STUDY OF THE EFFECT OF COPPER (CU) DOPING AND ANNEALING ON A ZINC OXIDE (ZNO) FILM GROWN BY DC MAGNETRON CO-SPUTTERING TECHNIQUE FOR VISIBLE LIGHT PHOTODETECTOR APPLICATIONS
Efforts to modify the structural, optical, and electrical properties of zinc oxide (ZnO) to improve the performance of visible light photodetectors have been conducted by doping copper (Cu). The Cu dopant was chosen due to its high electrical conductivity and its ion radius being close to Zn maki...
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Efforts to modify the structural, optical, and electrical properties of zinc oxide
(ZnO) to improve the performance of visible light photodetectors have been
conducted by doping copper (Cu). The Cu dopant was chosen due to its high
electrical conductivity and its ion radius being close to Zn making atomic insertion
easier. Cu-doped ZnO (CZO) films were grown using confocal DC magnetron cosputtering on a silicon (Si) substrate at Cu sputtering power varied (15 and 20 W),
while the Zn sputtering power was constant at 80 W. Furthermore, the effect of
annealing treatment at a temperature of 600? was also studied after the ZnO and
CZO films were deposited. The surface morphology and elemental composition,
structural properties, chemical bonds, absorbance and photoluminescence of the
ZnO and CZO films were characterized using Field Emission Scanning Electron
Microscopy (FE-SEM) and Energy dispersive X-ray (EDX), X-ray Diffraction
(XRD) , Fourier transforms-infrared (FT-IR), ultraviolet-visible (UV-Vis), and
photoluminescence (PL) spectroscopy. Furthermore, I-V measurements with a
metal-semiconductor-metal (MSM) configuration were investigated to determine
the electrical properties of ZnO and CZO films as visible light photodetector
materials.
The FESEM image exhibits changes in the shape and size of the rod particles to
become shorter as the Cu sputtering power increases. The annealed film produces
a granular shape and is reduced in size and more homogeneous. Cu dopant has been
successfully substituted in the ZnO system which was confirmed from EDX
analysis. Therefore, Cu influences the characteristics of the ZnO film. The XRD
spectrum identifies the ZnO structural phase with the (002) plane crystal orientation
direction along the c-axis perpendicular to the substrate. At a Cu sputtering power
of 20 W as grown (without annealing) and annealed films, a monoclinic CuO phase
with a (202) plane was found. Good crystallinity of CZO film due to the increase
in Cu sputtering power and the annealing effect as indicated by high crystallite size
also low lattice stress and dislocation density. Identification of chemical bonds from
the FT-IR spectrum confirms the strong vibrational bonds of Zn-O and becomes
sharper due to the annealing effect. Furthermore, peak shift indicates successful substitution of Cu in the ZnO lattice. The effect of annealing reveals the purity of
the film increases without the presence of impurities from carbon C=C.
Based on the UV-Vis absorbance spectrum, a redshift occurs due to Cu doping
which refers to a decrease in band gap energy due to the Burstein-Moss effect (BM).
It also occurs in annealed films. The band gap energy of the ZnO and CZO films
after annealing is smaller than without annealing because the band edge absorbance
is small. The photoluminescence properties show a decrease in PL intensity as the
Cu sputtering power increases, causing a decrease in defects and free excited state
energy levels. Moreover, the shift in the emission peak indicates recrystallization
due to annealing. Furthermore, the electrical properties of ZnO and CZO in light
detection were studied from the I-V (current-voltage) characteristic curve in dark
and visible light conditions using a solar simulator. The I-V curve exhibits
photocurrent of the Cu-doped ZnO is higher than the undoped ZnO film, both in
the annealed and non-annealed films. The increased sputtering power of Cu reveals
a high sensitivity twice that of ZnO, and responsivity increases three times at a bias
of 5 Volt. The sensitivity and the responsivity of annealed Cu-doped ZnO at
sputtering power 20 W produces the highest values of 10.01 and 6.7 mA/W. Also,
the low Schottky barrier height plays an important role in electron transport from
metals to semiconductors. Therefore, increasing the Cu sputtering power and
annealing treatment by modifying the structural and optical properties have
succeeded in improving the performance of visible light photodetectors. |
format |
Theses |
author |
Rati, Yolanda |
spellingShingle |
Rati, Yolanda STUDY OF THE EFFECT OF COPPER (CU) DOPING AND ANNEALING ON A ZINC OXIDE (ZNO) FILM GROWN BY DC MAGNETRON CO-SPUTTERING TECHNIQUE FOR VISIBLE LIGHT PHOTODETECTOR APPLICATIONS |
author_facet |
Rati, Yolanda |
author_sort |
Rati, Yolanda |
title |
STUDY OF THE EFFECT OF COPPER (CU) DOPING AND ANNEALING ON A ZINC OXIDE (ZNO) FILM GROWN BY DC MAGNETRON CO-SPUTTERING TECHNIQUE FOR VISIBLE LIGHT PHOTODETECTOR APPLICATIONS |
title_short |
STUDY OF THE EFFECT OF COPPER (CU) DOPING AND ANNEALING ON A ZINC OXIDE (ZNO) FILM GROWN BY DC MAGNETRON CO-SPUTTERING TECHNIQUE FOR VISIBLE LIGHT PHOTODETECTOR APPLICATIONS |
title_full |
