Document 7515707
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Transcript Document 7515707
Electronics and Trigger developments for the
Diffractive Physics Proposal at 220m from
LHC-ATLAS
By P. Le Dû
[email protected]
J.F. Genat1, O. Kepka2 , P. Le Dû, Ch. Royon
For the RP220 collaboration
1
CNRS/IN2P3
2 DAPNIA.SPP and Institute
1-Nov-07
of Physics, Prague, Czech Republic
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Goals of this presentation
Present the feasibility study, R&D and issues
for the development of detectors to measure
protons at 220 m from the IP, within low
optics at the LHC
Work associated or/and in collaboration with
– FP420 for the position detector (3D)
See N18-4 and N20-4
– UChicago/ANL/FNAL/Saclay/Photonis(Burle) for
the ultra fast timing detector (MCP)
N06-6 and N18-1
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Diffractive physics
Main physics aim pp p+ X + p
Exclusive Higgs Signal over background: ∼ 1 if Mass resolution <
1Gev
New physics :SUSY search, Diffractive top, stop pair production
QCD studies
Photon induced interactions
Objective : reconstruct the M with a precision better than 1 Gev
Kinematics variable is
= fractional momentum losses of the outgoing protons
b-jet
p
H
M 2= = 1 2 S
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p
h
b-jet
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RP220 vs. other projects
Luminosity Monitors
(Low Luminosity)
QuickTime™ et un
décompresseur TIFF (LZW)
sont requis pour visionner cette image.
ATLAS
RP220
FP420
High Luminosity 1033 to 1034
Additional signal and flag at the L1 ATLAS Trigger
Natural follow-up of the ATLAS luminosity project at 240 m to
measure total cross section
Complementary to the FP420
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Trigger topologies
RP220 only
PLtrack
PL. AND PR track with ζ cut
Et JET 1 AND 2 > 40 Gev
JET Rapidity correlation ?
Dijet ENERGY /TOTAL > 0,9
JET 1
RP 220
RP 220
1 KHz @ 1033
20-30 KHz @ 1034
RP220 + FP420
PL Track
JET 2
PR track
PL track with ζ cut
Et JET 1 AND 2 > 40 Gev
JET 1 Rapidity Cut
Dijet ENERGY /TOTAL > 0,9
JET 1
RP 220
1,6 KHz @ 1033
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JET 2
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FP420
5
Basics Requirements and Challenges
Measure of each outgoing proton
– Position and direction with a precision of 10
– Time of Flight (TOF) of the 2 outgoing protons with a
resolution of < 5 picoseconds
General system issues
– Mechanics and overall stability
integration with precision beam position monitor to reach 0(10) m
– Radiation for detectors at 220 meters (cryostat region)
– Detectors to operate very close to the beam (10 --> 1 mm)
– Trigger/selection issues
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Accumulated dose estimation @ 220 m (XRP3)
N. Mokhov, LHC Report 633
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Position Detectors
Position detectors
– Need to approach beam to the mm level
and stabilty of 10 m
– Should Achieve 10 m position
resolution
– Use EDGELESS Silicon detectors
TOTEM
Roman pot technique
For compact detectors
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Timing detectors
Measure the Time Of Flight of each diffracted
proton
Precision of few Picoseconds
– 1 mm on the vertex (select the right event among 35)
Technology --> Micro Channel Plate (MCP)
moving beampipe (HERA)
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Roman Pots location
RP
RP
220m
RP
RP
RP
RP
220m
IP
RP
{
Roman Pot Unit
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Each RP station consists of two Roman
Pot Units separated by 8 m, centered
at 220m from IP1
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{
RP
Roman Pot Station
10
Roman Pots Layout
8m
Beam
Optics
IP
220m
3cm
Silicon
Detectors
One Horizontal pot
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Two Vertical pots
Elastic events for
calibration
and alignment
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Layout
MCP-PMT
8x8
Pixels
X
U Y
V X
Radiator
3D pixels
Light
Guide
Size : 2,5 x 2,5 cm2
MCP
Timing detector
Movable Beam Pipe
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MCP
S
D
I U O
D P W
E
N
Roman Pot B
Roman Pot A
2 x 21 planes of Si detectors
