Resonant second harmonic generation between 1550 nm and 775 nm with outside
efficiency $> 4.4\times10^{-4}\, \text{mW}^{-1}$ is demonstrated in a gallium
phosphide microdisk cavity supporting high-$Q$ modes at visible ($Q \sim 10^4$)
and infrared ($Q \sim 10^5$) wavelengths. The double resonance condition was
satisfied through intracavity photothermal temperature tuning using $\sim
360\,\mu$W of 1550 nm light input to a fiber taper and resonantly coupled to
the microdisk. Above this pump power efficiency was observed to decrease. The
observed behavior is consistent with a simple model for thermal tuning of the
double resonance condition.Comment: 6 pages, 4 figure

Barclay, Paul E.

Curic, Davor

Jayakumar, Harishankar

Lake, David P.

Mitchell, Matthew

Santos, Laís Fujii dos

Applied Physics Letters

English

arXiv

CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOResonant second harmonic generation between 1550 nm and 775 nm with normalized outside efficiency > 3.8 × 10 - 4 mW - 1 is demonstrated in a gallium phosphide microdisk supporting high-Q modes at visible (Q ∼ 10 4) and infrared (Q ∼ 10 5) wavelengths. The double resonance condition is satisfied for a specific pump power through intracavity photothermal temperature tuning using ∼ 360 μ W of 1550 nm light input to a fiber taper and coupled to a microdisk resonance. Power dependent efficiency consistent with a simple model for thermal tuning of the double resonance condition is observed. © 2016 AIP Publishing LLC.Resonant second harmonic generation between 1550 nm and 775 nm with normalized outside efficiency > 3.8 × 10 - 4 mW - 1 is demonstrated in a gallium phosphide microdisk supporting high-Q modes at visible (Q ∼ 10 4) and infrared (Q ∼ 10 5) wavelengths. The double resonance condition is satisfied for a specific pump power through intracavity photothermal temperature tuning using ∼ 360 μ W of 1550 nm light input to a fiber taper and coupled to a microdisk resonance. Power dependent efficiency consistent with a simple model for thermal tuning of the double resonance condition is observed.108315CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOCNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOSem informaçãoFranken, P.A., Hill, A.E., Peters, C.W., Weinreich, G., (1961) Phys. Rev. Lett., 7, p. 118Nakagawa, S., Yamada, N., Mikoshiba, N., Mars, D., (1995) Appl. Phys. Lett., 66, p. 2159Mondia, J., Van Driel, H., Jiang, W., Cowan, A., Young, J.F., (2003) Opt. Lett., 28, p. 2500Ilchenko, V.S., Savchenkov, A.A., Matsko, A.B., Maleki, L., (2004) Phys. Rev. Lett., 92McCutcheon, M.W., Young, J.F., Rieger, G.W., Dalacu, D., Frédérick, S., Poole, P.J., Williams, R.L., (2007) Phys. Rev. B, 76Yamada, S., Song, B.-S., Jeon, S., Upham, J., Tanaka, Y., Asano, T., Noda, S., (2014) Opt. Lett., 39, p. 1768Mariani, S., Andronico, A., Mauguin, O., Lemaître, A., Favero, I., Ducci, S., Leo, G., (2013) Opt. Lett., 38, p. 3965Buckley, S., Radulaski, M., Biermann, K., Vučković, J., (2013) Appl. Phys. Lett., 103Diziain, S., Geiss, R., Zilk, M., Schrempel, F., Kley, E.-B., Tünnermann, A., Pertsch, T., (2013) Appl. Phys. Lett., 103Kuo, P.S., Solomon, G.S., (2011) Opt. Express, 19, p. 16898Wang, C., Burek, M.J., Lin, Z., Atikian, H.A., Venkataraman, V., Huang, I.-C., Stark, P., Lončar, M., (2014) Opt. Express, 22, p. 30924Kuo, P.S., Bravo-Abad, J., Solomon, G.S., (2014) Nat. Commun., 5, p. 3109Mariani, S., Andronico, A., Lemaître, A., Favero, I., Ducci, S., Leo, G., (2014) Opt. Lett., 39, p. 3062Pernice, W.H.P., Xiong, C., Schuck, C., Tang, H.X., (2012) Appl. Phys. Lett., 100Dominguez-Juarez, J.L., Kozyreff, G., Martorell, J., (2011) Nat. Commun., 2, p. 254Rivoire, K., Buckley, S., Hatami, F., Vuković, J., (2011) Appl. Phys. Lett., 98Lenglé, K., Bramerie, L., Gay, M., Simon, J.-C., Combrié, S., Lehoucq, G., De Rossi, A., (2013) Appl. Phys. Lett., 102Fürst, J.U., Strekalov, D.V., Elser, D., Lassen, M., Andersen, U.L., Marquardt, C., Leuchs, G., (2010) Phys. Rev. Lett., 104Buckley, S., Radulaski, M., Zhang, J.L., Petykiewicz, J., Biermann, K., Vučković, J., (2014) Opt. Lett., 39, p. 5673Carmon, T., Vahala, K.J., (2007) Nat. Phys., 3, p. 430Shambat, G., Rivoire, K., Lu, J., Hatami, F., Vučković, J., (2010) Opt. Express, 18, p. 12176Boyd, R.W., (2003) Nonlinear Optics, , (Academic Press)Dumeige, Y., Feron, P., (2006) Phys. Rev. A, 74http://dx.doi.org/10.1063/1.4940242, See supplementary material at E-APPLAB-108-019604 for discussion of the off-resonance second harmonic efficiencyCarmon, T., Yang, L., Vahala, K., (2004) Opt. Express, 12, p. 4742Yas'Kov, D., Pikhtin, A., (1969) Mater. Res. Bull., 4, p. 781Mitchell, M., Hryciw, A.C., Barclay, P.E., (2014) Appl. Phys. Lett., 104Borselli, M., (2006) High-Q microresonators as lasing elements for silicon photonics, , Ph.D. thesis, California Institute of TechnologyWong, C.W., Rakich, P.T., Johnson, S.G., Qi, M., Smith, H.I., Ippen, E.P., Kimerling, L.C., Kim, S.-G., (2004) Appl. Phys. Lett., 84, p. 1242Li, Q., Davanco, M.I., Srinivasan, K., (2015) CLEO: 2015 (Optical Society of America), p. JTu5A43Jiang, W.C., Lu, X., Zhang, J., Painter, O., Lin, Q., (2015) Opt. Express, 23, p. 20884Yang, Z., Sipe, J., (2007) Opt. Lett., 32, p. 3296Helt, L., Yang, Z., Liscidini, M., Sipe, J., (2010) Opt. Lett., 35, p. 3006We would like to thank Aaron C. Hryciw and J. P. Hadden for their assistance with this project. This work was supported by NRC, CFI, iCORE/AITF, NSERC, and CNPq

Repositorio da Producao Cientifica e Intelectual da Unicamp

Efficient telecom to visible wavelength conversion in doubly resonant gallium phosphide microdisks

Efficient telecom to visible wavelength conversion in doubly resonant
  GaP microdisks

Efficient telecom to visible wavelength conversion in doubly resonant GaP microdisks

Abstract

Similar works

Full text

Available Versions

Repositorio da Producao Cientifica e Intelectual da Unicamp