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Effect of Atomic-Scale Randomness on the
  Optical Polarization of Semiconductor
              Quantum Dots

         Vladan Mlinar and Alex Zunger

       National Renewable Energy Laboratory,
               Golden, Colorado USA




                                        Vladan.Mlinar@nrel.gov
Structure – Spectra relationship:

QD morphology:                      Single-dot spectroscopy:




Ga1-xInxAs QDs                                           (P. A. Dalgarno &
(~105 atoms)                                             R. J. Warburton)
Structure – Spectra relationship:

QD morphology:         Theory:               Single-dot spectroscopy:




                     Input structure


Ga1-xInxAs QDs     Strain minimization
                                                                  (P. A. Dalgarno &
(~105 atoms)                                                      R. J. Warburton)


                 Solve the single-particle
                 problem


                 Solve many-particle
                 Problem (CI calc.)


                   Emission Spectra
Structure – Spectra relationship:

QD morphology:         Theory:               Single-dot spectroscopy:




                     Input structure


Ga1-xInxAs QDs     Strain minimization
                                                                  (P. A. Dalgarno &
(~105 atoms)                                                      R. J. Warburton)


                 Solve the single-particle
                 problem


                 Solve many-particle
                 Problem (CI calc.)


                   Emission Spectra
Self-assembled QDs are usually alloyed:

Ga1-xInxAs:


                       As
                                                        In
                            Ga

                                       In


                                   Random realization (RR) -
                                   particular random assignment
                                   of the In and Ga atoms onto
                                   the cation sublattice.
Self-assembled QDs are usually alloyed:

Ga1-xInxAs:


                                As
                                                               In
                                     Ga

                                              In


                                          Random realization (RR) -
                                          particular random assignment
                                          of the In and Ga atoms onto
Different local environments:             the cation sublattice.
Optical Properties vs Atomic-Scale Randomness

Ga1-xInxAs:
                         Large bulk solids: different random
                         realizations    (RRs)    get    self-
                         averaged, so the measured physical
                         property does not resolve features
                         of individual RRs.

                         Finite nanosystems (≤105 atoms):
                         self-averaging of RRs may not be
                         complete, so we can observe the
                         effect of individual RRs (atomic-
                         scale alloy randomness effect).


What is the effect of atomic-scale randomness on the
optical properties of Gax-1InxAs QDs?
X0: Fine structure splitting (FSS)
X0: FSS & Polatization directions vs RRs?




              S. Seidl et al., Physica E 40, 2153 (2008) –Conference proceedings.
X0: FSS & Polatization directions vs RRs?




                                      ?


              S. Seidl et al., Physica E 40, 2153 (2008) –Conference proceedings.
X0: Linear Polarization Ratio (P) vs RRs?




• P is a measure of the in-plane polarization
  anisotropy

                P = (Ix - Iy)/(Ix + Iy)

Where Ix and Iy are intensities defined along [110] and
[1-10] direction


• Atomic-scale randomness vs geometrical
  anisotropy?
                                                          I. Favero et al., APL 86, 041904 (2005).
X0: Linear Polarization Ratio (P) vs RRs?




                                      ?
• P is a measure of the in-plane polarization
  anisotropy

                P = (Ix - Iy)/(Ix + Iy)

Where Ix and Iy are intensities defined along [110] and
[1-10] direction


• Atomic-scale randomness vs geometrical
  anisotropy?
                                                          I. Favero et al., APL 86, 041904 (2005).
X0: FSS changes by more than a factor 7 with RRs
X0: FSS changes by more than a factor 7 with RRs




  FSS exhibits significant dependence on the RRs (from 1.1 - 8.5 μeV)
X0: FSS changes by more than a factor 7 with RRs




  FSS exhibits significant dependence on the RRs (from 1.1 - 8.5 μeV)

  FSS shows almost no sensitivity to piezoelectric field, irrespective of
  piezoelectricity was included via linear term only, or both linear and
  nonlinear terms.
X0: Polarization Directions vs RRs




                          Vladan Mlinar and Alex Zunger, Phys. Rev. B 79, 115416 (2009)
X0: Polarization Directions vs RRs




                          Vladan Mlinar and Alex Zunger, Phys. Rev. B 79, 115416 (2009)
X0: Polarization Directions vs RRs




                          Vladan Mlinar and Alex Zunger, Phys. Rev. B 79, 115416 (2009)
X0: P is not affected only by geometrical elongation



                            • Even 50% elongation in [100] direction
                              gives the same range of P, as in
                              geometrically symmetric QD!




