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Modulator-Based, High Bandwidth Optical Links for HEP Experiments G. Drake, W. S. Fernando , R. W. Stanek ,D. G. Underwood High Energy Physics Division, Argonne National Lab, Argonne, Il, United States Jitter (ps) Noise (mV) Nice open eye at BER=10 -18 For a link at 10 Gb/s - - 10 -18 BER =1 error in ~1000 days ! 10 -12 BER = ~ 900 errors per day !

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Modulator-Based, High Bandwidth Optical Links for HEP Experiments G. Drake, W. S. Fernando , R. W. Stanek ,D. G. Underwood High Energy Physics Division, Argonne National Lab, Argonne, Il, United States. Log(BER). Noise (mV). Nice open eye at BER=10 -18. Jitter (ps). - PowerPoint PPT Presentation

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Page 1: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

Modulator-Based, High Bandwidth Optical Links

for HEP Experiments

G. Drake, W. S. Fernando , R. W. Stanek ,D. G. Underwood High Energy Physics Division, Argonne National Lab, Argonne,

Il, United States

Jitter (ps)

Noise (mV)

Nice open eye at BER=10-18

For a link at 10 Gb/s - - 10-18 BER =1 error in ~1000 days !

10-12 BER = ~ 900 errors per day !

Page 2: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

2

Electro-Optical Modulators• Two methods for optical data transmission

– Direct modulation of light: common in short distance, short wave length communication, all current LHC experiments use this technology

– Indirect modulation of light: long distance, long wave length communication. ATLAS TileCal will test this technology in 2013 (demonstrator) for use in Phase 2 upgrade

2

Current driverLaser

(VCSEL)

Receiver PIN diodes

Optical Tx

Optical Rx

Elec. Tx

Elec. Rx

Voltage driver Modulator

Receiver PIN diodes

Optical Tx

Optical Rx

Elec. Tx

Elec. Rx

Laser (CW)

Monolithically integrated Silicon photonic device

Page 3: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

3

Two main types of Modulators

– Mach–Zehnder interferometer basedΔVoltage Δrefractive index phase amplitudePockels effect, Kerr effect, free carrier dispersion effect Materials: LiNbO3, Si, InP

– Absorption basedΔVoltage Δoptical absorptionFranz-Keldysh (FK) effect in bulk semiconductors and quantum-confined Stark effect (QCSE) in quantum-well (QW) structures. Materials: InP, SiGe, Graphene

3

Input Output

Page 4: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

4

Modulating Materials for HEP

4

• LiNbO3 - based on the crystal property – High bandwidth, tested rad-hard, very long (~5 cm), expensive, high

drive voltages

• InP - based on the crystal property– Very High bandwidths, should be rad-hard, small (~2 mm), low drive

voltages, expensive at present, special-purpose technology

• Si - based on the free carrier dispersion effect – High bandwidth, rad-hard (?), small (~1 mm), inexpensive, could

monolithically integrate, commercially available, use existing Si Technology

Page 5: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

5

Reliability

• Modulators are very simple and reliable. No known failure mechanisms– e.g. Luxtera transceiver MTBF > 2.3 x 109 hrs (300 million

device hours accumulated without a single intrinsic failure)• E.g. 1 device failure in TileCal >34 years (9 months running, 1024

transceivers)

VCSEL Photonic Si modulator

5

Page 6: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

6

Other Considerations

• SM fiber is more rad-hard and cheaper than most MM fiber. Ge doped MM fiber is $

• Lasers designed to run as CW can be more reliable than switched VCSELs.

Also eliminates chirp.• CW lasers can be at the Modulator or remote,

depending on Radiation level.

Page 7: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

77

Modulator Selection for ATLAS TileCal • Modulator selection based on several criteria:

– Availability: COTS devices 1st choice– Reliability: Proven in the field– Radiation tolerance: ~100 krad TID, ~1012 p/cm2 (and rad-

hard SM fibers are cheaper than doped MM)

– Cost: Cost Savings over SNAP12 Baseline– Implementation: Ease over Baseline– Bandwidth: 56 Gb/s per readout board– BER: minimal correction needed

7

9.8 mm

4 x 10Gb/s transceiver from Luxtera, 130nm Silicon on Insulator (SOI)

We propose to implement optical links to be used in the TileCal Phase 2 upgrade based on Luxtera’s silicon photonic transceiver. This comes in a standard QSFP package which can be easily plugged into a motherboard. We are doing a Demonstrator.

