Saitoh Naoki, Akiba Norimitsu
Second Forensic Science Division, National Research Institute of Police Science, 6-3-1 Kashiwanoha, Kashiwa, Chiba 277-0882, Japan.
ScientificWorldJournal. 2005 May 2;5:355-66. doi: 10.1100/tsw.2005.43.
We have studied inherent fluorescence spectra and imaging of fingerprints in the deep ultraviolet (UV) region with a nanosecond-pulsed Nd-YAG laser system that consists of a tunable laser, a cooled CCD camera, and a grating spectrometer. In this paper, we have studied UV fluorescence spectra of fingerprints under 266-nm illumination. Fluorescence spectra of fingerprints have two main peaks, around 330 nm (peak A) and 440 nm (peak B). At first, when a fingerprint has just been pressed, peak A is dominant. However, its intensity reduces as the total illumination time increases. On the other hand, peak B is weak at first. It appears after enough 266-nm illumination and its intensity increases as time elapses. After 3 h of illumination, peak A almost diminishes and peak B becomes dominant. By leaving the fingerprint under a fluorescent lamp in a room without laser illumination, peak A can be restored partly, while the intensity of peak B still increases. Time-resolved fluorescence spectra were also measured for these two peaks. The lifetime of each peak is 2.0 nsec (peak A) and 6.2 nsec (peak B) on average. Both peaks seem to consist of several components with different lifetimes. In the case of peak A, the 330-nm peak decays fast and a new component at 360 nm becomes dominant when the delay time exceeds 20 nsec. In the case of peak B, unlike peak A, no clear peak separation is observed, but the peak position seems to move from 440 to 460 nm when the delay time becomes larger.
我们使用由可调谐激光器、冷却电荷耦合器件(CCD)相机和光栅光谱仪组成的纳秒脉冲Nd-YAG激光系统,研究了深紫外(UV)区域指纹的固有荧光光谱和成像。在本文中,我们研究了266纳米光照下指纹的紫外荧光光谱。指纹的荧光光谱有两个主要峰值,分别在330纳米左右(峰值A)和440纳米左右(峰值B)。起初,刚按下指纹时,峰值A占主导。然而,随着总光照时间增加,其强度会降低。另一方面,峰值B起初较弱。在足够的266纳米光照后出现,且其强度随时间增加。光照3小时后,峰值A几乎消失,峰值B占主导。将指纹置于室内无激光照射的荧光灯下,峰值A可部分恢复,而峰值B的强度仍会增加。还测量了这两个峰值的时间分辨荧光光谱。每个峰值的平均寿命分别为2.0纳秒(峰值A)和6.2纳秒(峰值B)。两个峰值似乎都由几个具有不同寿命的成分组成。对于峰值A,当延迟时间超过20纳秒时,330纳米的峰值快速衰减,360纳米处的新成分占主导。对于峰值B,与峰值A不同,未观察到明显的峰值分离,但当延迟时间变大时,峰值位置似乎从440纳米移至460纳米。