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James Arnemann Presentation

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Effective Masses in ZnGeN 2 James Arnemann Case Western Physics
Outline ,[object Object],[object Object],[object Object],[object Object],[object Object]
Semiconductors ,[object Object],[object Object],[object Object],[object Object],http://commons.wikimedia.org/wiki/File:Bandgap_in_semiconductor.svg
Semiconductors (continued) ,[object Object],[object Object],[object Object],http://www.hk-phy.org/energy/alternate/solar_phy/images/hole_theory.gif http://64.202.120.86/upload/image/new-news/2009/fabruary/led/led-big.jpg
Crystal Structure ,[object Object],[object Object],[object Object],http://geosphere.gsapubs.org/content/1/1/32/F5.small.gif http://www.tf.uni-kiel.de/matwis/amat/def_en/kap_2/basics/b2_1_6.html http://www.fuw.edu.pl/~kkorona/
ZnGeN 2 ,[object Object],[object Object],[object Object],http://www.bpc.edu/mathscience/chemistry/images/periodic_table_of_elements.jpg
Hamiltonian (Energy) ,[object Object],[object Object],[object Object],[object Object],Taken from Physical Review B Volume 56, Number 12 pg. 7364 (15 September 1997-II)
Wurtzite Hamiltonian ,[object Object],[object Object],[object Object],Taken from Physical Review B Volume 58, Number 7 pg. 3881 (15 August 1998-I)
Energy ,[object Object],[object Object],[object Object],[object Object],[object Object]
Calculating Effective Mass ,[object Object],[object Object]
Energy Bands for ZnGeN 2 in terms of the Brillion zone (without spin orbit splitting) E(eV) vs. к x
Calculations ,[object Object],[object Object]
Results AlN ZnGeN 2 GaN Δ 1 (meV) -219 65 24 Δ 1 ’ (meV) 0 3.73 0 A 1 -3.82 -4.53 -6.40 A 2 -0.22 -0.47 -0.80 A 3 3.54 4.19 5.93 A 4 -1.16 -1.93 -1.96 A 5 1.33 2.01 2.32
Conclusions ,[object Object],[object Object]
The End

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James Arnemann Presentation

  • 1. Effective Masses in ZnGeN 2 James Arnemann Case Western Physics
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  • 11. Energy Bands for ZnGeN 2 in terms of the Brillion zone (without spin orbit splitting) E(eV) vs. к x
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  • 13. Results AlN ZnGeN 2 GaN Δ 1 (meV) -219 65 24 Δ 1 ’ (meV) 0 3.73 0 A 1 -3.82 -4.53 -6.40 A 2 -0.22 -0.47 -0.80 A 3 3.54 4.19 5.93 A 4 -1.16 -1.93 -1.96 A 5 1.33 2.01 2.32
  • 14.