Soft Nanoscience Letters
Vol.2 No.3(2012), Article ID:19809,5 pages DOI:10.4236/snl.2012.23006

Detecting Ultra-Violet Radiation by Using Titanium Dioxide Nanoparticles

Naser Hatefi Kargan, Mousa Aliahmad, Samereh Azizi

Department of Physics, Faculty of Sciences, University of Sistan and Baluchestan, Zahedan, Iran.

Email: aliahmad@phys.usb.ac.ir

Received January 24th, 2012; revised March 2nd, 2012; accepted March 14th, 2012

Keywords: Ultra-violet photodetector; Titanium dioxide; Nanocrystals; Nanoparticles

ABSTRACT

In this paper sensitivity of chemically synthesized titanium dioxide (TiO2) nanoparticles to ultra-violet (UV) radiation is investigated. For this purpose three types of ultra-violet photodetectors were fabricated, one with as-synthesized TiO2 nanoparticles, another one with TiO2 nanoparticles annealed at 600˚C, and the third one with TiO2 nanoparticles annealed at 800˚C. In each case the annealing time duration was one hour. The photodetectors were fabricated on glass slides where on them a thin layer of fluorine doped tin oxide (FTO) was deposited by spray pyrolysis. The results show that all photodetectors are sensitive to UV radiation where the photodetectors fabricated from annealed TiO2 nanoparticles are more sensitive than the photodetectors fabricated from as-synthesized TiO2 nanoparticles.

1. Introduction

In recent years, UV photodetectors have got much consideration due to their civilian and military applications. These photodetectors are used in UV radiation measurement equipment, space research, detecting missiles at early stages of their launch, astronomy and biology [1,2]. In general, UV photodetectors are fabricated from large band gap inorganic semiconductor materials such as: GaN [3,4], CdS [5], diamond [6], or Si [7,8]. These materials are produced using complicated processing steps that are costly and are not appropriate for large scale applications. Recently semiconductor nanoparticles synthesized by chemical methods have been studied where in comparison to the semiconductor materials produced by previous techniques have advantages such as: low cost, simple preparation methods, capable of large scale applications, and vast options on substrate choice.

TiO2 is a wide band gap semiconductor material which can be used for UV photodetector fabrication [9]. This material crystalizes in three major phases: rutile, anatase, and brookite [10]. Rutile phase is thermodynamically more stable than the two other phases. Rutile TiO2 has direct and indirect band gaps. Its direct band gap makes TiO2 useful for photodetector fabrication. In this research TiO2 rutile phase nanoparticles were synthesized by a chemical method. Then by using these nanoparticles ultra-violet photodetectors were fabricated that are sensitive to ultra-violet radiation.

2. Synthesis of TiO2 Nanoparticles

We synthesized TiO2 nanoparticles by using 20 mL titanium (III) chloride solution (15%) in 10% hydrochloric acid from Merck Company. The solution was stirred vigorously in a reaction flask for 20 min at room temperature. Then 0.7 mL ammonia solution (25%) from Merck was diluted by 57.3 mL double distilled water and this 60 mL solution was added to the reaction flask drop wise very slowly (during 5 hours). Then the solution was left for 48 hours while it was stirred vigorously; during this time color of the solution gradually turns to white. White precipitation settle done properly. We centrifuged and washed the precipitation with water and ethanol a few times. This centrifuging and washing was repeated for three times.

We prepared three types of TiO2 samples, as-synthesized (sample A), annealed at 600˚C (sample B), and annealed at 800˚C. Duration of annealing time was one hour for both sample B and sample C.

3. Fabrication of Photodetectors

For fabricating UV photodetectors fluorine doped tin oxide (FTO) was coated on glass substrates by spray pyrolysis. For depositing FTO, 33.3 gr tin tetrachloride pentahydrate (SnCl4.5H2O, 98%) was dissolved in 50 mL double distilled water by using magnetic stirrer for a few minutes. Then 50 mL ethanol was added to the solution. Addition of alcohol turns the solution slightly blurred where by adding a few droplets of hydrochloric acid pH of the solution decreases. It leads to increasing of the solution solubility which causes the solution become clear again. Then to this solution we added 0.5 gr NH4F (99.99%). 10 mL of this solution was sprayed on glass slides where they were heated to 450˚C. The solution was sprayed at 2 atm air pressure with the speed of 10 mL/min where the spraying nozzle opening diameter was 0.3 mm and its distance from substrates was 35 cm. The deposited FTO layer had 200 nm thickness and its sheet resistance was 484 Ω.

