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Presented by ROLL #
PRESENTED TO
10/5/2022 1
TOPIC
Oxygen flux influence on the morphological, structural and optical
properties of π™π§πŸβˆ’π±πŒπ π± O thin films grown by plasma-assisted
molecular beam epitaxy
10/5/2022 2
Introduction
β€’ Recently, zno has attracted attention for its potential applications as a wide band
gap semiconductor in opto-electronics devices with a large exciton binding
energy of 60 MeV.
β€’ Zinc oxide is also being used in laser LEDs and optoelectronics devices etc.
β€’ The wurtzite structure between Mg2+
(0.57 A) and Zn2+
(0.60 A) has been widely
studied as a barrier material for ZnO/ZnMgO quantum wells due to the similarity
of ionic radius.
β€’ Several groups successfully reported the growth of single wurtzite phase
𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O layers with a maximum Mg concentration is up to 49% .We have
also obtained wurtzite structure 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O thin film with up to 30% Mg.
10/5/2022 3
β€’ Thin films containing a single hexagonal phase were grown by
𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O by P-MBE over a large range of oxygen fluxes.
β€’ The effects of oxygen flow on the structural, optical and
morphological properties of thin films were studied.
β€’ By controlling the flow rate of oxygen, thin films of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O was
obtained by two-dimensional growth of wurtzite structures.
β€’ The formation of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O thin films was controlled by adjusting
the oxygen flow rate
10/5/2022 4
Experiment
β€’ The growth was carried out using a V80H molecular-beam epitaxy system
equipped with Knudsen cells for a Zn solid source (99.9999%) and an Mg
solid source (99.999%) as well as an radio frequency (rf)-plasma cell for
oxygen source (𝑂2,99.999%).
β€’ A mass flux controller controls the oxygen flow rate.
β€’ The oxygen flow rate was varied 0.2–0.8 sccm, and the Zn source and Mg
source were controlled at 245 ⁰C and 280 ⁰C, respectively.
β€’ The c-plane sapphire (𝐴𝑙2𝑂3) was used as the substrate.
β€’ To get a Clean fresh surfaces the substrates were chemically etched in a hot
solution of H2SO4:H3PO4 = 3:1 at 160 ⁰C for 15 min.
10/5/2022 5
β€’ Before growth, the substrates were thermally pre-treated at 800 ⁰C for 30
min, which was expected to remove surface contaminant and obtain oxygen
terminated 𝐴𝑙2𝑂3 (0 0 0 1) surface. The (0001), or the basal plane, is the
most commonly used surface for growth.
β€’ The films were grown at 600 ⁰C
β€’ X-ray diffraction (XRD) spectra were collected with Cu Ka radiation of
0.1543 nm to obtain the structural information of the films.
β€’ The sample morphology was investigated by a filed emission scanning
electron microscope (SEM).
10/5/2022 6
Results and Discussion
β€’ The Mg contents were detected by the energy dispersive spectroscopy EDS
β€’ The details growth parameters and Mg contents are given in Table 1
10/5/2022 7
Sample Zn source
T (⁰C)
Mg source
T (⁰C)
Substrate
temperatur
e
T (⁰C)
O2 flow rate
(sccm)
Growth
pressure
(mbar)
Mg
content
(x)
a
b
c
d
245
245
245
245
280
280
280
280
600
600
600
600
0.2
0.4
0.6
0.8
6Γ—10βˆ’7
8Γ—10βˆ’7
3Γ—10βˆ’6
1Γ—10βˆ’5
0.20
0.15
0.06
0.03
β€’ The EDS for the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films are
shown in Fig. 1.
β€’ Only Zn, Mg, O and Al signals were
detected In all the samples, indicating
formation of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films
with high purity.
β€’ From EDS, it is found that all the
𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films show metallic-rich
characteristic.
10/5/2022 8
10/5/2022 9
Fig. 2 shows the SEM images of the surface of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O layer grown under different oxygen
flow rates.
β€’ When the oxygen flow rate is 0.2 sccm, a flat surface morphology
of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O film is obtained in Fig. 2(a).
β€’ With increasing of the oxygen flow rate,
the surface morphology of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O
films becomes rough gradually.
β€’ Many pits appear on the surface of the
𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films at the oxygen flow rate of
0.4 sccm, as shown in Fig. 2(b).
