MODIFICATION OF NANOSTRUCTURE IN CARBON-DOPED ZNO: ELECTRICAL AND OPTICAL PROPERTIES SYNTHESIZED VIA SPUTTERING AND PYROLYSIS OF ZN-MOF DERIVATIVES
Zinc oxide (ZnO) is a semiconductor with a wide band gap of 3.33-3.37 eV and exceptional optical properties within the UV region. Introducing carbon doping to ZnO has the potential to reduce the band gap energy, resulting in broader optical absorption and thus serving as an alternative to enhance...
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Zinc oxide (ZnO) is a semiconductor with a wide band gap of 3.33-3.37 eV and exceptional
optical properties within the UV region. Introducing carbon doping to ZnO has the potential
to reduce the band gap energy, resulting in broader optical absorption and thus serving as an
alternative to enhance device performance. This study involved the preparation of carbondoped ZnO using sputtering and pyrolysis methods to modify surface structures and investigate
their effects on electrical and optical properties. Density functional theory (DFT) was
employed to support the experimental findings. In the sputtering method, samples are obtained
in the form of thin films where ZnO and carbon-doped ZnO (ZnO:C-1, ZnO:C-2) grow on a
Silicon (100) substrate with optimized deposition parameters (Power= 12W, growth
temperature =300 ?, time= 4 hours, pressure = 0.3 kPa). Heating treatment after deposition
(thermal annealing) was applied to the ZnO thin film at a temperature of 600 ? (ZnO/ann600) and 800 ? (ZnO/ann-800) under oxygen gas flow for 10 minutes. Furthermore, using the
pyrolysis method, powdered samples were obtained, where Zn-MOF was converted into ZnO/C
after heating at a temperature of 450 ? for 2 hours in various atmospheric conditions:
nitrogen, oxygen, and air (ZnO/C-O2, ZnO/C-N2, ZnO/C-air). This research involved
photocatalytic tests with the aim of evaluating the degradation capability of Rhodamine-B
pollutant at a concentration of 20 ppm. Photocatalytic testing of ZnO/C samples derived from
Zn-MOF was carried out using a portable solar simulator PEC-L01 (1000 W/m2
).
ZnO thin films grown using the sputtering method produce cone-shaped nanocolumnar
structures (ZnO height= 850 nm) and change significantly into rods after annealing at
temperatures of 600 ? (ZnO/ann-600 height=600 nm) and 800 ? (ZnO/ann- height 800=300
nm). Thermal annealing treatment induces an increase in the lattice constant c from 5.224 Å
(ZnO) to 5.226 Å (ZnO/ann-600). Furthermore, we found an elliptical polarization response
without saturation, indicating the presence of dominant leakage current and oxygen vacancies
in the sample. The highest polarization is found in ZnO/ann-600 (|+Pr/-Pr|= 2.06) which is
associated with an increase in the lattice constant c. Besides, ferroelectric characteristics were
observed in ZnO/ann-800, with a lower polarization response (|+Pr/-Pr|= 1.14) due to the
high density of nanocolumnar rods formed in the sample.
Carbon-doped ZnO thin films grown using the sputtering method can reduce the height of ZnO
nanocolumnar cones from 850 nm to 800 nm at a C concentration of 12.43% (ZnO:C-1) and
300 nm at a C concentration of 31.76% (ZnO:C -2). Carbon doping on nanocolumnar ZnO
can effectively increase the lattice strain (????????????????= 1.658×10-4
, ????????????????:?????1= 5.995×10-4 and
????????????????:?????2= 7.249×10-3
). The P–E hysteresis loop shows that ZnO:C-1 has the highest coercivity (11.1 kV/cm) which comes from Zn vacancies, while ZnO:C-2 has remanent polarization (4.7
?C/cm2
) which comes from oxygen vacancies produces ferroelectric material. Carbon doping
reduces the band gap of ZnO from 3.28 eV to 3.25 eV (ZnO:C-1) and 3.23 eV (ZnO:C-2).
Density functional theory calculations show that C doping changes the energy band structure
in the Fermi energy region due to the contribution of the 2p orbital C atom.