After coating, FTO conducting oxide was disconnected by scribing a scribe line all along the width of glass slides. The scribe line was created by a diamond tip glass scriber and the width of the scribed line was 90 µm. Then TiO2 nanoparticles dispersed in diethylene glycol (50% by weight), and spin coated on the FTO film at 1000 rpm/min. TiO2 coating was done on the scribed line where the coating area was 5 mm by 5 mm. Then they are placed in an oven for 30 min and the oven temperature was 450˚C.

Three types of photodetectors were fabricated, one type with as synthesized TiO2 nanoparticles (type A), another one with TiO2 nanoparticles annealed at 600˚C (type B), and the other with TiO2 nanoparticles annealed at 800˚C (type C).

4. Characterization of TiO2 Nanoparticles

Some techniques were used for analyzing TiO2 nanoparticles such as: X-ray diffraction spectroscopy (XRD), scanning electron microscopy (SEM), and UV-VIS spectroscopy. Figure 1 shows UV-VIS spectrum of the samples. As Figure 1 shows by increasing annealing temperature absorption at peak point is shifted to longer

Figure 1. UV-VIS spectrum of TiO2 nanoparticles samples: as-synthesized TiO2 nanoparticles (A); TiO2 nanoparticles annealed at 600˚C (B) and TiO2 nanoparticles annealed at 800˚C (C).

wavelengths (red shift) which indicates increasing nanoparticles size by increasing annealing temperature.

Figure 2 shows XRD spectrum of the samples. The Xray wavelength used for measurements was 0.154 nm. It

(a)(b)(c)

Figure 2. XRD spectrum of TiO2 nanoparticles samples: as-synthesized TiO2 nanoparticles (a); TiO2 nanoparticles annealed at 600˚C (b) and TiO2 nanoparticles annealed at 800˚C (c).

is evident from the figure that as synthesized nanoparticles are in rutile phase. By increasing annealing temperature the intensity of the peaks increase which could be due to an increase in the size of as-synthesized nanoparticles, or may be the nanoparticles get more crystalized. We used Scherrer’s formula for average grain size of nanoparticles. By calculating it has been found 10 nm, 39 nm, and 104 nm for the samples A, B, and C respectively.

SEM images of the nanoparticles (Figure 3) show that they are approximately in spherical form and their sizes are approximately the same (57 nm) for samples A, B, and C. The SEM result is in contradiction with the grain size of particles which we have found from XRD patterns, and UV-VIS spectrum of the samples that indicate increase in nanoparticles size with increasing annealing temperature. Thus this contradiction indicates that the size of nanoparticles does not change by annealing, but they get more crystalized. In other words, as-synthesized TiO2 nanoparticles are more in polycrystalline phase and they change more and more to monocrystalline phase by increasing annealing temperature.

5. Characterization of Photodetectors

We did some measurements on the fabricated detectors. First of all we measured dark current, and photocurrent (at constant UV illumination power) of the fabricated photodetectors. Then we measured photocurrent of the samples as a function of illumination power at a constant applied voltage. Dark current measurements were done at room temperature where the samples were kept inside a closed box. Figure 4" target="_self"> Figure 4 shows dark current of the samples as a function of applied voltage. It is evident from the figure that the photodetectors fabricated from annealed TiO2 nanoparticles have higher dark currents than the photodetector fabricated from as-synthesized TiO2. This is due to the fact that annealed TiO2 nanoparticles are more crystalline, so their conductivity is increased as well.

Photocurrent measurements were done by placing the photodetectors inside a box where the devices were illuminated by an Hg 100 UV lamp (from Leybold) through a 2 cm diameter hole on the box. For measuring photocurrent as a function of voltage at constant illumination power, the UV lamp was kept at a constant distance (14 cm) from the devices. Photocurrent measurement as a function of illumination power at constant applied bias (10 V) was done by varying the UV lamp distance from photodetectors. Figure 5 shows the results. It is clear from the figure that sensitivity of the devices fabricated from annealed TiO2 nanoparticles increase with the annealing temperature. Although with increasing annealing temperature dark current increases as well, this is not a

(a)(b)(c)

Figure 3. SEM image of TiO2 nanoparticles samples: assynthesized TiO2 nanoparticles (a); TiO2 nanoparticles annealed at 600˚C (b) and TiO2 nanoparticles annealed at 800˚C (c).

disadvantage. This is due to the fact that photocurrent increases a few times more than dark current. For example if dark current and photocurrent for samples A and C are compared, it can be obtained that while dark current increases by about two times, photocurrent increases by about 8 times.

