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Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

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Page 1: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Upgrade Radiation Issues

Christopher O’GradyFor the DCH Electronics Upgrade Group

Based on work by Jerry Va’vra

Page 2: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Introduction In principle, we need to study SEU and

radiation “death” issues of all new chips (FPGA and flash perhaps most worrisome).

Worked on this in parallel with development.

Had hoped we could do “back of the envelope” calculation saying all OK, but didn’t happen.

Neutrons appear to be a problem This presentation will be “fuzzy”. Situation

in flux.

Page 3: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Complications Only have guess for the neutron rate

(depends on some assumptions) Only have guess for neutron spectrum Only have approximate answer for cross

section for our device Only have approximate answer for

number of configuration bits we rely on Rate scales with Luminosity!! (jerry

believes radiative bhabhas slamming into beam wall).

Page 4: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Proton Cross Section Per Bit VirtexII Proton Cross Section from

Xilinx Have read that neutrons>20MeV

similarProton SEU Cross Section for the Xilinx Virtex XQVR300

1.00E-18

1.00E-17

1.00E-16

1.00E-15

1.00E-14

1.00E-13

1.00E-12

1.00E-11

0 10 20 30 40 50 60

Proton Energy (MeV)

Cro

ss S

ecti

on p

er B

it (c

m2)

Outliers

Page 5: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Simulation of Neutron Production Alberto Fasso’s FLUKA simulation Iron Slab. Copper

similar. 10% of neutrons > 20MeV

Page 6: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Va’vras Detection Method Uses a Boron detector, which detects “thermal”

(low energy neutrons). Moderates “all” neutrons to be thermal using

polyethylene wrapper (if anything, undercounts).

Without polyethylene, no rate observed (good evidence he is really seeing neutrons).

1MeV neutrons act like a gas, fall off as 1/r**2 (not true for 20MeV neutrons).

Assuming a single point source of 1MeV neutrons, can calculate position of source and then rates everywhere.

Page 7: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Rates from Va’vra’s Logbook

Jerry says that KEK sees about 1kHz n/cm**2, not lumi dependent.

Page 8: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Neutron SEU Cross-Sections

Device Neutron Energy(MeV)

Cross Section Per Device

(cm**2)

XC4010E 14 <1.3E-11

XC4010E 0-11 <0.4E-11

XC4010E 100 4.0E-10

XC4036XLA >22 2.7E-9

XC3S1000 >10 5.4E-8 (XILINX)

XC3S1000 Cosmic ray (LANSCE)

2.6E-8 (XILINX)

XC3S1000 Cosmic ray (LANSCE)

1E-7 (ATMEL)

XC2V1000 >10 8.8E-8 (XILINX)

XC2V3000 14 3.3E-7 (ATMEL)

{{{

4000 series

Spartan3 series

VirtexII series

Page 9: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

SEU Estimates with XC3S1000 Xilinx claims to have study saying that

only 2-10% of configuration bits are used in a typical design. In addition, we are currently only using about 30% of CLBs.

(2000n/cm**2/s)*(2.6E-8cm**2/device)*(48devices)*0.1=0.00025/s (XILINX number) (2000n/cm**2/s)*(1E-7cm**2/device)*(48devices)*0.1=0.00096/s (ATMEL number)

Corresponds to about 1 SEU per hour. We’re using XC3S1500, which has factor 2

more configuration bits.

Page 10: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Are We Making Things Worse? Assume XC4010E bit cross-section is the same

as XC3000 series bit cross-section. Coincidentally, XC4010E (178kbit) =

1*XC3190(64kbit)+3*XC3142(30kbit)+2*XC3120 (14kbit)

i.e. one current box “equals” one XC4010E: (2000n/cm**2/s)*(4.0E-10cm**2/device)*(48devices)*0.1=3.8E-6/s (XILINX number)

This is one SEU every 72 hours. We could be making things ~100 times

worse.

Page 11: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Some Existing DCH Corruption Don’t think we see errors every 72

hours, but … See two sources of data corruption:

1. Elefant “lock” problem. Typically breaks in a whole quadrant

2. Illegal board addresses regularly. Not understood. Karl attempted to

reproduce (1) using high rate 1MeV neutrons. No success in 1 week.

Page 12: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

What should we do? If present, this problem affects more than

just FPGAs: elefant, atom chip SRAM and configurations, for example.

Seems like a bigger “experiment” problem.

Configuration corruption is the worst. Perhaps move to ATMEL flash based

FPGAs? (lower cross-sections by >100). Atmel downsides: not as much block RAM

(matt), more difficult to synthesize (herbst) TMR+partial reconfiguration?

Page 13: Upgrade Radiation Issues Christopher O’Grady For the DCH Electronics Upgrade Group Based on work by Jerry Va’vra

Other Ideas (that don’t fix problem)

Monte-Carlo directionality of 20MeV neutrons (hard to really believe)

Checksum FPGA every event Understand existing DCH corruption Work with Lockman/Bower on G4 neutron

simulation (long time scale) Put a neutron detector in DCH electronics

region Use SEUPI (xilinx tool) to understand how

many critical configuration bits we have