1.Deparment Física de Materiales, Instituto Nicolás Cabrera and Condensed Matter Physics Center (IFIMAC), Universidad Autónoma de Madrid, 28049, Madrid, Spain
2.Universitat Rovira i Virgili, Departament Química Física i Inorgànica, Fisica i Cristal·lografia de Materials i Nanomaterials (FiCMA-FiCNA) - EMaS, E-43007, Tarragona, Spain
Luisa E. Bausá (luisa.bausa@uam.es)
纸质出版日期:2019,
网络出版日期:2019-01-30,
收稿日期:2018-09-12,
修回日期:2019-01-01,
录用日期:2019-01-06
Scan QR Code
Plasmon-induced dual-wavelength operation in a Yb3+ laser[J]. LSA, 2019,8(1):127-135.
Sánchez-García, L. et al. Plasmon-induced dual-wavelength operation in a Yb3+ laser. Light: Science & Applications, 8, 127-135 (2019).
Plasmon-induced dual-wavelength operation in a Yb3+ laser[J]. LSA, 2019,8(1):127-135. DOI: 10.1038/s41377-019-0125-2.
Sánchez-García, L. et al. Plasmon-induced dual-wavelength operation in a Yb3+ laser. Light: Science & Applications, 8, 127-135 (2019). DOI: 10.1038/s41377-019-0125-2.
Expanding the functionalities of plasmon-assisted lasers is essential for emergent applications in nanoscience and nanotechnology. Here
we report on a novel ability of plasmonic structures to induce dual-wavelength lasing in the near-infrared region in a Yb
3+
solid-state laser. By means of the effects of disordered plasmonic networks deposited on the surface of a Yb
3+
-doped nonlinear RTP crystal
room-temperature dual-wavelength lasing
with a frequency difference between the lines in the THz range
is realized. The dual-wavelength laser is produced by the simultaneous activation of two lasing channels
namely
an electronic- and a phonon-terminated laser transition. The latter is enabled by the out-of-plane field components that are generated by the plasmonic structures
which excite specific Raman modes. Additionally
multiline radiation at three different wavelengths is demonstrated in the visible spectral region via two self-frequency conversion processes
which occur in the vicinities of the plasmonic structures. The results demonstrate the p
otential of plasmonic nanostructures for inducing drastic modifications in the operational mode of a solid-state laser and hold promise for applications in a variety of fields
including multiplexing
precise spectroscopies
and THz radiation generation via a simple and cost-effective procedure.
Ma, R. M., Oulton, R. F., Sorger, V. J.&Zhang, X. Plasmon lasers: coherent light source at molecular scales.Laser Photonics Rev.7, 1-21 (2013)..
Oulton, R. F. Surface plasmon lasers: sources of nanoscopic light.Mater. Today15, 26-34 (2012)..
Wang, D. Q., Wang, W. J., Knudson, M. P., Schatz, G. C.&Odom, T. W. Structural engineering in plasmon nanolasers.Chem. Rev.118, 2865-2881 (2018)..
Schuller, J. A. et al. Plasmonics for extreme light concentration and manipulation.Nat. Mater.9, 193-204 (2010)..
Wang, X. Y. et al. Lasing enhanced surface plasmon resonance sensing.Nanophotonics6, 472-478 (2017)..
Ma, R. M., Ota, S., Li, Y., Yang, S.&Zhang, X. Explosives detection in a lasing plasmon nanocavity.Nat. Nanotechnol.9, 600-604 (2014)..
Fang, Y. R.&Sun, M. T. Nanoplasmonic waveguides: towards applications in integrated nanophotonic circuits.Light.: Sci. Appl.4, e2942 (2015)..
Oulton, R. F. et al. Plasmon lasers at deep subwavelength scale.Nature461, 629-632(2009)..
Noginov, M. A. et al. Demonstration of a spaser-based nanolaser.Nature460, 1110-1112 (2009)..
Ma, R. M., Oulton, R. F., Sorger, V. J., Bartal, G.&Zhang, X. Room-temperature sub-diffraction-limited plasmon laser by total internal reflection.Nat. Mater.10, 110-113 (2011)..
Ramezani, M. et al. Plasmon-exciton-polariton lasing.Optica4, 31-37 (2017)..
Suh, J. Y. et al. Plasmonic bowtie nanolaser arrays.Nano. Lett.12, 5769-5774 (2012)..
Wang, D. Q. et al. Stretchable nanolasing from hybrid quadrupole plasmons.Nano. Lett.18, 4549-4555 (2018)..
Molina, P. et al. Plasmon-assisted Nd3+-based solid-state nanolaser.Nano. Lett.16, 895-899 (2016)..
Hernández-Pinilla, D. et al. Multiline operation from a single plasmon-assisted laser.ACS Photonics5, 406-412 (2018)..
