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Fabrication and Characterization of n-ZnO/p-Si Heterostructure

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During my final year project presentation (VIVA). Title of project : Fabrication and Characterization of n-ZnO/p-Si Heterostructure
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FABRICATION AND CHARACTERIZATION OF n-ZnO / p-Si HETEROSTRUCTURE BY NUR ATIQAH BINTI MASRI 109261 Applied Science (Engineering Physics) Supervisor : DR. Ng Sha Shiong Examiner : DR. Mutharasu Devarajan School of Physics, Universiti Sains Malaysia (USM), 11800 Minden, Penang, Malaysia.
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Page 1: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

FABRICATION AND CHARACTERIZATION OF n-ZnO

/ p-Si HETEROSTRUCTURE

BY

NUR ATIQAH BINTI MASRI

109261Applied Science (Engineering Physics)

Supervisor : DR. Ng Sha ShiongExaminer : DR. Mutharasu Devarajan

School of Physics, Universiti Sains Malaysia (USM), 11800 Minden, Penang, Malaysia.

Page 2: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Presentation’s Agenda

1. Introduction2. Objectives3. Definitions4. Literature Review5. Methodology6. Observations and Results7. Conclusion

Page 3: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Introduction

Background of Heterostructure A structure that has junctions between

different bandgap materials or a structure that made from a

heterojunction Advantages of n-ZnO

Wide direct optical bandgap Large exciton binding energy Large melting point Strong anti-radiation damaging ability

Page 4: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Advantages of p-Si Cheap Easier to cleave than that sapphire

Advantages of n-ZnO/p-Si Used for fabrication of solar cells and

optoelectronic devices

Page 5: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Objectives

To fabricate n-ZnO thin film on p-Si substrate by radio frequency (RF) sputtering.

To investigate the structural and electrical properties of the n-ZnO/p-Si heterojunction.

Page 6: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Definition

Depletion region, W - the regions of accumulation of net positively charge and negatively charged.

Page 7: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Literature Review

1. The properties of ZnO is depent on film thickness as well as properties of heterojunction.

Mridha, S., M. Dutta, and D. Basak

2. ZnO/Si heterojunction exhibit a good rectifying behaviour. Ocak, Y.S., and Chen, T., et al., and Xiao-Yun, T., et al., and Song, D., et al.,

and Zebbar, N., et al.

3. The small deviation from the ohmic behaviour indicates that the transport mechanism depends on the nature of contacts.

Zebbar, N., et al.

4. The smaller the FWHM, the higher the film’s crystallinity Qi, H., et al.

Page 8: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Methodology

Sample Preparation

ZnO thin film is deposited on p-type Si by RF

Sputtering

Characterizations

Structural Properties

XRD

To measured

the crystalline

structure of the ZnO film

FESEM

To view the surface

morphology of sample

To determine the thickness of the

sample

AFMTo scan the specimen surface

To determine the topography and

other properties of sample surfaces

Electrical Properties

Contact Characteristics

Al Contact

Annealing Process

To get ohmic (annealing

process at 550°C for 20 mins using

grey furnace)Hall Effect measurements

I-V and C-V Characteristics of

PN Junction

Page 9: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Observations and Results

STRUCTURAL CHARACTERIZATIONS

Page 10: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

XRD

To identify crystalline phases and orientation.

Showed three peaks :-(a) Si (111) at 28.75(b) ZnO (002) at 34.15 - highest peak(c) ZnO (004) at 71.94

The smaller the FWHM, the higher the crytallinity and the better the quality of the sample.

Page 11: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

FESEM

To analyse the film thickness and surface morphology of the sample.

The image of surface is analysed by two different magnification (30 kx and 100 kx) to obtain the clearer image of sample’s surface.

Results Granular shape of particles Thickness of wafer = 505.8 nm

Page 12: Fabrication and Characterization of n-ZnO/p-Si Heterostructure
Page 13: Fabrication and Characterization of n-ZnO/p-Si Heterostructure
Page 14: Fabrication and Characterization of n-ZnO/p-Si Heterostructure
Page 15: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

AFM

To determine the roughness, height steep measurement and image surface of sample.

Results RMS = 0.00513 m highness of peak = 20.9 nm

Page 16: Fabrication and Characterization of n-ZnO/p-Si Heterostructure
Page 17: Fabrication and Characterization of n-ZnO/p-Si Heterostructure
Page 18: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

ELECTRICAL CHARACTERIZATIONS

Page 19: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

I-V and C-V Characteristics

To obtain ohmic for contacts from I-V curve

To obtain the rectifying behaviour for the heterojunction.

To determine the ideality factor, barrier height and width of depletion region.

Page 20: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Ohmic contact

Not symmetry because of the differences in surface’s condition

Page 21: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

p-n junctions

I-V curve

Io = 2 x 10-6 A, 𝜱b = 0.86 eV , n = 3.26, W = 386.9 nm

Page 22: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

C-V curve

Vbi = 0.65 eV , 𝜱b = 0.81 eV , W = 402.7 nm

Page 23: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

Hall effect measurements

To obtain the carrier and holes concentration of the samples.

Electrons concentration, Nd : 1.83 1016

cm3 ; Hall mobility : 1.28 cm2/Vs Holes concentration, Na : 4.81015 cm3 ;

Hall mobility : 270 cm2/Vs.

Page 24: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

CONCLUSIONS

Not an ideal diode.

Barrier height of this heterojuction that is obtained from C-V curve, 0.05 eV lower than that obtained from I-V curve.

Width of depletion region obtained from C-V curve 15.8 nm higher than that I-V curve.

The differences of barrier height and width of depletion region obtained from I-V and C-V measurements are results of the different technique used.

Page 25: Fabrication and Characterization of n-ZnO/p-Si Heterostructure

THANK YOU!


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