5
International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: [email protected] Volume 3, Issue 5, May 2014 ISSN 2319 - 4847 Volume 3, Issue 5, May 2014 Page 94 Abstract In this research, MgO thin films deposited on quartz glass and silicon substrate with different thicknesses 100 and 200 nm by a radio frequency (R.F.) magnetron sputtering process using magnesium oxide target under Ar gas pressure. The sputtering deposition was performed by using R.F. power of 130 Watt. The average surface roughness (Ra) measured with atomic force microscopy (AFM) was ranged between 8nm and 20nm. Spectral transmittance of MgO thin films were measured in the range of 200-1200 nm. Optical band gaps were calculated from Tauc ' plots and were found to be 5.5eV and 5.9eV for sample thickness of 100 nm and 200 nm respectively. These films were tested in (NH3) gas at room temperature. The sensitivity after 100 sec from exposed to (NH3) gas were 6% and 13% for 100 and 200 nm film thickness respectively. Keywords: MgO : Thin Film; Nanostructure; Optical; Gas Sensor and Sputtering RF. 1. INTRODUCTION Magnesium oxide thin films are very important scientific and commercial material. They widely used as a protective layer for AC-plasma display panels because of their high durability and gas sensing systems[1].good protection characteristics against ion bombardment, high secondary electron emission coefficient and high transparency[2].MgO is a best candidate to be used as dielectric layer due to its excellent properties such as has high dielectric constant (~ 9.8), large band gap in the range of 7.3 eV -7.8 eV and has higher breakdown field (12 MV/cm) compared to commonly used dielectric layer which is silicon dioxide (SiO 2 ) [2] . Due to its excellent dielectric properties, MgO has been proposed to be used for capacitor applications because MgO can improve the storage capability of a capacitor. Other characteristics of MgO that comparable to SiO 2 are due to its chemical inertness, electrical insulation, optical transparency, high temperature stability, high thermal conductivity and secondary-electron emission with a lattice constant of 4.21 Å [3]. Due to its excellent properties, MgO has been proposed to replace current dielectric material (SiO 2 ) [4].Magnesium Oxide with rocksalt-structure has been extensively investigated due to its exceptional properties, such as chemical inertness, high electrical resistivity, optical transparency, and low thermal conductivity [5–6].The most used techniques to obtain these films are organ metallic using thermal evaporation [7], flame spray paralysis [8], combustion aerosol synthesis [9], chemical vapor deposition [10], hydrothermal [11], and surfactant methods [12] 2. EXPERIMENTAL DETAILS MgO thin films were prepared by RF magnetron sputtering system with a magnesium oxide target of 99.99% purity on quartz and (P + ) silicon as substrates. Firstly, the target was pre-sputtered in an argon atmosphere in order to remove oxide layer. The argon gas was introduced into the chamber through a flow controller with fine adjustments the sputtering was performed under Ar (99.999%) atmosphere supplied as working gas through mass-flow controller. The sputtering chamber was evacuated down to 5 × 10 -5 mbar by the turbo molecular pump. Microscope glass slides were used as the substrates for thin films. Prior to deposition, The quartz and (P + ) silicon substrates was cleaned by chromic acid followed by distilled water rinse. The optical properties of the MgO films were, determined by The UV-VIS spectrum (Optima Sp – 300 Plus) was used to study the change of thickness on absorption, transmittance and band gap energy. For morphological investigations, AFM images were recorded using Nano scope IIIa scanning probe microscope controller in a tapping mode. In addition to the effect of thickness on sensitivity. 3. Results and discussion: 3.1 Optical Properties The optical characterization of thin films gives us something about the physical properties such as the absorption , transmittance and band gap energy and band structure, determined by UV-VIS spectrum(Optima Sp – 300 Plus ). Transmittance spectra recorded for MgO films as a function of wavelength range (200-1200 nm).It is observed that the Influence of Thickness on Optical and Sensing Properties of MgO Thin Films Deposited by RF Magnetron Sputtering Mahana M. Habeeb 1 , Muneer H. Jaddaa 1 , Abdul Hussein K.Elttayef 2 and Hayder Mohammad Ajeel 2 1 University of Wasit , College of Science, 2 Ministry of Science and Technology

Web Site: Email: [email protected] Volume 3, … · International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: Email: [email protected] Volume

  • Upload
    vukiet

  • View
    217

  • Download
    0

Embed Size (px)

