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Nanophotonics Prof. Albert Polman Center for Nanophotonics FOM-Institute AMOLF, Amsterdam Debye Institute, Utrecht Unive

Nanophotonics Prof. Albert Polman Center for Nanophotonics FOM-Institute AMOLF, Amsterdam Debye Institute, Utrecht University. Nanophotonics: defined by its applications communications technology lasers solid-state lighting data storage lithography (bio-)sensors

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Nanophotonics Prof. Albert Polman Center for Nanophotonics FOM-Institute AMOLF, Amsterdam Debye Institute, Utrecht Unive

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  1. Nanophotonics Prof. Albert Polman Center for Nanophotonics FOM-Institute AMOLF, Amsterdam Debye Institute, Utrecht University

  2. Nanophotonics: defined by its applications • communications technology • lasers • solid-state lighting • data storage • lithography • (bio-)sensors • optical computers • solar cells • light-activated medical therapies • displays • smart materials Kenniseconomie Large interest from industry in fundamental research on nanophotonics Nanophotonics is a unique part of physics/chemistry/materials science because it combines a wealth of scientific challenges with a large variety of near-term applications.

  3. Decreasing length scales in photonics m km mm nm

  4. Optical fiber kern mantel bescherming

  5. Silica fiber transparent at 1.55 m 1012 Hz 1.3 m 1.55 m

  6. Optical fiber: long distance communication

  7. high index low index Si Planar optical waveguide 1 mm

  8. Photonic integrated circuits on silicon SiO2/Al2O3/SiO2/Si 1 mm Al2O3 technology by M.K. Smit et al., TUD

  9. Optical clock distribution on a Si microprocessor Photonics on silicon Intel Website

  10. Computer interconnects hierarchy Mihail M. Sigalas, Agilent Laboratories, Palo Alto, CA http://www.ima.umn.edu/industrial/2002-2003/sigalas/sigalas.pdf

  11. The world’s smallest erbium-doped optical amplifier 1.53 m signal, 1.48 m pump, 10 mW, gain: 2.3 dB erbium Waveguide spiral size: 1 mm2 minimum bending radius > 50 m

  12. Lanthanide ions as optical dopants H He Li Be B C N O F Ne Na Mg Al SiP S Cl Ar K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe Cs Ba La Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn Fr Ra Ac Rf Db Sg Bh Hs Mt Uun Uuu Uub Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb Lu Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No Lr La3+: [Xe] 4f n n=1-14 ….4f n 5s2 5p6

  13. Erbium transition at 1.5 m

  14. The world’s smallest erbium-doped optical amplifier 1.53 m signal, 1.48 m pump, 10 mW, gain: 2.3 dB erbium Waveguide spiral size: 1 mm2 minimum bending radius > 50 m

  15. From a prototype to a 40 M$ company … Symmorphix Sunnyvale CA, USA

  16. Nanophotonics examples (1) Surface plasmon polaritons Nanocavities Nanoscale energy transfer Field confinement in metal nanoparticle array

  17. 4 m Nanophotonics examples (2) W.L. Vos Anomalous transmission through nanohole arrays K. Kuipers Trapping light in photonic crystals M. Verschuuren Plasmonic solar cells Photonic nanowires J. Gomez Rivas

  18. Nanophotonics science fiction

  19. What will you learn in this class?! • Theory of nanophotonics • Applications of nanophotonics • Nanophotonics fabrication techniques • New developments in science and technology • Presentation skills

  20. Class schedule Sept. 5 Class 1 - Resonances and refractive index Sept. 12 Class 2 - Nanoparticle scattering Sept. 19 Class 3 - Surface plasmon polaritons Sept. 26 Tour through Ornstein Lab Oct. 3 No class / homework assistance Oct. 10 Class 4 - Photonic crystals Oct. 17 13.00-15.00 hr. Class 5 - Local density of optical states 16.00 hr. Debye Lecture “Nanobiophotonics” Oct. 24 No class Oct. 31 Excursion to AMOLF-Amsterdam Nov. 7 Class 6 – Rare earth ions and quantum dots Nov. 14 Class 7 - Microcavities Nov. 18 (Tuesday) Visit to Nanoned conference Nov. 21 No class Nov. 28 Class 8 - Near field optics Dec. 5 Class 9 - Nanophotovoltaics Dec. 12 Excursion to Philips Research- Eindhoven Dec. 19 Class 10 - Metamaterials Christmas break Jan. 9 Class 11 – Transformation optics Jan. 16 Nanophotonics summary Jan. 23 Closing symposium

  21. Fabrication technology: • Thin film deposition • Clean room fabrication technology • Lithography • Focused ion beam milling • Colloidal self-assembly • Bio-templating • Characterization technology: • Photoluminescence spectroscopy • Optical absorption/extinction spectroscopy • Near-field microscopy • Cathodoluminescence imaging spectroscopy • Pump-probe spectroscopy • Practical training at Debye Institute & FOM-Institute AMOLF

  22. Weekly schedule • Nanophotonics fundamentals • Fabrication technology • Characterization principles / techniques • Application example • News of the week • Paper/homework presentations • Excursions/labtours • Albert Polman • E-mail: polman@amolf.nl • Website: www.erbium.nl/nanophotonics

  23. Course grading • No final examination • Grades are determined by: • Homework: 60 % • Paper presentation 1: 10% • Paper presentation 2: 15% • Participation in class: 5% • Homework must he handed in on Friday. No exceptions! • Homework grade: average of (all homework – worst made) • Use help by teaching assistants! • Course time 11.00-13.00 • Absence: must be notified

  24. Resonances and optical constants of dielectrics: basic light-matter interaction

  25. Dielectric materials: All charges are attached to specific atoms or molecules Response to an electric field E:Microscopic displacement of charges Macroscopic material properties: electric susceptibility , dielectric constant (or relative dielectric permittivity) 

  26. Maxwell’s equations in a medium leading to wave equation:

  27. Solution in vacuum (P = J = 0): • In dielectric material (J = 0): • Consider response of electrons bound to atom nuclei:

  28. Equation of motion of electron: g: damping coefficient for given material k: restoring-force constant resonance frequency assume E is varying harmonically, and also

  29. inserting P in wave equation gives solution: with complex propagation constant kz = + iα : and therefore:

  30. So that we find the refractive index of the dielectric:

  31. multiple resonances wj for Z electrons per molecule: Where fj is the oscillator strength or (quantum mechanically) the transition probability N is a complex number:

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