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[论文解读] Polymer identification via undetected photons using a low footprint nonlinear interferometer

Atta Ur Rehman Sherwani, Emma Pearce|arXiv (Cornell University)|Mar 23, 2026
Mechanical and Optical Resonators被引用 0
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ABSTRACT

Plastic pollution has become a critical global challenge, with microplastics pervading ecosystems and entering human food chains. Effectively monitoring this widespread contamination demands rapid, reliable, and portable material identification techniques that often elude conventional Raman and FTIR spectroscopy. Undetected photon spectroscopy within a nonlinear interferometer (NLI) offers a solution, allowing the retrieval of mid-infrared absorption spectra by detecting only near-infrared signal photons using standard silicon-based technology. Here, we demonstrate a highly compact, micro-integrated, thermally-stabilised NLI with a Michelson-like geometry designed for the rapid spectroscopy of plastics. We benchmarked its room-temperature performance, demonstrating a signal-to-noise ratio of 34 with a measurement rate of 100 Hz and a spectral resolution of 6 cm$^{-1}$. We show that we can accurately and rapidly retrieve the characteristic vibrational absorption spectra of common polymers such as polypropylene, polyethene, and polystyrene, without using mid-infrared technology. These results establish our compact module as a promising field-deployable platform for robust, real-time environmental monitoring systems and other mid-infrared spectroscopy applications.

研究动机与目标

  • 为快速聚合识别在 3060–2790 cm⁻¹ 区间开发紧凑、热稳定的非线性干涉仪(NLI)模块。
  • 证明可以通过未探测的光子在近红外检测下获取中红外光谱。
  • 在室温下实现高信噪比和约 6 cm⁻¹ 的光谱分辨率,适用于常见聚合物。
  • 将性能与传统的 FTIR/ATR 光谱对 PP、PE、PS 等聚合物进行基准比较。

提出的方法

  • 使用 ppKTP 的自发参数下转换生成相关的近红外信号光子(901–923 nm)和 MIR 器光子(3.26–3.58 μm)。
  • 实现带双通道的 Michelson 式微集成 NLI,采用双通路几何,将器代吸收映射到信号可见度。
  • 利用 Hilbert 变换包络法和 Beer–Lambert 转换从单一干涉图提取透射光谱。
  • 通过 SNR、Allan-Werle 偏差,以及固定工作点(OPLD ~1.45 mm)来表征性能,以在分辨率 (~6 cm⁻¹) 与可见度 (≈18.5%) 之间取得平衡。
  • 通过比较获取的吸收光谱与 ATR-FTIR 参考,演示对 PP、PE、PS 的识别。
Figure 1: Schematic of the Michelson-type NLI. A pump laser (720 nm, shown in blue) is focused into a nonlinear crystal (ppKTP), generating correlated NIR signal (901 - 923 nm, shown in green) and MIR idler photons (3.26 - 3.58 µm, shown in red) via SPDC. The pump and signal are separated from the i
Figure 1: Schematic of the Michelson-type NLI. A pump laser (720 nm, shown in blue) is focused into a nonlinear crystal (ppKTP), generating correlated NIR signal (901 - 923 nm, shown in green) and MIR idler photons (3.26 - 3.58 µm, shown in red) via SPDC. The pump and signal are separated from the i

实验结果

研究问题

  • RQ1紧凑型 NLI 是否能够使用硅探测器在未探测 MIR 光子的条件下获取准确的 MIR 吸收光谱?
  • RQ2在用于聚合物光谱学的微集成 NLI 中,光谱分辨率、可见度和 SNR 之间的权衡为何?
  • RQ3与在野外便携光谱学相比,该系统在识别常见塑料方面的性能(SNR、分辨率)如何?
  • RQ4哪些优化路径(晶体长度、材料、泵提升)可以扩大动态范围并提速以便在野外部署?

主要发现

  • 在 10 ms 整合时间下实现单拍 SNR 为 34。
  • 在 3060–2790 cm⁻¹ MIR 窗口内实现约 6 cm⁻¹ 的光谱分辨率。
  • 获取的 PP、PE、PS 的中红外吸收特征与 ATR-FTIR 参考高度一致。
  • 识别 ppKTP 在 ~3.45 μm 附近的固有吸收,成为可见度及动态范围的限制因素。
  • 测得最大可见度约 18.5%(在强吸收处下降至 ~5%),影响某些波段的 SNR。
  • 在泵提升与晶体更短情况下预测可提升的 SNR,可能实现更快速率(高达 kHz)和高光谱成像。
Figure 2: Measurement and data-extraction procedure for a polypropylene (PP) film using our single-shot scheme (a) A reference interferogram taken without the sample (dark cyan) and an interferogram taken with the sample (red). The shaded region indicates the region omitted for further processing (b
Figure 2: Measurement and data-extraction procedure for a polypropylene (PP) film using our single-shot scheme (a) A reference interferogram taken without the sample (dark cyan) and an interferogram taken with the sample (red). The shaded region indicates the region omitted for further processing (b

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