Title: Jonathan P' Dowling
1QUANTUM IMAGING HAPPY-N00N YEAR!
Jonathan P. Dowling
Hearne Institute for Theoretical
Physics Department of Physics
Astronomy Louisiana State University Baton Rouge,
Louisiana USA
quantum.phys.lsu.edu
Quantum Imaging MURI Annual Review, 01 October
2007, Boston
2TABLE OF CONTENTS
Programmatics N00N State Characterization
N00N State Generation OPA! N00N State
Absorption Miscellaneous
3Hearne Institute for Theoretical Physics Quantum
Science Technologies Group
4The Pizzas Mine!
I Bet He Cheated
However, As We all Know, Some Students Require
a Little Arm Twisting!
5Quantum Imaging Theory
Objective Entangled Photons Beat Diffraction
Limit Lithography With Long-Wavelengths
Dispersion Cancellation Masking Techniques
N-Photon Resists
Accomplishments FY07 Properties of N00N
States Efficient N00N Generators Bright N00N
Generators Thy/Exp Masking Lithography
N-Photon Absorption Loss in N00N-State
Imaging Loss in Interaction Free Imaging
Approach Investigate Which States are
Optimal Design Efficient Quantum State
Generators Investigate Masking Systems
Develop Theory of N-Photon Resist Integrate
into Optical System Design
6PROGRAMMATICS
Budget 100K/Y Personnel Commitment Per
Year Dowling 1 Month ARO 1.5 Months LSU
Matching Hugo Cable (Postdoc) 12 Months
ARO Ryan Glasser (Grad) 12 Months LSU
Matching William Plick (Grad) 12 Months LSU
Matching Facilities 4 Dell Work Stations 2
From DURIP
7FY07 PUBLICATIONS PREPRINTS
- Durkin, GA Dowling, JP, Local and Global
Distinguishability in Quantum Interferometry,
PHYSICAL REVIEW LETTERS, 99 (7) Art. No. 070801
AUG 17 2007. - Kapale, KT Dowling, JP, Bootstrapping Approach
for Generating Maximally Path-Entangled Photon
States, PHYSICAL REVIEW LETTERS, 99 (5) Art. No.
053602 AUG 3 2007. - Cable H Dowling JP, Efficient Generation of
Large Number-path Entanglement Using Only Linear
Optics and Feed-forward, PHYSICAL REVIEW LETTERS,
in press, arXiv0704.0678 ltquant-phgt. - Wildfeuer CF, Lund A, Dowling JP, Strong
Violations of Bell-type Inequalities for
Path-Entangled Number States, PHYSICAL REVIEW A,
in press, arXivquant-ph/0610180. - VanMeter NM, Lougovski P, Uskov DB, Kieling K,
Eisert J, Dowling JP, A General Linear-Optical
Quantum State Generator, submitted to PHYSICAL
REVIEW LETTERS, arXivquant-ph/0612154. - DeMartini F, Sciarrino F, Vitelli C, Glasser RT,
Cable H, Dowling JP, Experimental Sub-Rayleigh
Resolution by an Unseeded High-gain Optical
Parametric Amplifier for Quantum Lithography,
submitted to PHYSICAL REVIEW LETTERS.
8FY07 LECTURES AT CONFERENCES
Generation and Characterization of N00N States
Using Linear Optics, Hugo Cable and Jonathan P.
Dowling, Symposium on Quantum Information and
Computation, Laser Physics Workshop, 2024 August
2007, León, Mexico (invited). Quantum Sensors,
Jonathan P. Dowling, Fourth SPIE International
Symposium on Fluctuations and Noise, 2024 May
2007, Florence, Italy (invited). Linear
Optical Quantum Computing, Imaging, and
Metrology, Jonathan P. Dowling, International
Conference on Quantum Communication, Measurement,
and Computing, 28 November 3 December, Tokyo,
Japan. Quantum Imaging and Precision
Measurements with N00N States, Jonathan P.
Dowling, Optical Society of America Annual
Meeting, 812 October 2006, Rochester, NY
(invited).
9FY07 Visitors Lecturers _at_ LSU
Malvin Teich, Director, Photonics Center, Boston
University, Boston. Francesco DeMartini,
Department of Physics of the University La
Sapienza, Rome, Italy. Claude Fabre,
Laboratoire Kastler-Brossel Ecole Normale
Superieure and University Pierre et Marie Curie,
Paris. Hans Bachor, Research Director and
Federation Fellow, Australian National Centre of
Excellence for Quantum-Atom Optics, Australian
National University, Canberra.
