Ultra-low material pixel layers for the Mu3e experiment
Sebastian Dittmeier
for the Mu3e Collaboration
Physikalisches Institut - UniversitΓ€t Heidelberg PIXEL 2016
Sestri Levante β 9 September 2016
β’ Decays of stopped muons β low momentum electrons
β’ Design sensitivity BR < 10 β16 requires
β’ High muon rates πͺ 10 8 β 10 9 s β1
β’ Excellent momentum resolution π π < 0.5 MeV/c
Mu3e - Experimental Concept
Search for the charged lepton flavor violating decay π + π + π β π +
36 cm
12 cm 2.1 cm 2.5 cm
7.6 cm
8.9 cm
Material budget of selected pixel detectors
Experiment Material budget per layer
ATLAS IBL 1.9 % π
0CMS (current) ~ 2.0 % π
0CMS (upgrade) ~ 1.1 % π
0ALICE (current)* 1.1 % π
0ALICE (upgrade)* 0.3 % π
0STAR 0.4 % π
0BELLE II 0.2 % π
0Mu3e 0.1 % πΏ
π* arXiv:1211.4494v1
β‘ ATL-INDET-PROC-2015-001
β CERN-LHCC-2012-016 ; CMS-TDR-11
β‘
β
β
β
β³
βtalk by G. Contin
β³
talk by C. KoffmaneHow to reach the material goal?
Approach for a Mu3e tracking detector layer
How to reach the material goal?
Approach for a Mu3e tracking detector layer
HV-MAPS MuPix
50 ΞΌm ~ 0.5 β° π
0Talk by Frank Meier Aeschbacher
about MuPix 7
How to reach the material goal?
Approach for a Mu3e tracking detector layer
HV-MAPS MuPix
50 ΞΌm ~ 0.5 β° π
0Talk by Frank Meier Aeschbacher about MuPix 7
FPC
Flexible printed circuit Sensor powering Signal transmission
45 ΞΌm Kapton + 28 ΞΌm Aluminium + 10 ΞΌm Glue
~ 0.5β° π
0How to reach the material goal?
Approach for a Mu3e tracking detector layer
HV-MAPS MuPix
50 ΞΌm ~ 0.5 β° π
0Talk by Frank Meier Aeschbacher about MuPix 7
FPC
Flexible printed circuit Sensor powering Signal transmission
45 ΞΌm Kapton + 28 ΞΌm Aluminium + 10 ΞΌm Glue
~ 0.5β° π
0Kapton support structure
Helium cooling distribution
25 ΞΌm ~ 0.1 β° π
0How to reach the material goal?
Approach for a Mu3e tracking detector layer
HV-MAPS MuPix
50 ΞΌm ~ 0.5 β° π
0Talk by Frank Meier Aeschbacher about MuPix 7
FPC
Flexible printed circuit Sensor powering Signal transmission
45 ΞΌm Kapton + 28 ΞΌm Aluminium + 10 ΞΌm Glue
~ 0.5β° π
0Kapton support structure
Helium cooling distribution
25 ΞΌm ~ 0.1 β° π
0How to reach the material goal?
Approach for a Mu3e tracking detector layer
HV-MAPS MuPix
50 ΞΌm ~ 0.5 β° π
0Talk by Frank Meier Aeschbacher about MuPix 7
Material budget estimated π ~ 1.15β° πΏ π per layer
FPC
Flexible printed circuit Sensor powering Signal transmission
45 ΞΌm Kapton + 28 ΞΌm Aluminium + 10 ΞΌm Glue
~ 0.5β° π
0+ 10-20 ΞΌm Glue
~ 0.05β° π
0Kapton support structure
Helium cooling distribution
25 ΞΌm ~ 0.1 β° π
0FPC technology
Two layer aluminium (LTU Ltd.)
β’ 14ΞΌm Al + 10ΞΌm polyimide per layer
β’ Structure sizes β₯ 65ΞΌm
β’ Dielectric spacing 45ΞΌm
Layer stack
FPC technology
Two layer aluminium (LTU Ltd.)
β’ 14ΞΌm Al + 10ΞΌm polyimide per layer
β’ Structure sizes β₯ 65ΞΌm
β’ Dielectric spacing 45ΞΌm
β’ SpTAB technology (by LTU)
Single point Tape Automated Bonding
ο No additional (high Z) material for bonding!
