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Squeezing eigenmodes in parametric down-conversion. Wojciech Wasilewski. Czes ław Radzewicz Warsaw University Poland. Konrad Banaszek Nicolaus Copernicus University Toru ń, Poland. Alex Lvovsky University of Calgary Alberta, Canada. - PowerPoint PPT Presentation
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Czesław RadzewiczWarsaw University
Poland
Konrad BanaszekNicolaus Copernicus University Toruń, Poland
Alex LvovskyUniversity of Calgary
Alberta, Canada
Squeezing eigenmodesin parametric down-conversion
National Laboratory for Atomic, Molecular, and Optical Physics, Toruń, Poland
Wojciech Wasilewski
Agenda
• Classical description• Input-output relations• Bloch-Messiah reduction• Single-pair generation limit• High-gain regime• Optimizing homodyne detection
Fiber optical parametric amplifier
c(2)tp
• Pump remains undepleted• Pump does not fluctuate
Linear propagation
Highorder effects
Group velocity
dispersion
Group velocity
Phase velocity
Three wave mixing
kp, p
p =+ ’k,
k’, ’
Classical optical parametric amplifier
[See for example: M. Matuszewski, W. Wasilewski, M. Trippenbach, and Y. B. Band,Opt. Comm. 221, 337 (2003)]
c(2)
Linear propagation
3WMInteraction
strength
Input-output relations
Quantization: etc.
Decomposition
As the commutation relations for the output field operators must be preserved, the two integral kernels can be decomposed using the Bloch-Messiah theorem:
S. L. Braunstein,Phys. Rev. A 71, 055801 (2005).
The Bloch-Messiah theorem allows us to introduce eigenmodes for input and output fields:
Squeezing modes
The characteristic eigenmodes evolve according to:
• describe modes that are described by pure squeezed states • tell us what modes need to be seeded to retain purity
a(0) a(z)
.... ....
G1G2G3G4U V
bin bout
.... ....
a(0) a(z)
Squeezing modes
a(0) a(z)
.... ....
G1G2G3G4U V
bin bout
.... ....
a(0) a(z)
The operation of an OPA is completely characterized by:• the mode functions nand n• the squeezing parameters n
Single pair generation regime
kp, p
p = + ’
L
k,
k’, ’Amplitude S sin(k L/2)/k
k = kp-k-k’
Single pair generation regime
’
pAmplitude S Pump x sin(k L/2)/k
Single pair generation
’
p
S(,’)=ei… ,’|out
=Σ j fj()gj(’)
Gaussian approximation of S
2
1
k=0
1+2=p
“Classic” approach
Schmidt decomposition for a symmetric two-photon wave function:C. K. Law, I. A. Walmsley, and J. H. Eberly,Phys. Rev. Lett. 84, 5304 (2000)
We can now define eigenmodes which yields:
The spectral amplitudes characterize pure squeezing modes
The wave function up to the two-photon term:
W. P. Grice and I. A. Walmsley, Phys. Rev. A 56, 1627 (1997);T. E. Keller and M. H. Rubin, Phys. Rev A 56, 1534 (1997)
Intense generation regime
• 1 mm waveguide in BBO• 24 fs pump @ 400nm
Squeezing parameters
RMS quadrature squeezing: e-2
Spectral intensity of eigenmodes
Input and ouput modes
| =| | |0 02 2
arg 0
arg 0
First mode vs. pump intensity
| |02
arg 0
L =100mmNL
L =1/ 15mmNL
Homodyne detection
LO
Noise budget
Detected squeezing vs. LO duration
1/LNL=1
2
3
4
ts
Contribution of various modes
Mn
n
15fstLO
30fs50fs
Optimal LOs
345
Optimizing homodyne detection
–
SHG
PDC
Conclusions• The Bloch-Messiah theorem allows us to introduce eigenmodes for input and output fields• For low pump powers, usually a large number of modes becomes squeezed with similar squeezing parameters• Any superposition of these modes (with right phases!) will exhibit squeezing• The shape of the modes changes with the increasing pump intensity!• In the strong squeezing regime, carefully tailored local oscillator pulses are needed.• Experiments with multiple beams (e.g. generation of twin beams): fields must match mode-wise.• Similar treatment applies also to Raman scattering in atomic vapor WW, A. I. Lvovsky, K. Banaszek, C. Radzewicz, quant-ph/0512215
A. I. Lvovsky, WW, K. Banaszek, quant-ph/0601170WW, M.G. Raymer, quant-ph/0512157