TY - JOUR
T1 - Time-Resolved Raman Spectrometer with High Fluorescence Rejection Based on a CMOS SPAD Line Sensor and a 573-nm Pulsed Laser
AU - Talala, Tuomo
AU - Kaikkonen, Ville A.
AU - Keranen, Pekka
AU - Nikkinen, Jari
AU - Härkönen, Antti
AU - Savitski, Vasili G.
AU - Reilly, Sean
AU - Dziechciarczyk, Ukasz
AU - Kemp, Alan J.
AU - Guina, Mircea
AU - Mäkynen, Anssi J.
AU - Nissinen, Ilkka
N1 - Funding Information:
Manuscript received November 9, 2020; accepted January 5, 2021. Date of publication January 26, 2021; date of current version February 12, 2021. The work at the University of Oulu was supported by the Academy of Finland, under Contract 314404, Contract 323719, and Contract 314405. The work at Tampere University was supported in part by the Academy of Finland, under Contract 281955 and in part by the Co-Innovation Project of Business Finland, “3DLidar.” The work at Strathclyde was supported in part by the European Research Council under Grant 278389 and Grant 727738, in part by the UK EPSRC under Grant EP/P00041X/1 and Grant EP/L015315/1, in part by the Fraunhofer UK Research Ltd., in part by the Royal Academy of Engineering, and in part by the Element 6 (UK) Ltd. The Associate Editor coordinating the review process was Sabrina Grassini. (Corresponding author: Tuomo Talala.) Tuomo Talala, Pekka Keränen, and Ilkka Nissinen are with the Circuits and Systems Research Unit, University of Oulu, 90014 Oulu, Finland (e-mail: [email protected]).
Publisher Copyright:
© 1963-2012 IEEE.
PY - 2021
Y1 - 2021
N2 - A time-resolved Raman spectrometer is demonstrated based on a 256\times 8 single-photon avalanche diodes fabricated in CMOS technology (CMOS SPAD) line sensor and a 573-nm fiber-coupled diamond Raman laser delivering pulses with duration below 100-ps full-width at half-maximum (FWHM). The collected backscattered light from the sample is dispersed on the line sensor using a custom volume holographic grating having 1800 lines/mm. Efficient fluorescence rejection in the Raman measurements is achieved due to a combination of time gating on sub-100-ps time scale and a 573-nm excitation wavelength. To demonstrate the performance of the spectrometer, fluorescent oil samples were measured. For organic sesame seed oil having a continuous wave (CW) mode fluorescence-to-Raman ratio of 10.5 and a fluorescence lifetime of 2.7 ns, a signal-to-distortion value of 76.2 was achieved. For roasted sesame seed oil having a CW mode fluorescence-to-Raman ratio of 82 and a fluorescence lifetime of 2.2 ns, a signal-to-distortion value of 28.2 was achieved. In both cases, the fluorescence-to-Raman ratio was reduced by a factor of 24-25 owing to time gating. For organic oil, spectral distortion was dominated by dark counts, while for the more fluorescent roasted oil, the main source of spectral distortion was timing skew of the sensor. With the presented postprocessing techniques, the level of distortion could be reduced by 88%-89% for both samples. Compared with common 532-nm excitation, approximately 73% lower fluorescence-to-Raman ratio was observed for 573-nm excitation when analyzing the organic sesame seed oil.
AB - A time-resolved Raman spectrometer is demonstrated based on a 256\times 8 single-photon avalanche diodes fabricated in CMOS technology (CMOS SPAD) line sensor and a 573-nm fiber-coupled diamond Raman laser delivering pulses with duration below 100-ps full-width at half-maximum (FWHM). The collected backscattered light from the sample is dispersed on the line sensor using a custom volume holographic grating having 1800 lines/mm. Efficient fluorescence rejection in the Raman measurements is achieved due to a combination of time gating on sub-100-ps time scale and a 573-nm excitation wavelength. To demonstrate the performance of the spectrometer, fluorescent oil samples were measured. For organic sesame seed oil having a continuous wave (CW) mode fluorescence-to-Raman ratio of 10.5 and a fluorescence lifetime of 2.7 ns, a signal-to-distortion value of 76.2 was achieved. For roasted sesame seed oil having a CW mode fluorescence-to-Raman ratio of 82 and a fluorescence lifetime of 2.2 ns, a signal-to-distortion value of 28.2 was achieved. In both cases, the fluorescence-to-Raman ratio was reduced by a factor of 24-25 owing to time gating. For organic oil, spectral distortion was dominated by dark counts, while for the more fluorescent roasted oil, the main source of spectral distortion was timing skew of the sensor. With the presented postprocessing techniques, the level of distortion could be reduced by 88%-89% for both samples. Compared with common 532-nm excitation, approximately 73% lower fluorescence-to-Raman ratio was observed for 573-nm excitation when analyzing the organic sesame seed oil.
KW - Fluorescence rejection
KW - Raman laser
KW - Raman spectrometer
KW - Raman spectroscopy
KW - single-photon avalanche diode (SPAD) sensor
KW - time gating
KW - time-correlated single-photon counting
KW - timing skew
U2 - 10.1109/TIM.2021.3054679
DO - 10.1109/TIM.2021.3054679
M3 - Article
AN - SCOPUS:85100492086
SN - 0018-9456
VL - 70
JO - IEEE Transactions on Instrumentation and Measurement
JF - IEEE Transactions on Instrumentation and Measurement
M1 - 9335980
ER -