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Position detectors specific requirements
Objective : Achieve 10 m position resolution
–Two staggered 50 m pitch strips read in digital :
– 25 / 12 = 7.2 m resolution
– Or larger pitch analog using centroids
–Trigger data available within a few 100 ns
Candidates:
– Baseline: “3D” Pixels detectors (S. Parker)
–- NEW : Under development for RP420
3D
Stanford, VTT, Sintef
- Backup: Edgeless Silicon strips Experienced technology
Canberra, Hamamatsu
1-Nov-07
50m strips
(Canberra)
(Stanford)
Semi-3D detector
(VTT, Finland)
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3D Detector
Benefits compared to standard Si strips detectors)
Collection time
x 10
Low voltage depletion
/10
Radiation hardness
x50
Edgeless using plasma etching /10
Same charge as planar
Drawbacks
-
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2 ns
10V
1015 p/cm2
5m
25 ke-/300
Thickness:
Needs a bump-bonded chip
(could be thinned to 50m)
-
Production yield
Presently 80%
(7.2 x 8 mm2 detectors)
-
Readout speed
Slow as is: 2-6 s,
-
No ‘fast’ trigger data
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FE13 Readout chip
(ATLAS b-layer upgrade)
2880 channels
50 x 400 m2 pixels
7.2 x 8 mm2
Binary & Time Over Threshold
Self triggering
Time over Threshold
Adjustable threshold
CMOS 250nm IBM
Readout 2-6 s @ 40 MHz
8mm
7.2mm
Readout chip
IZM + Bonn
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Baseline for FP420
Need to be modified
for extracting the
Fast Trigger information
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Fast (asynchronous) pixels digital readout
Trigger data
10-bit words
512
pixels
-
Fast ORs of columns (sufficient for the RP220 trigger)
Fast readout of every hit column
Fast address building takes a few ns in total (130nm CMOS)
Can be sent to the fast logic in the “alcove” at every BCO
X1
Y1---Y1n
X2
Y21---Y2m
--Xp
Yp---Ypq
Data transfer: 10 hits (disable noisy pixels) = 20 (10) words = 200 (100) bits
20ns (10) @ 10 Gb/s
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Jean-François Genat, RP220 meeting, Oct 17-19th 2007 Krakow, Poland
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Alternative Read Out solution
Pixels connected as strips
Standard ABCD strips readout
Capacitance is higher, but does not impact small detectors
QuickTime™ et un
décompresseur TIFF (LZW)
sont requis pour visionner cette image.
Need to extract the Fast OR signal for trigger
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Micro Channel Plate PMT Operation
photon
Faceplate
Photocathode
Photoelectron
Dual MCP
DV ~ 200V
DV ~ 2000V
MCP-OUT
Pulse
Gain ~ 106
DV ~ 200V
Anode
A 2” x 2” MCP
actual thickness ~3/4”
Burle- Photonis MCP
2” x 2” sensitive area
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Major advance for generating the signal
Incoming
rel. particle
Use Cherenkov light fast
Custom Anode with
EqualTime Transmission
Lines + Capacitative. Return
Collect charge here
differential Input to
200 GHz TDC chip
Development of MCP’s
with 6-10 micron pore
diameters
1-Nov-07
10 m pores
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e.g. Burle
(Photonis)
85022with
19
mods
Simulation
RF Transmission Lines
Summing smaller anode
pads into 1by 1 readout
pixels
An equal time sum make
transmission lines equal
propagation times
Work on leading edge
ringing not a problem for
this fine segmentation
QuickTime™ et un
décompresseur TIFF (LZW)
sont requis pour visionner cette image.
Ability to simulate electronics
and systems to predict design
performance
Oscillator with predicted jitters
<< 100 femtosec
860 fs
20 Pe
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Read Out :Direction to reach 1(few) psec (1)
Picking the time
Temps / s
0,00E+00
– Multithreshold discriminator
5,00E-08
1,00E-07
1,50E-07
2,00E-07
2,50E-07
3,00E-07
3,50E-07
4,00E-07
1,00E-02
0,00E+00
-1,00E-02
Tension / V (50 Ohms)
-2,00E-02
M
C
P
-3,00E-02
-4,00E-02
-5,00E-02
-6,00E-02
-7,00E-02
-8,00E-02
1
2
3
4
Sigma (picoseconds)
Multi-threshold time resolution with actual
MCP pulses (2d order fit)
Extrapolated time
400
350
300
250
200
150
100
50
0
1
3
5
7
9
11
13
15
Number of thresholds
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QuickTime™ et un
décompresseur TIFF (LZW)
sont requis pour visionner cette image.
