-
The laser frequency scanning interferometer has several advantages, such as non-contact, high accuracy and low signal to noise ratio in detection. In order to achieve higher resolution of the laser frequency scanning interferometer, increasing the tuning range of the light source and reducing the tuning non-linearity have become the key factors. The commonly used method is to correct the non-linearity of the wide bandwidth external cavity tuning laser by a fiber optical auxiliary interferometer constructed external frequency sampling clock. When using the broadband external cavity tuning laser and the auxiliary interferometer with an optical path difference of 220 m, it is found experimentally that the single-mode fiber dispersion makes the frequency of sampled signals change over time, causing the spectrum to broaden and resolution to decline. This paper has established the dispersion mismatch model which shows that the fiber dispersion of the auxiliary interferometer causes linear chirp frequency changes during the measurement of signals. The linear chirp frequency is proportional to the tuning bandwidth and measured distance. The phenomenon and theoretical model of dispersion mismatch is verified by experiments. The results for targets in the air are shown to linearly decrease as the tuning range increases with the maximum offset of 156.3 µm for the 20 nm tuning bandwidth. The experiment also proves the peak broadening intensifies with increasing distance measured, and thus verifies as the time delay of free space increase, and the peak broadening and distortion also increases. This result means that it will limit the ranging distance and make large errors in measurement result for long distance targets. The dispersion of the auxiliary interferometer should be compensated in the laser frequency scanning interferometer for large-sized high resolution measurements. In this paper, phase dispersion compensation method based on the evolution of peak variation distortion elimination is proposed, by taking the peak amplitude variation as the criterion; the phase compensation can offset the dispersion and improve the resolution. The original signal is multiplied by the complex phase compensation term, then regulating the phase compensation factor, the chirp becomes smaller as the phase compensation factor is approaching the distortion factor. Under the condition that the phase compensation factor is equal to the distortion factor, the chirp is offset. Then, the relationship between the amplitude and the peak FWHM is studied. It is found that the peak FWHM decreases while the amplitude shows a gradually increasing trend. Therefore, the amplitude can be referred to in order to determine whether the peak FWHM reaches the minimum. The resolution for target's peak can be improved by searching for the maximum amplitude of the spectrum and adjusting the phase distortion coefficient. The experiment shows that the peak FWHM of the target is obviously narrowed after dispersion compensation. The peak value becomes close to the theoretical resolution, and the static target at a distance of 975.216254 mm from the laser frequency scanning interferometer is measured. Results show the measurement accuracy of the interferometer is 584 nm. To further verify the accuracy of the laser frequency scanning interferometer, the laser frequency scanning interferometer is compared with the Renishaw laser interferometer in the measurement range of 0692 mm. The standard deviation between them is 4.5 m. The proposed method is put forward to provide basis for future studies on the large size high resolution laser frequency scanning interferometer.