Figure 4. Dark current of the fabricated photodetectors: fabricated from as-synthesized TiO2 nanoparticles (A); TiO2 nanoparticles annealed at 600˚C (B) and TiO2 nanoparticles annealed at 800˚C (C).

(a)(b)

Figure 5. Photocurrent of the fabricated photodetectors: fabricated from as-synthesized TiO2 nanoparticles (A); TiO2 nanoparticles annealed at 600˚C (B); and TiO2 nanoparticles annealed at 800˚C (C). (a) shows photocurrent at a constant illumination power, and (b) shows photocurrent as a function of UV lamp distance from the devices at a constant applied bias.

6. Conclusions

We synthesized TiO2 nanoparticles by a chemical method and annealed them at 600˚C, and 800˚C where the annealing time duration was one hour. SEM, UV-VIS, and XRD results show that as synthesized nanoparticles are in rutile phase and the nanoparticles get more crystalline by annealing at higher temperatures.

We fabricated photodetectors by using as-synthesized and annealed TiO2 nanoparticles. Measurements show that the sensitivity of the devices increase with increasing annealing temperature of TiO2 nanoparticles which from them the detectors were fabricated. This confirms the result obtained from UV-VIS, SEM and XRD measurements that annealing causes TiO2 nanoparticles to get more crystalline.

REFERENCES

  1. E. Monroy, F. Omnes and F. Calle, “Wide-Bandgap Semiconductor Ultraviolet Photodetectors,” Semiconductor Science and Technology, Vol. 18, No. 4, 2003, pp. R33- R51. doi:10.1088/0268-1242/18/4/201
  2. S. V. Averine, P. I. Kuznetzov, V. A. Zhitov and N. V. Alkeev, “Solar-Blind MSM-Photodetectors Based on AlxGa1–xN/GaN Heterostructures Grown by MOCVD,” Solid-State Electronics, Vol. 52, No. 5, 2008, pp. 618- 624. doi:10.1016/j.sse.2007.10.037
  3. S. K. Zhang, W. B. Wang, I. Shtau, F. Yun, L. He, H. Morkoc, X. Zhou, M. Tamargo and R. R. Alfano, “Backilluminated GaN/AlGaN Heterojunction Ultraviolet Photodetector with High Internal Gain,” Applied Physics Letters, Vol. 81, No. 25, 2002, pp. 4862-4864. doi:10.1063/1.1526166
  4. I.-S. Seo, I.-H. Lee, Y.-J. Park and C.-R. Lee, “Characteristics of UV Photodetector Fabricated by Al0.3Ga0.7N/ GaN Heterostructure,” Journal of Crystal Growth, Vol. 252, No. 1-3, 2003, pp. 51-57. http://dx.doi.org/10.1016/S0022-0248(02)02523-X
  5. M. S. Shur, S. Rumyantsev, R. Gaska, B. Q. Wei, R. Vajtai, P. M. Ajayan and J. Sinius, “Structural and Transport Properties of CdS Films Deposited on Flexible Substrates,” Solid-State Electronics, Vol. 46, No. 9, 2002, pp. 1417-1420. doi:10.1016/S0038-1101(02)00073-4
  6. S. Salvatori, G. Mazzeo, G. Conte, M. C. Rossi and V. Ralchenko, “Polycrystalline Diamond Position Sensitive Detector for Excimer Laser UV Radiation,” Diamond and Related Materials, Vol. 13, No. 4-8, 2004, pp. 948-953.
  7. R. F. Wolffenbuttel, “Silicon Photodetectors with a Selective Spectral Response,” Sensors Update, Vol. 9, No. 1, 2001, pp. 69-101. doi:10.1002/1616-8984(200105)9:1<69::AID-SEUP69>3.0.CO;2-Q
  8. D. Caputo, G. de Cesare, A. Nascetti and M. Tucci, “On the Fabrication and Characterization of Amorphous Silicon Ultra-Violet Sensor Array,” Thin Solid Films, Vol. 517, No. 23, 2009, pp. 6422-6425. doi:10.1016/j.tsf.2009.02.064
  9. X. Kong, C. Liu, W. Dong, X. Zhang, C. Tao, L. Shen, J. Zhou, Y. Fei and S. Ruan, “Metal-Semiconductor-Metal TiO2 Ultraviolet Detectors with Ni Electrodes,” Applied Physics Letters, Vol. 94, No. 12, 2009, Article ID: 123502. doi:10.1063/1.3103288
  10. X. Chen and S. S. Mao, “Titanium Dioxide NanoMaterials: Synthesis, Properties, Modifications, and Applications,” Chemical Reviews, Vol. 107, No. 7, 2007, pp. 2891-2959. doi:10.1021/cr0500535