Page 8: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

8

Speed 10 + Gb/fiber commercial integrated optics 40 Gb/fiber with other commercial unitsLaser reliability Either CW laser onboard Or displace laser outside detector. (DFL has Different junction structure than VCSELs)Low Bit Error Rate 10-18 vs typical 10-12 for current systems Simplified error correction schemesLow power One CW laser - split many ways Modulators are very efficient Short electrical paths – no cable drivers Low voltage drivers – not currentRad hard optical parts We have tested silicon integrated optics for >64 krad application Modulator parts should work at much higher levels Optical part expected to work at multi-Mrad

Commercial Integrated Optics Chips are a Promising Form of Modulators.

1 cm

1 cm

laser4 transmit and 4 receive fibers on one integrated optics silicon chip

10Gb/s each fiber

Use of modulators and CW laser

Low power, small size

Page 9: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

9

ANL Bench Tests of Quality and BER of the Complete Link(Modulator & Receiver with 200m SM fiber)

FPGA board generate PRBS7 bit stream @10.3125

Gb/s

QSFP Interface board

Luxtera Mod

DSA8200 Communication

Analyzer

4 SMA cables to Tx

SMA

100 m

8 SM fiber bundle

Tx

Rx

Feedback

9

Use FPGA to generate random bit stream 4 input ports, 4 output ports.

4 SMA cables from Rx

Scope to monitor Quality (eye diagram) and calculate Bit Error Rate (BER)

Page 10: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

10

Eye diagram of Complete Link

10

The quality of the link is measured and compared with IEEE 802.3ae and the performance exceeds the requirements by 40% more

Mask 140% of 10GBASE-R

Page 11: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

11

Verified* Luxtera 10-18 BER Spec

11

Per link @ 10 Gb/s

Why is Low BER important ?• High BER requires Forward Error Correction (FEC) which consumes 30% of the

bandwidth and requires error correction which consumes power and introduce susceptibility to radiation

• BER < 10-18 ~ ~ no need for FEC -> save money and bandwidth and more rad-hard!

Achieved:• Per Link 10Gb/s (faster by x2 the upgrade target)• BER < 10-18 (better by x106 over upgrade performance)• Lower power consumption (factor of x6 the upgrade target)

Jitter (ps)

Noise (mV)Nice open eye at

BER=10-18

10-18 BER =1 error in ~1000 days !

10-12 BER = ~ 900 errors per day

ANL test Luxtera / Molex

Test

Page 12: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

12

Summary of Comparison

Versatile Links (target) Luxtera40 G

InP Modulators

LiNbO3Modulator

Technology Directly modulated laser based ( eg. VCSEL) Modulator based

Bandwidth (Gb/s) 5 14 80 40

Bit Error Rate (BER) (10-12) 10-18

Fiber Type Multi Mode Single Mode

Reach (m) 100 4000 10000 10000

Power (mW/Gb/s) 100 8 <50* <50*

Reliability VCSELS have many failure mechanisms, complex No known failure mechanisms, very simple

12

* Estimate

Per fiber

Page 13: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

13

Overall Plan for Demo of Luxtera / Molex QSFP Modulator based Devices

On-Detector Counting House200 M

Page 14: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

14

A Proposed Interface to the TileCal Main Board

14

12 bit ADCs

TO USA15

PMTshaperIntegratorcharge injection

PMT

ADC low gain

ADC hi gainFP

GA

(Kin

tex-

7)

Seria

lizer

& C

ontr

olIntegrator

multiplexer

Integrator ADC

12 tubes

QSFP connector

6 differential serial links (4 Tx, 2 Rx)

6

Luxtera QSFP has 4 x 14 Gb/s transceiversQSFP: Quad Small Form Factor Pluggable

shaperIntegratorcharge injection

ADC low gain

ADC hi gain

Stockholm and Valencia are now designing the mainboard and ROD to accommodate the Luxtera QSFP package.