-
Keywords:
- interferometry /
- laser frequency scanning interferometer /
- laser ranging /
- fiber dispersion
[1] Tan L Q, Hua D X, Wang L, Gao F, Di H G 2014 Acta Phys. Sin. 63 224205 (in Chinese) [谭林秋, 华灯鑫, 汪丽, 高飞, 狄慧鸽 2014 物理学报 63 224205]
[2] Hao Y Q, Ye Q, Pan Z Q, Cai H W, Qu R H 2014 Chin. Phys. B 23 110703
[3] Wen X D, Ning T G, You H D, Kang Z X, Li J, Li C, Feng T, Yu S W, Jian W 2014 Chin. Phys. Lett. 31 034203
[4] Zhang R W, Sun X J, Yan W, Liu L, Li Y, Zhao J, Yan W X, Li H R 2014 Acta Phys. Sin. 63 140702 (in Chinese) [张日伟, 孙学金, 严卫, 刘磊, 李岩, 赵剑, 颜万祥, 李浩然 2014 物理学报 63 140702]
[5] Eric D M, Robert R M 2008 Opt. Express 16 13139
[6] John D, Ben H, Andrew J L, Andrew J L, Armin J H R, Matthew S W 2014 Opt. Express 22 24869
[7] Tao L, Liu Z G, L T, Deng Z W, Gong H 2014 Acta Optica Sinica34 0212002 (in Chinese) [陶龙, 刘志刚, 吕涛, 邓忠文, 龚海 2014 光学学报 34 0212002]
[8] Yan X, Dong J Q, Li Q H, Guo M S, Hu Y Q 2014 Chinese Journal of Lasers41 0908001 (in Chinese) [严鑫, 董俊卿, 李青会, 郭木森, 胡永庆 2014 中国激光 41 0908001]
[9] Koichi I, Shin-ichiro M, Takao K, Takeo M 2011 IEEE Photon. Technol. Lett. 23 703
[10] Ana B M, Zeb W B 2015 Appl. Opt. 54 5911
[11] Brian J S, Dawn K G, Matthew S W, Mark E F 2005 Opt. Express 13 666
[12] Zhao C, Chen Z Y, Ding Z H, Li P, Shen Y, Ni Y 2014 Acta Phys. Sin. 63 194201 (in Chinese) [赵晨, 陈志彦, 丁志华, 李鹏, 沈毅, 倪秧 2014 物理学报 63 194201]
[13] Zeb W B, Wm R B, Brant K, Randy R R, Peter A R 2010 Appl. Opt. 49 213
[14] Yusuke K, Fan X Y, Fumihiko I, He Z Y, Kazuo H 2013 J. Lightw. Technol. 31 866
[15] Evan M L, Justin W K, Mark E F, Emily E H US Patent 105911[2014-07-03]
[16] Maciej W, Vivek J S, Tony H K, James G F, Andrzej K, Jay S D 2004 Opt. Express 12 2404
-
[1] Tan L Q, Hua D X, Wang L, Gao F, Di H G 2014 Acta Phys. Sin. 63 224205 (in Chinese) [谭林秋, 华灯鑫, 汪丽, 高飞, 狄慧鸽 2014 物理学报 63 224205]
[2] Hao Y Q, Ye Q, Pan Z Q, Cai H W, Qu R H 2014 Chin. Phys. B 23 110703
[3] Wen X D, Ning T G, You H D, Kang Z X, Li J, Li C, Feng T, Yu S W, Jian W 2014 Chin. Phys. Lett. 31 034203
[4] Zhang R W, Sun X J, Yan W, Liu L, Li Y, Zhao J, Yan W X, Li H R 2014 Acta Phys. Sin. 63 140702 (in Chinese) [张日伟, 孙学金, 严卫, 刘磊, 李岩, 赵剑, 颜万祥, 李浩然 2014 物理学报 63 140702]
[5] Eric D M, Robert R M 2008 Opt. Express 16 13139
[6] John D, Ben H, Andrew J L, Andrew J L, Armin J H R, Matthew S W 2014 Opt. Express 22 24869
[7] Tao L, Liu Z G, L T, Deng Z W, Gong H 2014 Acta Optica Sinica34 0212002 (in Chinese) [陶龙, 刘志刚, 吕涛, 邓忠文, 龚海 2014 光学学报 34 0212002]
[8] Yan X, Dong J Q, Li Q H, Guo M S, Hu Y Q 2014 Chinese Journal of Lasers41 0908001 (in Chinese) [严鑫, 董俊卿, 李青会, 郭木森, 胡永庆 2014 中国激光 41 0908001]
[9] Koichi I, Shin-ichiro M, Takao K, Takeo M 2011 IEEE Photon. Technol. Lett. 23 703
[10] Ana B M, Zeb W B 2015 Appl. Opt. 54 5911
[11] Brian J S, Dawn K G, Matthew S W, Mark E F 2005 Opt. Express 13 666
[12] Zhao C, Chen Z Y, Ding Z H, Li P, Shen Y, Ni Y 2014 Acta Phys. Sin. 63 194201 (in Chinese) [赵晨, 陈志彦, 丁志华, 李鹏, 沈毅, 倪秧 2014 物理学报 63 194201]
[13] Zeb W B, Wm R B, Brant K, Randy R R, Peter A R 2010 Appl. Opt. 49 213
[14] Yusuke K, Fan X Y, Fumihiko I, He Z Y, Kazuo H 2013 J. Lightw. Technol. 31 866
[15] Evan M L, Justin W K, Mark E F, Emily E H US Patent 105911[2014-07-03]
[16] Maciej W, Vivek J S, Tony H K, James G F, Andrzej K, Jay S D 2004 Opt. Express 12 2404
Catalog
Metrics
- Abstract views: 5588
- PDF Downloads: 254
- Cited By: 0
下载:
