Engineering the light matter interaction with ultra-small open access microcavities Jason M. Smith Department of Materials, University of Oxford, Parks Road, Oxford OX1 3PH, UK Photonics in Oxford Engineering Science Physics Chemistry Materials Quantum optics and control Cavity ringdown Spectroscopy Liquid crystals Quantum optics,fundamentals and processing Absorption spectroscopy Nanocrystal quantum dots– synthesis, characterisation and modeling Optical wireless Metrology Novel spectroscopic techniques CMOS imagers/ detectors Microscopy Biophysics measurement CMOS imagers Telescope instrumentation Ultrafast spectroscopy Fluorescence imaging Fibre/waveguide theory Synthetic organic chemistry X ray generation Molecular electronics Metamaterials Optical techniques in nano-technology Organic chemistry Biophysics Soft condensed matter Photovoltaics Surface analysis Advanced microscopyMicron imaging centre Biochemistry Microscopy for single molecule Biochemistry Bionanotech, Biochemistry Molecular materials Spectroscopy Acousto-optics Carbon nanomaterials – synthesis, characterisation and modeling Biochemistry and Life sciences Correlative microscopy Wellcome trust centre for human genetics Cell imaging High speed imaging Cavity QED Photovoltaics – silicon and 3rd Gen materials Diamond photonics X-ray crystallography Diamond Processing of visual information. Exp. Psychology Imaging. Weatherall Inst. for Molecular Medicine. Radiation Oncology (Imaging) The Photonic Nanomaterials Group, Department of Materials Jason Smith Sub-femtolitre tunable microcavity arrays Engineering interfaces in quantum photonics / electronics / spintronics Novel optical microcavity arrays for enhanced light-matter interactions Engineering excitonic states in semiconductor nanocrystal quantum dots Photonics of diamond and its defects Optically Detected Magnetic Resonance of single spins (300K) Modified emission spectra and transition rates Characterisation of single colour centres in diamond Microwave frequency (GHz) Nanocrystal synthesis, characterisation and modeling http://www-png.materials.ox.ac.uk Outline • Optical microcavities – why small is beautiful • Fabrication and characterisation of novel femtoliter open-access cavities • Preliminary studies of light-matter coupling at room temperature Introduction to optical microcavities g ξ.d ξ V Strong coupling: g is the coupling strength is the field per photon 2 g g , Energy output time Weak coupling: g , Energy output time Fermi’s Golden Rule: Can either 2 ' f Hˆ ' i 2 f a) work out new matrix element with cavity vacuum field and ‘count’ photon states or b) use free space matrix element and work out change in the optical DoS (Purcell approach) 3Q / n FP 4 2V 3 Popular microcavity designs From E. L. Hu, (then) UCSB From K Vahala, Caltech From J P Reithmayer, Wurzburg. Planar-concave ‘half-symmetric’ cavities High quality dielectric mirrors • Fully tunable • Efficient coupling • Access to field maximum Stability criterion Trupke et al APL 2005, PRL 2007 Steinmetz et al APL 2006 Muller et al APL 2009 Cui et al Optics Express 2006 High Q open access microcavities with femtoliter mode volumes SEM of arrayed concave surfaces by ion beam milling Sub – nm surface roughness for high reflectivity mirrors 4 2 0.9998 Rmax exp P R Dolan et al, Femtoliter tunable optical cavity arrays, Optics Letters 35, p.3556 (2010). White light transmission spectra L 3m L 12m FSR 2 2L Hermite-Gauss mode structure 0,3 1,2 2,1 3,0 TEMx,y 3 2 0,2 1,1 2,0 0,1 1,0 0,0 1 0 Laser Transmission Imaging of mode structure Quality factors Q = 5 x104 achieved Q ~ 106 anticipated Photoluminescence measurements of solutions of intra-cavity quantum dots Z. Di, H. V. Jones, P. R. Dolan, S. M. Fairclough, M. B. Wincott, J. Fill, G. M. Hughes and J. M. Smith, Controlling the emission from semiconductor quantum dots using ultra-small tunable optical microcavities, New J. Phys. 14 103048 (2012). Fluorescence from CdSe/ZnS colloidal quantum dots coupled to cavity modes http://users.ox.ac.uk/~png Purcell effect at room temperature Best aligned quantum dots 𝑉 > 2𝜇𝑚3 Worst aligned quantum dots 3Q / n FP 4 2V 3 Q res QD cav 40 𝑉 = 0.53𝜇𝑚3 “Bad emitter” regime FDTD calculations F = FP +1 (assumes free space emission is unperturbed by cavity) Suppression of leaky modes Purcell factor of resonant mode Emission from a single quantum dot into a cavity Count rate ~ 100,000 s-1 into NA = 0.4. Compare ~50,000 s-1 with NA = 1.25 and no cavity. Apparatus for cryogenic operation… Nitrogen-vacancy centres in diamond N V …awaiting first low T results! Wavelength /nm How small can open access cavities be made (with decent Q)? • Mirrors: silica/titania (n=2.5) terminated with /4 titania. • Above: planar mirror, 8 pairs • Below: curved mirror, 10 pairs, β = 3 µm • Mirror spacing =/2 (222 nm), n=1.44 • Emitter = 6408nm, dipole //x Mode volume ~3 NB this is about as good as an L3 photonic crystal cavity (Chalcraft APL 90, 241117 2007) Summary of cavity specifications Current Possible Mirror reflectivity 99.9% >99.995% Q factor 5 x 104 >106 Mode volume 0.5 µm3 0.1 µm3 Field per photon ~1.8 kV cm-1 ~6 kV cm-1 Purcell factor * ~70 ~10000 Leakage rate ~60 GHz < 5 GHz Applications • Cavity QED/ quantum information science • Sensing & spectroscopy • Tunable lasers Acknowledgments Phil Dolan Ziyun Di Helene Jones Gareth Hughes Postdoc position available soon Aurélien Trichet Funding and support • EPSRC • The Leverhulme Trust • The Royal Society • Oxford Martin School • The KC Wong Foundation • Hewlett Packard Ltd