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Transient Four-Wave Mixing Spectroscopy on PbS Quantum Dots Kevin Blondino (Florida State University) Advisors: Dr. Denis Karaiskaj, USF (faculty) Jason.

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Presentation on theme: "Transient Four-Wave Mixing Spectroscopy on PbS Quantum Dots Kevin Blondino (Florida State University) Advisors: Dr. Denis Karaiskaj, USF (faculty) Jason."— Presentation transcript:

1 Transient Four-Wave Mixing Spectroscopy on PbS Quantum Dots Kevin Blondino (Florida State University) Advisors: Dr. Denis Karaiskaj, USF (faculty) Jason Byslma (graduate student) 10 September 2012

2 Introduction  Four-Wave Mixing – the mixing of three electromagnetic waves resulting in a fourth wave in the phase-matched direction  It is a weak process governed by the 3 rd order nonlinear electric susceptibility  (3)  The JILA Multidimensional Optical Nonlinear Spectrometer (MONSTR) produces the FWM signal

3 Objective  To study the light-matter interactions in PbS Quantum Dots for use in solar energy harvesting  Measure exciton dephasing time  Find causes for beating in signal  Determine homogeneous/inhomogeneous linewidth in spectrum

4 Excitons and Quantum Dots  Exciton – the bound state of an electron and a hole; a quasi-particle, exists in some insulator and semiconductors.  Quantum Dot – a portion of a semiconductor whose excitons are confined in all dimensions. Properties of in between semiconductors and discrete molecules [2].  Researched for use in qubits, transistors, and photovoltaics.

5 Setup  The experiment was done at low temperature (< 5 K) and with a near-infrared laser wavelength (833 nm).  3 nm is average size of quantum dot.  Laser pulses (labeled a, b, c) in box formation.  a is the excitation pulse, phase conjugated.  b creates a grating with a on the sample.  c diffracts off the sample, creating the FWM signal.  Ultra-fast (~femtoseconds)  HeNe laser is used in conjunction to act as a reference pulse that is routed around the sample. This is referred to as heterodyne detection.

6 JILA MONSTR Multidimensional Optical Nonlinear SpecTRometers [1]

7 Setup

8 SignalFWM The full signal is the result of the bare FWM signal along with the reference controlling the piezoelectric devices to adjust for environmental disturbances. Reference Full Signal

9 Beating Beats occur from the periodic change of pulse a and b being in and out of phase. We want to find out if this is caused by quantum beating or by polarization beating.

10 Linewidth  Characterized as the width of a spectral line, or the coherence of the source of light.  In terms of photovoltaics, the wider the material’s natural linewidth, the higher efficiency, in general.  The exciton dephasing time is inversely proportional to the homogeneous linewidth.

11 2D Fourier-Transform Scan Emission:  t (meV) Absorption:   (meV) The diagonal represents where the frequencies are absorbed and then immediately emitted. This means that the electrons jump between two energy levels to absorb and emit photons, rather than having a third intermediate level. Having only two energy levels is more efficient. The extra signals represent scattered light or phonon resonances.

12 Next Steps  Find true cause of beating  Find a new T to minimize beating  Do polarization-dependent scans of excitation beams  Experiment on InAs quantum dots and GaAs quantum wells References [1] http://jila.colorado.edu/content/meet-jila-monstrs [2] http://en.wikipedia.org/wiki/Quantum_Dot


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