Citation preview

International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: [email protected]

Volume 3, Issue 5, May 2014 ISSN 2319 - 4847

Volume 3, Issue 5, May 2014 Page 94

Abstract

In this research, MgO thin films deposited on quartz glass and silicon substrate with different thicknesses 100 and 200 nm by a radio frequency (R.F.) magnetron sputtering process using magnesium oxide target under Ar gas pressure. The sputtering deposition was performed by using R.F. power of 130 Watt. The average surface roughness (Ra) measured with atomic force microscopy (AFM) was ranged between 8nm and 20nm. Spectral transmittance of MgO thin films were measured in the range of 200-1200 nm. Optical band gaps were calculated from Tauc' plots and were found to be 5.5eV and 5.9eV for sample thickness of 100 nm and 200 nm respectively. These films were tested in (NH3) gas at room temperature. The sensitivity after 100 sec from exposed to (NH3) gas were 6% and 13% for 100 and 200 nm film thickness respectively. Keywords: MgO : Thin Film; Nanostructure; Optical; Gas Sensor and Sputtering RF. 1. INTRODUCTION Magnesium oxide thin films are very important scientific and commercial material. They widely used as a protective layer for AC-plasma display panels because of their high durability and gas sensing systems[1].good protection characteristics against ion bombardment, high secondary electron emission coefficient and high transparency[2].MgO is a best candidate to be used as dielectric layer due to its excellent properties such as has high dielectric constant (~ 9.8), large band gap in the range of 7.3 eV -7.8 eV and has higher breakdown field (12 MV/cm) compared to commonly used dielectric layer which is silicon dioxide (SiO2) [2] . Due to its excellent dielectric properties, MgO has been proposed to be used for capacitor applications because MgO can improve the storage capability of a capacitor. Other characteristics of MgO that comparable to SiO2are due to its chemical inertness, electrical insulation, optical transparency, high temperature stability, high thermal conductivity and secondary-electron emission with a lattice constant of 4.21 Å [3]. Due to its excellent properties, MgO has been proposed to replace current dielectric material (SiO2) [4].Magnesium Oxide with rocksalt-structure has been extensively investigated due to its exceptional properties, such as chemical inertness, high electrical resistivity, optical transparency, and low thermal conductivity [5–6].The most used techniques to obtain these films are organ metallic using thermal evaporation [7], flame spray paralysis [8], combustion aerosol synthesis [9], chemical vapor deposition [10], hydrothermal [11], and surfactant methods [12] 2. EXPERIMENTAL DETAILS MgO thin films were prepared by RF magnetron sputtering system with a magnesium oxide target of 99.99% purity on quartz and (P+) silicon as substrates. Firstly, the target was pre-sputtered in an argon atmosphere in order to remove oxide layer. The argon gas was introduced into the chamber through a flow controller with fine adjustments the sputtering was performed under Ar (99.999%) atmosphere supplied as working gas through mass-flow controller. The sputtering chamber was evacuated down to 5 × 10-5 mbar by the turbo molecular pump. Microscope glass slides were used as the substrates for thin films. Prior to deposition, The quartz and (P+) silicon substrates was cleaned by chromic acid followed by distilled water rinse. The optical properties of the MgO films were, determined by The UV-VIS spectrum (Optima Sp – 300 Plus) was used to study the change of thickness on absorption, transmittance and band gap energy. For morphological investigations, AFM images were recorded using Nano scope IIIa scanning probe microscope controller in a tapping mode. In addition to the effect of thickness on sensitivity. 3. Results and discussion: 3.1 Optical Properties The optical characterization of thin films gives us something about the physical properties such as the absorption , transmittance and band gap energy and band structure, determined by UV-VIS spectrum(Optima Sp – 300 Plus ). Transmittance spectra recorded for MgO films as a function of wavelength range (200-1200 nm).It is observed that the

Influence of Thickness on Optical and Sensing Properties of MgO Thin Films Deposited by RF

Magnetron Sputtering

Mahana M. Habeeb1, Muneer H. Jaddaa1, Abdul Hussein K.Elttayef2 and

Hayder Mohammad Ajeel2

1University of Wasit , College of Science, 2 Ministry of Science and Technology

International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: [email protected]

Volume 3, Issue 5, May 2014 ISSN 2319 - 4847

Volume 3, Issue 5, May 2014 Page 95

transmittance decreases with increase in thickness deposited with 100nm thickness shows higher transmittance compare to 200nm thickness as show in figure 1. This property of high transmittance makes it a good material for optical coatings. The optical band gaps of the films are calculated from the transmittance spectra. The absorption coefficient (α) is calculated using the equation, [13]:

α= ln (1/T) / d …….. (1) Where T is transmittance and d is film thickness. The absorption coefficient (α) and the incident photon energy (hν) are related by the following equation [14]: (αhν)2= A (hν-Eg) ……. (2) The film it shows the representatives of optical absorbance which reveals that the absorbance of the film decreases gradually with increase in wavelength as shown in figure 2.