β€’ Fig. 2(c) and (d) exhibits that the
nanostructures were formed on the surface
of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films grown under higher
oxygen flow rate conditions.
β€’ The thicknesses of the grown films are
measured by lateral image of SEM.
β€’ Fig. 3 shows the XRD spectra for the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films with different Mg contents of x = 0.20,
0.15, 0.06, 0.03 and 0,respectively. All the films have wurtzite structure with c-axis preferred
orientation. No peak from other phases and impurities were observed.
β€’ It should be noted that the diffraction
peaks show asymmetrical line shape,
which was caused by the superposition
of diffractions from Ka1 and Ka2 lines.
β€’ It indicates that the thin films have good
crystal quality.
β€’ With increasing oxygen flux, the
position of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O (0 0 2)
peaks shifts from 34.688 (x = 0.20) to
34.448 (x = 0).
β€’ This indicates that Mg2+ successfully replaces the Zn2+ in the ZnO lattice, and the Mg content is
decreased with increasing of oxygen flow rate.
10/5/2022 10
10/5/2022 11
Fig. 4. Oxygen flux dependences of the Mg content in the π’π’πŸβˆ’π’™π‘΄π’ˆπ’™O films(a)
and Mg content dependences of the c-axis lattice parameters in the π’π’πŸβˆ’π’™π‘΄π’ˆπ’™O
films(b).
Conclusion
β€’ In summary, the single-phase 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯ O films with c-axis oriented wurtzite
structure were grown on 𝐴𝑙2𝑂3 substrate by PMBE.
β€’ It is feasible to adjust the Mg contents by changing the oxygen flow rate. With
changing the oxygen flow rate from 0.2 sccm to 0.8 sccm, 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films with Mg
contents of 0.2–0.03 were obtained.
β€’ The morphology of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films becomes roughness with the decreasing the
oxygen flow rate.
β€’ The 2D growing of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O thin films with the wurtzite structure was
obtained under low oxygen flow rates.
β€’ This may be used as a method to realize precise control of growth parameters and alloy
composition in the fabrication of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O thin films.
10/5/2022 12
THANK YOU
10/5/2022 13

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research.pptx

  • 1. Presented by ROLL # PRESENTED TO 10/5/2022 1
  • 2. TOPIC Oxygen flux influence on the morphological, structural and optical properties of π™π§πŸβˆ’π±πŒπ π± O thin films grown by plasma-assisted molecular beam epitaxy 10/5/2022 2
  • 3. Introduction β€’ Recently, zno has attracted attention for its potential applications as a wide band gap semiconductor in opto-electronics devices with a large exciton binding energy of 60 MeV. β€’ Zinc oxide is also being used in laser LEDs and optoelectronics devices etc. β€’ The wurtzite structure between Mg2+ (0.57 A) and Zn2+ (0.60 A) has been widely studied as a barrier material for ZnO/ZnMgO quantum wells due to the similarity of ionic radius. β€’ Several groups successfully reported the growth of single wurtzite phase 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O layers with a maximum Mg concentration is up to 49% .We have also obtained wurtzite structure 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O thin film with up to 30% Mg. 10/5/2022 3
  • 4. β€’ Thin films containing a single hexagonal phase were grown by 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O by P-MBE over a large range of oxygen fluxes. β€’ The effects of oxygen flow on the structural, optical and morphological properties of thin films were studied. β€’ By controlling the flow rate of oxygen, thin films of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O was obtained by two-dimensional growth of wurtzite structures. β€’ The formation of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O thin films was controlled by adjusting the oxygen flow rate 10/5/2022 4
  • 5. Experiment β€’ The growth was carried out using a V80H molecular-beam epitaxy system equipped with Knudsen cells for a Zn solid source (99.9999%) and an Mg solid source (99.999%) as well as an radio frequency (rf)-plasma cell for oxygen source (𝑂2,99.999%). β€’ A mass flux controller controls the oxygen flow rate. β€’ The oxygen flow rate was varied 0.2–0.8 sccm, and the Zn source and Mg source were controlled at 245 ⁰C and 280 ⁰C, respectively. β€’ The c-plane sapphire (𝐴𝑙2𝑂3) was used as the substrate. β€’ To get a Clean fresh surfaces the substrates were chemically etched in a hot solution of H2SO4:H3PO4 = 3:1 at 160 ⁰C for 15 min. 10/5/2022 5
