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Nat Mater. 2015 Jun;14(6):607-12. doi: 10.1038/nmat4267. Epub 2015 Apr 13.

Continuous control of the nonlinearity phase for harmonic generations.

Nature materials

Guixin Li, Shumei Chen, Nitipat Pholchai, Bernhard Reineke, Polis Wing Han Wong, Edwin Yue Bun Pun, Kok Wai Cheah, Thomas Zentgraf, Shuang Zhang

Affiliations

  1. 1] School of Physics and Astronomy, University of Birmingham, Birmingham B15 2TT, UK [2] Department of Physics, Hong Kong Baptist University, Kowloon Tong, Hong Kong.
  2. 1] Department of Physics, University of Paderborn, Warburger Straße 100 D-33098 Paderborn, Germany [2] Department of Industrial Physics and Medical Instrumentation, King Mongkut's University of Technology North Bangkok, 1518 Pibulsongkram Road, Bangkok 10800, Thailand [3] Lasers and Optics Research Group, King Mongkut's University of Technology North Bangkok, 1518 Pibulsongkram Road Bangkok 10800, Thailand.
  3. Department of Physics, University of Paderborn, Warburger Straße 100 D-33098 Paderborn, Germany.
  4. Department of Electronic Engineering, City University of Hong Kong, 83 Tat Chee Avenue, Hong Kong.
  5. 1] Department of Electronic Engineering, City University of Hong Kong, 83 Tat Chee Avenue, Hong Kong [2] State Key Laboratory of Millimeter Waves, City University of Hong Kong, 83 Tat Chee Avenue, Hong Kong.
  6. Department of Physics, Hong Kong Baptist University, Kowloon Tong, Hong Kong.
  7. School of Physics and Astronomy, University of Birmingham, Birmingham B15 2TT, UK.

PMID: 25849530 DOI: 10.1038/nmat4267

Abstract

The capability of locally engineering the nonlinear optical properties of media is crucial in nonlinear optics. Although poling is the most widely employed technique for achieving locally controlled nonlinearity, it leads only to a binary nonlinear state, which is equivalent to a discrete phase change of π in the nonlinear polarizability. Here, inspired by the concept of spin-rotation coupling, we experimentally demonstrate nonlinear metasurfaces with homogeneous linear optical properties but spatially varying effective nonlinear polarizability with continuously controllable phase. The continuous phase control over the local nonlinearity is demonstrated for second and third harmonic generation by using nonlinear metasurfaces consisting of nanoantennas of C3 and C4 rotational symmetries, respectively. The continuous phase engineering of the effective nonlinear polarizability enables complete control over the propagation of harmonic generation signals. Therefore, this method seamlessly combines the generation and manipulation of harmonic waves, paving the way for highly compact nonlinear nanophotonic devices.

References

  1. Phys Rev Lett. 2000 May 8;84(19):4345-8 - PubMed
  2. Phys Rev Lett. 2007 Apr 20;98(16):167403 - PubMed
  3. Phys Rev Lett. 2011 Apr 1;106(13):133901 - PubMed
  4. Phys Rev Lett. 2008 Jul 25;101(4):043903 - PubMed
  5. Opt Lett. 2001 Sep 15;26(18):1424-6 - PubMed
  6. Science. 2011 Sep 23;333(6050):1720-3 - PubMed
  7. Phys Rev Lett. 2010 Jan 29;104(4):046803 - PubMed
  8. Phys Rev Lett. 2014 Apr 4;112(13):135502 - PubMed
  9. Nano Lett. 2013 Sep 11;13(9):4148-51 - PubMed
  10. Nano Lett. 2011 Dec 14;11(12):5519-23 - PubMed
  11. Nano Lett. 2012 Sep 12;12(9):4997-5002 - PubMed
  12. Nat Commun. 2012;3:1198 - PubMed
  13. Science. 2011 Oct 21;334(6054):333-7 - PubMed
  14. Phys Rev Lett. 2014 Jul 18;113(3):033901 - PubMed
  15. Science. 2013 Dec 6;342(6163):1223-6 - PubMed
  16. Science. 2013 Mar 22;339(6126):1405-7 - PubMed
  17. Science. 2012 Jan 27;335(6067):427 - PubMed
  18. Opt Lett. 1999 May 1;24(9):584-6 - PubMed

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