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Carrier Dynamics in Microdisk Photonic Molecules
Center for Spintronics and Quantum Computation, University of California,
Santa Barbara, CA 93106
Felix M. Mendoza, R. C. Myers, G. Calusine, G. D. Fuchs, A.C. Gossard and
D. D. Awschalom
AFOSR
Materials Research Institute, Penn State University, University Park, PA 16802
X. Li, B. J. Cooley and N. Samarth
APS March Meeting, New Orleans, LA,
March 11, 2008
Spatially, spectrally and time-resolved luminescence
measurements of single “Photonic Molecules”
Coupled Microdisk Cavities – “Photonic Molecules”
Motivation – Semiconductor Microcavities
 Solid-state system for studying the
interaction between light and matter, e.g.
between photons and electron spins in the
cavity
 Optoelectronic applications (e.g. as a on-chip
laser source)
 Possible platform for quantum information
processing schemes (e.g. A. Imamoglu et.al.,
PRL 1999)
Microdisk Resonators
1 µm
 The dominant modes in these planar cavities are the whispering-gallery
modes that are confined to the perimeter of the disk due to total internal
reflection (top right)
 Light emission from the edges and, thus, in the plane of the disk (red
arrows) highly directional emission
 In thin disks, only the lowest-order modes are supported
nmedium
ndisk
Active Region of Our Structures
1 μm
GaAs substrate
Al0.7Ga0.3As pedestal
(500 nm)
Single Disk Diameter = 2 µm
Disk thickness = 110 nm Al0.3Ga0.7As cap (40 nm)
Al0.3Ga0.7As buffer (40 nm)
4.2 nm undoped GaAs QWs with
10 nm Al0.3Ga0.7As barriers
(Ga,Al)As
 Grown by Molecular Beam Epitaxy (MBE)
 “Natural” or “Interface-Fluctuation”
Quantum Dots (QDs)
 large ~ 100 nm in diameter
 provide weak confinement of carriers
2 min
Gammon, PRL, 1996
growth interruption
Coupled Microdisks – “Photonic Molecules”
Coupling between individual microdisks
 Overlap of evanescent fields (extent ~150 nm from edge of disk)
 Splitting into a “bonding” and an “anti-bonding” mode
“photonic molecule”
~ 185 nm – 225 nm
SEM Image Photoluminescence
 Polarization-resolved photoluminescence and simulations indicate
coupling
Polarization-resolved PL
bonding
anti-bonding
Simulation
y
x
θ
Bonding and Anti-bonding Modes
Splitting the Single Mode of Individual Microdisks through Coupling
(analogous to molecules)
 “Bonding” occurs when there occurs overlap between two mode
maxima or minima at the nearest point (left figure)
 “Anti-bonding” occurs when there occurs overlap between a
mode maximum and minima at the nearest point (right figure)
Energies get shifted due to different nature of overlap
between the evanescent fields
Bonding Mode Anti-Bonding Mode
Max
Min
Experimental Setup
Pulsed Ti:Sapphire
laser
Probe
Pump
Spectrometer
with CCD
Streak
Camera
Flip Mirrors
Balanced
Photodiode
Bridge
Imaging
CCD
Delay Line
Flow
Cryostat
B
Sample
 High spatial resolution
limited by laser spot (~ 1 μm)
 Small magnetic field (B) up
to 0.25 T
 Photoluminescence
measurements with spectral
and temporal resolution
 Pump-probe path for time-
resolved Kerr Rotation studies
5 K – 300 K
Lock-in
detection
750 755 760 765 770 775 780
Wavelength (nm)
Photoluminescence(a.u.)
750 755 760 765 770 775 780
T = 20 K
λ = 730 nm
Pexc = 1.2 kW/cm2
Wavelength (nm)
Photoluminescence(a.u.)
1 μm
Counts
226
409
Mode at λdet = 767.8 nm
Spatial Imaging of Photoluminescence
1 μm
White Light Image
1 μm
Counts
226
509
Mode at λdet = 766.2 nm
1 μm
Counts
226
509
Quantum Well at λdet = 763.0 nm
Modes sensitive to location of
excitation
T = 20 K
λexc = 720 nm
Pexc = 0.82 kW/cm2
Wavelength (nm)
Photoluminescence(a.u.)
750 755 760 765 770 775
Photoluminescence
Time-Resolved Photoluminescence
0 200 400 600 800
Single “Photonic Molecule”
Time (ps)
Intensity(normaized)
T = 20 K
λdet = 759.5 nm
λexc = 720 nm
0.28 kW/cm2
0.78 kW/cm2
Carrier Dynamics
 Timescale similar to previous measurements on single circular
microdisks (right)
 More complex dynamics in stimulated emission regime
Time (ps)
Intensity(normaized)
T = 5 K
λdet = 770 nm
λexc = 730 nm
S. Ghosh et. al., Nature Materials 5, 261 (2006)
Single Circular Microdisk
0 200 400 600 800
0.03 kW/cm2
1.8 kW/cm2
Conclusions
“Photonic Molecules” – Splitting of cavity modes into “bonding” and “anti-
bonding” states
Time-resolved luminescence reveals
more complex carrier dynamics than for
individual microdisks
AFOSR
Modes sensitive to location of excitation on the structure
1 μm
Back-up Slides
Elliptical “Photonic Molecules”
SEM Image
765 766 767 768 769 770
Wavelength (nm)
Polarizerangleθ
(deg)
PL(a.u)
Polarization-resolved PL
0
30
60
90
y
x
θ
1 μm
Elliptical Photonic Molecules
 Influence of anisotropic shape on photonic properties
Photoluminescence polarization of microdisk pair (coupled along
the long axis) shows similar dependence to circular disks (right)

