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VCSEL Vertical Cavity Surface-Emitting Laser

VCSEL Vertical Cavity Surface-Emitting Laser. Docente: Mauro Mosca (www.dieet.unipa.it/tfl). A.A. 2013-14. Ricevimento: alla fine della lezione o per appuntamento. Università di Palermo – Facoltà di Ingegneria (DEIM). Edge-emitting e surface-emitting laser.

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VCSEL Vertical Cavity Surface-Emitting Laser

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  1. VCSELVertical Cavity Surface-Emitting Laser Docente: Mauro Mosca (www.dieet.unipa.it/tfl) A.A. 2013-14 Ricevimento: alla fine della lezione o per appuntamento Università di Palermo – Facoltà di Ingegneria (DEIM)

  2. Edge-emitting e surface-emitting laser • Advantage over edge emitting LDs: micrometric size, that allows larger devices density on substrates - No additional technology steps for the realization of good reflective facets (for edge emitting LDs: chemical assisted ion beam etching, cleaving focused ion beam polishing or wet chemical polishing) - Circularly shaped, low numerical aperture beam (ideal sources for fiber coupling and free space optics), single longitudinal mode operation (due to a cavity length of the order of one λ), low power dissipation and significantly lower operating currents - Applications: color displays, bio-sensing, printing applications (using VCSEL arrays would increase printing throughput) and optical data storage

  3. Sezione di una cavità VCSEL planare 99% epitaxially grown or dielectric l/n The emission wavelength is not determined anymore by the maximum gain of the active material but rather by the geometry of the cavity. Thus, VCSELs can lase only if the QW emission wavelength approximately coincides with the cavity mode Lasing in a VCSEL critically depends on the reflectivity of both the top and bottom mirrors. Only a few single longitudinal modes are supported by a VCSEL cavity

  4. Condizione di soglia (threshold) threshold material gain threshold modal gain • The lasing condition in a laser is reached when the amplitude of the optical field is maintained after a round trip in the cavity • This condition is reached when the optical gain in the cavity is sufficient to compensate all the losses the field experiences in the cavity during a round trip • INTERNAL LOSSES EXTERNAL LOSSES • absorption scattering diffraction mirror reflectivity The confinement factors (Γxy and Γz) accounts for the volume actually occupied by photons in the cavity, that is usually larger than the active region volume small… standing wave enhancement factor

  5. Distribuzione di campo longitudinale dentro la cavità Genh = 2

  6. Guadagno e corrente di soglia in funzione della riflettività

  7. Guadagno e corrente di soglia in funzione della riflettività (InGaAs QW)

  8. Guadagno e corrente di soglia in funzione della riflettività (InGaAs QW)

  9. Guadagno e corrente di soglia in funzione della riflettività (GaN QW)

  10. Guadagno e corrente di soglia in funzione della riflettività (GaN QW)

  11. Altre perdite (scattering alle interfacce e diffrazione)

  12. DBR (Distributed Bragg Reflectors) normal incidence + + a mirror with a wide stop-band ensures a higher tolerance with respect to emission wavelength variations the two contributions sum in phase at the design wavelength λ0

  13. DBR: lunghezza efficace della cavità The penetration of the optical mode into the DBR stack has to be taken into account, as it defines the effective cavity length and, subsequently, the wavelength of the lasing mode The penetration depth leffof the DBR is defined as the depth into the mirror, at which the optical field intensity is equal to 1/e of its value at the input of the mirror

  14. DBR: effetti delle perdite per assorbimento reflectivity of an m-pair DBR absorption coefficient of the DBR low Dn and high aDBR and l0 for long wavelength VCSEL high Dn helps to reduce the absorption losses of the mirrors

  15. Effetto interfacce graduali • Interfaces not abrupt! • The material is linearly graded • over a distance of some tens of • nm in orded to reduce the • electrical resistance across the • interface

  16. Resistenza degli specchi

  17. Resistenza degli specchi doping barrier for holes (high R) fabrication technology simpler

  18. Specchi graduali valence band

  19. Efficienza differenziale 3. 1. fattore di normalizzazione 2. mirror losses total losses

  20. Efficienza differenziale depends on cavity design depends on mirror design

  21. top mirror: 19 periods Wall-plug efficiency

  22. W Wall-plug efficiency Inoltre… se la riflettività diminuisce troppo, aumenta la corrente di soglia!!!

  23. Confinamento laterale • Injections schemes for GaAs-based VCSELs: • conductive DBRs with and without current confinement layers; • annular intra-cavity contacts in combination with one or two current confinement layers sacrificial layer

  24. . Ossidazione laterale dell’AlAs

  25. T W ? Ossidazione laterale dell’AlAs With GaAs (instead of AlAs): DG > 0!! Energia libera di Gibbs a 698 K < 0, vuol dire che la reazione è spontanea nella direzione indicata

  26. Ossidazione laterale dell’AlAs processo lineare… ma diventa dipendente dalla radice quadrata Controlled Evaporated and Mixing system i gas reagenti penetrano difficilmente attraverso l’ossido (per alti spessori dello stesso ossido)

  27. Ossidazione laterale dell’AlGaAs

  28. Fabbricazione di un VCSEL con ossidazione laterale

  29. Ossidazione laterale in VCSEL a nitruri

  30. Ossidazione laterale in VCSEL a nitruri

  31. Ossidazione laterale in VCSEL a nitruri

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