Carrier Temperatures in CdSe Quantum Dots Using Detailed Balance - - PowerPoint PPT Presentation

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Carrier Temperatures in CdSe Quantum Dots Using Detailed Balance - - PowerPoint PPT Presentation

Carrier Temperatures in CdSe Quantum Dots Using Detailed Balance Method Ben Eidelson 1,2 , Artjay Javier 3 , Geoffrey F. Strouse 3, * 1 Internships in Nanosystems Science, Engineering and Technology (INSET) 2 Santa Barbara City College 3 Center


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SLIDE 1

Ben Eidelson 08/01/03

Carrier Temperatures in CdSe Quantum Dots Using Detailed Balance Method

Ben Eidelson1,2, Artjay Javier3, Geoffrey F. Strouse3,*

1Internships in Nanosystems Science, Engineering and Technology (INSET) 2Santa Barbara City College 3Center for Polymer and Organic Solids (CPOS)

University of California Santa Barbara

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2

Ben Eidelson 08/01/03

Overview

  • CdSe Quantum Dots, the Band Gap, Phonon Bottleneck,

and Carrier Temperatures Explained

  • Motivation/Interest
  • Equipment
  • Our Method and Results
  • Data Comparison
  • Future Work
  • Acknowledgements
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Ben Eidelson 08/01/03

What is a CdSe quantum dot and why is it interesting?

R R E Color

Gap

1 1 ~

2 −

+

R

(simplified equation)

) R ( Terms Smaller R 1 4 e R 1 8 h E ) R ( E

2 2 h , e gap S 1 S 1

e 2 / 3

+         −         + =

2 −

ε πε µ ∆

Confinement Coulombic

[Brus, LE (1983)] [Strouse Group]

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Ben Eidelson 08/01/03

  • Band Edge Jumps = Couple,

then release photon

  • Hot Bands = Coupling is not

efficient, so release photon early

  • If Hot Bands are more

probable then there is a phonon bottleneck

The Band Gap

(cm-1)

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Ben Eidelson 08/01/03

Motivation/Interest

  • Quantum Computing
  • Solar Panels
  • For the sake of discovery
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Ben Eidelson 08/01/03

How we Arrive at a Carrier Temperature Value

  • By collecting fluorescence and absorption
  • Using the Bolton-Archer equation (derived

from the detailed balance method):

c E T Absorbance ce Fluorescen + 1 ~

(simplified version)

2 2 2

8 ln(10) ( ) ln l ( ) ( ) 10

g l r B A u B

E g f v h v v v v k T N c g k T π τ ε η       − = + +              

2.28 2.3 2.32 2.34 2.36 2.38 2.4 2.42 Energy (eV)

  • 81
  • 80
  • 79
  • 78

n l f h

2e n

E 2 h

2

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Ben Eidelson 08/01/03

Equipment

Cary Eclipse Fluorescence Spectrophotometer by Varian Labs Cary 50 Bio UV-Visible Spectrophotometer by Varian Labs

Fluorescence Absorption

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Ben Eidelson 08/01/03

Data Comparison

Anthracene in ethanol

~3.02nm CdSe, with peak absorbance at 520nm or 2.38eV

  • Note the relatively flat nature of

Anthracene compared to CdSe quantum dots

Control Experiment:

  • CdSe is much hotter!
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Ben Eidelson 08/01/03

Data Conformation and Correlation

  • Peaks match the electronic

quantized states

~3.02nm CdSe, with peak absorbance at 520nm or 2.38eV

[Norris and Bawendi (1996)]

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Ben Eidelson 08/01/03

Future Work

  • We now know that the carrier temperatures

are high, but why is this?

– What is the cause of the Phonon Bottleneck?

  • Boltzmann distribution reasoning
  • What things affect carrier temperature and

how?

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Ben Eidelson 08/01/03

Acknowledgements

  • My parents for their continued support
  • Family and friends
  • The INSET program and CNSI
  • Santa Barbara City College
  • The Strouse Group
  • Donny Magana for synthesis of CdSe QDs
  • University of California Santa Barbara
  • Funding provided by:

National Science Foundation-Division of Materials Research and Office of Naval Research

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Ben Eidelson 08/01/03

What is a Carrier Temperature and Detailed Balance Method?

  • The exciton (hole and electron) system is in

a Boltzmann distribution cycle

  • This thermodynamic cycle has an

equilibrium temperature (hence ‘Detailed Balance’)

  • That temperature can be extracted as the

carrier temperature