• Chinese Journal of Lasers
  • Vol. 51, Issue 9, 0907001 (2024)
Kexiang Mou1、2, Zheng Tan1、3, Li Wang1、3, Xianping Sun1、3, Chaohui Ye1、2、3, and Xin Zhou1、2、3、*
Author Affiliations
  • 1National Key Laboratory of Magnetic Resonance Spectroscopy and Imaging, Innovation Academy for Precision Measurement Science and Technology, Chinese Academy of Sciences, Wuhan 430071, Hubei, China
  • 2Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan 430074, Hubei, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.3788/CJL231186 Cite this Article Set citation alerts
    Kexiang Mou, Zheng Tan, Li Wang, Xianping Sun, Chaohui Ye, Xin Zhou. Advancements in Nuclear Magnetic Resonance Research Based on Laser Pumped Atomic Sensors[J]. Chinese Journal of Lasers, 2024, 51(9): 0907001 Copy Citation Text show less
    Schematic diagram of NMR measurement based on LPAS (ST: sample transmission; MS: magnetic shield; LPAS: laser-pumped atomic sensors). (a) Enhanced polarization of the sample under investigation; (b) the sample after enhanced polarization is transferred to the LPAS measurement area for NMR measurement
    Fig. 1. Schematic diagram of NMR measurement based on LPAS (ST: sample transmission; MS: magnetic shield; LPAS: laser-pumped atomic sensors). (a) Enhanced polarization of the sample under investigation; (b) the sample after enhanced polarization is transferred to the LPAS measurement area for NMR measurement
    Schematic diagram of LPAS (BD: balanced photodetector; PBS: polarizing beam splitter)
    Fig. 2. Schematic diagram of LPAS (BD: balanced photodetector; PBS: polarizing beam splitter)
    Schematic diagram of an NMOR LPAS
    Fig. 3. Schematic diagram of an NMOR LPAS
    Zero-field NMR spectrum of natural isotope abundance 15N-pyridine with SABRE polarization measured by commercial LPAS, where the SABRE reaction scheme is shown in the inset[49]
    Fig. 4. Zero-field NMR spectrum of natural isotope abundance 15N-pyridine with SABRE polarization measured by commercial LPAS, where the SABRE reaction scheme is shown in the inset[49]
    Detailed structure of the high-frequency multiplets in the ZF-TOCSY spectrum of 1-13C ethanol[64]
    Fig. 5. Detailed structure of the high-frequency multiplets in the ZF-TOCSY spectrum of 1-13C ethanol[64]
    Magnetic shieldless 3D ultralow field MRI of digital model[89]. (a) FT-LPAS 3D ultralow field MRI measuring device; (b) geometry of the digital model; (c) digital model 3D imaging slices, the direction is from H plane to K plane of the model
    Fig. 6. Magnetic shieldless 3D ultralow field MRI of digital model[89]. (a) FT-LPAS 3D ultralow field MRI measuring device; (b) geometry of the digital model; (c) digital model 3D imaging slices, the direction is from H plane to K plane of the model
    LPASYearTypeAtomic vapor cellSensitivity /(fT/Hz1/2Ref.
    Conventional2010SERFK0.1612
    2010SERFRb567
    2012SERFRb6‒1168
    2013NMORCs15032
    2014SERFK-Rb569
    2015SERFCs5570
    2017SERFRb1871
    2022SERFRb8.8972
    2023NMORRb42.6773
    Miniaturization2017SERFRb2074
    2017SERFCs4075
    2018SERFRb676
    2018SERFRb1077
    2020SERFRb1678
    2022SERFRb2579
    Table 1. Advances in LPAS
    Kexiang Mou, Zheng Tan, Li Wang, Xianping Sun, Chaohui Ye, Xin Zhou. Advancements in Nuclear Magnetic Resonance Research Based on Laser Pumped Atomic Sensors[J]. Chinese Journal of Lasers, 2024, 51(9): 0907001
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