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Detecting single<br />
photons<br />
Andrea Fiore
Why single-photon<br />
detectors?<br />
Measure "very efficient" nonlinear frequency conversion...<br />
A PhD student "under Rosencher's rule":<br />
Wikipedia<br />
Will I ever get a<br />
few photons<br />
and my thesis?<br />
Solution n. 1: Change field and work on lasers...<br />
Andrea Fiore
Single-photons again...<br />
"Les photons ... présentent un certain nombre de comportements paradoxaux"<br />
Emmanuel Rosencher, Optoélectronique, Masson ed.<br />
"We estimate the potential market for Quantum Cryptography is<br />
likely to reach $1 billion per annum"<br />
Bob Gelfond, MagiQ Corporation, New York<br />
id201 Singlephoton<br />
APD<br />
Presently limits<br />
system performance<br />
Let's get this fixed for good: Single-photon detectors<br />
Andrea Fiore
t<br />
3-<strong>10</strong>nm<br />
Nanowire Superconducting<br />
Single-Photon Detector<br />
NbN<br />
T>T C<br />
I~I C<br />
Golts'man et al., APL (2001)<br />
+ V -<br />
R hs<br />
J>J C<br />
w<br />
60-<strong>10</strong>0nm<br />
Andrea Fiore
5μm<br />
Meander SSPDs<br />
5μm<br />
Nanofabrication: CNR-IFN Rome<br />
<strong>10</strong>0nm<br />
150nm<br />
Marsili et al., Optics Express 2008<br />
Andrea Fiore
+<br />
V<br />
-<br />
Bias T<br />
i<br />
SSPD operation<br />
Voltage (a.u.)<br />
0<br />
1.6 ns<br />
-1<br />
-<strong>10</strong> 0 <strong>10</strong> 20<br />
Time(ns)<br />
• <strong>10</strong>00x more sensitive than InGaAs APDs at 1300-1500 nm<br />
• Can run in continuous mode, with counting rates>80 MHz<br />
• Timing resolution
Photon-number-resolving<br />
detectors<br />
Meander SSPDs do not resolve the photon number<br />
+<br />
V<br />
-<br />
Time<br />
Bias T<br />
?<br />
i<br />
Light Voltage<br />
Rhs Rhs Single-φ PNR<br />
det.<br />
R L<br />
Time<br />
PNR functionality<br />
needed in many<br />
quantum protocols<br />
Andrea Fiore
+<br />
V<br />
-<br />
Parallel-Nanowire Detector<br />
Bias T<br />
Output pulse ∝ photon number if:<br />
• N. wires >> N. photons<br />
• Other wires do no shunt switching wire<br />
Andrea Fiore
R L<br />
V b<br />
+<br />
-<br />
I<br />
R hs<br />
L kin<br />
R 0<br />
Electrical equivalent<br />
circuit<br />
S l<br />
S l<br />
R hs<br />
I b<br />
L kin<br />
R 0<br />
Sl Sl R hs<br />
L kin<br />
Sl Sl R hs<br />
L kin<br />
S l<br />
I b I b I b<br />
R 0<br />
R 0<br />
R A<br />
+<br />
V OUT<br />
-<br />
Andrea Fiore
Fabricated PNDs<br />
R<br />
Film growth and meas. @ EPFL,<br />
nanofab. @CNR-IFN<br />
R<br />
Andrea Fiore
Experimental PND output<br />
PND output voltage under<br />
illumination with laser pulses:<br />
Experimental I out (a.u.)<br />
5<br />
4<br />
3<br />
2<br />
1<br />
0<br />
0 50 <strong>10</strong>0 150<br />
Time (ns)<br />
Divochiy et al., Nature Photonics, 2008<br />
Simulation:<br />
Andrea Fiore
Voltage<br />
Proving the PNR<br />
functionality<br />
Pulse height statistics with a sampling scope:<br />
4 wires PND-R<br />
66 nW<br />
Most promising technology for fast and<br />
sensitive PNR detection in the telecom range<br />
Time<br />
Detected pulses follow Poissonian statistics ⇒ Proof of PNR operation<br />
