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Analysis of optical properties of bio-smoke materials in the 0.25–14 μm band 被引量:2

Analysis of optical properties of bio-smoke materials in the 0.25–14 μm band
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摘要 At present, research into optical properties of bio-smoke materials mostly concentrates on single band or single germplasm. Herein, we measured the spectral reflectance of three eukaryotic bio-smoke materials and three prokaryotic bio-smoke materials in the waveband from 0.25 μm to 14μm. Based on the Kramers-Kroning algorithm, the complex refractive index m(λ) was calculated and the Fourier-transform infrared(FTIR) spectra of materials were analyzed. The results show that n(λ) of bio-smoke materials varies between 1.1-2, and n(λ) values in the visible light to near-infrared wavebands are significantly larger than those in other wavebands. The k(λ) of bio-smoke materials varies between 0-0.4.At 6-6.5 μm, k(λ) of prokaryotic materials is 3 times that of eukaryotic materials, which is caused by C=O stretching vibration of amide I and C-N stretching vibration of amide Ⅱ in proteins. At 2.5-3 μm and 9.75 μm, k(λ) values of eukaryotic bio-smoke materials are nearly 2 times that of prokaryotic ones. The absorption peak at 2.5-3 μm is mainly triggered by C-H stretching vibration in lipid and O-H stretching vibration in bound water. The absorption peak at 9.75 μm is mainly caused by symmetric stretching vibration of PO2-in nucleic acids. At present, research into optical properties of bio-smoke materials mostly concentrates on single band or single germplasm. Herein, we measured the spectral reflectance of three eukaryotic bio-smoke materials and three prokaryotic bio-smoke materials in the waveband from 0.25 μm to 14μm. Based on the Kramers-Kroning algorithm, the complex refractive index m(λ) was calculated and the Fourier-transform infrared(FTIR) spectra of materials were analyzed. The results show that n(λ) of bio-smoke materials varies between 1.1-2, and n(λ) values in the visible light to near-infrared wavebands are significantly larger than those in other wavebands. The k(λ) of bio-smoke materials varies between 0-0.4.At 6-6.5 μm, k(λ) of prokaryotic materials is 3 times that of eukaryotic materials, which is caused by C=O stretching vibration of amide I and C-N stretching vibration of amide Ⅱ in proteins. At 2.5-3 μm and 9.75 μm, k(λ) values of eukaryotic bio-smoke materials are nearly 2 times that of prokaryotic ones. The absorption peak at 2.5-3 μm is mainly triggered by C-H stretching vibration in lipid and O-H stretching vibration in bound water. The absorption peak at 9.75 μm is mainly caused by symmetric stretching vibration of PO2-in nucleic acids.
作者 赵欣颖 胡以华 顾有林 陈曦 王新宇 王鹏 董骁 Xinying Zhao;Yihua Hu;Youlin Gu;Xi Chen;Xinyu Wang;Peng Wang;Xiao Dong(State Key Laboratory of Pulsed Power Laser Technology,National University of Defense Technology,Hefei 230037,China;Anhui Province Key Laboratory of Electronic Restriction,National University of Defense Technology,Hefei 230037,China;Key Laboratory of Ion Beam Bioengineering,Hefei Institutes of Physical Science,Chinese Academy of Sciences,Hefei 230001,China)
出处 《Chinese Physics B》 SCIE EI CAS CSCD 2019年第3期168-174,共7页 中国物理B(英文版)
基金 supported by the National Natural Science Foundation of China(Grant Nos.61271353 and 60908033) the Natural Science Foundation of Anhui Province,China(Grant No.1408085MKL47)
关键词 bio-smoke MATERIALS complex refractive index EUKARYOTIC PROKARYOTIC bio-smoke materials complex refractive index eukaryotic prokaryotic
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