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Epitaxial lateral overgrowth of AlN layers on patterned sapphire substrates

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Title: Epitaxial lateral overgrowth of AlN layers on patterned sapphire substrates


1
Epitaxial lateral overgrowth of AlN layerson
patterned sapphire substrates
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2
Outline
  • Introduction
  • Experiments
  • Results and discussion
  • Conclusion
  • References

3
Introduction
  • The realization of high-performance UV
    light-emitting devices is one of the most
    important targets for group III nitride
    semiconductors.
  • To realize high-performance UV devices such as
    light emitting diodes . the growth of
    high-quality AlN is essential. It is still a
    critical issue to obtain high-quality AlN .
  • A combination of high-temperaturegrowth and ELO
    will lead to the reduction of threading
    dislocation density and thus achieve to much
    higher quality AlN

4
Experiments
  • Two different directions of pattrned sapphire
    substrates (0001) have been used in this
    investigation. In the first type of substrate,
    linear trenches have been formed along the (1010)
    direction. In the secondtype, trenches have been
    formed along the (1120) direction. The width and
    depth of the trenches are both 500 nm. The
    adjacent terrace width is 3 µm.
  • The ELO-AlN layers were grown on these substrates
    by high-temperature MOVPE technique under H2
    atmosphere.

5
  • The growth is carried out at a constant pressure
    of 100 Torr
  • the substrate is annealed at a temperature of
    1330 C for 5
  • minutes.
  • the growth is carried out at a temperature of
    1300 C, for 7 120 minutes.
  • For comparison, the growth of AlN at a relatively
    low temperature of 1100 C on a trench pattern
    along (1120) direction was also performed.

6
Results and discussion
  • Figure 2 shows a SEM cross-sectional image of AlN
    grown at a temperature of 1100 C, which is the
    temperature commonly used for the growth of AlN
    on sapphire. Although AlN was coalesced, the
    surfaceis quite rough. In comparison, the surface
    of AlN grown at temperatures higher than 1300 C
    is
  • atomically flat.

7
  • Figure 3 shows the SEM cross-section image of the
    AlN layer grown on the sapphire substrate with
    grooves formed along (1010) direction. As clearly
    seen in the SEM image, AlN layer was not
    coalesced. There is a gap between the adjacent
    layers. analyze the dislocations in the
    layersespecially in the regions between the
    vertical portions,

8
  • Figure 4 shows the TEM image of portion
    surrounded by black dotted lines in the Fig. 3.
    Dislocations are found
  • to propagate vertically from the seed region
    through the top surface. From these observations,
    it can be concluded that the grooves formed on
    sapphire substrates along the (1010) direction is
    not suitable for growing AlN layers with reduced
    dislocation density.

9
  • The SEM image of the cross-section of the AlN
    layers grown on the sapphire substrates with the
    linear grooves formed along the (1120) direction
    is presented in Fig. 5. As seen in the SEM image.
    TEM analysis was done on a prominent portion of
    the AlN layer indicated by the white dotted lines
    in order to analyze the dislocation propagation
    behaviour in detail. substrates.

10
Conclusion
  • High temperature MOVPE growth of AlN on the
    sapphire substrate having trench pattern was
    conducted.
  • We found a strong difference of the property of
    ELO between two trench directions. In order to
    obtain coalesced AlN, (1120) trench is essential.
    The average dislocation density of a coalesced
    AlN was 6.7 108 cm2, which is less than a half
    that of AlN grown on planer sapphire.
  • (1120) trench (0002) XRD rocking curve FWHM 314
    aresec is better than (1010) 352 aresec. These
    results show that ELO technique is also suitable
    for reducing dislocation density of AlN on
    sapphire.

11
References
  • 1 S. Nitta, M. Kariya, T. Kashima, S.
    Yamaguchi, H. Amano, and I. Akasaki, Appl. Surf.
    Sci. 159/160, 421 (2000).
  • 2 N. Fujimoto, T. Kitano, G. Narita, T. Fuse,
    K. Balakrishnan, M. Iwaya, S. Kamiyama, H. Amano,
    I. Akasaki, K.
  • Shimono, T. Noro, T. Takagai, and A. Bandoh, 52nd
    JSAP 30p-L-9 (2005).
  • 3 M. Imura, K. Nakano, T. Kitano, T. Fuse, N.
    Fujimoto, K. Balakrishnan, M. Iwaya, S. Kamiyama,
    H. Amano, T.Noro, and T. Takagi, 52nd JSAP
    30p-L-10 (2005).
  • 4 T. M. Katona, M. D. Craven, J. S. Speck, and
    S. P. DenBaars, Appl. Phys. Lett. 85, 1350 (2004).
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