Abstract Hexagonal WO3 nanorods are fabricated by a facile hydrothermal process at 180 ℃ using sodium tungstate and sodium chloride as starting materials. The morphology, structure, and composition of the prepared nanorods are studied by scanning electron microscopy, X-ray diffraction spectroscopy, and energy dispersive spectroscopy. It is found that the agglomeration of the nanorods is strongly dependent on the PH value of the reaction solution. Uniform and isolated WO3 nanorods with diameters ranging from 100 nm-150 nm and lengths up to several micrometers are obtained at PH=2.5 and the nanorods are identified as being hexagonal in phase structure. The sensing characteristics of the WO3 nanorod sensor are obtained by measuring the dynamic response to NO2 with concentrations in the range 0.5 ppm-5 ppm and at working temperatures in the range 25 ℃-250 ℃. The obtained WO3 nanorods sensors are found to exhibit opposite sensing behaviors, depending on the working temperature. When being exposed to oxidizing NO2 gas, the WO3 nanorod sensor behaves as an n-type semiconductor as expected when the working temperature is higher than 50 ℃, whereas, it behaves as a p-type semiconductor below 50 ℃. The origin of the n-to p-type transition is correlated with the formation of an inversion layer at the surface of the WO3 nanorod at room temperature. This finding is useful for making new room temperature NO2 sensors based on hexagonal WO3 nanorods.
Fund: Project supported by the National Natural Science Foundation of China (Grant Nos. 60771019, 61271070, and 61274074) and the Tianjin Key Research Program of Application Foundation and Advanced Technology, China (Grant No. 11JCZDJC15300).
Corresponding Authors:
Hu Ming
E-mail: huming@tju.edu.cn
About author: 07.07.Df; 61.62.Fk; 78.67.Qa
Cite this article:
Wu Ya-Qiao (武雅乔), Hu Ming (胡明), Wei Xiao-Ying (韦晓莹) A study of transition from n-to p-type based on hexagonal WO3 nanorods sensor 2014 Chin. Phys. B 23 040704
[1]
Wongchoosuk C, Wisitsoraat A, Phokharatkul D, Horprathum M, Tuantranont A and Kerdcharoen T 2013 Sens. Actuators B 181 388
[2]
He J, Su Y M, Ma Y T, Chen Q, Wang R N, Ye Y, Ma Y and Liang H L 2012 Chin. Phys. B 21 076104
[3]
Xia L, Zhong K, Song Y, Lu X, Xu L S, Yan Y, Li H D, Yuan F L, Jiang J Z, Yu D P and Zhang S L 2012 Chin. Phys. B 21 097801
[4]
Afzal A, Cioffi N, Sabbatini L and Torsi L 2012 Sens. Actuators B 171-172 25
[5]
You L, Sun Y F, Ma J, Guan Y, Sun J M, Du Y and Lu G Y 2011 Sens. Actuators B 157 401
[6]
Qin Y X, Hu M and Zhang J 2010 Sens. Actuators B 150 339
[7]
Zhang C, Debliquy M, Boudiba A, Liao H and Coddet C 2010 Sens. Actuators B 144 280
[8]
Kim S J, Hwang I S, Choi J K and Lee J H 2011 Thin Solid Films 519 2020
[9]
Meng D, Yamazaki T, Shen Y, Liu Z and Kikuta T 2009 Appl. Surf. Sci. 256 1050
[10]
Cao B, Chen J, Tang X and Zhou W 2009 J. Mater. Chem. 19 2323
[11]
Hieu N V, Quang V V, Hoa N D and Kim D 2011 Curr. Appl. Phys. 11 657
[12]
Hu M, Liu Q L, Jia D L and Li M D 2013 Acta Phys. Sin. 62 057102 (in Chinese)
[13]
Solis J L, Saukko S, Kish L B, Gqanqvist C G and Lantto V 2001 Sens. Actuators B 77 316
[14]
Kim Y S, Ha S C, Kim K, Yang H, Choi S Y and Kim Y T 2005 Appl. Phys. Lett. 86 213105
[15]
Qin Y X, Sun X B, Li X and Hu M 2012 Sens. Actuators B 162 244
[16]
Chen H Q, Hu M, Zeng J and Wang W D 2012 Chin. Phys. B 21 058201
[17]
Wang J, Khoo E, Lee S P and Ma J 2009 J. Phys. Chem. C 113 9655
[18]
Zheng F, Zhang M and Guo M 2013 Thin Solid Films 534 45
[19]
Sonia A, Djaoued Y, Subramanian B, Jacques R, Eri M C, Ralf B and Achour B 2012 Mater. Chem. Phys. 136 80
[20]
Gu Z, Li H, Zhai T, Yang W, Xia Y, Ma Y and Yao 2007 J. Solid State Chem. 180 98
[21]
Balázsi C, Sedláckov K, Llobet E and Ionescu R 2008 Sens. Actuators B 133 151
[22]
Moseley P T 1997 Meas. Sci. Technol. 8 223
[23]
Williams D E 1999 Sens. Actuators B 57 1
[24]
Bai S, Zhang K, Luo R, Li D, Chen A and Liu C C 2012 J. Mater. Chem. 22 12643
[25]
Kim Y S, Hwang I S, Kim S J, Lee C Y and Lee J H 2008 Sens. Actuators B 135 298
[26]
Gurlo A, Barsan N, Oprea A, Sahm M, Sahm T and Weimar U 2004 Appl. Phys. Lett. 85 2280
[27]
Galatsis K, Cukrov L, Wlodarski W, McCormick P, Kalantar-zadeh K, Comini E and Sberveglieri G 2003 Sens. Actuators B 93 562
[28]
Dräger G, Czolbe W and Leiro J A 1992 Phys. Rev. B 45 8283
[29]
Zhang C, Debliquy M, Boudiba A, Liao H and Coddet C 2010 Sens. Actuators B 144 280
[30]
Siciliano T, Tepore A, Micocci G, Genga A, Siciliano M and Filippo E 2009 Sens. Actuators B 138 207
[31]
Ruhland B, Becker Th and Muller G 1998 Sens. Actuators B 50 85
[32]
Prasad A K, Kubinski D J and Gouma P I 2003 Sens. Actuators B 93 25
Molecular beam epitaxy growth of monolayer hexagonal MnTe2 on Si(111) substrate S Lu(卢帅), K Peng(彭坤), P D Wang(王鹏栋), A X Chen(陈爱喜), W Ren(任伟), X W Fang(方鑫伟), Y Wu(伍莹), Z Y Li(李治云), H F Li(李慧芳), F Y Cheng(程飞宇), K L Xiong(熊康林), J Y Yang(杨继勇), J Z Wang(王俊忠), S A Ding(丁孙安), Y P Jiang(蒋烨平), L Wang(王利), Q Li(李青), F S Li(李坊森), and L F Chi(迟力峰). Chin. Phys. B, 2021, 30(12): 126804.
[7]
LnCu3(OH)6Cl3 (Ln = Gd, Tb, Dy): Heavy lanthanides on spin-1/2 kagome magnets Ying Fu(付盈), Lianglong Huang(黄良龙), Xuefeng Zhou(周雪峰), Jian Chen(陈见), Xinyuan Zhang(张馨元), Pengyun Chen(陈鹏允), Shanmin Wang(王善民), Cai Liu(刘才), Dapeng Yu(俞大鹏), Hai-Feng Li(李海峰), Le Wang(王乐), and Jia-Wei Mei(梅佳伟). Chin. Phys. B, 2021, 30(10): 100601.
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.