CODEX-b and the Quest for Longevity
Philip Ilten May 13, 2020 Imperial Seminar
Ilten The Quest for Longevity 1 / 50
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CODEX-b and the Quest for Longevity Philip Ilten May 13, 2020 Imperial Seminar Ilten The Quest for Longevity 1 / 50 Introduction Dark Matter t d SM matter dark c s 5% matter g u b 25% H e quarks dark energy W Z
Philip Ilten May 13, 2020 Imperial Seminar
Ilten The Quest for Longevity 1 / 50
Introduction
H g W Z γ νe νμ ντ u c t b s d e μ τ dark energy 70% dark matter 25% SM matter 5% force carriers quarks leptons
1 interacts through gravity 2 does not interact through the electromagnetic or strong forces 3 interacts weakly (or not at all) with itself
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Introduction
H g W Z γ νe νμ ντ u c t b s d e μ τ b s d t c u e μ τ νe νμ ντ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ g ~
2
N ~
3
N ~
4
N ~
1
C ~
2
C ~
1
N ~ h A H
+
~
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Introduction
axion dark Higgs sterile neutrino dark photon
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Introduction
arXiv:1707.04591 [hep-ph]
SIMPs / ELDERS
Ultralight Dark Ma5er
Muon g-2 Small-Scale Structure Microlensing
Dark Sector Candidates, Anomalies, and Search Techniques
Hidden Sector Dark Ma5er
Small Experiments: Coherent Field Searches, Direct DetecIon, Nuclear and Atomic Physics, Accelerators
GeV TeV keV eV neV feV zeV MeV aeV peV µeV meV PeV 30M☉
WIMPs QCD Axion
GeV TeV keV eV neV feV zeV MeV aeV peV µeV meV PeV 30M☉
Beryllium-8 Black Holes Hidden Thermal Relics / WIMPless DM Asymmetric DM Freeze-In DM Pre-InflaIonary Axion Post-InflaIonary Axion Ilten The Quest for Longevity 5 / 50
Introduction
arXiv:1903.04497 [hep-ex]
displaced leptons, lepton-jets, or lepton pairs displaced multitrack vertices multitrack vertices in the muon spectrometer quasi-stable charged particles trackless, low-EMF jets emerging jets non-pointing (converted) photons disappearing or kinked tracks
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Introduction
γ∗ e− e− e− e− ge ge γ∗ A′ g ≡ g′
e
ge
A′ DM DM DM DM g′
e
g′
e 1 broken U(1) gauge symmetry in dark sector 2 allow mixing between dark and SM hypercharge fields
L ⊃ −1 4FµνF µν − 1 4F ′
µνF ′µν + mA′2
2 A′
µA′µ + geJµAµ + εgeJµA′ µ
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Introduction
displaced prompt
target shield detector beam detector beam
lifetimes
background
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Introduction
JHEP 06 (2018) 10−2 10−1 100 101
mA′ [GeV]
10−6 10−5 10−4 10−3 10−2
ε
prompt displaced
50 fs 1500 fs 100000 fs
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Experimental Landscape
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Experimental Landscape
Cherenkov drift tube pixel silicon strip ECAL HCAL muon
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Experimental Landscape
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Experimental Landscape
LHCb, JINST 8 (2013)
detector hardware software disk Run 2 Run 3 5 TB/s O(10) GB/s 0.7 GB/s 50 GB/s 1 TB/s
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Experimental Landscape
arXiv:1310.1762
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Experimental Landscape
arXiv:1310.1762
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Experimental Landscape
arXiv:1811.10243
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Experimental Landscape
arXiv:1811.10243
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Experimental Landscape