The pyrolysis method of Zn-MOF converted into ZnO/C produces various morphological forms
depending on the variation of gas applied during pyrolysis. The morphology of Zn-MOF with
a rod shape changes to granular (ZnO/C?O2) and spherical (ZnO/C?air) while ZnO/C-N2 still
maintains a rod shape. The carbon atom concentration of Zn-MOF changed significantly from
57.43% to 68.41% (ZnO/C?N2), 62.56% (ZnO/C?O2), and 27.7% (ZnO/C?air ). The diffraction
peak of ZnO/C?O2 shows the highest crystallinity compared to ZnO/C?air and ZnO/C-N2 where
the dominant peak grows in the (101) direction. Furthermore, the BET-specific surface areas
obtained were 16.8, 6.81, 12.15, 29.26 m2
/g for the Zn-MOF, ZnO/C?N2, ZnO/C?O2, and
ZnO/C-air samples, respectively. ZnO/C?air shows optimal stability performance with a
degradation efficiency of up to 94.1% against Rhodamine-B. This research has the potential to
provide stable photocatalytic for wastewater purification, especially in the decomposition of
Rhodamine-B pollutants. In addition, the results of this research also open up opportunities to
obtain multifunctional devices with higher sensitivity and accuracy. Multifunctional devices
apply the principles of coupling and integration between the resulting electrical and optical
properties. It can also contribute to understanding carbon-doped ZnO materials through
method comparisons, thermal annealing treatment, carbon doping, and converting Zn-MOF
materials into ZnO/C.
|
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Dissertations |
author |
Novi Hendri, Yasni |
spellingShingle |
Novi Hendri, Yasni MODIFICATION OF NANOSTRUCTURE IN CARBON-DOPED ZNO: ELECTRICAL AND OPTICAL PROPERTIES SYNTHESIZED VIA SPUTTERING AND PYROLYSIS OF ZN-MOF DERIVATIVES |
author_facet |
Novi Hendri, Yasni |
author_sort |
Novi Hendri, Yasni |
title |
MODIFICATION OF NANOSTRUCTURE IN CARBON-DOPED ZNO: ELECTRICAL AND OPTICAL PROPERTIES SYNTHESIZED VIA SPUTTERING AND PYROLYSIS OF ZN-MOF DERIVATIVES |
title_short |
MODIFICATION OF NANOSTRUCTURE IN CARBON-DOPED ZNO: ELECTRICAL AND OPTICAL PROPERTIES SYNTHESIZED VIA SPUTTERING AND PYROLYSIS OF ZN-MOF DERIVATIVES |
title_full |
MODIFICATION OF NANOSTRUCTURE IN CARBON-DOPED ZNO: ELECTRICAL AND OPTICAL PROPERTIES SYNTHESIZED VIA SPUTTERING AND PYROLYSIS OF ZN-MOF DERIVATIVES |
title_fullStr |
MODIFICATION OF NANOSTRUCTURE IN CARBON-DOPED ZNO: ELECTRICAL AND OPTICAL PROPERTIES SYNTHESIZED VIA SPUTTERING AND PYROLYSIS OF ZN-MOF DERIVATIVES |
title_full_unstemmed |
MODIFICATION OF NANOSTRUCTURE IN CARBON-DOPED ZNO: ELECTRICAL AND OPTICAL PROPERTIES SYNTHESIZED VIA SPUTTERING AND PYROLYSIS OF ZN-MOF DERIVATIVES |
title_sort |
modification of nanostructure in carbon-doped zno: electrical and optical properties synthesized via sputtering and pyrolysis of zn-mof derivatives |
url |
https://digilib.itb.ac.id/gdl/view/79513 |
_version_ |
1822008908220203008 |
spelling |
id-itb.:795132024-01-09T07:52:10ZMODIFICATION OF NANOSTRUCTURE IN CARBON-DOPED ZNO: ELECTRICAL AND OPTICAL PROPERTIES SYNTHESIZED VIA SPUTTERING AND PYROLYSIS OF ZN-MOF DERIVATIVES Novi Hendri, Yasni Indonesia Dissertations Ferroelectric, Nanocolumnar, Polarization, Sputtering, Thermal Annealing, Carbon-doped ZnO, Zn-MOF. INSTITUT TEKNOLOGI BANDUNG https://digilib.itb.ac.id/gdl/view/79513 Zinc oxide (ZnO) is a semiconductor with a wide band gap of 3.33-3.37 eV and exceptional optical properties within the UV region. Introducing carbon doping to ZnO has the potential to reduce the band gap energy, resulting in broader optical absorption and thus serving as an alternative to enhance device performance. This study involved the preparation of carbondoped ZnO using sputtering and pyrolysis methods to modify surface structures and investigate their effects on electrical and optical properties. Density functional theory (DFT) was employed to support the experimental findings. In the sputtering method, samples are obtained in the form of thin films where ZnO and carbon-doped ZnO (ZnO:C-1, ZnO:C-2) grow on a Silicon (100) substrate with optimized deposition