Cleo: 2013 2013
DOI: 10.1364/cleo_si.2013.ctu3e.3
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Pulsed and CW IR Detection in Wide-gap Semiconductors using Extremely Nondegenerate Two-photon Absorption

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Cited by 3 publications
(14 citation statements)
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“…In these plots, the sum of the photon energies is shown scaled to the respective linear absorption edge energies of the bulk and QW since this allows comparing bulk and QW, semiconductors on the same scale. For the bulk case, 𝛼 2 𝐷 is plotted against the two-photon energy normalized to the bandgap, whereas for the QW, 𝛼 2 𝐷 | βˆ₯ is plotted against the two-photon energy normalized to 𝐸 𝑔 + 𝐸 β„Žβ„Ž 11 for the TE-TE case, and 𝛼 2 𝐷 | βŠ₯ is plotted against the two-photon energy normalized to 𝐸 𝑔 + 𝐸 π‘™β„Ž 11 for the TM-TM case. As we go higher in two-photon energy (2β„πœ”), 𝛼 2 𝐷 increases for photon energies close to the middle of the bandgap, goes through a maximum and then decreases for photon energies close to the bandgap.…”
Section: Degenerate Two-photon Absorption In Quantum Wellsmentioning
confidence: 99%
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“…In these plots, the sum of the photon energies is shown scaled to the respective linear absorption edge energies of the bulk and QW since this allows comparing bulk and QW, semiconductors on the same scale. For the bulk case, 𝛼 2 𝐷 is plotted against the two-photon energy normalized to the bandgap, whereas for the QW, 𝛼 2 𝐷 | βˆ₯ is plotted against the two-photon energy normalized to 𝐸 𝑔 + 𝐸 β„Žβ„Ž 11 for the TE-TE case, and 𝛼 2 𝐷 | βŠ₯ is plotted against the two-photon energy normalized to 𝐸 𝑔 + 𝐸 π‘™β„Ž 11 for the TM-TM case. As we go higher in two-photon energy (2β„πœ”), 𝛼 2 𝐷 increases for photon energies close to the middle of the bandgap, goes through a maximum and then decreases for photon energies close to the bandgap.…”
Section: Degenerate Two-photon Absorption In Quantum Wellsmentioning
confidence: 99%
“…As discussed earlier, for the TE-TE case only βˆ†π‘› = 0, and for the TM-TM case Δ𝑛 = Β±1, are considered. In the TM-TM case, the first transition is from the 2 nd light-hole subband to the 1 st electron subband, thus the onset of 2PA occurs at 2β„πœ” = 𝐸 𝑔 + 𝐸 π‘™β„Ž 12 , rather than 2β„πœ” = 𝐸 𝑔 + 𝐸 π‘™β„Ž 11 . In the limiting case of a wide QW, both 𝛼 2 𝐷 | βˆ₯ and 𝛼 2 𝐷 | βŠ₯ approach the bulk value 𝛼 2 𝐷 as seen in Fig.…”
Section: Degenerate Two-photon Absorption In Quantum Wellsmentioning
confidence: 99%
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“…There are many potential practical applications of optical nonlinearities in condensed matter, including all-optical switching [1][2][3][4], optical limiting [5,6], sensing [7,8], and imaging [9,10]. Additionally, these same nonlinearities limit the performance, particularly in optical telecommunication, and can lead to unwanted absorption or even damage of solid-state devices [11].…”
Section: Introductionmentioning
confidence: 99%