arXiv:1606.06298
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Experimental Landscape
arXiv:1810.03636
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CODEX-b
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CODEX-b
arXiv:1911.00481 [hep-ex]
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CODEX-b
ϕ
SM SM
CODEX-b box UXA shield shield veto IP8 Pb shield DELPHI
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CODEX-b
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CODEX-b
cτ mLLP
← lighter (. 10 MeV) heavier (& 10 GeV) → ← near ∼m far→
Forward
(FASER, SHiP, NA62, . . . )
Transverse
(CODEX-b, MATHUSLA, AL3X, . . . )
LHC coverage
(ATLAS, CMS, LHCb)
SCHEMATIC
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CODEX-b
√ˆ s mLLP
← lighter (. 10 MeV) heavier (& 10 GeV) → ← lighter ∼ cc, bb, ττ h, t heavier →
LHC coverage
(ATLAS, CMS, LHCb)
Forward
(FASER, SHiP, NA62, . . . )
Transverse
(CODEX-b, MATHUSLA, AL3X, . . . )
SCHEMATIC
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CODEX-b
1 we need a transverse detector at the LHC 2 probes a wide range of LLP models; complementary or
competitive with existing/proposed detectors
3 accessible zero background location with necessary services,
DELPHI/UXA cavern
4 integration with LHCb trigger-less readout 5 compact size and modest cost with ability to extend
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CODEX-b
2020 2021 2022 2023 2024 2025 2026
LS 2 Run 3 LS 3 CODEX-β Production Install data taking Removal CODEX-b Production
Partial Install 2027 2028 2029 2030 2031 2032 2033
Run 4 LS 4 Run 5 CODEX-b Production data taking
Remaining Install
data taking
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Minimal Models
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Minimal Models
Vector (A′) hA′A′ F ′F F ′F yes no reach Scalar (S) SH†H S2H†H SH†H yes yes HNL (N) HLN HLN yes ALP (a) ∂µa¯ qγµγ5q a ˜ GG a ˜ FF a(W ˜ W −B ˜ B) yes yes pending pending Production portal Decay portal UV operator
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Minimal Models
10−5 10−4 10−3 10−2 10−1 10−1 101 103 Br[ℎ → 𝐵′𝐵′] 𝑑𝜐 [m] 𝑛𝐵′ = 0.5 GeV
ATLAS 2DV CODEX-b AL3X (100 fb−1) MATHUSLA(200)
10−1 101 103 105 𝑑𝜐 [m] 𝑛𝐵′ = 10 GeV
ATLAS 1DV ATLAS 2DV CODEX-b Ilten The Quest for Longevity 30 / 50
Minimal Models
λ = 0 λ = 1.6 × 10−3
0.5 1.0 2.0 4.0
mS (GeV)
10−14 10−12 10−10 10−8 10−6
sin2 θ
10 fb−1 CODEX-b 300 fb−1 NA62 SHiP MATHUSLA FASER 2 CHARM LHCb, 3 fb−1 LHCb, 300 fb−1 AL3X 0.5 1.0 2.0 5.0
mS (GeV)
10−14 10−12 10−10 10−8 10−6
sin2 θ
CODEX-b 300 fb−1 10 fb−1 NA62 CHARM LHCb, 3 fb−1 LHCb, 300 fb−1 FASER2 SHiP MATHUSLA AL3X b W − S t s V ∗
tb
mt Vts
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tb
mt Vts
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<latexit sha1_base64="w6eR0vPC6lEtaqv5FjPCS63I2dA=">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</latexit>Ilten The Quest for Longevity 31 / 50
Minimal Models
CODEX-b, 300/fb LHCb, B→Kμμ LHCb, B→K*μμ CHARM REDTop, 1017 pot E949 FASER2, 3/ab KLEVER, 5·1019pot MATHUSLA200, 3/ab w/ ϵfloor=10-5
0.05 0.10 0.50 1 5 10 10-7 10-6 10-5 10-4 10-3 10-2 10-1 100 10-7 10-6 10-5 10-4 10-3 10-2 10-1 mA[GeV] cf gY ALP w/ universal fermion couplings, Λ=1TeV
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Minimal Models
CODEX-b, 300/fb CHARM
FASER2, 3/ab REDTop, 1017pot CODEX-b w/calo MATHUSLA200, 3/ab, ϵfloor=10-5
0.05 0.10 0.50 1 5 10 10-7 10-6 10-5 10-4 10-3 10-2 10-1 100 10-9 10-8 10-7 10-6 10-5 10-4 10-3 mA[GeV] cG 1/fPBC [GeV-1] ALP w/ gluon couplings, Λ=1TeV
