Conference on Lasers and Electro-Optics 2021
DOI: 10.1364/cleo_si.2021.sw3d.3
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Entangled Two-Photon Absorption in Commercial Fluorophores

Abstract: Our study addresses the applicability of simple and common fluorophores for entangled two-photon fluorescence microscopy. Using CW-pumped SPDC waveguides, we can measure linear absorption rates of entangled photons in standard fluorophores in life science.

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Cited by 2 publications
(3 citation statements)
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“…Even with the limitations of the pump laser used here, the nanophotonic device presented in this work exhibits substantially improved brightness and efficiency compared to the state of the art for visible photon pair sources. 25,26 Our visible-near-IR device demonstrates improved efficiency and brightness even over other TFLN sources at the better-explored telecom band 12,58,59 and has comparable performance to the most efficient telecom TFLN source (Ref. 6 ) to date.…”
Section: Visible and Near-ir Spontaneous Parametric Down Conversionmentioning
confidence: 88%
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“…Even with the limitations of the pump laser used here, the nanophotonic device presented in this work exhibits substantially improved brightness and efficiency compared to the state of the art for visible photon pair sources. 25,26 Our visible-near-IR device demonstrates improved efficiency and brightness even over other TFLN sources at the better-explored telecom band 12,58,59 and has comparable performance to the most efficient telecom TFLN source (Ref. 6 ) to date.…”
Section: Visible and Near-ir Spontaneous Parametric Down Conversionmentioning
confidence: 88%
“…The device produces an on-chip efficiency of (2.3 ± 0.5) × 10 11 pairs/s/mW, which corresponds to a per-photon conversion efficiency of more than 1 photon pair converted in every 10,000 pump photons ((1.1 ± 0.2) × 10 −4 pairs/s/photon). This efficiency is nearly two orders of magnitude better than visible-light diffused waveguide SPDC sources 25 and is on par with the leading TFLN sources in the better-explored telecom regime. 6 The SPDC from this device exhibits a broad spectrum centered at 811 nm with a degenerate FWHM bandwidth of 117 nm and an average brightness of (1.6±0.3)×10 9 pairs/s/mW/nm, a number limited by at least an order of magnitude by the pump laser linewidth (0.8 nm).…”
Section: Introductionmentioning
confidence: 91%
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