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11Quantum Imaging A Systems Approach
Non-Classical Photon Sources
N-Photon Absorbers
Imaging System
Ancilla Devices
12AN Boto, DS Abrams, CP Williams, JPD, PRL 85
(2000) 2733
N-Photon Absorber
a N a N
13TABLE OF CONTENTS
Programmatics N00N State Characterization
N00N State Generation OPA! N00N State
Absorption Miscellaneous
14N00N
15PRA, in press, arXivquant-ph/0610180.
16TABLE OF CONTENTS
Programmatics N00N State Characterization
N00N State Generation OPA! N00N State
Absorption Miscellaneous
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18PRL, in press, arXiv0704.0678
19submitted to PRL, arXivquant-ph/0612154
20TABLE OF CONTENTS
Programmatics N00N State Characterization
N00N State Generation OPA! N00N State
Absorption Miscellaneous
21Ryan, Hugo, and Bill The Early Years!
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24Entanglement-Seeded Dual OPARyan Glasser, Hugo
Cable, JPD (in preparation)
- Two identical OPAs pumped with the same laser are
seeded with the entangled input - Input state created from a spontaneous parametric
downconverter and the Hong-Ou-Mandel effect. - Output state is
- The factor depends on the phase of the
OPAs, the gain (r) and the values of n and m. - Inner two modes b and c are highly path
entangled. - Detecting n and m photons at Da and Dd allows
with certainty knowledge of the state the inner
two modes are in.
25Entanglement-Seeded Dual OPARyan Glasser, Hugo
Cable, JPD (see poster)
- Probability of obtaining an output state with a
given n and m is
- Most probable joint detection outcome is nm1,
which occurs at an easily experimentally
obtainable gain of r0.66 - This results in the state
- This state input on a 50/50 beamsplitter results
in the N4 N00N state
- If perfect number resolving detectors exist at Da
and Dd , and we detect those modes out, we can
use the entangled modes b and c for a quantum
cryptography protocol.
Output probabilities of a given n and m
Whats Next???
- Recently finished calculation of output state
including vacuum input. - Need to quantify amount of entanglement in output
state. - Does output state beat the shot-noise limit?
- Viable source for noiseless amplification (one
quadrature)? - How do phase sensitive versus phase insensitive
parametric amplifiers affect the scheme? - Is degenerate parametric amplification required
for the input? - Effect of imperfect detectors on phase
resolution.
26TABLE OF CONTENTS
Programmatics N00N State Characterization
N00N State Generation OPA! N00N State
Absorption Miscellaneous
27Multi-Photon Absorption William Plick, Christoph
Wildfeuer, JPD (poster)
Output of a BBO Crystal
Information about pump
Creation operators only part affected by beam
splitter.
Phase Mismatch K(pump) K(signal) K(idler)
Rate of two photon absorption
Detuned Virtual Level
One photon transition energy
- Equation found by B. R. Mollow using second
order perturbation theory. - For most cases of interest the atomic response
(g) separates from the integral. - The most important quantity is then the second
order field correlation function (G).
Two photon transition energy
28Multi-Photon Absorption William Plick, Christoph
Wildfeuer, JPD (poster)
- Generalization of the perturbative approach to
N-Photon interactions by G.S. Agarwal. - Again the key quantity is shown to be the field
correlation function. This time to Nth order and
scaled by the intensity (1st order correlation). - Obtaining a more concrete result for N-photon
absorption rates for N00N states will require
further investigation and knowledge of how these
states are to be generated.
The rate of change of the average number of
photons in the field (in point of fact the
absorption rate) is proportional to the following
ratio
Note Scaled to coherent state
- In the meantime the normalized field correlation
functions give a good approximation of how these
absorption rates will scale.
29TABLE OF CONTENTS
Programmatics N00N State Characterization
N00N State Generation OPA! N00N State
Absorption Miscellaneous
30Quantum Optical Masking Imaging S. Vinjanampathy,
S. Thanvanthri, H. Cable, JPD (in progress)
Quantum Masking Lithography
Diffraction in Ghost Imaging
31Loss Noise in Interaction-Free Imaging Daniel
Lum JPD (in progress)
- Modeling
- Loss
- Scattering
- Turbulence
- Clutter
32TABLE OF CONTENTS
Programmatics N00N State Characterization
N00N State Generation OPA! N00N State
Absorption Miscellaneous