Divochiy et al., Nature Photonics, 2008<br />
Collaboration with MSPU<br />
Andrea Fiore
Curiosity-driven: A singlephoton<br />
nanodetector?<br />
Detection mechanism in SSPDs is nanoscale,<br />
but meander SSPDs usually cover large areas<br />
⇒ We lose spatial information<br />
Near-field imaging<br />
Det.<br />
• Direct detection in near-field<br />
• Smaller detector ⇒ Lower noise<br />
≈30 nm<br />
Sub-λ quantum imaging<br />
D'Angelo et al., Phys. Rev. Andrea Lett. 2001 Fiore
Nanoscale single-φ<br />
detector<br />
≈50 nm<br />
QE<br />
< 30 nm active<br />
area possible<br />
Andrea Fiore
<strong>10</strong> -3 <strong>10</strong> 5<br />
<strong>10</strong> -2<br />
n-SSPD performance<br />
Proof of single-φ detection:<br />
Counts (s -1 )<br />
<strong>10</strong> 7<br />
<strong>10</strong> 6<br />
I b =8.5μA<br />
50 nm<br />
<strong>10</strong> -1<br />
Slope=0.99<br />
Data<br />
Linear fit<br />
Light power (a. u.)<br />
<strong>10</strong> 0<br />
Diffraction spot of<br />
microscope objective:<br />
Bitauld et al., Nano Lett. 20<strong>10</strong><br />
•Able to image submicrometer (down to 500 nm) features<br />
with single-photon sensitivity<br />
•Expected detector resolution ≈50-<strong>10</strong>0 nm<br />
Andrea Fiore
Nanoscale PNR?<br />
High bias current: Single-φ response<br />
Andrea Fiore
Count rate (s -1 )<br />
<strong>10</strong> 7<br />
<strong>10</strong> 6<br />
<strong>10</strong> 5<br />
Nanoscale PNR detection<br />
I =17μA<br />
b s=1.9<br />
I =14.4μA<br />
b<br />
Low bias current: s=2.98 (≥n)-photon detector<br />
I =11.2μA<br />
b<br />
s=3.99<br />
I =9.2μA<br />
b<br />
<strong>10</strong> 4<br />
<strong>10</strong> 3<br />
<strong>10</strong> 2<br />
<strong>10</strong> 0<br />
C∝<br />
<strong>10</strong> 1<br />
n<br />
s=1.03<br />
s<br />
<strong>10</strong> 2<br />
<strong>10</strong> 3<br />
<strong>10</strong> 4<br />
Average n. photons/pulse<br />
Linear Fits<br />
Andrea Fiore
Detection prob.<br />
1,2<br />
1<br />
0,8<br />
0,6<br />
0,4<br />
0,2<br />
Multiphoton imaging<br />
N=1<br />
N=2<br />
N=3<br />
N=4<br />
0<br />
-3 -2 -1 0 1 2 3<br />
Position (μm)<br />
FWHM (μm)<br />
N=1: FWHM=0.9 μm<br />
N=4: FWHM=0.41 μm<br />
1<br />
0.8<br />
0.6<br />
0.4<br />
FWHM<br />
S = -0.53<br />
1 2 3 4<br />
• Increased contrast<br />
Bitauld et al., Nano Lett. 20<strong>10</strong><br />
• Increased resolution possible with entangled light<br />
N<br />
∝<br />
1<br />
N<br />
Andrea Fiore
Summary<br />
Photodetection in superconducting nanowires opens new<br />
avenues in single- and multi-photon detection<br />
• PNRs detection possible at telecom wavelengths<br />
• Nanoscale detection opens the way to nanoscale quantum<br />
photonics<br />
• Integration with GaAs-based (quantum) photonics possible<br />
Andrea Fiore
Acknowledgements<br />
Contributors:<br />
- F. Marsili, D. Bitauld, S. Jahanmiri Nejad, J.P. Sprengers,<br />
D. Sahin, G.J. Hamhuis, R. Notzel (TU Eindhoven)<br />
- A. Gaggero, R. Leoni, F. Mattioli (CNR Rome, Italy)<br />
- F. Lévy, R. Sanjines (EPF Lausanne)<br />
Funding: EU-FP6 SINPHONIA and FP7 QUANTIP<br />
Dutch STW-Vici, Swiss NCCR Quantum Photonics<br />
Andrea Fiore