Boulon, G. Why so deep research on Yb3+-doped optical inorganic materials?J. Alloy. Compd.451, 1-11 (2008)..
Hemmer, E. et al. Upconverting and NIR emitting rare earth based nanostructures for NIR-bioimaging.Nanoscale5, 11339-11361 (2013)..
Deng, R. R. et al. Temporal full-colour tuning through non-steady-state upconversion.Nat. Nanotechnol.10, 237-242 (2015)..
Zhou, Z. P., Yin, B.&Michel, J. On-chip light sources for silicon photonics.Light.: Sci. Appl.4, e358 (2015)..
Tang, Y. N., Di, W. H., Zhai, X. S., Yang, R. Y.&Qin, W. P. NIR-responsive photocatalytic activity and mechanism of NaYF4:Yb, Tm@TiO2core-shell nanoparticles.ACS Catal.3, 405-412 (2013)..
Van der Ende, B. M., Aarts, L.&Meijerink, A. Near-infrared quantum cutting for photovoltaics.Adv. Mater.21, 3073-3077 (2009)..
Peña, A. et al. Yb3+spectroscopy in (Nb or Ta):RbTiOPO4 single crystals for laser applications.Opt. Express15, 14580-14590 (2007)..
Royon, R., Lhermite, J., Sarger, L.&Cormier, E. High power, continuous-wave ytterbium-doped fiber laser tunable from 976 to 1120 nm.Opt. Express21, 13818-13823 (2013)..
Hönninger, C. et al. Ultrafast ytterbium-doped bulk lasers and laser amplifiers.Appl. Phys. B69, 3-17 (1999)..
Denker, B.&Shklovsky, E.Handbook of Solid-State Lasers: Materials, Systems and Applications. (Woodhead Publishing, Cambridge, 2013).
Sánchez-García, L. et al. Anisotropic enhancement of Yb3+luminescence by disordered plasmonic networks self-assembled on RbTiOPO4 ferroelectric crystals.Nanoscale9, 16166-16174 (2017)..
Pack, M. V., Armstrong, D. J.&Smith, A. V. Measurement of theX2 tensors of KTiOPO4, KTiOAsO4, RbTiOPO4, and RbTiOAsO4crystals.Appl. Opt.43, 3319-3323 (2004)..
Sánchez-García, L. et al. Plasmonic enhancement of second harmonic generation from nonlinear RbTiOPO4 crystals by aggregates of silver nanostructures.Opt. Express24, 8491-8500 (2016)..
Chen, Y. F., Chen, Y. S.&Tsai, S. W. Diode-pumped Q-switched laser with intracavity sum frequency mixing in periodically poled KTP.Appl. Phys. B79, 207-210 (2004)..
Zhang, S. L., Tan, Y. D.&Li, Y. Orthogonally polarized dual frequency lasers and applications in self-sensing metrology.Meas. Sci. Technol.21, 054016 (2010)..
Zhang, S. L.&Bosch, T. Orthogonally polarized lasers and their applications.Opt. Photonics News18, 38-43 (2007)..
Thomas, P. A., Mayo, S. C.&Watts, B. E. Crystal structures of RbTiOAsO4, KTiO(P0.58, A0.42)O4, RbTiOPO4and (Rb0.465, K0.535)TiOPO4, and analysis of pseudosymmetry in crystals of the KTiOPO4family.Acta Cryst.B48, 401-407 (1992)..
Carvajal, J. J. et al. Broad emission band of Yb3+in the nonlinear Nb:RbTiOPO4crystal: origin and applications.Opt. Express18, 7228-7242 (2010)..
Lupei, A., Lupei, V., Presura, C., Enaki, V. N.&Petraru, A. Electron-phonon coupling effects on Yb3+spectra inseveral laser crystals.J. Phys: Condens Matter11, 3769-3778 (1999)..
Seal, K. et al. Coexistence of localized and delocalized surface plasmon modes in percolating metal films.Phys. Rev. Lett.97, 206103 (2006)..
Damen, T. C., Porto, S. P. S.&Tell, B. Raman effect in zinc oxide.Phys. Rev.142, 570-574 (1966)..
Carvajal, J. J. et al. Structural and optical properties of RbTiOPO4:Nb crystals.J. Phys: Condens Matter19, 116214 (2007)..
Carvajal, J. J. et al. Crystal growth of RbTiOPO4:Nb: a new nonlinear optical host for rare earth doping.Cryst. Growth Des.1, 479-484 (2001)..
Palik, E. D.Handbook of Optical Constants of Solids. (Academic Press, San Diego, 1998).
Guillien, Y. et al. Crystal growth and refined Sellmeier equations over the complete transparency range of RbTiOPO4.Opt. Mater.22, 155-162 (2003)..
0
浏览量
0
Downloads
0
CSCD
关联资源
相关文章
相关作者
相关机构
京公网安备11010802024621