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Dive into the research topics where Jonathan P. Dowling is active.

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Featured researches published by Jonathan P. Dowling.


Reviews of Modern Physics | 2007

Linear optical quantum computing with photonic qubits

Pieter Kok; W. J. Munro; Kae Nemoto; Timothy C. Ralph; Jonathan P. Dowling; G. J. Milburn

Linear optics with photon counting is a prominent candidate for practical quantum computing. The protocol by Knill, Laflamme, and Milburn [Nature 409, 46 (2001)] explicitly demonstrates that efficient scalable quantum computing with single photons, linear optical elements, and projective measurements is possible. Subsequently, several improvements on this protocol have started to bridge the gap between theoretical scalability and practical implementation. We review the original theory and its improvements, and we give a few examples of experimental two-qubit gates. We discuss the use of realistic components, the errors they induce in the computation, and how these errors can be corrected.


quantum electronics and laser science conference | 2000

Quantum interferometric lithography: exploiting entanglement to beat the diffraction limit

Agedi N. Boto; Daniel S. Abrams; Colin P. Williams; Jonathan P. Dowling

Classical optical lithography is diffraction limited to writing features of a size lambda/2 or greater, where lambda is the optical wavelength. Using nonclassical photon-number states, entangled N at a time, we show that it is possible to write features of minimum size lambda/(2N) in an N-photon absorbing substrate. This result allows one to write a factor of N2 more elements on a semiconductor chip. A factor of N = 2 can be achieved easily with entangled photon pairs generated from optical parametric down-conversion. It is shown how to write arbitrary 2D patterns by using this method.


Journal of Applied Physics | 1994

THE PHOTONIC BAND EDGE LASER : A NEW APPROACH TO GAIN ENHANCEMENT

Jonathan P. Dowling; Michael Scalora; Mark J. Bloemer; Charles M. Bowden

Near the band edge of a one‐dimensional photonic band gap structure the photon group velocity approaches zero. This effect implies an exceedingly long optical path length in the structure. If an active medium is present, the optical path length increase near the photonic band edge can lead to a better than fourfold enhancement of gain. This new effect has important applications to vertical‐cavity surface‐emitting lasers.


quantum electronics and laser science conference | 1996

Analytic expressions for the electromagnetic mode density in finite, one-dimensional, photonic band-gap structures

Jon M. Bendickson; Michael Scalora; Jonathan P. Dowling

Summary form only given. We derive an exact expression for the electromagnetic mode density, and hence the group velocity, for a finite N period, one-dimensional photonic band-gap structure. We begin by deriving a general formula for the mode density in terms of the complex transmission coefficient of an arbitrary index profile. Then we develop a formula that gives the N-period mode density in terms of the transmission coefficient of the unit cell. The special cases of mode-density enhancement and suppression at the photonic band edge and at mid gap, respectively are derived. The specific example of a quarter-wave stack is analyzed, and applications to 3D structures, spontaneous emission control, delay lines, band-edge lasers, and superluminal tunneling times are discussed.


Journal of Applied Physics | 1998

Transparent, metallo-dielectric, one-dimensional, photonic band-gap structures

Michael Scalora; Mark J. Bloemer; A. S. Pethel; Jonathan P. Dowling; Charles M. Bowden; A. S. Manka

We investigate numerically the properties of metallo-dielectric, one-dimensional, photonic band-gap structures. Our theory predicts that interference effects give rise to a new transparent metallic structure that permits the transmission of light over a tunable range of frequencies, for example, the ultraviolet, the visible, or the infrared wavelength range. The structure can be designed to block ultraviolet light, transmit in the visible range, and reflect all other electromagnetic waves of lower frequencies, from infrared to microwaves and beyond. The transparent metallic structure is composed of a stack of alternating layers of a metal and a dielectric material, such that the complex index of refraction alternates between a high and a low value. The structure remains transparent even if the total amount of metal is increased to hundreds of skin depths in net thickness.


Contemporary Physics | 2008

Quantum optical metrology – the lowdown on high-N00N states

Jonathan P. Dowling

Quantum states of light, such as squeezed states or entangled states, can be used to make measurements (metrology), produce images, and sense objects with a precision that far exceeds what is possible classically, and also exceeds what was once thought to be possible quantum mechanically. The primary idea is to exploit quantum effects to beat the shot-noise limit in metrology and the Rayleigh diffraction limit in imaging and sensing. Quantum optical metrology has received a boost in recent years with an influx of ideas from the rapidly evolving field of optical quantum information processing. Both areas of research exploit the creation and manipulation of quantum-entangled states of light. We will review some of the recent theoretical and experimental advances in this exciting new field of quantum optical metrology, focusing on examples that exploit a particular two-mode entangled photon state – the High-N00N state.


Applied Physics Letters | 1995

Thin‐film nonlinear optical diode

Michael D. Tocci; Mark J. Bloemer; Michael Scalora; Jonathan P. Dowling; Charles M. Bowden

We present results of a theoretical investigation into a nonlinear thin‐film multilayer device that exhibits passive anisotropic optical transmission—the analogue of the electronic diode. This optical diode is a nonlinear, asymmetric, distributed Bragg reflector. Material parameters for a nonlinear polymer (polydiacetylene 9‐BCMU) and rutile are used in alternating layers to model a realistic device. The diode exhibits more than five times as much transmittance in one direction as in the opposite direction. It has a thickness of only 2 μm and is polarization insensitive.


Journal of Applied Physics | 1994

The photonic band edge optical diode

Michael Scalora; Jonathan P. Dowling; Charles M. Bowden; Mark J. Bloemer

Using numerical methods, we study pulse propagation near the band edge of a one‐dimensional photonic band gap material with a spatial gradiation in the linear refractive index, together with a nonlinear medium response. We find that such a structure can result in unidirectional pulse propagation. That is, the field will be transmitted for, say, a left‐to‐right direction of propagation, while for right‐to‐left nearly complete reflection occurs. This behavior constitutes the operational mechanism for a passive optical diode.


Philosophical Transactions of the Royal Society A | 2003

Quantum Technology: The Second Quantum Revolution

Jonathan P. Dowling; G. J. Milburn

We are currently in the midst of a second quantum revolution The first quantum revolution gave us new rules that govern physical reality. The second quantum revolution will take these rules and use them to develop new technologies. In this review we discuss the principles upon which quantum technology is based and the tools required to develop it. We discuss a number of examples of research programs that could deliver quantum technologies in coming decades including: quantum information technology, quantum electromechanical systems, coherent quantum electronics, quantum optics and coherent matter technology.


Journal of Modern Optics | 1994

Photonic band calculations for woodpile structures

H.S. Sözüer; Jonathan P. Dowling

Abstract Photonic band structure has been computed for ‘woodpile’ structures having the periodicity of the simple tetragonal lattice. Bandgaps have been found. Further research directions are explored.

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Hwang Lee

California Institute of Technology

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Charles M. Bowden

Sapienza University of Rome

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Petr M. Anisimov

Louisiana State University

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Pieter Kok

University of Sheffield

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Chenglong You

Louisiana State University

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Zhihao Xiao

Louisiana State University

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