other new physics ...
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We are entering a “data-rich” era:
B-factories (SLAC, KEK): test CP violation;
Neutrino Oscillation Experiments: Neutrino masses and mixing;
µ-magnetic moment: g − 2;
neutron/electron electric-dipole-moments ...
Cosmological observations: Dark matter, mν, and dark energy ...
Astroparticle physics experiments:
Cosmic rays, neutrinos, dark matter, other new physics ...
Tevatron: (pp at 1.96 TeV, FNAL, till 2009?)
top quark, new particle searches, Higgs (?) ...
LHC: (pp at 14 TeV at CERN, 2007)
comprehensive Higgs studies, extensive new particle searches ...
ILC: (e+e− at 500 GeV − 1 TeV)
more on top quark, precision Higgs and new light particles ...
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Physics Expectations at the LHC
Major discoveries and excitement ahead ...
Feb.16, 2006: ATLAS (90m underground) CMS
(pilot run at the end of 2007.)
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LHC Event rates for various SM processes:
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LHC Event rates for various SM processes:
Annual yield: 1B W±; 100M tt; 10M W+W−; 1M H0...
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LHC Event rates for various SM processes:
Annual yield: 1B W±; 100M tt; 10M W+W−; 1M H0...
Great potential to open a new chapter of HEP !Challenge: Small signal-to-background ratio!
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Leptons(e, µ)
Photons
Taus
JetsMissing ET
y98014_416dPauss rd
H → WW→lνjjH → ZZ→lljjZZH
H→WW→lνlν
H→WW→lνlν
→ → νν
H →
Z Z
→
4 le
pton
s*(
(
H γγ→
H ZZ→0
n lept.+ x
∼g → n jets + E
MT
→ n leptons + Xq similar∼
H+→τν
0H, A , h0 0→ττ(H ) γγ→h0 0
g∼ → h + x0
χ χ∼ ∼0 +→
*( (
W'→lν
V,ρ →WZTC→ lνll
Z' → ll
unpredicted discovery
4l→
g, q →b jets + X∼ ∼
b- Jet-tag
WH→
lνbb
ttH→lν
bb+X
––
H ll→ ττZZ→
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Leptons(e, µ)
Photons
Taus
JetsMissing ET
y98014_416dPauss rd
H → WW→lνjjH → ZZ→lljjZZH
H→WW→lνlν
H→WW→lνlν
→ → νν
H →
Z Z
→
4 le
pton
s*(
(
H γγ→
H ZZ→0
n lept.+ x
∼g → n jets + E
MT
→ n leptons + Xq similar∼
H+→τν
0H, A , h0 0→ττ(H ) γγ→h0 0
g∼ → h + x0
χ χ∼ ∼0 +→
*( (
W'→lν
V,ρ →WZTC→ lνll
Z' → ll
unpredicted discovery
4l→
g, q →b jets + X∼ ∼
b- Jet-tag
WH→
lνbb
ttH→lν
bb+X
––
H ll→ ττZZ→
With optimal triggering and kinematical selections:
pT ≥ 30 − 100 GeV, |η| ≤ 3 − 5; /ET ≥ 100 GeV.
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For any scenario beyond SM, LHC WILL contribute:
• Higgs fully covered at the LHC:
1
10
10 2
102
103
mH (GeV)
Sig
nal s
igni
fica
nce
H → γ γ + WH, ttH (H → γ γ ) ttH (H → bb) H → ZZ(*) → 4 l
H → ZZ → llνν H → WW → lνjj
H → WW(*) → lνlν
Total significance
5 σ
∫ L dt = 100 fb-1
(no K-factors)
ATLAS
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• LHC will have great chance for SUSY discovery: ∗m0 > 4000 GeV, m1/2 > 1400 GeV, tanβ >∼ 45.
