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ORGANIC MOLECULES in photonics
Progress in Photonics, Florence 16.10. 2015
probe
scattered waves surface
Costanza Toninelli www.lens.unifi.it/quantum-‐nanophotonics
ps |1〉 |1’〉
|0〉 |0’〉
ps |0〉
|1〉
narrow line 50% ZPL
Cryogenic T
Single molecule in the solid state Fermi’s golden rule
( ) ( )rirEdfT fi
ωω ρπ 22
⋅=→
Local DOS Radiative and non
Transition dipole moment
J. Hwang, et al., Nature 460, 76 (2009)
Single Molecules: From Sensing To Quantum Optics
Electron-‐phonon coupling
• Quantum ICTs
• Sense LDOS by lifetime measurements or frequency shift
Sense on nanoscale Quantum sensors
Opt
ical tr
ansitio
n
Single photon source Coherenceà nln. element Coupling to photonics
C. Toninelli et al., Opt. Express 18, 6577 (2010)
Dibenzoterrylene (DBT) in Anthracene
Anthracene crystal
5 µm
DBT /Anthracene
• Stable at room temperature
• Thin films (~50 nm)
• Orient on the plane
• ZPL at 785 nm
DBT Optical Properties Brightness Second order correlation
98% suppression Single Photon Source
1 MHz Bright
C. Toninelli et al., Opt. Express 18, 6577 (2010)
Exciation spectrum Scanning laser frequency over 2 GHz at 3.5 K
DBT at Cryo Temperatures
Narrow molecules
Inhomogeneously broadened (0.1 nm)
Lifetime-limited linewidth
40 MHz
ü Single Photon Source ü No dephasing/ Coherence ü Tunability by Stark shift ü Coupling
Nano-Positioning
(Berlin)
Fluorescence
Intensity autocorrelation
Kewes et al., arxiv.:1501.04788 (2015)
AFM manipulation
• Coupled to Hybrid WG for SPS and coop. effects
• Coupled to graphene to sense position
!
• A nice competitor for DBT SiV centers
Collaboration with M. Agio Collaboration with O. Benson, W. Pernice, S. Meier groups Collaboration with F. Koppens group Collaboration with S. Lagomarsino
• Coupled to optical antennas for enhanced collection
Sense/communicate at the n-scale
Hwang and Hinds., New Journal of Physics, 13, (2011)
Dielectric Waveguides: Towards integrated SPS
Rate = (1/4)*(σ/A)*(1/n^2) σ = 3λ^2/2π A = effective Area depending on Jield @ emitter position
Fluorescence
Dielectric Waveguides: Towards integrated SPS
Dense sample à Fluorescence is coupled into the WG
Kewes et al., arxiv.:1501.04788 (2015)
Output coupler
Pump light
Small crystal
SEM White light image
Pump
Fluorescence
Dielectric Waveguides: Towards integrated SPS Fluorescence spectra
Big highly-‐doped molecular crystal
Dark waveguide à light is coupled to SP Cooperative effects?
Plasmonic Wedge-Waveguides: Towards Cooperative effects
Au is everywhere
Fluorescence scan
Theoretical model: What to look at, what to expect ?
• Coupled to Hybrid WG for SPS and coop. effects
• Coupled to graphene to sense position
!
• A nice competitor for DBT SiV centers
Collaboration with M. Agio Collaboration with O. Benson, W. Pernice, S. Meier groups Collaboration with F. Koppens group Collaboration with S. Lagomarsino
• Coupled to optical antennas for enhanced collection
Sense/communicate at the n-scale
FRET from DBT to graphene
Γg
Γref
=1+9να
256π 3 εsub +εref( )2
λ0
d
"
#$
%
&'
4
1 or 2 (orientation) fine structure constant
distance from graphene
• Universal scaling law • Long interaction length
Graphene-based Nanoruler
• Measure lifetime vs distance…statistical analysis • Get a good reference
E >1.3EF Plasmons are strongly damped
• Lifetime reduction is associated to quenching N(t) =QYρee(t)Γrad
DBT-energy transfer to Graphene
Mazzamuto et al., New J. Phys. 16 (2014) 113007
Proof of principle for G-ruler
• Good agreement btw model and data
Guess from model
Exper. values
Proof for Graphene-based Nanoruler
ηMax ≈ (61± 20)%
• Estimators
η =1−Γref
Γg
Mazzamuto et al., New J. Phys. 16 (2014) 113007
In progress: Casimir force-ruler
Modified Vacuum potential Distance-‐dependent Level shift
C. A. Muschik, et alt. Phys. Rev. Lett. 112, 223601 (2014)
• Coupled to Hybrid WG for SPS and coop. effects
• Coupled to graphene to sense position
!
• A nice competitor for DBT SiV centers
Collaboration with M. Agio Collaboration with O. Benson, W. Pernice, S. Meier groups Collaboration with F. Koppens group Collaboration with S. Lagomarsino
• Coupled to optical antennas for enhanced collection
Sense/communicate at the n-scale
SiV centers in diamond
• Inversion symmetric potential: -‐ narrow line @ room temp. (1 nm) -‐ 70% brunching ratio for ZPL -‐ no charge dynamic spectral diffusion -‐ weak coupling with host matrix -‐ low inhomogeneous broadening (1 GHz) • Single SiV centers both in nDiamonds and in bulk • 150MHz ZPL @ cryo temp.
D3d geometry
Around 5 nm ensamble linewidth
@ RT
pump @ 632 nm
HOME-‐MADE implanted SiV (collaboration with CNR-‐Firenze) • Mono-‐crystalline diamonds • Implantation depth: 2um (impl. Energy Mev)
A. Sipahigil et al., PRL 113, 113602 (2014)
LAB ALBUM 2014/2015
O. Benson W. Pernice S. Meier
F. Koppens
G. Mazzamuto
D.S. Wiersma M. Gurioli
F.S. Cataliotti
S. Rizvi S. Pazzagli
F. Sgrignuoli P.E. Lombardi
S. Checcucci
Post-Doc
PhD students
Collaborators:
!
THANK YOU FOR YOUR ATTENTION
Costanza Toninelli www.lens.unifi.it/quantum-‐nanophotonics
On-‐demand source of single indistinguishable
photons
WG-‐ Integrated SPS SP-‐mediated coop. effects
SM-‐graphene nanoposition sensor
planar antennas
Implanted SiV