This thesis presents photon-counting intensity interferometry measurements of spectrally filtered thermal light (λ = 653 nm, Δλ ≈ 1 nm) using a zero-baseline Hanbury Brown–Twiss setup. Two single-photon detector technologies are compared: silicon avalanche photodiodes (APDs) and superconducting nanowire single-photon detectors (SNSPDs) fabricated at TU Delft. Five configurations are investigated, progressing from an APD pair through single-pixel SNSPDs to four-pixel SNSPD arrays with TTCombiner channel combining. Photon bunching is observed in all configurations. The APD pair yields a bunching contrast of C = 2.28 × 10⁻³ with a FWHM of 510 ps. Single-pixel SNSPD operation reduces the FWHM to 293 ps but reveals jitter degradation at high count rates. The four-pixel configuration recovers the intrinsic timing resolution, achieving a FWHM of 89 ps — 5.7× narrower than the APD peak — and a bunching contrast of 8.96 × 10⁻³, a 3.9× improvement driven by the relation C ∝ 1/FWHM. The results validate multi-pixel SNSPD arrays as a transformative technology for stellar intensity interferometry.

This thesis presents photon-counting intensity interferometry measurements of spectrally filtered thermal light (λ = 653 nm, Δλ ≈ 1 nm) using a zero-baseline Hanbury Brown–Twiss setup. Two single-photon detector technologies are compared: silicon avalanche photodiodes (APDs) and superconducting nanowire single-photon detectors (SNSPDs) fabricated at TU Delft. Five configurations are investigated, progressing from an APD pair through single-pixel SNSPDs to four-pixel SNSPD arrays with TTCombiner channel combining. Photon bunching is observed in all configurations. The APD pair yields a bunching contrast of C = 2.28 × 10⁻³ with a FWHM of 510 ps. Single-pixel SNSPD operation reduces the FWHM to 293 ps but reveals jitter degradation at high count rates. The four-pixel configuration recovers the intrinsic timing resolution, achieving a FWHM of 89 ps — 5.7× narrower than the APD peak — and a bunching contrast of 8.96 × 10⁻³, a 3.9× improvement driven by the relation C ∝ 1/FWHM. The results validate multi-pixel SNSPD arrays as a transformative technology for stellar intensity interferometry.

Photon-Counting Intensity Interferometry with Superconducting Nanowire Single-Photon Detectors

HAKAMI NAJAFI, MOHSEN
2025/2026

Abstract

This thesis presents photon-counting intensity interferometry measurements of spectrally filtered thermal light (λ = 653 nm, Δλ ≈ 1 nm) using a zero-baseline Hanbury Brown–Twiss setup. Two single-photon detector technologies are compared: silicon avalanche photodiodes (APDs) and superconducting nanowire single-photon detectors (SNSPDs) fabricated at TU Delft. Five configurations are investigated, progressing from an APD pair through single-pixel SNSPDs to four-pixel SNSPD arrays with TTCombiner channel combining. Photon bunching is observed in all configurations. The APD pair yields a bunching contrast of C = 2.28 × 10⁻³ with a FWHM of 510 ps. Single-pixel SNSPD operation reduces the FWHM to 293 ps but reveals jitter degradation at high count rates. The four-pixel configuration recovers the intrinsic timing resolution, achieving a FWHM of 89 ps — 5.7× narrower than the APD peak — and a bunching contrast of 8.96 × 10⁻³, a 3.9× improvement driven by the relation C ∝ 1/FWHM. The results validate multi-pixel SNSPD arrays as a transformative technology for stellar intensity interferometry.
2025
Photon-Counting Intensity Interferometry with Superconducting Nanowire Single-Photon Detectors
This thesis presents photon-counting intensity interferometry measurements of spectrally filtered thermal light (λ = 653 nm, Δλ ≈ 1 nm) using a zero-baseline Hanbury Brown–Twiss setup. Two single-photon detector technologies are compared: silicon avalanche photodiodes (APDs) and superconducting nanowire single-photon detectors (SNSPDs) fabricated at TU Delft. Five configurations are investigated, progressing from an APD pair through single-pixel SNSPDs to four-pixel SNSPD arrays with TTCombiner channel combining. Photon bunching is observed in all configurations. The APD pair yields a bunching contrast of C = 2.28 × 10⁻³ with a FWHM of 510 ps. Single-pixel SNSPD operation reduces the FWHM to 293 ps but reveals jitter degradation at high count rates. The four-pixel configuration recovers the intrinsic timing resolution, achieving a FWHM of 89 ps — 5.7× narrower than the APD peak — and a bunching contrast of 8.96 × 10⁻³, a 3.9× improvement driven by the relation C ∝ 1/FWHM. The results validate multi-pixel SNSPD arrays as a transformative technology for stellar intensity interferometry.
Intensity interferom
Photon bunching
SNSPDs
Hanbury Brown Twiss
g2 correlation
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.12608/109629