                            • Measuring P cannot tell:
                              (1) the geometrical anisotropy
                              (2) composition
FSS & Polarization Directions of Multiexcitons


• QD can be charged by controllable number of electrons and holes: X-2, XX0, XX-1, XX+1

     • FSS of multiexcitons is sensitive to RRs.

     • Optically active transitions of different multiexcitons do not have fixed polarization
       directions




Poem et al., PRB 76, 235304 (2007): Different multiexcitonic transitions have well defined
polarization directions.
X-2: Conflicting experimental results




Poem et al., PRB 76, 235304 (2007):          Ediger et al., PRL 98, 036808 (2007):

• Polarization directions of the optically   Polarization directions of the optically
  active transitions oriented along          active transitions oriented along
  [120] and [2-10]                           [110] and [1-10]
• Optically active transitions of X-2 have
  well define polarization directions
X-2: Conflicting experimental results




Poem et al., PRB 76, 235304 (2007):             Ediger et al., PRL 98, 036808 (2007):

• Polarization directions of the optically      Polarization directions of the optically
  active transitions oriented along             active transitions oriented along
  [120] and [2-10]                              [110] and [1-10]
• Optically active transitions of X-2 have
  well define polarization directions




       Different X-2 emission lines DO NOT have fixed polarization directions!
Conclusions:


We provided a clear evidence for the effect of atomic-scale
randomness on the optical properties of alloyed Ga1-xInxAs QDs.

• Fine structure splitting of the monoexciton changes by more than a factor
  of 7 with RRs.

• For multiexcitons, the polarization directions strongly depend on the atomic
  scale randomness, so different multiexciton emission lines do not have
  fixed polarization directions.

• Optical polarization is affected both by atomic-scale randomness and by
  possible geometric elongation of the QD in one direction.

                                      Vladan Mlinar and Alex Zunger, Phys. Rev. B 79, 115416 (2009)

Thank you for your attention!
Comparison with other calculations:

   PRB 77, 113305 (2008):                                      This work:
• Investigated effect of intermixing profiles   • Investigated effect of atom-by-atom
                                                  random substitution

• EBOM does not have atomic resolution          • LCBB full atomic resolution

•Uniform composition profile vs.                •Uniform composition profile, but
 nonuniform profile                              different random realizations

• Linear polarization ratio as a tool for       • Linear polarization ratio cannot be used
  structural characterization                     as a tool for structural characterization
FSS & Polarization Directions of Multiexcitons
FSS vs RRs of Multiexcitons:
Polarization Directions of Multiexcitons:

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Vladan Mlinar 2009 American Physical Society March Meeting