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0.5 1 1.5 2 2.5 3 3.5 4 4.5 5
LHC, ET miss
-2
-5
-10
-30
5
4
5
mSUGRA: tanβ=45, A0=0, µ<0
m0(TeV)
m1/
2(T
eV)
LEP2no REWSB
Z~
1 no
t LS
P
mh LEP2 limit aµSUSY×1010 Br(b→sγ)×104
Br(Bs→µ+µ-)×108 0.094<Ωh2<0.129 stage 3
fσ(Z~
1p)×1011 pb 100 10 1
∗Baer, Balazs, Belyaev, O’Farrill, hep-ph/0305191.
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• LH: The heavy T signal at LHC ∗
gg → T T phase-space suppression;
qb → q′T via t-channel WLb → T .
∗Han, Logan, McElrath, Wang, hep-ph/0301040.
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ATLAS simulations for T → tZ, bW :∗
Invariant Mass (GeV)
0 500 1000 1500 2000
-1E
vent
s/40
GeV
/300
fb
0.5
1
1.5
2
2.5
3
3.5
4
ATLAS
Invariant Mass (GeV)
0 500 1000 1500 2000
-1E
vent
s/40
GeV
/300
fb
50
100
150
200
250
300
350
400
ATLAS
Reach MT ∼ 1 (2) TeV for xλ = 1 (2).
∗G. Azuelos et al.: hep-ph/0402037.
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ATLAS simulations for T → tZ, bW :∗
Invariant Mass (GeV)
0 500 1000 1500 2000
-1E
vent
s/40
GeV
/300
fb
0.5
1
1.5
2
2.5
3
3.5
4
ATLAS
Invariant Mass (GeV)
0 500 1000 1500 2000
-1E
vent
s/40
GeV
/300
fb
50
100
150
200
250
300
350
400
ATLAS
Reach MT ∼ 1 (2) TeV for xλ = 1 (2).
Cross-sectiions measure coupling xλ.
Mass peak MT determines f : v/f = mt/MT (xλ + x−1λ )
=⇒ check consistency with f from MZH.∗
∗G. Azuelos et al.: hep-ph/0402037.∗Perelstein, Peskin, Pierce: hep-ph/0310039.
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• Deep into extra-dimensions at the LHC:
Large extra-dim ADD & warped extra-dim RS: ∗
left: ADD with M⋆ = 20, 25, 30, 35 TeV;
right: RS with MKK = 16 TeV.
∗T. Rizzo
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Black hole to ℓ and γ events at the LHC: ∗
1
10
10 210 310 410 510 610 710 8
0 2000 4000 6000 8000 10000MBH, GeV
dN/d
MB
H ×
500
GeV
MP = 1 TeV
MP = 3 TeV
MP = 5 TeV
MP = 7 TeV
∗Greg Landsberg
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High Energy Astroparticle Physics
UHECRs exist:
+++++++ ++++++++++++
++++++++++++++++
++
+
+++++++
+++++++++
+++ + +
+
+
++++++++++++
++
+
++++
+
⊕ ⊕ ⊕ ⊕ ⊕ ⊕ ⊕
⊕ ⊕ ⊕
⊕ ⊕ ⊕ ⊕ ⊕ ⊕ ⊕ ⊕ ⊕
⊕ ⊕
⊕ ⊕
⊕ ⊕
⊕ ⊕ ⊕ ⊕
⊕ ⊕ ⊕ ⊕
⊕ ⊕
⊕ ⊕ ⊕
∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅
⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗
⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗
∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇
∇ ∇ ∇ ∇
⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄⁄ ⁄
⁄ ⁄ ⁄⁄ ⁄
⁄⁄
⁄
⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄⁄ ⁄ ⁄ ⁄ ⁄
⁄ ⁄⁄ ⁄
+ AGASA+ Akeno 20 km2+ Akeno 1 km2 AUGER
BLANCA CASA-MIA◊ DICE BASJE-MAS EAS-Top Fly’s Eye
Haverah ParkHaverah Park FeHaverah Park p HEGRA
⊕ HiRes-I⊕ HiRes-II
⊕ HiRes/MIA⁄ KASCADE (e/m QGSJET)⁄ KASCADE (e/m SIBYLL)
KASCADE (h/m) KASCADE (nn)∅ MSU
Mt. Norikura SUGAR⊗ Tibet ASγ⊗ Tibet ASγ-III∇ Tunka-25
Yakutsk
direct: JACEERUNJOBSOKOLGrigorov
Flu
x dΦ
/dE
× E
2.5
[m−2
s−1
sr−
1 G
eV1.
