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Optical properties of IIInitride compounds

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High quality heteroepitaxies come into the play ... Hypothesis : a biaxial strain splits the valence band states ... The hydrogenic series in 1/n2 is lost. 11 ... – PowerPoint PPT presentation

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Title: Optical properties of IIInitride compounds


1
Optical properties of III-nitride compounds
  • Bernard Gil
  • Groupe dEtude des Semiconducteurs
  • Université Montpellier II
  • 34095 Montpellier cedx5 - France

2
Identification of the bandgap of GaN
Ilegems Dingle (1971)
3
High quality heteroepitaxies come into the play
(mid nineties)
4
The band gap of GaN and the lattice parameter
5
Hypothesis a biaxial strain splits the valence
band states
  • The crystal field splitting varies with c/a
  • Gil, 1995
  • Shikanai, 1995
  • Kim 1997

6
Treating it more seriously requires text book
quantum mechanics
  • One parameter to account of the crystal-field
    splitting
  • two parameters to account for the matrix elements
  • of the spin-orbit interaction
  • Four deformation potentials



  • Igt -(px ipy)/2


  • I-gt (px - ipy)/2

7
Evolution of band to band transitions with stress
8
Excitonic corrections
  • I?5gt I?5gt I?5 gt
  • ?1 ?2 ?1 ?2 -1/2? -?
    0
  • -? ?1 - ?2 ?1 ?2 -1/2? ?2?3
  • 0 ?2?3 ?1 1/2?
  • ?exc?5 ?I?5gt ? I?5gt ??5 gt
  • ??exc?5 ?2 ( ? ? )2 / 2.

? 0.6 meV in GaN
9
It works!
10
The excitonic binding energies in GaN films
  • Effective masses are anisotropic
  • Schrödinger equation should include this
    anisotropy
  • The hydrogenic series in 1/n2 is lost

11
Orthorhombically strained GaN films in-plane
anisotropy
12
Photoluminescence
13
Photoluminescence and reflectance
14
The excitonic polariton in GaN films
15
Neutral-donor bound excitons / Rotational excited
statesCourtesy G.Neu
Almost strain free GaN
Free-standing
(HVPE)
Homoepitaxy
(MOCVD)
16
GaN/SiC heterostructures (0001) Courtesy G.Neu
  • ? resonant lines are observed over more than 10
    meV
  • ?the energy difference between the resonant picks
    and the excitation is no more strictly constant
  • a pick b is rapidly shifting
  • by extrapolation it corresponds to D0XB

17
Rotational excited states of D0XA Courtesy G.Neu
18
Donor spectroscopy two electron transitions
Courtesy G.Neu
HVPE grown free-standing layer
2K - the D0X initial state is the ground state
- the final state is D0(n2,..)
  • Above 2K
  • The initial states are the
  • D0X excited states

I2a (2p)
19
Donor bound excitons in semiconductors a three
decade-long storyB.Gil et al , to be published
? Ed / 30
Jtot Lrot Jhole
20
Wave functions of the rotator and two electron
transitions B.Gil , B. Monemar , to be published
  • The angular momentum of the topmost valence band
    Bloch state J is 3/2.
  • For the ground state 0,0gt, the total hole wave
    function has the symmetry of the valence band,
    Jtot 3/2. The ground state of the donor bound
    exciton complex has odd parity. When one of the
    electrons and the hole recombine leaving the last
    electron in a nS state, the ground state has even
    parity. This recombination process is dipole
    allowed and efficiently couples with the
    electromagnetic field.
  • The first excited state correspond to the first
    excited state of the hole rotator. The total
    wave function of the complex is even and the most
    probable recombination process is a complex
    process leaving the remaining electron in a 2 p
    state.

21
Zinc oxyde?
22
Acknowledgements
  • Olivier Briot,
  • Nicolas Grandjean,
  • Marc Ilegems,
  • Mathieu Leroux,
  • Bo Monemar,
  • Hadis Morkoç,
  • Gérard Neu,
  • Shuji Nakamura,
  • Sandra Ruffenach,
  • Magloire Tchounkeu,
  • Andenet Alemu
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