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Minimal Models
10−10 10−8 10−6 10−4 10−2 0.2 1 10 |𝑉𝑓𝑂|2 𝑛𝑂 [GeV] NA62 DUNE SHiP MATHUSLA(200) FASER2 CODEX-b 10−10 10−8 10−6 10−4 10−2 0.2 1 10 |𝑉𝜈𝑂|2 𝑛𝑂 [GeV] NA62 DUNE SHiP MATHUSLA(200) FASER2 CODEX-b 10−10 10−8 10−6 10−4 10−2 0.2 1 10 |𝑉𝜐𝑂|2 𝑛𝑂 [GeV] NA62 B factory SHiP MATHUSLA(200) FASER2 CODEX-b
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Complete Models
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Complete Models
(2019) benchmark coupling production decay products 1 λ′
122, λ′ 112
D±
s → ˜
χ0
1 + e±
η, η′, φ, K0,± + νe, e∓ 4 λ′
131, λ′ 121
B0,± → ˜ χ0
1 + X0,±
D±, D∗± + e∓
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Complete Models
2 5 10 20 0.1 0.2 0.5 1 50 10-4 10-3 10-2 10-1 1 101 102 103 104 105 106 107 mχ1
0 [GeV]
cτ [m] Br(Z→2χ1
0)=10-5 MATHUSLA CODEX-b FASERR
2 5 10 20 0.1 0.2 0.5 1 50 10-4 10-3 10-2 10-1 1 101 102 103 104 105 106 107 mχ1
0 [GeV]
cτ [m] Br(Z→2χ1
0)=10-3 MATHUSLA CODEX-b FASERR
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Complete Models
5 10 15 20 25 600 800 1000 1200 1400 1600 1800 2000 m0 (GeV) mT (GeV)
CODEX-b MATHUSLA ATLAS 1DV ATLAS 2DV
LHCb substruct. h→invisible
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Complete Models
co-annihilation, etc.
10 5 40 20 10-4 10-3 10-2 mχ1(GeV) Sin θ mZD = 0.6 mχ1 ϵ = 10-3 α = 1 α = 4π
C O D E X
( α = 4 π ) C O D E X
( α = 1 ) MATHUSLA (α=4π) MATHUSLA (α=1)
Coannihilation (α=1) Coannihilation (α=4π)
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Building CODEX-b
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Building CODEX-b
L per 300 fb−1
L per 300 fb−1 pass through the shield
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Building CODEX-b
L
p r e
e t
p
t
e t
d
n s t r e a m ’ s t
p e d
a r e n t s e c
d a r y r e j e c t e d b y s h i e l d v e t
K0, n, . . . µ K0, n, . . .
‘upstream’ stopped-parent secondary suppressed by passive shield
CODEX-b UXA wall shield veto IP8 Pb shield
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Building CODEX-b
1 10−2 102 104 19 21 23 25 27 BG Flux/300 fb−1 𝑀shield [𝜇Pb]
Type; 𝜁veto
𝑜; 10−2 𝑜; 10−3 𝑜; 10−4 𝑜; 10−5
15 + 4 15 + 5 15 + 6 17 + 4 17 + 5 17 + 6 19 + 4 19 + 5 19 + 6 20 + 4 20 + 5 20 + 6
𝐿0
𝑀; 10−2
𝐿0
𝑀; 10−3
𝐿0
𝑀; 10−4
𝐿0
𝑀; 10−5
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Building CODEX-b
0º (1) to beam line 0º (2) and 90º (3) to beam line 0º (4) to beam line 0º (5) and 45º (6) to beam line Beam line
1 2,3 4 5,6
D3 platform
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Building CODEX-b
conservative
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Building CODEX-b
1 Demonstrate the ability to detect and reconstruct charged particles
which penetrate into the DELPHI cavern as well as the decay products of neutral particles decaying within the DELPHI cavern.
2 Detect and reconstruct a reasonable rate of neutral particles
decaying inside the hermetic detector volume.
3 Show that CODEX-b can be integrated into the LHCb DAQ and
demonstrate an ability to give a trigger to LHCb to retain an event that looks interesting in CODEX-b.
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Building CODEX-b
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Building CODEX-b
1951 mm 1892 mm Ilten The Quest for Longevity 48 / 50
Outlook
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Outlook
medium/long lifetimes and low √ ˆ s
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