5]
104 105 106 107 108 109 1010 1011
103
104
102
10
1
Energy E [GeV]
ANKLE
KNEE
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High Energy Astroparticle Physics
UHECRs exist:
+++++++ ++++++++++++
++++++++++++++++
++
+
+++++++
+++++++++
+++ + +
+
+
++++++++++++
++
+
++++
+
⊕ ⊕ ⊕ ⊕ ⊕ ⊕ ⊕
⊕ ⊕ ⊕
⊕ ⊕ ⊕ ⊕ ⊕ ⊕ ⊕ ⊕ ⊕
⊕ ⊕
⊕ ⊕
⊕ ⊕
⊕ ⊕ ⊕ ⊕
⊕ ⊕ ⊕ ⊕
⊕ ⊕
⊕ ⊕ ⊕
∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅ ∅
⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗
⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗ ⊗
∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇ ∇
∇ ∇ ∇ ∇
⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄⁄ ⁄
⁄ ⁄ ⁄⁄ ⁄
⁄⁄
⁄
⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄ ⁄⁄ ⁄ ⁄ ⁄ ⁄
⁄ ⁄⁄ ⁄
+ AGASA+ Akeno 20 km2+ Akeno 1 km2 AUGER
BLANCA CASA-MIA◊ DICE BASJE-MAS EAS-Top Fly’s Eye
Haverah ParkHaverah Park FeHaverah Park p HEGRA
⊕ HiRes-I⊕ HiRes-II
⊕ HiRes/MIA⁄ KASCADE (e/m QGSJET)⁄ KASCADE (e/m SIBYLL)
KASCADE (h/m) KASCADE (nn)∅ MSU
Mt. Norikura SUGAR⊗ Tibet ASγ⊗ Tibet ASγ-III∇ Tunka-25
Yakutsk
direct: JACEERUNJOBSOKOLGrigorov
Flu
x dΦ
/dE
× E
2.5
[m−2
s−1
sr−
1 G
eV1.
5]
104 105 106 107 108 109 1010 1011
103
104
102
10
1
Energy E [GeV]
ANKLE
KNEE
To compare with collider experiments:Advantage: Higher energies.Disadvantage: Low and imprecise knowlege of fluxes.
Event reconstruction much harder.
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protons/heavy ions below the “knee”:
Large event sample available for Ecm > 1 TeV,
the QCD interactions/showering become overwhelming.
• SUSY production simulated at Auger: ∗Signal hardly observable.
• TeV-scale BH production simulated at Auger: †Possible for observation if the cross section is high enough.
∗Cafarella, Coriano, Faraggi, hep-ph/0308169.†Cafarella, Coriano, Tomaras, hep-ph/0410358.
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protons/heavy ions below the “knee”:
Large event sample available for Ecm > 1 TeV,
the QCD interactions/showering become overwhelming.
• SUSY production simulated at Auger: ∗Signal hardly observable.
• TeV-scale BH production simulated at Auger: †Possible for observation if the cross section is high enough.
Particle multiplicity is the key for signal/background separation;
Can we make use of the “transverse energy”?
∗Cafarella, Coriano, Faraggi, hep-ph/0308169.†Cafarella, Coriano, Tomaras, hep-ph/0410358.
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protons/heavy ions below the “knee”:
Large event sample available for Ecm > 1 TeV,
the QCD interactions/showering become overwhelming.
