Mid-infrared (longwave infrared) passive spectroscopic imaging with an uncooled microbolometer array sensor
Mid-infrared (longwave infrared) passive spectroscopic imaging with an uncooled microbolometer array sensor
复制标题
使用非制冷微测辐射热计阵列传感器进行中红外(长波红外)被动光谱成像
DOI:
10.1117/12.2635375
复制
发表时间:
2022
期刊:
影响因子:
--
通讯作者:
Ichiro Ishimaru
中科院分区:
文献类型:
--
作者:
Yusuke Morimoto;Shiori Tahara;So Yamashita;Daichi Anabuki;Tomoya Kitazaki;Hiroko Shimizu;Akira Nishiyama M.D;Kenji Wada;Ichiro Ishimaru
We aim to measure the glucose concentration in the body through passive mid-infrared spectroscopy using a palm-sized imaging two-dimensional Fourier spectrometer. Radiation in the mid-infrared region (at a wavelength of approximately 10 µm) is emitted from the object surface, with the intensity of the radiated light corresponding to the object temperature. Passive spectroscopy acquires component information from the spectral intensity of the radiated light emitted from the object without a light source. Intrinsic vibrations of molecules in the object itself are detected, and the spectral characteristics are thus the emission spectrum of intrinsic vibration peaks. In contrast, conventional active spectroscopy irradiates the measurement target with light and acquires spectral characteristics from the reflected light. Molecular vibrations excited by the light source are measured, and the spectral characteristics are thus absorption spectra of the energy absorbed at the eigenfrequency of the molecule. The wavelengths that are confirmed as absorption wavelengths in active spectroscopy are confirmed as emission wavelengths in passive spectroscopy. Active spectroscopy and passive spectroscopy thus have a negative–positive relationship. The imaging-type two-dimensional Fourier spectrometer (7 to 14 µm) used in past measurement has transmission optics. Using three Ge lenses for the front lens, objective lens, and imaging lens, we constructed reflective optics using reflective mirrors for the objective and imaging lenses. The reflective mirror guarantees flatness and high spectral reflectance over a wide bandwidth (3 to 20 µm), and the measurement bandwidth is thus extended.
影响因子:
1.9
作者:
Qi, Wei;Suzuki, Yo;Ishimaru, Ichiro
通讯作者:
Ishimaru, Ichiro
DOI:
10.1117/1.oe.55.11.110506
发表时间:
2016
期刊:
Opt. Eng.
影响因子:
--
作者:
Natsumi Kawashima;Ichiro Ishimaru;Ichiro Ishimaru;Ichiro ISHIMARU;Natsumi Kawashima
通讯作者:
Natsumi Kawashima