Note Extra I2C and monitor links through QSFP connector to emulate non-rad-hard PIC uC

Inside ATLAS Tilecal Iron Girder

Includes duplicate backup links

Page 15: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

15

First Steps of ANL Radiation Test Program

3 technologies

Integrated Silicon – CMOS (4-channel)

InP single channel

LiNO3 single channel

NO SEE @ 1012 protons/cm2 & 64 krad TID OK after ~100 krad TID

Proton Beam Electron Beam

Links run continuously at 10 Gb/s during irradiation

and 3.5 x min ionizing

Page 16: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

16

Levels of Radiation Sensitivity in Modulator-based COTS devices

• Modulator • Logic and RF circuitry in Modulator chip• Attached CW Laser• Voltage regulators• Glue, Capacitors, etc• Control Unit ( PIC uC or..)• Working Group Wednesday 16:00

Only issue so far

Page 17: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

17

In this Luxtera / Molex device

uC is used for startup

reads and sets parameters for operation

also allows readout of temperature, current, etc

After startup, the device will continue to operate

until power down

(or perhaps some large change in device)

We can use external I2C, etc through spare pins on QSFP connector to eliminate uC

Page 18: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

18

FPGA board PC

QSFP board

I2C Main+ Power

QSFP connect

I2C

QSFPQSF

P

QSFP

InP

Receivers

LiNbO3

Electrical feedback

Radiation Exposure Region

8 SMA

USB

USB

8 Fiber

12 V

2 x Differential I2C

I2C

SMA

PM Fiber

~100 m8 SMA

CW LasersShielded from radiation

Fiber SM

Fiber SM

2 Fibers SM

Monitoring optical power, Voltages, currents

4 x 10Gb/s BER testing

Page 19: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

19

Summary: Modulators• Modulators are a robust replacement for VCSEL-based optical readout:

– High Speed: >10 Gb/s. No speed limits– Reliable: Rad hard, BER ~10-18. MTBF ~2.3 x 109 hrs

• We have proposed an optical link be used in TileCal and have built a prototype link based on Luxtera transceiver– Characterized it for use @ 10 Gb/s with < 10-18 BER– Tested radiation hardness up to 8 x 1011 p/cm2

• No SEU at this level• Need some changes to the controller ----

• Investigating other COTS modulator devices made of other materials. • Investigating options to use modulators in very high radiation environments

such as tracker upgrades

19

Page 20: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

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• Advantages:– Low latency (no velocity factor)– Work over distances from few mm (internal triggers)

to ~Km (counting house) or far ( to satellite orbit)– Low mass – No fiber routing– Communicate between ID layers for trigger

decisions.

20

Development of Free-Space (fiberless) Links Utilizing Modulators

Page 21: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

21

Data path for on-board tracking trigger which could couple 2 planes of 3D doublets.

A trigger concept using modulators and prisms

Page 22: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

22 22

MEMS Mirrors for steering over ~ order 1 M distance

April 20, 2023 22

A commercially available MEMS mirror (Developed at ARI, Berkeley)

Argonne Center for Nan-scale Materials (CNM) developed novel MEMS mirrors that should solve the problems of commercial mirrors. The mirror is supported laterally and it can be actuated using 4 torsional actuators.

Page 23: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

23 23

A nice demonstration 1 Gb/s to a target moving ~1 cm at > 100 Hz

23

CW LASER1550 nm

optical electricADC TIA

DAC

SPI

SPI

X

Y

X

YAmpMEMS Mirrorto steer

Small Prism

850 nm LASER For alignment

ReflectionReflective lens

Rigid Coupling

GRIN lens to Capture

wires

wires

1550 LASER Beam

Modulator

Asphere Lensto launch

Si Detectors

This Assembly moves

SFP

FPGA Bit Error Tester

FPGAFPGA

Lookup table

Lookup table

Digital filter

Digital filter

No Bit errors overnight

Page 24: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

24 24

1 Gb/s over 80 Meters

ANL Long Range Free-Space Communication Telescope Demo

24

Page 25: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

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Modulator Plans• Radiation Test Luxtera Molex without the

microcontroller Protons 3.5 x min ioni. Gammas total dose up to 3 MR Neutrons • Radiation test components of Luxtera/Molex Voltage Regulator LaserATLAS Tilecal Demonstrator Tests Kintex 7 FPGARadiation test Other Devices and other materials For higher radiation environmentsDevelop other Optical Communication capabilities

Page 26: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

2626

Summary• Modulators are simple, reliable, fast• Silicon Integrated Technology exists for some HEP

applications• For ATLAS Tilecal demonstrator we expect: factor 106 lower BER, factor ~ 3 cost savings factor ~ 6 power savings simplification• We are continuing to test commercial and other

modulators• Have demonstrated precise beam steering with

MEMS mirrors

Page 27: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

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Backup

Page 28: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

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References

[1] KK. Gan, F. Vasay, T Weidberg, “Lessons Learned and to be Learned from LHC”, Joint ATLAS-CMS Working Group on Opto-Electronics for SLHC, ATL-COM-ELEC-2007-001 CMS-IN-2007/066

