Instrumentation Division Report Veljko Radeka Presentation to the DOE RHIC Program Review July 10, 2003 Outline • Core Technologies and Facilities • Key Accomplishments and R&D for future NP Program managed by Brookhaven Science Associates for the U.S. Department of Energy
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Outline Core Technologies and Facilities Key ...Instrumentation Division Report Veljko Radeka Presentation to the DOE RHIC Program Review July 10, 2003 Outline • Core Technologies
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Instrumentation Division Report
Veljko RadekaPresentation to the DOE RHIC Program Review
July 10, 2003
Outline
• Core Technologies and Facilities• Key Accomplishments and R&D for future NP Program
managed by Brookhaven Science Associates for the U.S. Department of Energy
Program 04-08In support of vital BNL programs:•RHIC Detector Upgrades (silicon and
TPC)• e-cooler; e-RHIC:
High Current Photocathodes• ATLAS Dets., and LHC upgrade• Si-detectors for Polarimeters• Si-detectors & microelectronics:
-EXAFS at high photon rates-X-ray Microscopy-Protein crystallography-Position sensitive modification
• New small animal PETs, MRI• Neutron detectors for SNS• Neutrino detectors• Detectors and Microelectronics for
Homeland Security Program
State-of-the-art core technology:
• Fine-grained Si and gas detectors
• Low noise microelectronics fromsubmicron to nanoscale
• Femtosecond, photon and particlebeam generation & diagnostics
o Large Roman pot stripdetectors for RHIC PP2PPexperiment
o Large stripixel detectors for PHENIX upgrade
Radiation Hard Detectorso Low resistivity
detectorso Oxygenated detectorso Cryogenic Si detectorso Detectors with novel
structures (semi-3d)
o High resistivity CZSi detectors
8.5 µm
X-strips(2nd metal)
Y-strips(1st metal)
X
Y
0 100 200
0
25
50
75
100
125
150
175
200
Elen+n+ p+
n+
d (µm)
(µm)
Simulation of potential profile and E-field lines after inversion
8.5 µm pitch pixelsBondingpads
Strips1st Al
Readoutlines2nd Al
Hole(6mmdia.)
InnerGR
OuterGR
8 cm
SPIN POLARIMETER for RHIC and AGS
Measure the beam polarization at RHIC and AGS bymeasuring the left-right spin asymmetry of polarizedprotons scattering off a carbon (proton) target by detecting the the low energy recoil carbons (protons) with Si detectors.
1. RHIC polarimeter installed in 20022. AGS polarimeter installed in 20033. RHIC absolute polarimeter using a double-sided
strip detector under development for 2004 recoil Carbon energy (keV)
mea
sure
d as
ymm
etry
εN
polarizedbeam
recoilcarbon
target
Si detector
field shaping electrodes(instead of p+ implants)
p+ implants
Si detectors and Front EndElectronics Developed atBNL Instrumentation Division(Z. Li & S. Rescia)
Si detector
Si detector
• Minimum channel number (2N)
But:
• Two-sided processabout 3-4 times morecomplicated/expensive than single-sided process
• Radiation soft due to thethe complicated structureon the n-side
n strips
p strips
p+ channel stoppers
• Two polarities of readout electronics
Double-sided strip detectors on high resistivity silicon (~3-5 kohm cm):
• Two dimensional position sensitivity
The new concept:Alternating stripixel detectors (ASD)
Individual pixels are alternately connected by X and Y readout lines (strips)
• Two dimensional position sensitivity is achieved by charge sharing between X and Y pixels
• In principle, the pixel pitch should not be larger than the size of charge cloud caused by diffusion process
Schematic of the Prototype Stripixel DetectorFor PHENIX Upgrade
1000 µm
80 µm
X-cell(1st metal)
Y-cell(1st metal)
2nd MetalY-strip
2nd MetalX-strip
FWHMfor chargediffusion
BondingPad forY-strip
Go toBondingPad forX-strip
Z. Li, Inst. Div., BNLZ. Li, Inst. Div., BNL
Pixel pitches: 1000 µm in X, and 80 µm in Y
4.6° stereo angle between X and Y strips
Pixel arrays: 30x384σy = ~25 µm
Y
XFWHMfor chargediffusion
X-cell contacts
Y Contacts 16 µm Lines for X
X-cell contactsY-Cells 7 µm Lines
X-Cells 7 µm Lines
Photo ofprocesseddetector
80 µm
Novel Stripixel Detector for Sub-micron Position Resolution in Two Dimensions with One-sided Process
8.50 µm pitch in both X and Y strips
8.5 µm
X-strips(2nd metal)
Design and illustration of diffused charge cloud
Y-strips(1st metal)
Photo of processed detector
Laser Electron Gamma Source : Time Projection Chamber (TPC)
Spin ASYmmetry Array (SASY)
TPC Candouble GEM planes
HV mesh plane and UV window forlaser calibration
anode pad plane with front-end electronics
Interpolating Pad Readout for GEM (Gas Electron Multiplier)
Window
Anode Pad Plane
Upper GEM
Lower GEM
<100µm rmsposition resolution with 2mm pad pitch
Readout Electronics – Specifications
Tracking Measurement• Energy - triggered pad (xy)• Energy - neighbor pads (xy) • Timing (z)