Fig.1. Transmittance Spectra of MgO Thin Films a. 100nm b. 200nm

Fig. 2. Absorbance Spectra of MgOThin Films a. 100nm b. 200nm

Fig. (3): (a) Allowed and (b) Forbidden Direct Electronic Transitions of MgO

International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: [email protected]

Volume 3, Issue 5, May 2014 ISSN 2319 - 4847

Volume 3, Issue 5, May 2014 Page 96

The typical plots of (αhν)2 versus hν for MgO thin films with 100nm thickness and 100nm thickness deposited on quartz substrate is shown in figure (3). It is observed that increase in thickness of MgOlead to increase in optical band gap from 5.6eV to 5.9eV. 3.2 Morphology The surface morphology of all the MgO films is offered by AFM images in tapping mode shown in Fig. 3. All the MgO films presentation a smooth surface with uniform grains. In Fig. 3, the surface morphology discovers the nana-crystalline MgO grains, which rise to make intensive films significantly with the increased thickness. From the images, it was observed that the surfaces of the films exhibited a confirmed degree of coarseness and the film came rougher when the thickness increases.

Figure (4) Image AFM of Thickness (a) 100nm , (b) 200nm 3.3Gas sensing properties The figure (5) shows the sensitivity to prepared MgO thin films on silicon p-type (n-p) by RF magnetron sputtering system with thickness 100nm and 200nm for the gas (NH3).The working gases were pumped in to the chamber and recording the change in thin films resistance with time (per 10 seconds), MgO thin films suffer from the height of potential barrier in the reducer by using (NH3) gas closed to 6 ppm. The sensitivity is higher for sensors on the MgO with 200 nm thickness because increase in number of electrons lead to increased charge carries (electron - hole).

Figure (5) MgO thin Films Sensitivity NH3 a. 100nm b. 200nm

4. Conclusion The magnesium oxide thin films have been successfully deposited by RF reactive sputtering method on unheated quartz and silicon substrates. The transmittance is found to increase slightly in the decreased film thickness. AFM images also

International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: [email protected]

Volume 3, Issue 5, May 2014 ISSN 2319 - 4847

Volume 3, Issue 5, May 2014 Page 97

support the slow growth of crystallite sizes for the as-grown films and increasing thickness. The MgO films are highly transparent in the visible range and decreasing thickness causes slight increase in visible transmittance. It is observed that the allowed direct optical band gap of the films increases from 5.5 eV to 5.9eV with the increase of film thickness. The high sensitivity increasing thickness, the sensitivity was improved by increasing thickness.

References [1] G. Ertl, H. Kno ¨zinger, J. Weitkamp (Eds.), Handbook of Heterogenous Catalysis, vol. 4, Wiley–VCH, Weinheim,

1997, p. 2111. [2] Choi E-H, Oh H-J, Kim Y-G, J.-J. K, Lim J-Y, Kim J-G, Kim D-I, Cho G, Kang S-O, (1998) Jpn. J. Appl. Phys. 37

7015. [3] I. -C. Ho, Y. Xu, and J. D. Mackenzie, "Electrical and Optical Properties of MgO Thin Film Prepared by Sol-Gel

Technique," Journal of Sol-Gel Science and Te1. Renaud, G. Oxide surfaces and metal/oxide interfaces studied by grazing angle incidence X-ray

[4] E. Miranda, E. O'Connor, G. Hughes, P. Casey, K. Cherkaoui, S. Monaghan, R. Long, D. O'Connell, and P. K. Hurley, "Soft breakdown in MgO dielectric layers," in Reliability Physics Symposium, 2009 IEEE International, pp. 688-691, 2009

