1 Institute of Modern Optics, Nankai University, Tianjin 300350, China; 2 Tianjin Key Laboratory of Optoelectronic Sensor and Sensing Network Technology, Tianjin 300350, China
Abstract The terahertz (THz) resonance, chirality, and polarization conversion properties of a double-layer chiral metasurface have been experimentally investigated by THz time domain spectroscopy system and polarization detection method. The special symmetric geometry of each unit cell with its adjacent cells makes a strong chiral electromagnetic response in this metasurface, which leads to a strong polarization conversion effect. Moreover, compared with the traditional THz transmission resonance sensing for film thickness, the polarization sensing characterized by polarization elliptical angle (PEA) and polarization rotation angle (PRA) shows a better Q factor and figure of merit (FoM). The results show that the Q factors of the PEA and PRA reach 43.8 and 49.1 when the interval film is 20 μm, while the Q factor of THz resonance sensing is only 10.6. And these PEA and PRA can play a complementary role to obtain a double-parameter sensing method with a higher FoM, over 4 times than that of resonance sensing. This chiral metasurface and its polarization sensing method provide new ideas for the development of high-efficiency THz polarization manipulation, and open a window to the high sensitive sensing by using THz polarization spectroscopy.
Fund: Project supported by the National Key Research and Development Program of China (Grant No. 2017YFA0701000), the National Natural Science Foundation of China (Grant Nos. 61971242, 61831012, and 61671491), the Natural Science Foundation of Tianjin City, China (Grant No. 19JCYBJC16600), and the Young Elite Scientists Sponsorship Program by Tianjin, China (Grant No. TJSQNTJ-2017-12).
Zi-Yang Zhang(张子扬), Fei Fan(范飞), Teng-Fei Li(李腾飞), Yun-Yun Ji(冀允允), Sheng-Jiang Chang(常胜江) Terahertz polarization conversion and sensing with double-layer chiral metasurface 2020 Chin. Phys. B 29 078707
[1]
Jansen C, Wietzke S, Peters O, Scheller M, Vieweg N, Salhi M, Krumbholz N, Jördens C, Hochrein T and Koch M 2010 Appl. Opt. 49 E48
[2]
Tu X C, Kang L L Xin H, Mao Q K, Wan C, Chen J, Jin B B, Ji Z M, Xu W W and Wu P H 2013 Chin. Phys. B 22 040701
[3]
Kleine-Ostmann T and Nagatsuma T 2011 J. Infrared Millimeter Terahertz Waves 32 143
[4]
Daryoosh Saeedkia 2013 Handbook of terahertz technology for imaging, sensing and communications, Vol. 1 (Woodhead Publishing) pp. 2, 3
[5]
Kaveev A K, Kropotov G I, Tsygankova E V, Tzibizov I A, Ganichev S D, Danilov S N, Olbrich P, Zoth C, Kaveeva E G, Zhdanov A I, Ivanov A A, Deyanov R Z and Redlich B 2013 Appl. Opt. 52 B60
[6]
Prinz V Y, Naumova E V, Golod S V, Seleznev V A, Bocharov A A and Kubarev V V 2017 Sci. Rep. 7 43334
[7]
Rahm M, Li J S and Padilla W J 2013 J. Infrared Millimeter Terahertz Waves 34 1
[8]
Mo W C, Wei X L, Wang K J, Li Y and Liu J S 2016 Opt. Express 24 13621
[9]
Monticone F and Alu A 2014 Chin. Phys. B 23 047809
[10]
Chen H Y, Wang J F, Ma H, Qu S B, Zhang J Q, Xu Z and Zhang A X 2015 Chin. Phys. B 24 014201
[11]
Smith D R, Pendry J B and Wiltshire M C K 2004 Science 305 788
[12]
Valev V K, Baumberg J J, Sibilia C and Thierry V 2013 Adv. Mater. 25 2517
[13]
Singh R, Plum E, Menzel C, Rockstuhl C, Azad A K, Cheville R A, Lederer F, Zhang W and Zheludev N I 2009 Phys. Rev. B 80 153104
[14]
Collins J T, Kuppe C, Hooper D C, Sibilia C, Centini M and Valev V K 2017 Adv. Opt. Mater. 5 1700182
[15]
Wegener M and Linden S 2009 Physics 2 3
[16]
Rodger A and Nordén B 1997 Circular dichroism and linear dichroism, Vol. 1 (Oxford: Oxford University Press) p. 2
[17]
Liu W W, Chen S Q, Li Z C, Cheng H, Yu P, Li J X and Tian J G 2015 Opt. Lett. 40 3185
[18]
Cheng Z and Cheng Y 2019 Opt. Commun. 435 178
[19]
Decker M, Zhao R, Soukoulis C M, Linden S and Wegener M 2010 Opt. Lett. 35 1593
[20]
O'Hara J F, Withayachumnankul W and Al-Naib I 2012 J. Infrared Millimeter Terahertz Waves 33 245
[21]
Beruete Mand Jáuregui-López I 2019 Adv. Opt. Mater. 1900721
[22]
Cong L Q, Tan S Y, Yahiaoui R, Yan F P, Zhang W L and Singh R J 2015 Appl. Phys. Lett. 106 031107
[23]
O'Hara J F, Singh R, Brener I, Smirnova E, Han J G, Taylor A J and Zhang W L 2008 Opt. Express 16 1786
[24]
Chen M, Fan F, Shen S, Wang X H and Chang S J 2016 Appl. Opt. 55 6471
[25]
Neu J, Aschaffenburg D J, Williams M R C and Schmuttenmaer C A 2017 IEEE Trans. Terahertz Sci. Technol. 7 755
[26]
Aydin K and Ozbay E 2007 J. Appl. Phys. 101 024911
[27]
Berry M V 1984 Proc. Roy. Soc. A: Math. Phys. Eng. Sci. 392 45
A self-powered and sensitive terahertz photodetection based on PdSe2 Jie Zhou(周洁), Xueyan Wang(王雪妍), Zhiqingzi Chen(陈支庆子), Libo Zhang(张力波), Chenyu Yao(姚晨禹), Weijie Du(杜伟杰), Jiazhen Zhang(张家振), Huaizhong Xing(邢怀中), Nanxin Fu(付南新), Gang Chen(陈刚), and Lin Wang(王林). Chin. Phys. B, 2022, 31(5): 050701.
No Suggested Reading articles found!
Viewed
Full text
Abstract
Cited
Altmetric
blogs
tweeters
Facebook pages
Wikipedia page
Google+ users
Online attention
Altmetric calculates a score based on the online attention an article receives. Each coloured thread in the circle represents a different type of online attention. The number in the centre is the Altmetric score. Social media and mainstream news media are the main sources that calculate the score. Reference managers such as Mendeley are also tracked but do not contribute to the score. Older articles often score higher because they have had more time to get noticed. To account for this, Altmetric has included the context data for other articles of a similar age.