parameters (Power= 12W, growth temperature =300 ?, time= 4 hours, pressure = 0.3 kPa). Heating treatment after deposition (thermal annealing) was applied to the ZnO thin film at a temperature of 600 ? (ZnO/ann600) and 800 ? (ZnO/ann-800) under oxygen gas flow for 10 minutes. Furthermore, using the pyrolysis method, powdered samples were obtained, where Zn-MOF was converted into ZnO/C after heating at a temperature of 450 ? for 2 hours in various atmospheric conditions: nitrogen, oxygen, and air (ZnO/C-O2, ZnO/C-N2, ZnO/C-air). This research involved photocatalytic tests with the aim of evaluating the degradation capability of Rhodamine-B pollutant at a concentration of 20 ppm. Photocatalytic testing of ZnO/C samples derived from Zn-MOF was carried out using a portable solar simulator PEC-L01 (1000 W/m2 ). ZnO thin films grown using the sputtering method produce cone-shaped nanocolumnar structures (ZnO height= 850 nm) and change significantly into rods after annealing at temperatures of 600 ? (ZnO/ann-600 height=600 nm) and 800 ? (ZnO/ann- height 800=300 nm). Thermal annealing treatment induces an increase in the lattice constant c from 5.224 Å (ZnO) to 5.226 Å (ZnO/ann-600). Furthermore, we found an elliptical polarization response without saturation, indicating the presence of dominant leakage current and oxygen vacancies in the sample. The highest polarization is found in ZnO/ann-600 (|+Pr/-Pr|= 2.06) which is associated with an increase in the lattice constant c. Besides, ferroelectric characteristics were observed in ZnO/ann-800, with a lower polarization response (|+Pr/-Pr|= 1.14) due to the high density of nanocolumnar rods formed in the sample. Carbon-doped ZnO thin films grown using the sputtering method can reduce the height of ZnO nanocolumnar cones from 850 nm to 800 nm at a C concentration of 12.43% (ZnO:C-1) and 300 nm at a C concentration of 31.76% (ZnO:C -2). Carbon doping on nanocolumnar ZnO can effectively increase the lattice strain (????????????????= 1.658×10-4 , ????????????????:?????1= 5.995×10-4 and ????????????????:?????2= 7.249×10-3 ). The P–E hysteresis loop shows that ZnO:C-1 has the highest coercivity (11.1 kV/cm) which comes from Zn vacancies, while ZnO:C-2 has remanent polarization (4.7 ?C/cm2 ) which comes from oxygen vacancies produces ferroelectric material. Carbon doping reduces the band gap of ZnO from 3.28 eV to 3.25 eV (ZnO:C-1) and 3.23 eV (ZnO:C-2). Density functional theory calculations show that C doping changes the energy band structure in the Fermi energy region due to the contribution of the 2p orbital C atom. The pyrolysis method of Zn-MOF converted into ZnO/C produces various morphological forms depending on the variation of gas applied during pyrolysis. The morphology of Zn-MOF with a rod shape changes to granular (ZnO/C?O2) and spherical (ZnO/C?air) while ZnO/C-N2 still maintains a rod shape. The carbon atom concentration of Zn-MOF changed significantly from 57.43% to 68.41% (ZnO/C?N2), 62.56% (ZnO/C?O2), and 27.7% (ZnO/C?air ). The diffraction peak of ZnO/C?O2 shows the highest crystallinity compared to ZnO/C?air and ZnO/C-N2 where the dominant peak grows in the (101) direction. Furthermore, the BET-specific surface areas obtained were 16.8, 6.81, 12.15, 29.26 m2 /g for the Zn-MOF, ZnO/C?N2, ZnO/C?O2, and ZnO/C-air samples, respectively. ZnO/C?air shows optimal stability performance with a degradation efficiency of up to 94.1% against Rhodamine-B. This research has the potential to provide stable photocatalytic for wastewater purification, especially in the decomposition of Rhodamine-B pollutants. In addition, the results of this research also open up opportunities to obtain multifunctional devices with higher sensitivity and accuracy. Multifunctional devices apply the principles of coupling and integration between the resulting electrical and optical properties. It can also contribute to understanding carbon-doped ZnO materials through method comparisons, thermal annealing treatment, carbon doping, and converting Zn-MOF materials into ZnO/C. text |