  • 6. β€’ Before growth, the substrates were thermally pre-treated at 800 ⁰C for 30 min, which was expected to remove surface contaminant and obtain oxygen terminated 𝐴𝑙2𝑂3 (0 0 0 1) surface. The (0001), or the basal plane, is the most commonly used surface for growth. β€’ The films were grown at 600 ⁰C β€’ X-ray diffraction (XRD) spectra were collected with Cu Ka radiation of 0.1543 nm to obtain the structural information of the films. β€’ The sample morphology was investigated by a filed emission scanning electron microscope (SEM). 10/5/2022 6
  • 7. Results and Discussion β€’ The Mg contents were detected by the energy dispersive spectroscopy EDS β€’ The details growth parameters and Mg contents are given in Table 1 10/5/2022 7 Sample Zn source T (⁰C) Mg source T (⁰C) Substrate temperatur e T (⁰C) O2 flow rate (sccm) Growth pressure (mbar) Mg content (x) a b c d 245 245 245 245 280 280 280 280 600 600 600 600 0.2 0.4 0.6 0.8 6Γ—10βˆ’7 8Γ—10βˆ’7 3Γ—10βˆ’6 1Γ—10βˆ’5 0.20 0.15 0.06 0.03
  • 8. β€’ The EDS for the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films are shown in Fig. 1. β€’ Only Zn, Mg, O and Al signals were detected In all the samples, indicating formation of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films with high purity. β€’ From EDS, it is found that all the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films show metallic-rich characteristic. 10/5/2022 8
  • 9. 10/5/2022 9 Fig. 2 shows the SEM images of the surface of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O layer grown under different oxygen flow rates. β€’ When the oxygen flow rate is 0.2 sccm, a flat surface morphology of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O film is obtained in Fig. 2(a). β€’ With increasing of the oxygen flow rate, the surface morphology of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films becomes rough gradually. β€’ Many pits appear on the surface of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films at the oxygen flow rate of 0.4 sccm, as shown in Fig. 2(b). β€’ Fig. 2(c) and (d) exhibits that the nanostructures were formed on the surface of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films grown under higher oxygen flow rate conditions. β€’ The thicknesses of the grown films are measured by lateral image of SEM.
  • 10. β€’ Fig. 3 shows the XRD spectra for the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films with different Mg contents of x = 0.20, 0.15, 0.06, 0.03 and 0,respectively. All the films have wurtzite structure with c-axis preferred orientation. No peak from other phases and impurities were observed. β€’ It should be noted that the diffraction peaks show asymmetrical line shape, which was caused by the superposition of diffractions from Ka1 and Ka2 lines. β€’ It indicates that the thin films have good crystal quality. β€’ With increasing oxygen flux, the position of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O (0 0 2) peaks shifts from 34.688 (x = 0.20) to 34.448 (x = 0). β€’ This indicates that Mg2+ successfully replaces the Zn2+ in the ZnO lattice, and the Mg content is decreased with increasing of oxygen flow rate. 10/5/2022 10
  • 11. 10/5/2022 11 Fig. 4. Oxygen flux dependences of the Mg content in the π’π’πŸβˆ’π’™π‘΄π’ˆπ’™O films(a) and Mg content dependences of the c-axis lattice parameters in the π’π’πŸβˆ’π’™π‘΄π’ˆπ’™O films(b).
  • 12. Conclusion β€’ In summary, the single-phase 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯ O films with c-axis oriented wurtzite structure were grown on 𝐴𝑙2𝑂3 substrate by PMBE. β€’ It is feasible to adjust the Mg contents by changing the oxygen flow rate. With changing the oxygen flow rate from 0.2 sccm to 0.8 sccm, 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films with Mg contents of 0.2–0.03 were obtained. β€’ The morphology of 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O films becomes roughness with the decreasing the oxygen flow rate. β€’ The 2D growing of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O thin films with the wurtzite structure was obtained under low oxygen flow rates. β€’ This may be used as a method to realize precise control of growth parameters and alloy composition in the fabrication of the 𝑍𝑛1βˆ’π‘₯𝑀𝑔π‘₯O thin films. 10/5/2022 12