Progress of Semiconductor Quantum Dots Chuan-Pu Liu ( 劉全璞 ) Department of Materials Science...

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Progress of Semiconductor Quantum Dots Chuan-Pu Liu ( 劉劉劉 ) Department of Materials Science and Engineering, National Cheng-Kung University Taiwan

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Progress of Semiconductor Quantum Dots Chuan-Pu Liu ( 劉全璞 ) Department of Materials Science and Engineering, National Cheng-Kung University Taiwan. Outline Introduction Fabrication methods Recent achievements Our achievements Application in quantum devices. - PowerPoint PPT Presentation

Transcript of Progress of Semiconductor Quantum Dots Chuan-Pu Liu ( 劉全璞 ) Department of Materials Science...

Page 1: Progress of Semiconductor  Quantum Dots Chuan-Pu Liu ( 劉全璞 ) Department of Materials Science and

Progress of Semiconductor Quantum Dots

Chuan-Pu Liu (劉全璞 )Department of Materials Science and

Engineering,National Cheng-Kung University

Taiwan

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Outline

•Introduction

• Fabrication methods

• Recent achievements

• Our achievements

• Application in quantum devices

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Page 4: Progress of Semiconductor  Quantum Dots Chuan-Pu Liu ( 劉全璞 ) Department of Materials Science and
Page 5: Progress of Semiconductor  Quantum Dots Chuan-Pu Liu ( 劉全璞 ) Department of Materials Science and

Fabrication methods

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(a) metal and metal oxide systems patterned by lithography. (b) metallic dots out of chemical suspensions. (c) lateral quantum dots through electrical gating of heterostructures. (d) vertical quantum dots through wet etching of quantum well structures. (e) pyramidal quantum dots through self-assembled growth. (f) trench quantum wire.

Typical QD structures

Non-isotropic etching

Damage on sidesdue to RIE

Limited size

Limited size

Integration problem

Best

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Other techniques

1.Patterned substrate: V-grooves or inverted pyramids. But a. growth is complex, such as corrugation of facet surfaces tilting of facets, non-uniform growth rate b. understanding of complex surface, interfacet kinetics and energetics is required2. Cleaved edge overgrowth quantum dots form at the junction of three orthogonal quantum wells a. complicated process b. difficult to control size and shape

Quantum dot

Barrier

Barrier

AlGaAs

AlGaAsGaAs001

Quantum wires

Page 8: Progress of Semiconductor  Quantum Dots Chuan-Pu Liu ( 劉全璞 ) Department of Materials Science and

Other techniques

1.Patterned substrate: V-grooves or inverted pyramids. But a. growth is complex, such as corrugation of facet surfaces tilting of facets, non-uniform growth rate b. understanding of complex surface, interfacet kinetics and energetics is required2. Cleaved edge overgrowth quantum dots form at the junction of three orthogonal quantum wells a. complicated process b. difficult to control size and shape

Quantum dot

Barrier

Barrier

AlGaAs

AlGaAsGaAs001

Quantum wires

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Growth mode for QD2 + 12 <? 1 Surface + Strain energy

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Stranski-Krastanow growth mode

What happen when together?

Shape evolution

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Recent Achievements

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Ordering of QD (recently achieved)

InAs QD

APL, 78, 105 (2001)

PbSe QD

Science, 282, 734 (1998)

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Our experimental Results

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0 0.50 1.00 1.50m

0.0 nm

25.0 nm

50.0 nm

m0 0.50 1.00 1.50

0.0 nm

17.5 nm

35.0 nm

Co magnetic Nanoparticles prepared by PVD

Without Electron Charging With Electron Charging

Size: 10~100nm Size: 10~20nm

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Ge/Si(001)• Self-assembly• by MBE or CVD

20nm

Ge quantum dots on Si(001) substrate

PyramidDome

Dome Superdome

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Stability of Ge quantum dot against water vapor

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40nm

40nm

• Si/Ge(111)• Self-assembly• by MBE or CVD

• InAs/GaAs(001)• Self-assembly• by MOCVD

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Nanocluster fabrication by UHV-Sputtering

• Ge / Si (001) • By UHV–Sputtering• Size shrinkage• 4 quantum dot a cell

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Nanocluster characterization with TEM

Pyramid Dome

Strain

Composition

Shape

Size

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Application in quantum devices

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Advantages of implementing quantum dot

for quantum computation

• Compactness and Robustness

• Large number of qubits

• No statistical mixture of pure quantum states

like in NMR

• compatible with current Si based technology

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Wireless logic devices

Inverter Majority Gate

Parallel

Opposite

4 dot cellt :energy barrier a :spacing

The extra two electrons will move around until the lowest energy configuration depending on the Schrödinger equation

By University of Notre Dame

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Field-effect Spin Resonance Transistor

Prof. Kang L. Wang, Electrical Engineering Department, UCLA

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by NC State

Silicon quantum dot quantum computation

Single electron is trapped at each quantum dot at low temperatureZeeman spin states of these electrons constitute the qubitsExchange coupling between electron spins

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III - V Pillar Quantum Computer

• Asymmetric dots produce a large dipole moment

• Dephasing due to electron- phonon scattering and spontaneous emission is strongly minimized.

• Strong dipole-dipole coupling and long dephasing time

by NC State