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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


  1. 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 for Polymer and Organic Solids (CPOS) University of California Santa Barbara Ben Eidelson 08/01/03

  2. 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 Ben Eidelson 2 08/01/03

  3. What is a CdSe quantum dot and why is it interesting? 1 1 + 2 − Color ~ E Gap R R R (simplified equation) [ Strouse Group ]   2   2 h 1 e 1     ∆ = + − + E ( R ) E Smaller Terms ( R )     − 1 S 1 S gap µ πε ε 2 8 R 4 R 3 / 2 e     e , h 0 [ Brus, LE (1983) ] Confinement Coulombic Ben Eidelson 3 08/01/03

  4. The Band Gap •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 (cm -1 ) Ben Eidelson 4 08/01/03

  5. Motivation/Interest • Quantum Computing • Solar Panels • For the sake of discovery Ben Eidelson 5 08/01/03

  6. How we Arrive at a Carrier Temperature Value • By collecting fluorescence and absorption • Using the Bolton-Archer equation (derived from the detailed balance method): Fluorescen ce 1 - 78 + ~ E c (simplified version) Absorbance T 2 h - 79 E 2 2 e n l f h n - 80       π τ E − f v ( ) h v 8 ln(10) g = + + g ln l r l       ε η - 81 2 2 2 ( ) v ( ) v v k T 10 N c g k T         B A u B 2.28 2.3 2.32 2.34 2.36 2.38 2.4 2.42 Energy (eV) Ben Eidelson 6 08/01/03

  7. Equipment Cary Eclipse Fluorescence Spectrophotometer Cary 50 Bio UV-Visible Spectrophotometer by Varian Labs by Varian Labs Fluorescence Absorption Ben Eidelson 7 08/01/03

  8. Data Comparison ~3.02nm CdSe, with peak absorbance at 520nm or 2.38eV •CdSe is much hotter! Control Experiment: Anthracene in ethanol •Note the relatively flat nature of Anthracene compared to CdSe quantum dots Ben Eidelson 8 08/01/03

  9. Data Conformation and Correlation •Peaks match the electronic ~3.02nm CdSe, with peak quantized states absorbance at 520nm or 2.38eV [ Norris and Bawendi (1996) ] Ben Eidelson 9 08/01/03

  10. 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? Ben Eidelson 10 08/01/03

  11. 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 Ben Eidelson 11 08/01/03

  12. 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 Ben Eidelson 12 08/01/03

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