Direction to reach 1 psec (2)
Time Stretcher Scheme
“Slow” TDC
kd
IBM 8 HP Chip
M
C
P
DAQ
QuickTime™ et un
décompresseur TIFF (LZW)
sont requis pour visionner cette image.
Chip
Fukung Tang et al (UC-ANL).
200 MHz
TDC
(FPGA)
d
Resolution:
a few ps
1
2
3
4
Issues
– Power consumption (250 mWatts/ch)
– Ramp zero crossing induces important Jitter
QuickTime™ et un
décompresseur TIFF (non compressé)
sont requis pour visionner cette image.
Synoptic
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Direction to reach 1(few) psec (3)
Alternative to Time stretcher
– Replace the TDC ---> ADC
DC level to ADC
ADC
Digitized dt
dt
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Best results with 2 TOF counters in tandem
QuickTime™ et un
décompresseur TIFF (non compressé)
sont requis pour visionner cette image.
1-Nov-07
From J. Va’vra (SLAC)
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Diffractive Trigger
Horizontal roman pots
(a la TOTEM)
- 224 m
xA
7 plans Si /Roman Pot
positionmicrons
time < 5 psec
- 216 m
xB
jet
Front end
PA
SH
xA xB
T
Left
Pretrigger
T
R
jet
Right
Pretrigger
ATLAS detector
xD - xC =0
xA - xB =0
LR Trigger Logic
Pipeline
buffer
(6.4 sec)
+850 ns (air cable)
+730 ns
T
1,0 sec
• LP AND RP
•TR - TL
2,0 sec
L1 CTP
2 Jets with
Pt > 40 Gev/c
Max 75KHz
2,5sec
ATLAS standard
R
O
D
1-Nov-07
30 nov 2006
US15
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HLT Trigger
(ROB)
ATLAS Standard
Refined Jet Pt cut
Vertice within millimeter
D time < 5 to 10 psec
25
Timing and Data flow
BXing
0 ns
Proton @ RP
733 ns
Flight path
1024 ns
Pretrigger Data available
@ 220 m(Alcove)
Processing
Detector response 11 ns
ABCD response 150 ns
20 ms cable 80 ns
Pretrigger Processing 50 ns
RP ASIC & FPGA
SI ---> 4 Events x 2 Si Strips x 10 bit words
MCP ---> 4 Events x 6 bit words per Xing
= 104 bit/Bx
Average Rate = 4,16 Gbit/sec (11ns through cable to Alcove)
ALCOVE CTA crate PRETRIGGER
Matching 2RPs with overlap Si Strips
Add Timing information from relevant MCP PMT pixel (1 mm2))
1921 ns
RP Triigger Data @ ATLAS CTP
Cable
LVL1 ACCEPT (75 KHz)
80 bit/BX x 40 MHz = 3,2 Gb/s
80 bit @ 10 GB/s - 880 transfert time
Processing
Max
2500 ns
588 ns
5120ns
RPs data @ ROD
Cable
2x 1100 ns + 7.4 K bit @ 4x 5 Gb/s= 2620 ns
Data Production per Roman Pot to ROD
4 events x(7 Si detectors x10 bit word stored in the pipeline)
4 events x 1 MCP-PMT detector x (6 bit adress + 8 bit fine timing)
Total per LV1 Accet = 336 bit
Total x 75 KHz =25 Mb/s
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Implementation block diagram
MBP
Detector
ASIC
Local
Logic
FPGA
RP B
RP A
X X
XX XX
X X
XX XX
FPGA
FPGA
//
IP
Picosecond CLK 160 MHz
Trigger DATA
4,16 Gb/s
RO DATA
670 kb/s
RP Left Trigger
1Cable
DATA
2 x 3,2 Gb/s
CTA crate
4 fiberss
ATLAS ROD
(LVL2
DAQ)
LHC&CLK
75 KHz
25 Mb/s
Pretrigger logic
Read Out
Control & Monitoring
160 MHz CLK (fiber)
Reference clock
(Atomic)
LHC CLK
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RP Right
Trigger
L1 ACCEPT
20 m
Cables
Shielded
Alcove
ATLAS
LVL1
CTP
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Conclusions
A challenging ‘small’ experiment
Need to use State of the art technologies
Tracking Silicon hodoscopes with 10 m precision
Ultra fast timing with few Psec TOF resolution
Input signals forTrigger @ L1 in ATLAS
System aspect non obvious (stability, radiation …)
But the Physics results
might be outstanding !
Thanks a lot for your attention!
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