Modeling of Quantum Cascade Laser Sources with Giant Optical Nonlinearities

By Christian Jirauschek

Institute for Nanoelectronics, Technische Universität München, München, Germany

Published on

Abstract

IWCE 2015 Presentation. a characteristic feature of the quantum cascade laser (qcl) is that the optical properties of the active region can be custom-tailored by quantum engineering. recently, the possibility to integrate giant artificial optical nonlinearities has enabled various novel applications, such as room temperature terahertz generation based on difference frequency mixing and the qcl-based generation of mid-infrared and terahertz frequency combs. we extend established modeling approaches, such as the ensemble monte carlo method, to the simulation of such nonlinear optical qcl sources. the obtained theoretical results are shown to be consistent with available experimental data.

Credits

This work was funded by the Heisenberg program of the German Research Foundation (DFG, JI115/4-1).

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Cite this work

Researchers should cite this work as follows:

  • Jirauschek, Christian, "Modeling of quantum cascade laser sources with giant optical nonlinearities," in Computational Electronics (IWCE) 2015 International Workshop on, DOI: 10.1109/IWCE.2015.7301968

  • Christian Jirauschek (2016), "Modeling of Quantum Cascade Laser Sources with Giant Optical Nonlinearities," https://nanohub.org/resources/23961.

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Time

Location

North Ballroom, PMU, Purdue University, West Lafayette, IN

Tags

Modeling of Quantum Cascade Laser Sources with Giant Optical Nonlinearities
  • Modeling of Quantum Cascade Laser Sources with Giant Optical Nonlinearities 1. Modeling of Quantum Cascade La… 0
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  • Overview 2. Overview 14.214214214214215
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  • Quantum Cascade Laser 3. Quantum Cascade Laser 39.873206539873209
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  • Quantum Engineering of Active Region 4. Quantum Engineering of Active … 131.23123123123125
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  • Ensemble Monte Carlo (EMC) 5. Ensemble Monte Carlo (EMC) 188.82215548882218
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  • Boltzmann Equation and Scattering 6. Boltzmann Equation and Scatter… 234.50116783450119
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  • Overview 7. Overview 270.970970970971
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  • Inclusion of Optical Cavity Field 8. Inclusion of Optical Cavity Fi… 275.64230897564232
    00:00/00:00
  • Carrier-Light Coupling in Monte Carlo 9. Carrier-Light Coupling in Mont… 333.66700033366703
    00:00/00:00
  • Simulation of High Efficiency Mid-Infrared QCL 10. Simulation of High Efficiency … 375.975975975976
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  • Overview 11. Overview 437.2038705372039
    00:00/00:00
  • THz Difference Frequency Generation QCL Structure 12. THz Difference Frequency Gener… 445.87921254587923
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  • Modeling of Nonlinear Susceptibility 13. Modeling of Nonlinear Suscepti… 555.7891224557892
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  • Multi-Domain Simulation Approach 14. Multi-Domain Simulation Approa… 610.04337671004339
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  • Comparison Simulation - Experiment 15. Comparison Simulation - Experi… 650.05005005005012
    00:00/00:00
  • Temperature Degradation of THz Power 16. Temperature Degradation of THz… 770.10343677010349
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  • Contributions of Individual Subband Triplets 17. Contributions of Individual Su… 834.76810143476814
    00:00/00:00
  • Susceptibility of Widely Tunable THz DFG Structure 18. Susceptibility of Widely Tunab… 918.21821821821823
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  • Overview 19. Overview 947.8812145478812
    00:00/00:00
  • Extended Maxwell-Bloch Equations 20. Extended Maxwell-Bloch Equatio… 957.65765765765764
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  • Rate Equations 21. Rate Equations 979.87987987987992
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  • Coherent Effects 22. Coherent Effects 1010.3770437103771
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  • Manifestation of Coherent Effects 23. Manifestation of Coherent Effe… 1018.4851518184852
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  • Simulation of Actively Mode-Locked QCLs 24. Simulation of Actively Mode-Lo… 1081.3480146813481
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  • Multi-Domain Simulation Approach 25. Multi-Domain Simulation Approa… 1136.8368368368369
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  • QCL-Based Frequency Combs 26. QCL-Based Frequency Combs 1209.3093093093094
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  • Terahertz Frequency Comb 27. Terahertz Frequency Comb 1309.3093093093094
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  • Conclusion 28. Conclusion 1340.3737070403738
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  • Acknowledgment 29. Acknowledgment 1399.6329662996329
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