Via Sensor bond
Layer stack
36 cm
12 cm
FPC design considerations
β’ Clock, reset, configuration as bus
β’ High Voltage (β 85 V)
β’ Power (π
ππ’πππ₯β€ 400 mW/cm
2)
β’ Readout at both ends
FPC Length Sensors LVDS links @ 1.25 Gb/s
Inner layers 12 cm 6 3 per sensor
Outer layers 36 cm 18 1 per sensor
FPC feasibility studies
Two layer FPC with test structures bonded to testboard
6.85 cm
1.90 cm
FPC studies β preliminary results
Bit error rate measurements
β’ 10 differential pairs
β’ Data rate = 1.25 Gbit/s
β’ No bit errors observed BER < 2 β 10
β13per pair
β’ Up to 2.5 Gbit/s: no bit errors
BER < 3 β 10
β13FPC studies β preliminary results
Time Domain Reflectometry
β’ Differential target impedance π
ππππ= 100 Ξ©
β’ Off by more than 10%
β’ Bottom: glue and board coating Will behave differently with MuPix
β’ Top: missing Kapton foil
Also tested:
β’ Resistance of power lines: 50 β 120 mΞ©
β compatible with actual conductor thickness ~12.3 ΞΌm
Mu3e cooling concept
β’ Cool sensors below 70β for up to 400 mW/cm
2β’ Minimize material budget of cooling in active volume
β’ Gaseous Helium: low density, reasonable cooling capabilities
Mu3e cooling concept
β’ Cool sensors below 70β for up to 400 mW/cm
2β’ Minimize material budget of cooling in active volume
β’ Gaseous Helium: low density, reasonable cooling capabilities
Mu3e cooling concept
β’ Cool sensors below 70β for up to 400 mW/cm
2β’ Minimize material budget of cooling in active volume
β’ Gaseous Helium: low density, reasonable cooling capabilities
Mu3e cooling concept
V-shapes for local cooling channels
Kapton Frame
V-shape
Cooling outlets
Mu3e cooling concept
β’ Cool sensors below 70β for up to 400 mW/cm
2β’ Minimize material budget of cooling in active volume
β’ Gaseous Helium: low density, reasonable cooling capabilities
Mu3e cooling concept
β’ Cool sensors below 70β for up to 400 mW/cm
2β’ Minimize material budget of cooling in active volume
β’ Gaseous Helium: low density, reasonable cooling capabilities
Simulation of Mu3e helium cooling
π£
πππππ= 16 m s π£
πππ= 3.5 m/s
π£
πππ¦ππ1β2= 4 m s π£
ππππππ= 3.5 m/s π = 250 mW/cm
2β’ Target power consumption (π = 250 mW/cm
2) seems feasible
β’ Higher power consumption (π = 400 mW/cm
2) requires higher flow velocities
Cooling tests with detector model
Heatable Kapton and glass staves
Measurement
β’ Large benefit from local cooling in outer detector layers
β’ Reduces maximum
temperature by 20Β°C
Summary and Outlook
β’ Ultra-low material tracking detector using HV-MAPS for Mu3e
β’ Material budget of ~ 1.15β° πΏ π per layer
β’ Aluminium FPC prototype works very well: BER < 2 β 10 β13 @ 1.25 Gb/s
β’ Cooling of sensors with Helium gas seems feasible
β’ End of this year: MuPix 8 (β 2 Γ 2 ππ 2 )
β’ Integration of MuPix with FPC
ο First inner detector modules
The Mu3e Experiment
Search for the charged lepton flavor violating decay π + π + π β π +
Standard Model
Highly suppressed branching ratio BR πΊπ΄ < ππ βππ
Probe physics beyond SM Any observation is a clear
sign for new physics!
Searching for New Physics with Mu3e
AndrΓ© de GouvΓͺa, Petr Vogel,
Lepton flavor and number conservation, and physics beyond the standard model,
π 1 + π
1 Ξ
2π
π1 + π
1 Ξ
2+
The Mu3e Experiment
Current limit on π + π + π β π + BR ππππ < ππ βππ (SINDRUM 1988)
Goal of Mu3e
Enhance sensitivity to BR < ππ βππ
How to achieve this in a reasonable time?
β’ High muon rate π ππ π π¬ βπ
ο Beamline at PSI (CH)
β’ Radiative SM decay π + π + π β π + π π
β’ Accidental combinations
What are the main backgrounds?
Event Topologies
β’ Common vertex
β’ Coincident
β’ π = 0
β’ πΈ = π
πβ’ Common vertex
β’ Coincident
β’ π β 0
β’ πΈ β π
πβ’ No common vertex
β’ Not coincident
β’ π β 0
β’ πΈ β π
πSignal Background
Material budget constraints
β’ Momentum resolution π
ππ β π₯ π
0β’ Requirement
R.M Djilkibaev and R.V. Konoplich, Phys.Rev., D79 073004, 2009
Material budget required
Major background contribution
Radiative SM decay π
+π
+π
βπ
+π π
History of CLFV Experiments
Updated from W.J Marciano et al., Ann.Rev.Nucl.Part.Sci. 58, 315 (2008)