STUDY OF THE EFFECT OF COPPER (CU) DOPING AND ANNEALING ON A ZINC OXIDE (ZNO) FILM GROWN BY DC MAGNETRON CO-SPUTTERING TECHNIQUE FOR VISIBLE LIGHT PHOTODETECTOR APPLICATIONS |
title_fullStr |
STUDY OF THE EFFECT OF COPPER (CU) DOPING AND ANNEALING ON A ZINC OXIDE (ZNO) FILM GROWN BY DC MAGNETRON CO-SPUTTERING TECHNIQUE FOR VISIBLE LIGHT PHOTODETECTOR APPLICATIONS |
title_full_unstemmed |
STUDY OF THE EFFECT OF COPPER (CU) DOPING AND ANNEALING ON A ZINC OXIDE (ZNO) FILM GROWN BY DC MAGNETRON CO-SPUTTERING TECHNIQUE FOR VISIBLE LIGHT PHOTODETECTOR APPLICATIONS |
title_sort |
study of the effect of copper (cu) doping and annealing on a zinc oxide (zno) film grown by dc magnetron co-sputtering technique for visible light photodetector applications |
url |
https://digilib.itb.ac.id/gdl/view/79509 |
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id-itb.:795092024-01-08T15:10:00ZSTUDY OF THE EFFECT OF COPPER (CU) DOPING AND ANNEALING ON A ZINC OXIDE (ZNO) FILM GROWN BY DC MAGNETRON CO-SPUTTERING TECHNIQUE FOR VISIBLE LIGHT PHOTODETECTOR APPLICATIONS Rati, Yolanda Indonesia Theses annealing, co-sputtering, doping Cu, photodetector, redshift, dan ZnO INSTITUT TEKNOLOGI BANDUNG https://digilib.itb.ac.id/gdl/view/79509 Efforts to modify the structural, optical, and electrical properties of zinc oxide (ZnO) to improve the performance of visible light photodetectors have been conducted by doping copper (Cu). The Cu dopant was chosen due to its high electrical conductivity and its ion radius being close to Zn making atomic insertion easier. Cu-doped ZnO (CZO) films were grown using confocal DC magnetron cosputtering on a silicon (Si) substrate at Cu sputtering power varied (15 and 20 W), while the Zn sputtering power was constant at 80 W. Furthermore, the effect of annealing treatment at a temperature of 600? was also studied after the ZnO and CZO films were deposited. The surface morphology and elemental composition, structural properties, chemical bonds, absorbance and photoluminescence of the ZnO and CZO films were characterized using Field Emission Scanning Electron Microscopy (FE-SEM) and Energy dispersive X-ray (EDX), X-ray Diffraction (XRD) , Fourier transforms-infrared (FT-IR), ultraviolet-visible (UV-Vis), and photoluminescence (PL) spectroscopy. Furthermore, I-V measurements with a metal-semiconductor-metal (MSM) configuration were investigated to determine the electrical properties of ZnO and CZO films as visible light photodetector materials. The FESEM image exhibits changes in the shape and size of the rod particles to become shorter as the Cu sputtering power increases. The annealed film produces a granular shape and is reduced in size and more homogeneous. Cu dopant has been successfully substituted in the ZnO system which was confirmed from EDX analysis. Therefore, Cu influences the characteristics of the ZnO film. The XRD spectrum identifies the ZnO structural phase with the (002) plane crystal orientation direction along the c-axis perpendicular to the substrate. At a Cu sputtering power of 20 W as grown (without annealing) and annealed films, a monoclinic CuO phase with a (202) plane was found. Good crystallinity of CZO film due to the increase in Cu sputtering power and the annealing effect as indicated by high crystallite size also low lattice stress and dislocation density. Identification of chemical bonds from the FT-IR spectrum confirms the strong vibrational bonds of Zn-O and becomes sharper due to the annealing effect. Furthermore, peak shift indicates successful substitution of Cu in the ZnO lattice. The effect of annealing reveals the purity of the film increases without the presence of impurities from carbon C=C. Based on the UV-Vis absorbance spectrum, a redshift occurs due to Cu doping which refers to a decrease in band gap energy due to the Burstein-Moss effect (BM). It also occurs in annealed films. The band gap energy of the ZnO and CZO films after annealing is smaller than without annealing because the band edge absorbance is small. The photoluminescence properties show a decrease in PL intensity as the Cu sputtering power increases, causing a decrease in defects and free excited state energy levels. Moreover, the shift in the emission peak indicates recrystallization due to annealing. Furthermore, the electrical properties of ZnO and CZO in light detection were studied from the I-V (current-voltage) characteristic curve in dark and visible light conditions using a solar simulator. The I-V curve exhibits photocurrent of the Cu-doped ZnO is higher than the undoped ZnO film, both in the annealed and non-annealed films. The increased sputtering power of Cu reveals a high sensitivity twice that of ZnO, and responsivity increases three times at a bias of 5 Volt. The sensitivity and the responsivity of annealed Cu-doped ZnO at sputtering power 20 W produces the highest values of 10.01 and 6.7 mA/W. Also, the low Schottky barrier height plays an important role in electron transport from metals to semiconductors. Therefore, increasing the Cu sputtering power and annealing treatment by modifying the structural and optical properties have succeeded in improving the performance of visible light photodetectors. text |