[5] Scattering. Surf. Sci. Rep. 1998, 32, 1–90. chnology, vol. 9, pp. 295-301, 1997. [6] Nagashima, K.; Yanagida, T.; Tanaka, H.; Kawai,T. Epitaxial growth of MgO nanowires by pulsed laser

deposition.J. Appl. Phys. 2007, 101, 124304:1–124304:4. [7] Q. Yang, J. Sha, L. Wang, J. Wang, D. Yang, Mater. Sci. Eng., C 26 (2006) 1097 -1101. [8] Xie Yi, Wang Wenzhong, QianYitai, Yang Li, Chen Zhiwen, Surf. Coat. Technol. 82 (1996) 291-293. [1] G. Ertl, H. Kno ¨zinger, J. Weitkamp (Eds.), Handbook of Heterogenous Catalysis, vol. 4, Wiley–VCH, Weinheim,

1997, p. 2111. [2] Choi E-H, Oh H-J, Kim Y-G, J.-J. K, Lim J-Y, Kim J-G, Kim D-I, Cho G, Kang S-O, (1998) Jpn. J. Appl. Phys. 37

7015. [3] I. -C. Ho, Y. Xu, and J. D. Mackenzie, "Electrical and Optical Properties of MgO Thin Film Prepared by Sol-Gel

Technique," Journal of Sol-Gel Science and Te1. Renaud, G. Oxide surfaces and metal/oxide interfaces studied by grazing angle incidence X-ray

[4] E. Miranda, E. O'Connor, G. Hughes, P. Casey, K. Cherkaoui, S. Monaghan, R. Long, D. O'Connell, and P. K. Hurley, "Soft breakdown in MgO dielectric layers," in Reliability Physics Symposium, 2009 IEEE International, pp. 688-691, 2009

[5] scattering. Surf. Sci. Rep. 1998, 32, 1–90. chnology, vol. 9, pp. 295-301, 1997. [6] 4. Nagashima, K.; Yanagida, T.; Tanaka, H.; Kawai,T. Epitaxial growth of MgO nanowires by pulsed laser

deposition.J. Appl. Phys., 101, 124304:1–124304:4,2007. [7] Q. Yang, J. Sha, L. Wang, J. Wang, D. Yang, Mater. Sci. Eng., C 26 ,pp 1097 -1101,2006. [8] Xie Yi, Wang Wenzhong, QianYitai, Yang Li, Chen Zhiwen, Surf. Coat.

Technol. 82 ,pp 291-293,1996. [9] J.J. Helble, J. Aerosol Sci. 29 ,pp 721-736,1998. [10] Y. Li, Y. Bando, T. Sato, Chem. Phys. Lett. 359 ,pp 141-1452002. [11] L. Kumari, W.Z. Li, C.H. Vannoy, R.M. Leblanc, D.Z. Wang, Ceram. Int. 35, pp 3355– 3364,2009. [12] P. Ouraipryvan, T. Sreethawong, S. Chavadej, Mater. Lett. 63 , 1862-1865,2009. [13] W.Miao, X.Li, Q.Zhang, L.Huang, L.Zhang and X.Yan, “Transparent conducting In2O3 dopedMo thin films

prepared by reactive direct current magnetron sputtering at room temperature”.Thin Sold Films, 500, pp 70,2006. [14] V.R.Shinde, T.P.Gujar, C.D.Lokhande, R.S.Mane and S.H.Han, “ Mn doped and undopedZnO films: A

comparative structural, optical and electrical properties study” Mater.Chem.Phys., 96, pp 326,2006.

Author Mahana M. Habeeb, M.SC student in physics department, college of science, Wasit University. His research interest includes the preparation of nano films and applications.

Muneer H.Jaduaa, He is Assistant Proff. ,at physics dept., college of science, Wasit university. He is leading research group in the field of solid state and material Science.

International Journal of Application or Innovation in Engineering & Management (IJAIEM) Web Site: www.ijaiem.org Email: [email protected]

Volume 3, Issue 5, May 2014 ISSN 2319 - 4847

Volume 3, Issue 5, May 2014 Page 98

Abdulhussein K.Elttayef is currently a professor of physics At the Applied physics center, Baghdad, Iraq. He received his Ph.D Degree from Herriot –Watt University (U.K) in 1990. His currently research Interests include the preparation of nano films (semiconductors and polymers) by different methods for applications of gas sensors, solar cells and optical detectors. He has written 40 scientific publications in this area.

Hayder Mohammad Ajeel ,He has B.SC in physics.Currently working at the Applied physics center,. His research Interests include the preparation of nano films.