• SUSY production simulated at Auger: ∗Signal hardly observable.
• TeV-scale BH production simulated at Auger: †Possible for observation if the cross section is high enough.
Particle multiplicity is the key for signal/background separation;
Can we make use of the “transverse energy”?
• The “near-by” sources from heavy particle annihilation: ‡Possible explanation/observation above GZK.
∗Cafarella, Coriano, Faraggi, hep-ph/0308169.†Cafarella, Coriano, Tomaras, hep-ph/0410358.‡Albuquerque, Farrar, Kolb, hep-ph/9805288; Protheroe, Stanev, (1996);Barbot, Drees, Halzen, Hooper, hep-ph/0207133.
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High-energy cosmic neutrinos:
They serve as a better tool for new physics search!
⋄ No attenuation in Eν,
⋄ Avoid large QCD backgrounds.
⋄ ... ...
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High-energy cosmic neutrinos:
They serve as a better tool for new physics search!
⋄ No attenuation in Eν,
⋄ Avoid large QCD backgrounds.
⋄ ... ...
• Enhanced νN cross section:†
νN → q, ℓq, ν8;
→ KK states, stringy states, BH′s...
→ EW instantons
→ ......
†M.Carena et al. (1998); Domokos, Kovesi-Domokos (1999); Nussinov, Shrock (1999);Jain, McKay, Panda, Ralston (2000); Ringwald, Tu (2002); Feng, Shapere (2002);Anchordoqui, Goldberg (2002); Kusenko Weiler (2002); Friess, Han, Hooper (2002);J.Alvarez-Muniz et al. (2002); Han, Hooper (2004).
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For instance, BH signal at Auger: †
†L. Anchordoqui et al., hep-ph/0508312.
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Possible EW instanton effects at IceCube: †
†T.Han, D.Hooper, hep-ph/0307120.
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• Long-lived charged particles:‡
For instance, τR as the NLSP (next-lightest...).
SUSY production not enhanced,
but the long travel range of τR (∼ 103 km) compensates it.
Search for a pair of parallel upward charged tracks: τ+R τ−R .
Great potential for discovery!
‡I.Albuquerque, G.Burdman, Z.Chacko, hep-ph/0312197;M.H. Reno, I.Sarcevic, S.Su, hep-ph/0503030.
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Dark Matter Searches:
• Collider/Indirect/Direct Dark Matter searches:†
†D.Hooper and A.Taylor, hep-ph/0607086.
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Two points in order:
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Two points in order:
(1). Folk theorem: Precision EW data need a symmetry
(R, T, KK, Z2 ...), that leads to a CDM candidate.
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Two points in order:
(1). Folk theorem: Precision EW data need a symmetry
(R, T, KK, Z2 ...), that leads to a CDM candidate.
(2). More than “complementary”:
Indirect/Direct searches more conclusive than collider search!
A WIMP needs only to live for about 1 µs to be “DM” ...
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Recap:
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Recap:
• TeV scale new physics highly expected
EWSB, Naturalness/hierarchy problem with H.
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Recap:
• TeV scale new physics highly expected
EWSB, Naturalness/hierarchy problem with H.
• LHC anticipated for major discovery
Higgs, weak-scale SUSY?
new strong dynamics?
extra-dimensions?
dark matter ...
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Recap:
• TeV scale new physics highly expected
EWSB, Naturalness/hierarchy problem with H.
• LHC anticipated for major discovery
Higgs, weak-scale SUSY?
new strong dynamics?
extra-dimensions?
dark matter ...
• TeV scale astroparticle physics complementary
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Recap:
• TeV scale new physics highly expected
EWSB, Naturalness/hierarchy problem with H.
• LHC anticipated for major discovery
Higgs, weak-scale SUSY?
new strong dynamics?
extra-dimensions?
dark matter ...
• TeV scale astroparticle physics complementary
Join the excitement!