[2] Philippe Farthouat’s 2011 ATLAS upgrade talk[3] T. Weidberg “VCSEL Reliability Studies and Development of Robust VCSEL Arrays” TWIPP 2011 [4] W. Fernando, “Overview and status of ATLAS pixel detector”, Nucl.Instrum.Meth., A596, 58-62 (2008)[5] D. Giugni, S. Michal, R. Boyd, ATLAS PIXEL nSQP Project, ATL-IP-ES-0150[6] Papotti et. al ,“An Error-Correcting Line Code for a HEP Rad-Hard Multi-GigaBit Optical Link”, 12th Workshop on

Electronics For LHC and Future Experiments, Valencia, Spain, 25 - 29, pp.258-262 (2006)[7] Molex specifications (http://www.molex.com/molex/products/family?

key=fourteen_data_rate_fdr__active_optical_cable_aoc&channel=products&chanName=family&pageTitle=Introduction&parentKey=fiber_optic_product_families)

[8] J. Gilmore, TMB Mezzanine SEU Testing - Preliminary Results (www.physics.ohio-state.edu%2F~gilmore%2Fcms%2Fregulators%2Fcyclotron_report_v2.ppt)

[9] W. Pascher et al., “Modelling and design of a travelling-wave electro-optic modulator on InP”, Opt. Quant. Electron., vol. 35(4), 453-464 (2003)

[10] R. A. Soref and B.R. Bennett , “Electrooptical Effects In Silicon”, J. Quantum Electron., 23, 123 (1987)[11] M. Bruzzi, "Radiation damage in silicon detectors for high-energy physics experiments," Nuclear Science, IEEE

Transactions on , vol.48, no.4, pp.960-971, Aug 2001[12] S.T. Liu et al., "Total dose radiation hard 0.35 μm SOI CMOS technology," Nuclear Science, IEEE Transactions on , 45(6),

2442-2449 (1998)[13] F Vasey et al, “The Versatile Link common project: feasibility report”, JINST 7 C01075 (2012) doi:10.1088/1748-

0221/7/01/C01075 [14] HHI specifications (http://www.hhi.fraunhofer.de/en/departments/photonic-components/inp-modulators/)

[15] T. Pinguet et al. , "Monolithically integrated high-speed CMOS photonic transceivers," Group IV Photonics, 2008 5th IEEE International Conference on , vol., no., pp.362-364, 17-19 Sept. 2008

[16] C. Gunn, et al., “A 40Gbps CMOS Photonics Transceiver”, Proceedings of SPIE 6477, 64770N (2007).[17] BT Huffman et al.The Radiation Hardness of Certain Optical Fibres for the LHC Upgrades at -25C. JINST 2010 5 C11023.

28

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2929

ReferencesRD23 Collaboration, “Optoelectronic Analog Signal Transfer for LHC Detectors”.

CERN/DRDC/91-41/DRDC/P31. CERN, Geneva 1991.[PIXEL]W. Fernando, “Overview and status of ATLAS pixel detector”,. Nucl.

Instrum.Meth 2008; 58-62: A596.[KK] K.K.Gan, W. Fernando, H. Kagan, R. Kass, A. Law et al, “Radiation-Hard

Optical Link for SLHC”. Nucl.Instrum.Meth,2008:88, 2008:88-92:A596. L.S. Yan, Q.Yu, A.E.Willner (UCLA), "Simple Measurement of the Chirp Parameter

of Optical Modulators Using Partial Optical Filtering", Optoelectronics and semiconductor integrated Devices, P2.28, IEEE.

[CHIRP] "Simple Measurement of the Chirp Parameter of Optical Modulators Using Partial Optical Filtering", L.S. Yan, Q.Yu, A.E.Willner (UCLA) Optoelectronics and semiconductor integrated Devices P2.28 IEEE.

[LITHIUM] E.L. Wooton, et. al. (JDS Uniphase), ‘  “« A Review of Lithium Niobate Modulators for Fiber-Optic Communications Systems”, » ) IEEE Journal of Selected Topics in Quantum Electronics, Vol.6 No1,(, (2000) S 1077-260X(260X (00)01136-9.

[TIPP2011] W. Fernando, D. Underwood, R. Stanek, “Optical Data Links – Technology for Reliability and Free Space Links”, Physics Procedia, TIPP11-D-11-00045, (2012) to be published.

