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The Future of High Powered Electrical Devices

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The Future of High Powered Electrical Devices. Mpumelelo Richards. Mary Ellen Zvanut ... These devices will be used in power generation, automobiles, ... – PowerPoint PPT presentation

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Title: The Future of High Powered Electrical Devices


1
The Future of High Powered Electrical Devices
  • Mpumelelo Richards
  • Mary Ellen Zvanut

Research Experience for Undergraduates
Department of Physics
2
So whats in the future of electronics?
Silicon Carbide
3
But why silicon carbide ?
  • Higher temperatures
  • High radiation
  • High power

These devices will be used in power generation,
automobiles, aircraft, spacecraft, communications
and radar.
4
However!
The problem is that
Silicon carbide incurs defects during the growth
process which affect its conductive properties.
These defects number along the order of 1 defect
for 1 x 106 regular Si C bonds.
5
Common Defects
Silicon atom
Regular structure
Carbon atom
6
Electron Paramagnetic Resonance (EPR)
  • To determine the detailed electronic structure
    and symmetry of a point defect
  • Detect defects with unpaired electrons
  • Zeeman Effect g
    hv/ß B0

7
Goals
  • Long term goal is to identify defects
    incorporated and correlate them with method of
    growth
  • My particular research is focused on using
  • electron paramagnetic resonance to
    identify/characterize what is believed to be a
    previously unreported defect.

8
Now for the work!
9
Data Collection
  • Use EPR spectrometer to gather spectra of the
    as-grown samples.
  • Determining optimum orientation
  • Varying EPR parameters
  • Exposing samples to different wavelengths of
    light

AND
10
  • Sitting in front of the EPR spectrometer for
    hours at a time.

11
Annealing
  • The samples were annealed at 600 C,800 C,1000
    C, 1200 C ,1400 C,1600 C.

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13
Simulation Time
  • Using EPRMNR computer software the collected
    data was simulated

14
What do the simulations tell us?
  • We are able to determine the characteristic
    values of the center from the simulation.Namely
  • The g-tensor value
  • D E values (fine structure constants)
  • A- values (nuclei hyperfine constant)

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17
Integration
  • The integral of the data was taken in order to
    find the contributions of the hyperfine Peaks I
    and II.

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Putting it all together1
  • The defect that we are observing is not a primary
    contributor to the samples semi-insulating
    property.

20
Putting it all together 2An unstudied defect!
  • The found characterizing g-tensor, A, d and E
    values do indeed differ from previously reported
    defect values.

21
Putting it all together3
  • The number of hyperfine lines and their percent
    contributions lead us to search for isotopes with
    nuclei spin ½ and natural abundance near our
    found values.
  • After eliminating radioactive isotopes and
    elements highly unlikely to be incorporated
    during the growth process we were left with Si
    and C- an intrinsic defect.

22
Conclusions
  • The defect is not a primary contributor to the
    SiC semi-insulating properties.
  • The defect is believed to be intrinsic.
  • We believe it to be a pair defect involving many
    Si and C atoms but the actual arrangement is
    still uncertain.

23
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