Photonic Crystal Cavities (coupled with InAs Quantum Dots) Wayne - - PowerPoint PPT Presentation

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Photonic Crystal Cavities (coupled with InAs Quantum Dots) Wayne - - PowerPoint PPT Presentation

Photonic Crystal Cavities (coupled with InAs Quantum Dots) Wayne McKenzie Introduction Quantum Dots Photonic Crystal Cavities Current Research Future Research What are Quantum Dots? Semi-conductor devices Artificial


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SLIDE 1

Photonic Crystal Cavities (coupled with InAs Quantum Dots)

Wayne McKenzie

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SLIDE 2

Introduction

  • Quantum Dots
  • Photonic Crystal Cavities
  • Current Research
  • Future Research
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SLIDE 3
  • Semi-conductor devices
  • Artificial atom’s
  • Resonance pumping results in s-shell population
  • Quasi-resonant (off resonant) results in p-shell population

What are Quantum Dots?

Quantum Memory Candidate 1us lifetime

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SLIDE 4

What are Quantum Dots?

  • InP/InAs/GaAs dots emit 1um-1.55um photons

(telecom wavelength)

  • We use AlInAs/InP dots grown through Molecular

Beam Epitaxy

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SLIDE 5

Why do we need photonic crystal cavities?

  • Quantum Dots
  • Incredibly useful for quantum experiments but,
  • Spontaneous emission (SE) from QD can occur in any direction
  • Emission efficiency is low
  • Introducing a cavity enhances the spontaneous emission of the QD

through the Purcell effect. Q: Quality Factor, V: mode volume of cavity

/

P

F Q V 

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SLIDE 6
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SLIDE 7

Low index of refraction (n=~1, air) High index of refraction (n = ~3)

Photonic Crystal with 2D periodic structure

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SLIDE 8
  • Measuring photons in the vertical

direction while changing the lattice spacing (a)

  • When emission spectrum overlaps with

PBG:

  • Vertical efficiency increases
  • SE can only occur vertically
  • Time of SE increases
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SLIDE 9
  • A cavity can be created by removing three holes in

the lattice, and shifting the holes on either side

  • This combination of removing/shifting has resulted

in a Q ‘s of 4000-45,000 while attempting to minimize V (to maximize Purcell effect)

  • Introducing this defect creates a cavity for

wavelengths that fall within the PBG defined by the periodicity

Creation of a Cavity

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SLIDE 10
  • Q-factor
  • M1: 7000
  • M2: 4300
  • M3: 380
  • M4: 2000
  • M5: 1000
  • L3 Defect cavity
  • a = 370nm
  • Hole radius = 0.27a
  • Slab thickness = 280 nm
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SLIDE 11
  • Quantum dot needs to be cooled to 4K in a cryostat
  • The distance between the PC and lens at the entry of the cryostat can cause photons to

spread

  • M1 mode has the highest Q-factor, but a far field measurement of the electric field (Ey

and Ex) shows that most of the light would not couple with the lens White line: 45o collection angle

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SLIDE 12

Current Research: Investigation of Biexcitons

Applying a magnetic field can reduce Fine Structure Splitting (FSS) ~4 nm split ~1 nm

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SLIDE 13

How to find Biexcitons?

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SLIDE 14

Spectrometer Mirror

Mirror’s for Vertical transition Variable Attenuator Lens

Cryostat

PBS

Camera

Excitation (blue) and Emission Path (red) Laser

780 nm pulsed laser

Microscope slide

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SLIDE 15
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SLIDE 16

5 1 1 5 2 2 5 3

P

  • w

e r

7 5 8 8 5 9 9 5 1 1 5

Intensity 1 2 3 3 .8 7

5 1 1 5 2 2 5 3

P

  • w

e r

7 6 7 8 8 8 2 8 4 8 6 8 8 9 9 2 9 4

Intensity 1 2 3 4 .3 6 5 1 1 5 2 2 5 3

P

  • w

e r

7 5 8 8 5 9 9 5 1 1 5

Intensity 1 2 5 .8 5 1 1 5 2 2 5 3

P

  • w

e r

7 4 7 6 7 8 8 8 2 8 4 8 6 8 8 9 9 2 9 4

Intensity 1 2 6 7 .5 7

X2 response

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SLIDE 17
  • +

s-shell s-shell p-shell p-shell

  • +

+ Energy GaAS (Coduction Band) GaAS (Valence Band) Wetting Layer Wetting Layer

Future Work

Resonance

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SLIDE 18

Continuing Research

  • On resonance pumping scheme
  • Photoluminescence excitation (PLE) measurements
  • Vary the pump wavelength and take spectrum measurments
  • Graph Pump wavelength vs. spectrum to determine s-shell (resonance) or p-

shell (quasi-resonant) behavior

  • Find additional QD’s that are better candidates for find biexcitons
  • This is limited due to the constraint of photons that are telecom wavelength
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SLIDE 19

Questions??