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[DPF] W. Fernando, D. Underwood, R. Stanek “New Optical Link Technologies for HEP Experiments”, Meeting of the Division of Particles and Fields of the American Physical Society, Brown University, August, 2011 arXiv:1109.6842v1.[IEEE] D. Underwood, P. DeLurgio, G. Drake, W. Fernando, D. Lopez, G. Drake, B. Salvachua-Ferrando, R. Stanek, “Development of Low Mass Optical Readout for High Data Bandwidth Systems” IEEE Nuclear Science Symposium Conference Record (NSS/MIC), 624-629, 2010.[IBM]W. Green, M. Rooks, L. Sekaric, and Y. Vlasov “Ultra-compact, low RF power, 10 Gb/s silicon Mach-Zehnder modulator”, Opt. Express 2007; 17106-17113:15.[JINST] D. Underwood, B. Salvachua-Ferrando, R. Stanek, D. Lopez, J. Liu, J. Michel, L. C. Kimerling, “New Optical Technology for low mass intelligent trigger and readout”,. JINST 5:C07011,2010.[InP] 40Gb/s InP Modulator ……………………………………… http://www.hhi.fraunhofer.de/fileadmin/hhi/downloads/PC/flyer/40_Gbits_InP_Web.pdf. [PIC] I.Galysh, K.Doherty, J. McGuire, H.Heidt, D.Niemi,G.Dutchover, (The StenSat Group) "CubeSat: Developing a Standard Bus for Picosatellites" http://www.stensat.org/Publications/SPIE.PDF.[FPGA] Z.K.Baker, M.E.Dunham, K.Morgan, M.Pigue, M.Stettler, P.Graham, E.N.Schmierer, J.Power (Los Alamos) “Space Based FPGA Radio receiver Design, Debug, and Development of a Radiation Tolerant Computing System”.International Journal of reconfigurable Computing, Volume 2010,Article ID 546217, doi:10.1155/2010/546217.

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Commercial integrated optics chips are a promising form of modulatorsFeatures - Speed- 10 Gb/fiber commercial integrated optics 40 Gb/fiber with some commercial units Laser reliability- Either CW laser onboard (different junction structure than VCSELs) Or displace laser outside detector. Low Error Rate 10-18 vs typical 10-12 for current systems Simplified error correction schemes Low power One CW laser - split many ways Modulators are very efficient Short electrical paths – no cable drivers Low voltage drivers – not current drivers Rad hard optical parts We have thoroughly tested silicon integrated optics for 64 K rad application Modulator parts should work at much higher levels Optical part expected to work at multi-Mrad levels

The Future of Optical Links - Light Modulators

Page 32: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

32 32

The commercial MEMS mirrors have ~40 dB resonance peaks at 1 and 3 KHz.

To use the direct feedback, developed an inverse Chebyshev filter which has a notch at 1 kHz, and appropriate phase characteristics (Left Figure)

With the filter we were able to make the beam follow a reflecting lens target within about 10 μm when the target moved about 1 mm (Right Figure).

Still has some fundamental issues at large excursion (~1 cm)

A separate feedback link solves this issue

The amplitude-frequency map of our analog feedback loop, demonstrating phase stability at 100 Hz.

A test setup used to demonstrate MEMS mirror steering with an analog control loop which compensates for the mirror resonances at 1 and 3 KHz.

April 20, 2023 32

Studies of Direct Feedback Concept

Page 33: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

33 33

Beams in Air: Size vs DistanceDue to diffraction, there is an optimum diameter for a beam for a given

distance in order to reduce 1/r2 losses

The Rayleigh distance acts much like Beta-Star in accelerators – Relates waist size and divergence– Depends on wavelength

If we start with a diameter too small for the distance of interest, the beam will diverge, and will become 1/r2 at the receiver, and we will have large losses (We can still focus what we get to a small device like an APD or PIN diode ). This is typical of space, Satellite, etc. applications.

If we start with an optimum diameter, the waist can be near the receiver, and we can capture almost all the light and focus it to a small spot

Examples, ~ 1 mm for 1 m, ~ 50 mm for 1 KmApril 20, 2023

Page 34: Modulator-Based, High Bandwidth Optical Links  for HEP Experiments

3434

Proven with a long term BER test on a random cable samples

Tests proved that there is no noise floor

BER Tested by Luxtera

A system has been developed to test in a Voltaire switch (model 4036) with continuous data flow

Switch is fully populated (36 ports) and data is injected in each port at 40Gbps.

Infiniband port counters are used to monitor the actual data flow and presence of errors

Test is run at room temperature.