development of radiation hard microstrip detectors for the cbm experiment

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1 Development of radiation hard microstrip detectors for the CBM Experiment Sudeep Chatterji GSI Helmholtz Centre for Heavy Ion Research CBM Collaboration Meeting 12 April, 2010

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Development of radiation hard microstrip detectors for the CBM Experiment. Sudeep Chatterji GSI Helmholtz Centre for Heavy Ion Research CBM Collaboration Meeting 12 April, 2010. CBM Silicon Tracking System Layout. Fluka Simulation. 1m. - PowerPoint PPT Presentation

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Page 1: Development of radiation hard microstrip detectors for the CBM Experiment

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Development of radiation hard microstrip detectors for the CBM Experiment

Sudeep Chatterji

GSI Helmholtz Centre for Heavy Ion Research

CBM Collaboration Meeting

12 April, 2010

Page 2: Development of radiation hard microstrip detectors for the CBM Experiment

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CBM Silicon Tracking System Layout

Fluka Simulation

STS has 8 stations of DSSDs, Strip Pitch ~ 58 m, Strip Width ~ 20 m, stereo angle ~ 7.5 0 Expected Radiation Damage ~ 1 x 1014 neq cm-2 year-1

Need detailed simulations to optimize device parameters to maximize VBD and minimize Noise. Also simulation needed to understand the impact of radiation damage.

1m

Page 3: Development of radiation hard microstrip detectors for the CBM Experiment

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x set by strip pitchy set by stereo angle

3-Dimensional Grid

3-D TCAD simulation tools “SYNOPSYS” Sub packages

SentaurusInspectTecplotSPICE (Mixed Mode)

Page 4: Development of radiation hard microstrip detectors for the CBM Experiment

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Stereo Angle in Strips

X-Y plane of the 3D grid. One can see there is a stereo angle on either side of 7.50.

Page 5: Development of radiation hard microstrip detectors for the CBM Experiment

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Backside View

Page 6: Development of radiation hard microstrip detectors for the CBM Experiment

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Implementing Bias Ring & Resistor

System { Strip sample (nplus1=c1 nplus2=c2 nplus3=c3 nplus4=c4 pplus1=cp1 pplus2=cp2 pplus3=cp3 pplus4=cp4) Vsource_pset vn (dd 0) {dc=0} Vsource_pset vp (dd1 0) {dc=0} Resistor_pset rn1 (c1 dd) {resistance=2000000} Resistor_pset rn2 (c3 dd) {resistance=2000000} Resistor_pset rp1 (cp1 dd1) {resistance=2000000} Resistor_pset rp2 (cp3 dd) {resistance=2000000} } Solve {

Circuit Coupled (Iterations=100) {Poisson} Coupled {Poisson Electron Hole Contact Circuit} Quasistationary ( InitialStep=1e-3 MaxStep=0.025 Minstep=3e-5 Increment=1.2 Goal { Parameter = vp.dc Voltage = -100} Goal {Parameter = vn.dc Voltage=0} ) }

Implementing Pulse Generator (Future Plan) Vsource_pset vin (node1 node2) {pulse=(DCStart Vamp td tr tf tperiod)} Can simulate the entire readout chain

Mixed Mode Simulation (PSpice in TCAD)

Page 7: Development of radiation hard microstrip detectors for the CBM Experiment

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Understanding the Geometry

Using SYNOPSYS TCAD 3-D simulation package Silicon volume ~ Cuboid (Six Rectangular faces). Dopant Implants, P-Stop and Contacts ~ Parallelogram Oxide ~ Cuboid, Enough space needed at the corners for junction curvature (0.8*Junction Depth)

Page 8: Development of radiation hard microstrip detectors for the CBM Experiment

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Determination of full depletion voltage

c

Page 9: Development of radiation hard microstrip detectors for the CBM Experiment

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Determination of full depletion voltage

Page 10: Development of radiation hard microstrip detectors for the CBM Experiment

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Potential & Electric Field Distribution

0 V

50V

Page 11: Development of radiation hard microstrip detectors for the CBM Experiment

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Some Static Characteristics

CTotal = Cback+2*Cint

ENC α CTotal

Optimization needed to maximize breakdown voltage & minimize ENC

Page 12: Development of radiation hard microstrip detectors for the CBM Experiment

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Optimization of W/P & P-Spray Width

When W/P is too small, there is inappreciable impact of ↑ the strip width on VBD

A narrower strip width and a wide P-Spray width can reduce the ENC.

Page 13: Development of radiation hard microstrip detectors for the CBM Experiment

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Optimization of P-Spray Dose

With ↑ in P-Spray dose, the VBD ↓

Using P-Spray rather than P-Stop seems better for detector performance

What happens at high radiation damage?

Mixed Mode Simulation (TCAD + SPICE)

Page 14: Development of radiation hard microstrip detectors for the CBM Experiment

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Radiation Damage in Silicon

The major effect expected from bulk damage is the change in the effective carrier concentration (Neff) leading to Type Inversion.

The change in Neff is parameterized using Hamburg model:

eqK

TtNNTtNTtNNN aeqYeqcaeqAaeqeffeffeff

0/1/1

))(,()())(,())(,(0,

The change in Minority carrier lifetime is parameterized using Kraners model:

For high quality oxide, the value of surface oxide charge (Q f) is expected to be 3e11cm-2 (for non-irradiated detector) while after irradiation Q f increases and saturates at about 1e12 cm-2. Flatband Voltage gives an approx. of Qf.

Year Fluence (assumed each year) x 1014 (neq/cm2)

Integrated Fluencex 1014 (neq/cm2)

Neff x 1012

(cm-3)

1 1 1 - 1.73

2 1 2 - 5.47

3 1 3 - 9.87

4 1 4 - 14.8

5 1 5 - 19.25

6 1 6 - 23.78

Page 15: Development of radiation hard microstrip detectors for the CBM Experiment

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Impact of Radiation Damage

Trap Model, University of Perugia

0.92.5*10-152.5*10-14CiOi Ev+0.36Donor

0.95.0*10-145.0*10-15VVVEc-0.46Acceptor

1.6132.0*10-142.0*10-15VVEc-0.42Acceptor

η (cm-1)σh (cm2)σe (cm2)Trap

Energy (eV)Type VBD ↑ with fluence

Current ↑ by 3 orders Rint ↓ with fluence Detailed study needed

eqcmConc )( 3

Page 16: Development of radiation hard microstrip detectors for the CBM Experiment

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Transient Simulations

Can simulate the passage of Heavy Ion, α-particle and Laser. Can include angle in the passage of MIPs. Plan to do complete scan of interstrip region and compare with test beam data.

Page 17: Development of radiation hard microstrip detectors for the CBM Experiment

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Simulation of Readout Cables

Two connecting layers with constant pitch of 100 m are laminated together with a lateral shift of 50 m. A spacer layer is inserted between the two layers to reduce the capacitance. An external shielding layer is applied to reduce the noise.

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Simulation of Readout Cables

3-D grid of the kapton cable 3-D grid without insulator

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Summary

We need radiation hard Double Sided Silicon Strip detectors. TCAD simulation package, SYNOPSYS has been installed on

CBM batch farm and running. We are doing Mixed Mode simulation using SPICE models

available in Sentaurus. Have procured the Probe Station. Plan to carry out measurements before and after irradiation both

with proton and with neutrons. Carry out systematic annealing studies. Work closely with CiS, Erfurt on microstrip detector R&D.