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Step 07 Metrology / Characterization / Quantum Test Lab

Single-Photon Detectors (SPADs)

Room-temperature quantum herald measurements: single-photon generation verification, path entanglement, Hong-Ou-Mandel dip visibility. Si SPAD + InGaAs SPAD for 1550 nm telecom operation.

Excelitas SPCM / ID Quantique id230 CRITICAL ● Single-photon detection validates quantum coherence and entanglement on-chip

Role in QLT Fabrication

Single-photon avalanche diodes (SPADs) are the eyes of QLT's quantum photonic processor. Every quantum metric — g²(0) autocorrelation proving single-photon emission, Hong-Ou-Mandel (HOM) dip visibility proving photon indistinguishability, coincidence rates proving entanglement, and heralding efficiency proving source quality — depends on detecting individual photons with picosecond timing resolution at room temperature.

QLT's architecture requires two complementary detector technologies: silicon SPADs for visible-wavelength herald detection (from SPDC pump at 775 nm) and InGaAs/InP SPADs for telecom C-band (1550 nm) signal detection. Together with a time-to-digital converter (TDC), these detectors form the quantum characterization backbone that validates every fabrication step from waveguide loss measurement through final system-level boson sampling demonstrations.

  • g²(0) autocorrelation ● proves non-classical light: g²(0) < 0.5 confirms single-photon emission
  • HOM dip visibility ● measures photon indistinguishability: target V > 90%
  • Coincidence counting ● verifies entanglement and multi-photon interference
  • Heralding efficiency ● validates source brightness and coupling quality
  • Photon count rate ● measures quantum channel throughput (~10⁵–10⁶ counts/s)
  • SPAD timing jitter ● characterizes detector timing resolution (< 100 ps FWHM)

Key Quantum Measurements Enabled

MeasurementDetectors UsedChannelsSuccess Criterion
g²(0) autocorrelation2 × InGaAs SPAD (HBT setup)2 (start + stop)g²(0) < 0.5 → non-classical
HOM dip2 × InGaAs SPAD at BS outputs2–4Visibility > 90%
Photon count rate1 × SPAD per channel1–8~10⁵–10⁶ counts/s
Heralded single-photon1 × Si SPAD (herald) + 1 × InGaAs (signal)2Herald-conditioned g²(0) < 0.1
Multi-photon coincidence4–8 × InGaAs SPAD4–8N-fold rate matches theory
Dead-time characterization1 × SPAD + TDC1Dead time ≈ 20–50 ns

Technical Specifications

Silicon SPAD (Visible / Herald Channel)

ParameterExcelitas SPCM-AQRHMPD PDM Series
Spectral range400–1060 nm400–900 nm
Peak PDE> 70% @ 700 nm> 49% @ 550 nm
Dark count rate< 25 counts/s (typical)< 25 counts/s (50 μm)
Timing jitter350 ps FWHM35 ps FWHM (20 μm)
Dead time22 ns77 ns
Max count rate~35 Mcounts/s~13 Mcounts/s
After-pulse probability< 0.5%< 1%
Active area180 μm diameter20, 50, or 100 μm
OutputTTL pulse (4.2 V, 25 ns)NIM or TTL
CoolingInternal TEC (passive)Internal TEC
Fiber inputFC connector (multimode)FC/PC (SM optional)

InGaAs/InP SPAD (Telecom C-Band / 1550 nm)

ParameterID Quantique id230ID Quantique id Qube NIRMPD InGaAs
Spectral range900–1700 nm900–1700 nm900–1700 nm
PDE @ 1550 nm25% (free-running)25% (gated/free-run)20–30% (gated)
Dark count rate< 2 kHz @ 25% PDE< 1 kHz~5 kHz
Timing jitter~200 ps FWHM~250 ps FWHM~200 ps FWHM
Dead time1–25 μs (adjustable)~20 μs5–50 μs
Operating modeFree-running or gatedFree-runningGated
CoolingInternal TEC to -90°CTEC cooledTEC cooled
OutputTTL / NIMTTL (0–3.3 V)NIM (-0.8 V)
After-pulse< 3% @ 10 μs dead< 5%< 5%
Fiber inputFC/PC or FC/APC (SM)FC/PC (SM)FC/PC (SM)

System Timing Resolution

TIMING BUDGET — SPAD + TDC System:

Source of uncertainty         │ Value              │ Bottleneck?
──────────────────────────────┼────────────────────┼───────────
TDC digital resolution        │ 1 ps               │ No
TDC RMS jitter                │ 34 ps              │ No
TDC FWHM jitter               │ 80 ps              │ No
Si SPAD jitter (Excelitas)    │ 350 ps FWHM        │ YES — herald
Si SPAD jitter (MPD 20μm)    │ 35 ps FWHM         │ No
InGaAs SPAD jitter (id230)   │ 200 ps FWHM        │ YES — signal
──────────────────────────────┼────────────────────┼───────────
System timing (herald path)   │ √(80² + 350²)      │ ≈ 359 ps FWHM
System timing (signal path)   │ √(80² + 200²)      │ ≈ 215 ps FWHM
Coincidence window (HOM)      │ 1–10 ns            │ Adequate ✓

NOISE EQUIVALENT POWER (Si SPAD):
NEP = (hν / PDE) × √(2 × DCR)
    = (2.84e-19 / 0.70) × √(2 × 25)
    ≈ 2.9 × 10⁻¹⁸ W/√Hz   → excellent

Process Integration

QLT QUANTUM TEST LAB ● SPAD Detector Setup (Step 07):