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APS08_Felix_CoupledMicrodisks

  • 1. Carrier Dynamics in Microdisk Photonic Molecules Center for Spintronics and Quantum Computation, University of California, Santa Barbara, CA 93106 Felix M. Mendoza, R. C. Myers, G. Calusine, G. D. Fuchs, A.C. Gossard and D. D. Awschalom AFOSR Materials Research Institute, Penn State University, University Park, PA 16802 X. Li, B. J. Cooley and N. Samarth APS March Meeting, New Orleans, LA, March 11, 2008 Spatially, spectrally and time-resolved luminescence measurements of single “Photonic Molecules” Coupled Microdisk Cavities – “Photonic Molecules”
  • 2. Motivation – Semiconductor Microcavities  Solid-state system for studying the interaction between light and matter, e.g. between photons and electron spins in the cavity  Optoelectronic applications (e.g. as a on-chip laser source)  Possible platform for quantum information processing schemes (e.g. A. Imamoglu et.al., PRL 1999)
  • 3. Microdisk Resonators 1 µm  The dominant modes in these planar cavities are the whispering-gallery modes that are confined to the perimeter of the disk due to total internal reflection (top right)  Light emission from the edges and, thus, in the plane of the disk (red arrows) highly directional emission  In thin disks, only the lowest-order modes are supported nmedium ndisk
  • 4. Active Region of Our Structures 1 μm GaAs substrate Al0.7Ga0.3As pedestal (500 nm) Single Disk Diameter = 2 µm Disk thickness = 110 nm Al0.3Ga0.7As cap (40 nm) Al0.3Ga0.7As buffer (40 nm) 4.2 nm undoped GaAs QWs with 10 nm Al0.3Ga0.7As barriers (Ga,Al)As  Grown by Molecular Beam Epitaxy (MBE)  “Natural” or “Interface-Fluctuation” Quantum Dots (QDs)  large ~ 100 nm in diameter  provide weak confinement of carriers 2 min Gammon, PRL, 1996 growth interruption
  • 5. Coupled Microdisks – “Photonic Molecules” Coupling between individual microdisks  Overlap of evanescent fields (extent ~150 nm from edge of disk)  Splitting into a “bonding” and an “anti-bonding” mode “photonic molecule” ~ 185 nm – 225 nm SEM Image Photoluminescence  Polarization-resolved photoluminescence and simulations indicate coupling Polarization-resolved PL bonding anti-bonding Simulation y x θ
  • 6. Bonding and Anti-bonding Modes Splitting the Single Mode of Individual Microdisks through Coupling (analogous to molecules)  “Bonding” occurs when there occurs overlap between two mode maxima or minima at the nearest point (left figure)  “Anti-bonding” occurs when there occurs overlap between a mode maximum and minima at the nearest point (right figure) Energies get shifted due to different nature of overlap between the evanescent fields Bonding Mode Anti-Bonding Mode Max Min
  • 7. Experimental Setup Pulsed Ti:Sapphire laser Probe Pump Spectrometer with CCD Streak Camera Flip Mirrors Balanced Photodiode Bridge Imaging CCD Delay Line Flow Cryostat B Sample  High spatial resolution limited by laser spot (~ 1 μm)  Small magnetic field (B) up to 0.25 T  Photoluminescence measurements with spectral and temporal resolution  Pump-probe path for time- resolved Kerr Rotation studies 5 K – 300 K Lock-in detection
  • 8. 750 755 760 765 770 775 780 Wavelength (nm) Photoluminescence(a.u.) 750 755 760 765 770 775 780 T = 20 K λ = 730 nm Pexc = 1.2 kW/cm2 Wavelength (nm) Photoluminescence(a.u.) 1 μm Counts 226 409 Mode at λdet = 767.8 nm Spatial Imaging of Photoluminescence 1 μm White Light Image 1 μm Counts 226 509 Mode at λdet = 766.2 nm 1 μm Counts 226 509 Quantum Well at λdet = 763.0 nm Modes sensitive to location of excitation
  • 9. T = 20 K λexc = 720 nm Pexc = 0.82 kW/cm2 Wavelength (nm) Photoluminescence(a.u.) 750 755 760 765 770 775 Photoluminescence Time-Resolved Photoluminescence 0 200 400 600 800 Single “Photonic Molecule” Time (ps) Intensity(normaized) T = 20 K λdet = 759.5 nm λexc = 720 nm 0.28 kW/cm2 0.78 kW/cm2 Carrier Dynamics  Timescale similar to previous measurements on single circular microdisks (right)  More complex dynamics in stimulated emission regime Time (ps) Intensity(normaized) T = 5 K λdet = 770 nm λexc = 730 nm S. Ghosh et. al., Nature Materials 5, 261 (2006) Single Circular Microdisk 0 200 400 600 800 0.03 kW/cm2 1.8 kW/cm2
  • 10. Conclusions “Photonic Molecules” – Splitting of cavity modes into “bonding” and “anti- bonding” states Time-resolved luminescence reveals more complex carrier dynamics than for individual microdisks AFOSR Modes sensitive to location of excitation on the structure 1 μm
  • 12. Elliptical “Photonic Molecules” SEM Image 765 766 767 768 769 770 Wavelength (nm) Polarizerangleθ (deg) PL(a.u) Polarization-resolved PL 0 30 60 90 y x θ 1 μm Elliptical Photonic Molecules  Influence of anisotropic shape on photonic properties Photoluminescence polarization of microdisk pair (coupled along the long axis) shows similar dependence to circular disks (right)

Editor's Notes

  1. 6 QWs in disk
  2. Formula for power density: [(power meter reading)/62.41 * 9]/(pi*4* (10-8)) = power density in mW/cm^2