Table 1. Calculated Frequencies of Raman-Active Phonon Modes for a GaAs/GaP SL Structure with 3 Different Periodsa.
frequencies for L = 3.83 nm (cm–1) | frequencies for L = 5.12 nm (cm–1) | frequencies for L = 6.39 nm (cm–1) |
---|---|---|
247.53 | 245.55 | 243.87 |
259.88 | 254.87 | 250.83 |
272.02 | 264.73 | 259.57 |
279.57 | 273.24 | 267.39 |
285.13 | 281.13 | 274.60 |
366.94 | 282.45 | 279.78 |
368.35 | 288.12 | 283.64 |
371.79 | 367.25 | 285.71 |
379.98 | 368.09 | 290.04 |
370.23 | 367.33 | |
372.06 | 367.86 | |
375.85 | 369.49 | |
382.31 | 370.64 | |
373.38 | ||
378.84 |
Phonon modes with a Raman intensity more than 100 times smaller than that of the most intense mode were considered nondetectable.