CONFIGURATION A: Heralded Single-Photon Characterization
├── SPDC source (ppKTP, 775 nm pump)
│   ├── Signal (1550 nm) → fiber → chip input
│   └── Idler (775 nm herald) → fiber → Si SPAD (Excelitas)
├── Chip output → fiber → InGaAs SPAD (id230)
├── Both SPADs → SMA cables → Time Tagger 20 (TDC)
├── TDC → USB → Python (TimeTagger API)
│
├── Measurement 1: Count rate (singles on each channel)
├── Measurement 2: Coincidence rate (herald-signal pairs)
├── Measurement 3: g²(0) (Hanbury-Brown-Twiss correlation)
└── Measurement 4: Heralding efficiency = coincidence/herald

CONFIGURATION B: Hong-Ou-Mandel Dip
├── Two indistinguishable photons → two chip inputs
├── On-chip beam splitter (MZI)
├── Two outputs → 2 × InGaAs SPAD (id230)
├── Both SPADs → TDC channels 1 & 2
├── Scan: optical delay between input photons
├── Record: coincidence rate vs. delay
└── Result: HOM dip → visibility V = (R_max - R_min)/R_max
    Target: V > 90% (proves photon indistinguishability)

CONFIGURATION C: Boson Sampling Verification
├── 4–8 photons into mesh (from multiplexed source)
├── 8 mesh outputs → 8 × InGaAs SPAD
├── All 8 SPADs → TDC (8 channels)
├── Record: all multi-fold coincidence combinations
├── Compare: measured vs. permanent matrix theory
└── Result: validates quantum computational advantage

Vendor Options & Pricing

Silicon SPAD Modules (Visible / Herald)

ModelVendorKey SpecPrice (2025–2026)Lead Time
SPCM-AQRH-1xExcelitas Technologies> 70% PDE, 25 cps DCR, 350 ps jitter$3,500–$5,0004–6 weeks
PDM Series (50 μm)Micro Photon Devices49% PDE, 25 cps DCR, 35 ps jitter$8,000–$12,0006–8 weeks
τ-SPADPicoQuant~70% PDE, < 100 cps DCR$4,000–$7,0004–8 weeks
COUNT SeriesLaser Components~65% PDE, < 50 cps DCR$3,000–$5,0004–6 weeks

InGaAs SPAD Modules (1550 nm / Signal)

ModelVendorKey SpecPrice (2025–2026)Lead Time
id230ID Quantique25% PDE, 2 kHz DCR, free-running$15,000–$25,0004–8 weeks
id Qube NIRID Quantique25% PDE, 1 kHz DCR, compact$8,000–$12,0004–6 weeks
InGaAs SPADMicro Photon Devices20–30% PDE, gated mode$10,000–$18,0006–10 weeks
NIR SPAD ModuleAurea Technology25% PDE, free-running$12,000–$20,0006–8 weeks

SNSPD Upgrade Path (Future)

ModelVendorKey SpecPriceNotes
Eos SeriesSingle Quantum> 90% PDE, < 10 cps DCR, 15 ps jitter$150,000–$300,000Includes cryo-cooler; 4-channel
Photon SpotPhoton Spot Inc.> 85% PDE, < 100 cps DCR$100,000–$200,000Compact cryo-system; fiber-coupled
SNSPD SystemQuantum Opus> 80% PDE, fiber-coupled$120,000–$250,000Closed-cycle cryo; 2.1 K operation

Total System Budget

QLT SINGLE-PHOTON DETECTOR LAB:

Herald channel (visible):
├── 2 × Excelitas SPCM-AQRH          $7,000–$10,000
├── 2 × MPD PDM (low-jitter option)   $16,000–$24,000

Signal channel (1550 nm):
├── 4 × ID Quantique id Qube NIR      $32,000–$48,000
├── 4 × ID Quantique id230            $60,000–$100,000

Time-to-digital converter:
├── Swabian Time Tagger 20 (8 ch)     $8,000–$10,000

Accessories:
├── FC/PC fiber patch cords (×16)      $800
├── SMA cables 50Ω (×8)               $200
├── Optical attenuators (×4)           $400
├── BNC/SMA adapters                   $100

═══════════════════════════════════════════
MINIMUM CONFIG (4-ch InGaAs + 2-ch Si):
  $55,000–$80,000

FULL 8-CHANNEL CONFIG:
  $120,000–$200,000

WITH SNSPD UPGRADE (Phase 3):
  $1,000,000–$2,000,000
═══════════════════════════════════════════

Facility Requirements

ParameterSpecification
Optical tableVibration-isolated (Newport or TMC), 1.2 × 2.4 m minimum
Dark enclosureLight-tight box or curtained area (ambient light → false counts)
Power (SPAD modules)100–240 VAC, 50/60 Hz, < 100 W total (internal TEC)
Power (TDC)USB-powered (5 V, 500 mA) — no external supply
Temperature20–25°C (SPAD dark counts increase with temperature)
Humidity< 60% RH (prevent condensation on TEC-cooled detectors)
EMIKeep away from high-power switching supplies; shielded cables
Floor space~4 m² (optical table + detector rack)
Fiber infrastructureSM fiber (SMF-28e+) patch panels; FC/PC connectors throughout

Safety & Handling

HazardSourceRisk LevelControls
SPAD damage from ambient lightRoom lighting saturates detectorHIGHAlways cap fiber inputs when not in use; dark enclosure during measurements
SPAD damage from laser inputOptical power > 1 μW destroys detectorCRITICALAlways use attenuator before SPAD input; never connect laser directly
High voltage (SPAD bias)Internal bias ~25–75 V (InGaAs SPADs)LOWEnclosed module; no user-accessible HV; factory sealed
Laser safety (SPDC pump)775 nm pump laser (Class 3B/4)MEDIUMLaser safety eyewear; enclosed beam path; interlocked enclosure
ESD damageHandling fiber connectorsLOWESD wrist strap; proper connector cleaning procedure
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