  • 1. Effect of Atomic-Scale Randomness on the Optical Polarization of Semiconductor Quantum Dots Vladan Mlinar and Alex Zunger National Renewable Energy Laboratory, Golden, Colorado USA Vladan.Mlinar@nrel.gov
  • 2. Structure – Spectra relationship: QD morphology: Single-dot spectroscopy: Ga1-xInxAs QDs (P. A. Dalgarno & (~105 atoms) R. J. Warburton)
  • 3. Structure – Spectra relationship: QD morphology: Theory: Single-dot spectroscopy: Input structure Ga1-xInxAs QDs Strain minimization (P. A. Dalgarno & (~105 atoms) R. J. Warburton) Solve the single-particle problem Solve many-particle Problem (CI calc.) Emission Spectra
  • 4. Structure – Spectra relationship: QD morphology: Theory: Single-dot spectroscopy: Input structure Ga1-xInxAs QDs Strain minimization (P. A. Dalgarno & (~105 atoms) R. J. Warburton) Solve the single-particle problem Solve many-particle Problem (CI calc.) Emission Spectra
  • 5. Self-assembled QDs are usually alloyed: Ga1-xInxAs: As In Ga In Random realization (RR) - particular random assignment of the In and Ga atoms onto the cation sublattice.
  • 6. Self-assembled QDs are usually alloyed: Ga1-xInxAs: As In Ga In Random realization (RR) - particular random assignment of the In and Ga atoms onto Different local environments: the cation sublattice.
  • 7. Optical Properties vs Atomic-Scale Randomness Ga1-xInxAs: Large bulk solids: different random realizations (RRs) get self- averaged, so the measured physical property does not resolve features of individual RRs. Finite nanosystems (≤105 atoms): self-averaging of RRs may not be complete, so we can observe the effect of individual RRs (atomic- scale alloy randomness effect). What is the effect of atomic-scale randomness on the optical properties of Gax-1InxAs QDs?
  • 8. X0: Fine structure splitting (FSS)
  • 9. X0: FSS & Polatization directions vs RRs? S. Seidl et al., Physica E 40, 2153 (2008) –Conference proceedings.
  • 10. X0: FSS & Polatization directions vs RRs? ? S. Seidl et al., Physica E 40, 2153 (2008) –Conference proceedings.
  • 11. X0: Linear Polarization Ratio (P) vs RRs? • P is a measure of the in-plane polarization anisotropy P = (Ix - Iy)/(Ix + Iy) Where Ix and Iy are intensities defined along [110] and [1-10] direction • Atomic-scale randomness vs geometrical anisotropy? I. Favero et al., APL 86, 041904 (2005).
  • 12. X0: Linear Polarization Ratio (P) vs RRs? ? • P is a measure of the in-plane polarization anisotropy P = (Ix - Iy)/(Ix + Iy) Where Ix and Iy are intensities defined along [110] and [1-10] direction • Atomic-scale randomness vs geometrical anisotropy? I. Favero et al., APL 86, 041904 (2005).
  • 13. X0: FSS changes by more than a factor 7 with RRs
  • 14. X0: FSS changes by more than a factor 7 with RRs FSS exhibits significant dependence on the RRs (from 1.1 - 8.5 μeV)
  • 15. X0: FSS changes by more than a factor 7 with RRs FSS exhibits significant dependence on the RRs (from 1.1 - 8.5 μeV) FSS shows almost no sensitivity to piezoelectric field, irrespective of piezoelectricity was included via linear term only, or both linear and nonlinear terms.
  • 16. X0: Polarization Directions vs RRs Vladan Mlinar and Alex Zunger, Phys. Rev. B 79, 115416 (2009)
  • 17. X0: Polarization Directions vs RRs Vladan Mlinar and Alex Zunger, Phys. Rev. B 79, 115416 (2009)
  • 18. X0: Polarization Directions vs RRs Vladan Mlinar and Alex Zunger, Phys. Rev. B 79, 115416 (2009)
  • 19. X0: P is not affected only by geometrical elongation • Even 50% elongation in [100] direction gives the same range of P, as in geometrically symmetric QD! • Measuring P cannot tell: (1) the geometrical anisotropy (2) composition
  • 20. FSS & Polarization Directions of Multiexcitons • QD can be charged by controllable number of electrons and holes: X-2, XX0, XX-1, XX+1 • FSS of multiexcitons is sensitive to RRs. • Optically active transitions of different multiexcitons do not have fixed polarization directions Poem et al., PRB 76, 235304 (2007): Different multiexcitonic transitions have well defined polarization directions.
  • 21. X-2: Conflicting experimental results Poem et al., PRB 76, 235304 (2007): Ediger et al., PRL 98, 036808 (2007): • Polarization directions of the optically Polarization directions of the optically active transitions oriented along active transitions oriented along [120] and [2-10] [110] and [1-10] • Optically active transitions of X-2 have well define polarization directions
  • 22. X-2: Conflicting experimental results Poem et al., PRB 76, 235304 (2007): Ediger et al., PRL 98, 036808 (2007): • Polarization directions of the optically Polarization directions of the optically active transitions oriented along active transitions oriented along [120] and [2-10] [110] and [1-10] • Optically active transitions of X-2 have well define polarization directions Different X-2 emission lines DO NOT have fixed polarization directions!
  • 23. Conclusions: We provided a clear evidence for the effect of atomic-scale randomness on the optical properties of alloyed Ga1-xInxAs QDs. • Fine structure splitting of the monoexciton changes by more than a factor of 7 with RRs. • For multiexcitons, the polarization directions strongly depend on the atomic scale randomness, so different multiexciton emission lines do not have fixed polarization directions. • Optical polarization is affected both by atomic-scale randomness and by possible geometric elongation of the QD in one direction. Vladan Mlinar and Alex Zunger, Phys. Rev. B 79, 115416 (2009) Thank you for your attention!
  • 24. Comparison with other calculations: PRB 77, 113305 (2008): This work: • Investigated effect of intermixing profiles • Investigated effect of atom-by-atom random substitution • EBOM does not have atomic resolution • LCBB full atomic resolution •Uniform composition profile vs. •Uniform composition profile, but nonuniform profile different random realizations • Linear polarization ratio as a tool for • Linear polarization ratio cannot be used structural characterization as a tool for structural characterization
  • 25. FSS & Polarization Directions of Multiexcitons
  • 26. FSS vs RRs of Multiexcitons:
  • 27. Polarization Directions of Multiexcitons: