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VR1.0
PT J
AU Wang, L
Huang, JH
Dowling, JP
Zhu, SY
AF Wang, Lei
Huang, Jie-Hui
Dowling, Jonathan P.
Zhu, Shi-Yao
TI Quantum information transmission
SO QUANTUM INFORMATION PROCESSING
AB We present a scheme of quantum information transmission, which transmits the quantum information contained in a single qubit via the quantum correlation shared by two parties (a two-qubit channel), whose quantum discord is non-zero. We demonstrate that quantum correlation, which may have no entanglement, is sufficient to transmit the information needed to reconstruct a quantum state. When the correlation matrix of the two-qubit channel is of full rank (rank three), the information of the qubit (in either a mixed state or a pure state) can be transmitted. The quantum discord of a channel with rank larger than or equal to three is always non-zero. Therefore, non-zero quantum discord is also necessary for our quantum information transmission protocol. The scheme may be useful in remote state tomography and remote state preparation.
TC 0
Z9 0
SN 1570-0755
PD FEB
PY 2013
VL 12
IS 2
BP 899
EP 906
DI 10.1007/s11128-012-0435-2
UT WOS:000313370000018
ER

PT J
AU Wang, XT
Byrd, M
Jacobs, K
AF Wang, Xiaoting
Byrd, Mark
Jacobs, Kurt
TI Numerical method for finding decoherence-free subspaces and its applications
SO PHYSICAL REVIEW A
AB In this work, inspired by the study of semidefinite programming for block-diagonalizing matrix *-algebras, we propose an algorithm that can find the algebraic structure of decoherence-free subspaces (DFS's) for a given noisy quantum channel. We prove that this algorithm will work for all cases with probability 1, and it is more efficient than the algorithm proposed by J. A. Holbrook, D. W. Kribs, and R. Laflamme, [Quantum. Inf. Proc. 80, 381 (2003)]. In fact, our results reveal that this previous algorithm only works for special cases. As an application, we discuss how this method can be applied to increase the efficiency of an optimization procedure for finding an approximate DFS. DOI: 10.1103/PhysRevA.87.012338
TC 0
Z9 0
SN 1050-2947
PD JAN 31
PY 2013
VL 87
IS 1
AR 012338
DI 10.1103/PhysRevA.87.012338
UT WOS:000314333500005
ER

PT J
AU Gao, Y
Lee, H
AF Gao, Yang
Lee, Hwang
TI Generalized limits for parameter sensitivity via quantum Ziv-Zakai bound
SO JOURNAL OF PHYSICS A-MATHEMATICAL AND THEORETICAL
AB We study the generalized limit for parameter sensitivity in quantum estimation theory considering the effects of repeated and adaptive measurements. Based on the quantum Ziv-Zakai bound, we derive some lower bounds for parameter sensitivity when the Hamiltonian of a system is unbounded and when the adaptive measurements are implemented on the system. We also prove that the parameter sensitivity is bounded by the limit of the minimum detectable parameter. In particular, we examine several known states in quantum phase estimation with non-interacting photons and show that they cannot perform better than the Heisenberg limit in a much simpler way with our result.
TC 2
Z9 2
SN 1751-8113
PD OCT 19
PY 2012
VL 45
IS 41
AR 415306
DI 10.1088/1751-8113/45/41/415306
UT WOS:000309550400013
ER

PT J
AU Horrom, T
Singh, R
Dowling, JP
Mikhailov, EE
AF Horrom, Travis
Singh, Robinjeet
Dowling, Jonathan P.
Mikhailov, Eugeniy E.
TI Quantum-enhanced magnetometer with low-frequency squeezing
SO PHYSICAL REVIEW A
AB We report the demonstration of a magnetometer with noise-floor reduction below the shot-noise level. This magnetometer, based on a nonlinear magneto-optical rotation effect, is enhanced by the injection of a squeezed vacuum state into its input. The noise spectrum shows squeezed noise reduction of about 2 +/- 0.35 dB spanning from close to 100 Hz to several megahertz. We also report on the observation of two different regimes of operation of such a magnetometer: one in which the detection noise is limited by the quantum noise of the light probe only, and one in which we see additional noise originating from laser noise which is rotated into the vacuum polarization.
TC 2
Z9 2
SN 1050-2947
PD AUG 3
PY 2012
VL 86
IS 2
AR 023803
DI 10.1103/PhysRevA.86.023803
UT WOS:000307125600008
ER

PT J
AU Boyd, RW
Dowling, JP
AF Boyd, Robert W.
Dowling, Jonathan P.
TI Quantum lithography: status of the field
SO QUANTUM INFORMATION PROCESSING
AB This contribution provides an analysis of progress in the field of quantum lithography. We review the conceptual foundations of this idea and the status of research aimed at implementing this idea in the laboratory. The selection of a highly sensitive recording material that functions by means of multiphoton absorption seems crucial to the success of the proposal of quantum lithography. This review thus devotes considerable attention to these materials considerations.
TC 2
Z9 2
SN 1570-0755
PD AUG
PY 2012
VL 11
IS 4
SI SI
BP 891
EP 901
DI 10.1007/s11128-011-0253-y
UT WOS:000305530200002
ER

PT J
AU Howell, JC
Anisimov, PM
Dowling, JP
Boyd, RW
AF Howell, John C.
Anisimov, Petr M.
Dowling, Jonathan P.
Boyd, Robert W.
TI Single and biphoton imaging and high dimensional quantum communication
SO QUANTUM INFORMATION PROCESSING
AB Here, we present recent developments in the field of quantum imaging focusing on the high dimensionality aspects of single and biphoton imaging. We discuss some systems that have a "quantum advantage" over classical counterparts. We highlight some recent experiments in single-photon image discrimination, large alphabet quantum key distribution and image buffering.
TC 0
Z9 0
SN 1570-0755
PD AUG
PY 2012
VL 11
IS 4
SI SI
BP 925
EP 948
DI 10.1007/s11128-011-0299-x
UT WOS:000305530200004
ER

PT J
AU Jiang, KB
Brignac, CJ
Weng, Y
Kim, MB
Lee, H
Dowling, JP
AF Jiang, Kebei
Brignac, Chase J.
Weng, Yi
Kim, Moochan B.
Lee, Hwang
Dowling, Jonathan P.
TI Strategies for choosing path-entangled number states for optimal robust quantum-optical metrology in the presence of loss
SO PHYSICAL REVIEW A
AB To acquire the best path-entangled photon Fock states for robust quantum-optical metrology with parity detection, we calculate phase information from a lossy interferometer by using twin entangled Fock states. We show that (a) when loss is less than 50% twin entangled Fock states with large photon number difference give higher visibility, while when loss is higher than 50%, the ones with less photon number difference give higher visibility; and (b) twin entangled Fock states with large photon number difference give sub-shot-noise limit sensitivity for phase detection in a lossy environment. This result provides a reference on what particular path-entangled Fock states are useful for real world metrology applications.
TC 0
Z9 0
SN 1050-2947
PD JUL 19
PY 2012
VL 86
IS 1
AR 013826
DI 10.1103/PhysRevA.86.013826
UT WOS:000306543200006
ER

PT J
AU Brown, KL
Horsman, C
Kendon, V
Munro, WJ
AF Brown, Katherine L.
Horsman, Clare
Kendon, Viv
Munro, William J.
TI Layer-by-layer generation of cluster states
SO PHYSICAL REVIEW A
AB Cluster states can be used to perform measurement-based quantum computation. The cluster state is a useful resource, because once it has been generated only local operations and measurements are needed to perform universal quantum computation. In this paper, we explore techniques for quickly and deterministically building a cluster state. In particular, we consider generating cluster states on a qubus quantum computer, a computational architecture which uses a continuous variable ancilla to generate interactions between qubits. We explore several techniques for building the cluster, with the number of operations required depending on whether we allow the ability to destroy previously created controlled-phase links between qubits. In the case where we cannot destroy these links, we show how to create an n x m cluster using just 3nm - 2n - inverted right perpendicular3m/2inverted left perpendicular + 3 operations. This gives more than a factor of 2 savings over a naive method. Further savings can be obtained if we include the ability to destroy links, in which case we only need inverted right perpendicular1/3(8nm - 4n - 4m - 8)inverted left perpendicular operations. Unfortunately, the latter scheme is more complicated so choosing the correct order to interact the qubits is considerably more difficult. A halfway scheme, that keeps a modular generation but saves additional operations over never destroying links requires only 3nm - 2n - 2m + 4 operations. The first scheme and the last scheme are the most practical for building a cluster state because they split up the generation into the repetition of simple sections.
RI
Munro, William A-8453-2011 
TC 0
Z9 0
SN 1050-2947
PD MAY 7
PY 2012
VL 85
IS 5
AR 052305
DI 10.1103/PhysRevA.85.052305
UT WOS:000303651200004
ER

PT J
AU Richardson, CD
Dowling, JP
AF Richardson, Chris D.
Dowling, Jonathan P.
TI POPPER'S THOUGHT EXPERIMENT REINVESTIGATED
SO INTERNATIONAL JOURNAL OF QUANTUM INFORMATION
AB Popper's original thought experiment probed some fundamental and subtle rules of quantum mechanics. He claimed that quantum mechanics was incomplete and devised an experiment to prove it. Two experiments have directly and indirectly tested Popper's hypothesis, and they provide some evidence that Popper's prediction may have been correct. The equations governing these two experiments and Popper's thought experiment will be derived from basic quantum principles. The experimental constants will be inputted and it will show that the two experiments reinforce each other and agree completely with quantum theory.
TC 0
Z9 0
SN 0219-7499
PD APR
PY 2012
VL 10
IS 3
AR 1250033
DI 10.1142/S0219749912500335
UT WOS:000304611800008
ER

PT J
AU Bardhan, BR
Anisimov, PM
Gupta, MK
Brown, KL
Jones, NC
Lee, H
Dowling, JP
AF Bardhan, Bhaskar Roy
Anisimov, Petr M.
Gupta, Manish K.
Brown, Katherine L.
Jones, N. Cody
Lee, Hwang
Dowling, Jonathan P.
TI Dynamical decoupling in optical fibers: Preserving polarization qubits from birefringent dephasing
SO PHYSICAL REVIEW A
AB One of the major challenges in quantum computation has been to preserve the coherence of a quantum system against dephasing effects of the environment. The information stored in photon polarization, for example, is quickly lost due to such dephasing, and it is crucial to preserve the input states when one tries to transmit quantum information encoded in the photons through a communication channel. We propose a dynamical decoupling sequence, to protect photonic qubits from dephasing, by integrating wave plates into optical fiber at prescribed locations. We simulate random birefringent noise along realistic lengths of optical fiber and study preservation of polarization qubits through such fibers enhanced with Carr-Purcell-Meiboom-Gill (CPMG) dynamical decoupling. This technique can maintain photonic qubit coherence at high fidelity, making a step toward achieving scalable and useful quantum communication with photonic qubits.
TC 0
Z9 0
SN 1050-2947
PD FEB 28
PY 2012
VL 85
IS 2
AR 022340
DI 10.1103/PhysRevA.85.022340
UT WOS:000300827200001
ER

PT J
AU Thanvanthri, S
Kapale, KT
Dowling, JP
AF Thanvanthri, Sulakshana
Kapale, Kishore T.
Dowling, Jonathan P.
TI Ultra-stable matter-wave gyroscopy with counter-rotating vortex superpositions in Bose-Einstein condensates
SO JOURNAL OF MODERN OPTICS
AB Matter-wave interferometers are, in principle, orders of magnitude more sensitive than their optical counterparts. Nevertheless, creation of matter-wave currents to achieve such a sensitivity is a continuing challenge. Here, we propose the use of Optical-Angular-Momentum (OAM) induced vortex superpositions in Bose-Einstein condensates (BECs) as an alternative to other atom interferometers for gyroscopy. The coherent superposition of two counter-rotating vortex states of a trapped condensate leads to an interference pattern that rotates by an angle proportional to the angular velocity of the rotating trap - in accordance with the Sagnac effect. We show that the rotation rate can be easily read out, and that the device is highly stable. The signal-to-noise ratio and sensitivity of the scheme are also estimated.
TC 0
Z9 0
SN 0950-0340
PY 2012
VL 59
IS 13
BP 1180
EP 1185
DI 10.1080/09500340.2012.702228
UT WOS:000307873300009
ER

PT J
AU O'Brien, C
Anisimov, PM
Rostovtsev, Y
Kocharovskaya, O
AF O'Brien, Chris
Anisimov, Petr M.
Rostovtsev, Yuri
Kocharovskaya, Olga
TI Coherent control of refractive index in far-detuned Lambda systems
SO PHYSICAL REVIEW A
AB Enhancement and control of the index of refraction in a mixture of two three-level atomic species that form a pair of far-detuned Lambda schemes under two-photon resonance has been studied. We employ the density-matrix approach to properly take population relaxation into account and to describe the interaction of each Lambda system with the electromagnetic fields. Both Lambda systems are driven by a corresponding far-detuned coherent field at one atomic transition and are probed by the same weak field. In the dressed-state basis, it represents a superposition of effective two-level subsystems with the positions, widths, and amplitudes of the resonances controlled by the driving fields and allows for efficient control of the susceptibility of the total system; leading to refractive index (RI) enhancement with vanishing absorption in the absence of amplification. We analyze the experimental implementation of such a system in a cell of Rb atoms with a natural abundance of isotopes. An upper limit estimate of the RI enhancement is obtained.
RI
O'Brien, Christopher C-8232-2013 
TC 3
Z9 3
SN 1050-2947
PD DEC 15
PY 2011
VL 84
IS 6
AR 063835
DI 10.1103/PhysRevA.84.063835
UT WOS:000298113500005
ER

PT J
AU Sete, EA
Dorfman, KE
Dowling, JP
AF Sete, Eyob A.
Dorfman, Konstantin E.
Dowling, Jonathan P.
TI Phase-controlled entanglement in a quantum-beat laser: application to quantum lithography
SO JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS
AB We study entanglement generation and control in a quantum-beat laser coupled to a two-mode squeezed vacuum reservoir. We show that the generated entanglement is robust against cavity losses and environmental decoherence and can be controlled by tuning the phases of the microwave and the squeezed input fields. Moreover, we discuss two-photon correlations, absorption and implementations in quantum optical lithography.
RI
Sete, Eyob E-7813-2012 
TC 3
Z9 3
SN 0953-4075
PD NOV 28
PY 2011
VL 44
IS 22
AR 225504
DI 10.1088/0953-4075/44/22/225504
UT WOS:000296796600017
ER

PT J
AU Wang, XT
Vinjanampathy, S
Strauch, FW
Jacobs, K
AF Wang, Xiaoting
Vinjanampathy, Sai
Strauch, Frederick W.
Jacobs, Kurt
TI Ultraefficient Cooling of Resonators: Beating Sideband Cooling with Quantum Control
SO PHYSICAL REVIEW LETTERS
AB The present state of the art in cooling mechanical resonators is a version of sideband cooling. Here we present a method that uses the same configuration as sideband cooling-coupling the resonator to be cooled to a second microwave (or optical) auxiliary resonator-but will cool significantly colder. This is achieved by varying the strength of the coupling between the two resonators over a time on the order of the period of the mechanical resonator. As part of our analysis, we also obtain a method for fast, high-fidelity quantum information transfer between resonators.
RI
Jacobs, Kurt E-7049-2011 
TC 7
Z9 7
SN 0031-9007
PD OCT 19
PY 2011
VL 107
IS 17
AR 177204
DI 10.1103/PhysRevLett.107.177204
UT WOS:000296984100017
ER

PT J
AU Anisimov, PM
Dowling, JP
Sanders, BC
AF Anisimov, Petr M.
Dowling, Jonathan P.
Sanders, Barry C.
TI Objectively Discerning Autler-Townes Splitting from Electromagnetically Induced Transparency
SO PHYSICAL REVIEW LETTERS
AB Autler-Townes splitting (ATS) and electromagnetically induced transparency (EIT) both yield transparency in an absorption profile, but only EIT yields strong transparency for a weak pump field due to Fano interference. Empirically discriminating EIT from ATS is important but so far has been subjective. We introduce an objective method, based on Akaike's information criterion, to test ATS vs EIT from experimental data for three-level atomic systems and determine which pertains. We apply our method to a recently reported induced-transparency experiment in superconducting-circuit quantum electrodynamics.
RI
Sanders, Barry A-3891-2008 
TC 13
Z9 13
SN 0031-9007
PD OCT 12
PY 2011
VL 107
IS 16
AR 163604
DI 10.1103/PhysRevLett.107.163604
UT WOS:000296370800003
ER

PT J
AU Seshadreesan, KP
Anisimov, PM
Lee, H
Dowling, JP
AF Seshadreesan, Kaushik P.
Anisimov, Petr M.
Lee, Hwang
Dowling, Jonathan P.
TI Parity detection achieves the Heisenberg limit in interferometry with coherent mixed with squeezed vacuum light
SO NEW JOURNAL OF PHYSICS
AB The interference between coherent and squeezed vacuum light effectively produces path entangled N00N states with very high fidelities. We show that the phase sensitivity of the above interferometric scheme with parity detection saturates the quantum Cramer-Rao bound, which reaches the Heisenberg limit when the coherent and squeezed vacuum light are mixed in roughly equal proportions. For the same interferometric scheme, we draw a detailed comparison between parity detection and a symmetric-logarithmic-derivative-based detection scheme suggested by Ono and Hofmann.
TC 5
Z9 5
SN 1367-2630
PD AUG 24
PY 2011
VL 13
AR 083026
DI 10.1088/1367-2630/13/8/083026
UT WOS:000294672800002
ER

PT J
AU Seshadreesan, KP
Ghosh, S
AF Seshadreesan, Kaushik P.
Ghosh, Sibasish
TI Constancy of maximal nonlocal probability in Hardy's nonlocality test for bipartite quantum systems
SO JOURNAL OF PHYSICS A-MATHEMATICAL AND THEORETICAL
AB We give the generic form of the entangled states of a system of two spin-1 (and two spin-3/2) particles and the appropriate set of spin observables that together exhibit maximum nonlocality under Hardy's nonlocality test. We show the maximum nonlocality to be 0.090 17 just as in the case of two spin-1/2 particles. We conjecture that this result holds good for a system of two spin-j particles for all values of j.
TC 2
Z9 2
SN 1751-8113
PD AUG 5
PY 2011
VL 44
IS 31
AR 315305
DI 10.1088/1751-8113/44/31/315305
UT WOS:000292736300013
ER

PT J
AU Stack, D
Elgin, J
Anisimov, PM
Metcalf, H
AF Stack, Daniel
Elgin, John
Anisimov, Petr M.
Metcalf, Harold
TI Numerical studies of optical forces from adiabatic rapid passage
SO PHYSICAL REVIEW A
AB We present a numerical study of the properties of optical forces on moving atoms derived from purely stimulated processes produced by multiple adiabatic rapid-passage sequences. The optical Bloch equations are solved for a carefully timed sequence of frequency-swept pulses that can produce a force much larger than the ordinary radiative force. We describe the effects of the sweep range, peak intensity, sweep direction, number of pulses, atomic velocity, and spontaneous emission. Since the momentum of thermal atoms is much larger than that transferred by a single absorption-stimulated emission cycle, multiple repetitions are needed to make a significant velocity change.
TC 1
Z9 1
SN 1050-2947
PD JUL 25
PY 2011
VL 84
IS 1
AR 013420
DI 10.1103/PhysRevA.84.013420
UT WOS:000293126500012
ER

PT J
AU Jacobs, K
Finn, J
Vinjanampathy, S
AF Jacobs, Kurt
Finn, Justin
Vinjanampathy, Sai
TI Real-time feedback control of a mesoscopic superposition
SO PHYSICAL REVIEW A
AB We show that continuous real-time feedback can be used to track, control, and protect a mesoscopic superposition of two spatially separated wave packets. The feedback protocol is enabled by an approximate state estimator and requires two continuous measurements, performed simultaneously. For nanomechanical and superconducting resonators, both measurements can be implemented by coupling the resonators to superconducting qubits.
RI
Jacobs, Kurt E-7049-2011 
TC 1
Z9 1
SN 1050-2947
PD APR 20
PY 2011
VL 83
IS 4
AR 041801
DI 10.1103/PhysRevA.83.041801
UT WOS:000290104500001
ER

PT J
AU Yurtsever, U
AF Yurtsever, Ulvi
TI MODELING LOSSY PROPAGATION OF NON-CLASSICAL LIGHT
SO INTERNATIONAL JOURNAL OF QUANTUM INFORMATION
AB The lossy propagation law (generalization of Lambert-Beer's law for classical radiation loss) for non-classical, dual-mode entangled states is derived from first principles, using an infinite-series of beam splitters to model continuous photon loss. This model is general enough to accommodate stray-photon noise along the propagation, as well as amplitude attenuation. An explicit analytical expression for the density matrix as a function of propagation distance is obtained for completely general input states with bounded photon number in each mode. The result is analyzed numerically for various examples of input states. For N00N state input, the loss of coherence and entanglement is super exponential, as predicted by a number of previous studies. However, for generic input states, where the coefficients are generated randomly, the decay of coherence is very different; in fact no worse than the classical Beer-Lambert law. More surprisingly, there is a plateau at a mid-range interval in propagation distance where the loss is in fact sub-classical, following which it resumes the classical rate. The qualitative behavior of the decay of entanglement for two-mode propagation is also analyzed numerically for ensembles of random states using the behavior of negativity as a function of propagation distance.
TC 0
Z9 0
SN 0219-7499
PD MAR
PY 2011
VL 9
IS 2
BP 739
EP 750
DI 10.1142/S0219749911006806
UT WOS:000290857800009
ER

PT J
AU Chiruvelli, A
Lee, H
AF Chiruvelli, Aravind
Lee, Hwang
TI Parity measurements in quantum optical metrology
SO JOURNAL OF MODERN OPTICS
AB We investigate the utility of parity detection to achieve Heisenberg-limited phase estimation for optical interferometry. We consider the parity detection with several input states that have been shown to exhibit subshot-noise interferometry with their respective detection schemes. We show that with parity detection, all these states achieve the sub-shot-noise limited phase uncertainty. Thus making the parity detection a unified detection strategy for quantum optical metrology. We also consider quantum states that are a combination of a NOON state and a dual-Fock state, which gives a great deal of freedom in the preparation of the input state, and is found to surpass the shot-noise limit.
TC 5
Z9 5
SN 0950-0340
PY 2011
VL 58
IS 11
BP 945
EP 953
DI 10.1080/09500340.2011.585251
UT WOS:000294681500008
ER

PT J
AU Plick, WN
Anisimov, PM
Dowling, JP
Lee, H
Agarwal, GS
AF Plick, William N.
Anisimov, Petr M.
Dowling, Jonathan P.
Lee, Hwang
Agarwal, Girish S.
TI Parity detection in quantum optical metrology without number-resolving detectors
SO NEW JOURNAL OF PHYSICS
AB We present a method for directly obtaining the parity of a Gaussian state of light without recourse to photon-number counting. The scheme uses only a simple balanced homodyne technique and intensity correlation. Thus interferometric schemes utilizing coherent or squeezed light and parity detection may be practically implemented for an arbitrary photon flux. Specifically, we investigate a two-mode, squeezed light, Mach-Zehnder interferometer and show how the parity of the output state may be obtained. We also show that the detection may be described independently of the parity operator and that this 'parity-by-proxy' measurement has the same signal as traditional parity.
TC 7
Z9 7
SN 1367-2630
PD NOV 11
PY 2010
VL 12
AR 113025
DI 10.1088/1367-2630/12/11/113025
UT WOS:000284774100003
ER

PT J
AU Yurtsever, U
AF Yurtsever, Ulvi
TI Fundamental limits on the speed of evolution of quantum states
SO PHYSICA SCRIPTA
AB This paper reports on some new inequalities of Margolus-Levitin-Mandelstam-Tamm type involving the speed of quantum evolution between two orthogonal pure states. The clear determinant of the qualitative behavior of this time scale is the statistics of the energy spectrum.
TC 2
Z9 2
SN 0031-8949
PD SEP
PY 2010
VL 82
IS 3
AR 035008
DI 10.1088/0031-8949/82/03/035008
UT WOS:000281537200009
ER

PT J
AU Anisimov, PM
Lum, DJ
McCracken, SB
Lee, H
Dowling, JP
AF Anisimov, Petr M.
Lum, Daniel J.
McCracken, S. Blane
Lee, Hwang
Dowling, Jonathan P.
TI An invisible quantum tripwire
SO NEW JOURNAL OF PHYSICS
AB We present here a quantum tripwire, which is a quantum optical interrogation technique capable of detecting an intrusion with very low probability of the tripwire being revealed to the intruder. Our scheme combines interaction-free measurement (IFM) with the quantum Zeno effect in order to interrogate the presence of the intruder without interaction. The tripwire exploits a curious nonlinear behaviour of the quantum Zeno effect we discovered, which occurs in a lossy system. We also employ a statistical hypothesis testing protocol, allowing us to calculate a confidence level of IFM after a given number of trials. As a result, our quantum intruder alert system is robust against photon loss and dephasing under realistic atmospheric conditions and its design minimizes the probabilities of false positives and false negatives as well as the probability of becoming visible to the intruder.
TC 4
Z9 4
SN 1367-2630
PD AUG 6
PY 2010
VL 12
AR 083012
DI 10.1088/1367-2630/12/8/083012
UT WOS:000281278900001
ER

PT J
AU Plick, WN
Dowling, JP
Agarwal, GS
AF Plick, William N.
Dowling, Jonathan P.
Agarwal, Girish S.
TI Coherent-light-boosted, sub-shot noise, quantum interferometry
SO NEW JOURNAL OF PHYSICS
AB We present in this paper a new scheme for optical interferometry. We utilize coherent-beam-stimulated two-mode squeezed light, which interacts with a phase shifter and is then squeezed again before detection. Our theoretical device has the potential to reach far below the shot-noise limit in phase sensitivity. This new proposal avoids the pitfalls of other setups, such as difficulty in creating the required resource. Furthermore, our scheme requires no complicated detection protocol, relying instead only on simple intensity measurement. Also, bright, coherent sources 'boost' squeezed light, creating a very sensitive device. This hybrid scheme relies on no unknown components and can be constructed with current technology. In this paper, we present our analysis of this relatively straightforward device, using the operator propagation method. We derive the phase sensitivity and provide a simple numerical example of the power of our new proposal. Sensitivity to unknown phase shifts scales as a shot-noise-limited Mach-Zehnder interferometer, multiplied by a sub-Heisenberg contribution from the squeezed light.
TC 6
Z9 6
SN 1367-2630
PD AUG 6
PY 2010
VL 12
AR 083014
DI 10.1088/1367-2630/12/8/083014
UT WOS:000281278900003
ER

PT J
AU Gao, Y
Anisimov, PM
Wildfeuer, CF
Luine, J
Lee, H
Dowling, JP
AF Gao, Yang
Anisimov, Petr M.
Wildfeuer, Christoph F.
Luine, Jerome
Lee, Hwang
Dowling, Jonathan P.
TI Super-resolution at the shot-noise limit with coherent states and photon-number-resolving detectors
SO JOURNAL OF THE OPTICAL SOCIETY OF AMERICA B-OPTICAL PHYSICS
AB There has been much recent interest in quantum optical interferometry for applications to metrology, subwavelength imaging, and remote sensing such as in quantum laser radar (LADAR). For quantum LADAR, atmospheric absorption rapidly degrades any quantum state of light, so that for high-photon loss the optimal strategy is to transmit coherent states of light, which suffer no worse loss than the Beer law for classical optical attenuation, and which provides sensitivity at the shot-noise limit. We show that coherent light coupled with photon-number-resolving detectors can provide a super-resolution much below the Rayleigh diffraction limit, with sensitivity no worse than shot noise in terms of the detected photon power. (C) 2010 Optical Society of America
TC 8
Z9 8
SN 0740-3224
PD JUN
PY 2010
VL 27
IS 6
BP A170
EP A174
UT WOS:000278433500047
ER

PT J
AU Jacobs, K
AF Jacobs, Kurt
TI Wave-function Monte Carlo method for simulating conditional master equations
SO PHYSICAL REVIEW A
AB Wave-function Monte Carlo methods are an important tool for simulating quantum systems, but the standard method cannot be used to simulate decoherence in continuously measured systems. Here I present a Monte Carlo method for such systems. This was used to perform the simulations of a continuously measured nanoresonator in [Phys. Rev. Lett. 102, 057208 (2009)].
RI
Jacobs, Kurt E-7049-2011 
TC 3
Z9 3
SN 1050-2947
PD APR
PY 2010
VL 81
IS 4
AR 042106
DI 10.1103/PhysRevA.81.042106
UT WOS:000277227300024
ER

PT J
AU Pearlman, AJ
Ling, A
Goldschmidt, EA
Wildfeuer, CF
Fan, J
Migdall, A
AF Pearlman, A. J.
Ling, A.
Goldschmidt, E. A.
Wildfeuer, C. F.
Fan, J.
Migdall, A.
TI Enhancing image contrast using coherent states and photon number resolving detectors
SO OPTICS EXPRESS
AB We experimentally map the transverse profile of diffraction-limited beams using photon-number-resolving detectors. We observe strong compression of diffracted beam profiles for high detected photon number. This effect leads to higher contrast than a conventional irradiance profile between two Airy disk-beams separated by the Rayleigh criterion. (C) 2010 Optical Society of America
TC 5
Z9 5
SN 1094-4087
PD MAR 15
PY 2010
VL 18
IS 6
BP 6033
EP 6039
UT WOS:000276002500073
ER

PT J
AU Anisimov, PM
Raterman, GM
Chiruvelli, A
Plick, WN
Huver, SD
Lee, H
Dowling, JP
AF Anisimov, Petr M.
Raterman, Gretchen M.
Chiruvelli, Aravind
Plick, William N.
Huver, Sean D.
Lee, Hwang
Dowling, Jonathan P.
TI Quantum Metrology with Two-Mode Squeezed Vacuum: Parity Detection Beats the Heisenberg Limit
SO PHYSICAL REVIEW LETTERS
AB We study the sensitivity and resolution of phase measurement in a Mach-Zehnder interferometer with two-mode squeezed vacuum ((n) over bar photons on average). We show that superresolution and sub-Heisenberg sensitivity is obtained with parity detection. In particular, in our setup, dependence of the signal on the phase evolves (n) over bar times faster than in traditional schemes, and uncertainty in the phase estimation is better than 1/(n) over bar, and we saturate the quantum Cramer-Rao bound.
TC 33
Z9 33
SN 0031-9007
PD MAR 12
PY 2010
VL 104
IS 10
AR 103602
DI 10.1103/PhysRevLett.104.103602
UT WOS:000275543500020
ER

PT J
AU Lee, TW
Huver, SD
Lee, H
Kaplan, L
McCracken, SB
Min, CJ
Uskov, DB
Wildfeuer, CF
Veronis, G
Dowling, JP
AF Lee, Tae-Woo
Huver, Sean D.
Lee, Hwang
Kaplan, Lev
McCracken, Steven B.
Min, Changjun
Uskov, Dmitry B.
Wildfeuer, Christoph F.
Veronis, Georgios
Dowling, Jonathan P.
TI Optimization of quantum interferometric metrological sensors in the presence of photon loss
SO PHYSICAL REVIEW A
AB We optimize two-mode entangled number states of light in the presence of loss in order to maximize the extraction of the available phase information in an interferometer. Our approach optimizes over the entire available input Hilbert space with no constraints, other than fixed total initial photon number. We optimize to maximize the Fisher information, which is equivalent to minimizing the phase uncertainty. We find that in the limit of zero loss, the optimal state is the maximally path-entangled (so-called N00N) state, for small loss, the optimal state gradually deviates from the N00N state, and in the limit of large loss, the optimal state converges to a generalized two-mode coherent state, with a finite total number of photons. The results provide a general protocol for optimizing the performance of a quantum optical interferometer in the presence of photon loss, with applications to quantum imaging, metrology, sensing, and information processing.
RI
min, changjun E-6699-2011 
TC 18
Z9 18
SN 1050-2947
PD DEC
PY 2009
VL 80
IS 6
AR 063803
DI 10.1103/PhysRevA.80.063803
UT WOS:000273233800154
ER

PT J
AU Plick, WN
Wildfeuer, CF
Anisimov, PM
Dowling, JP
AF Plick, William N.
Wildfeuer, Christoph F.
Anisimov, Petr M.
Dowling, Jonathan P.
TI Optimizing the multiphoton absorption properties of maximally path-entangled number states
SO PHYSICAL REVIEW A
AB In this paper we examine the N-photon absorption properties of maximally path-entangled number states (N00N states). We consider two cases. The first involves the N-photon absorption properties of the ideal N00N state, one that does not include spectral information. We study how the N-photon absorption probability of this state scales with N, confirming results presented by others in a previous paper by a different method. We compare this to the absorption probability of various other states. The second case is that of two-photon absorption for an N=2 N00N state generated from a type-II spontaneous down-conversion event. In this situation we find that the absorption probability is both better than analogous coherent light (due to frequency entanglement) and highly dependent on the optical setup. We show that the poor production rates of quantum states of light may be partially mitigated by adjusting the spectral parameters to improve their two-photon absorption rates. This work has application to quantum imaging, particularly quantum lithography, where the N- photon absorbing process in the lithographic resist must be optimized for practical applications.
TC 3
Z9 3
SN 1050-2947
PD DEC
PY 2009
VL 80
IS 6
AR 063825
DI 10.1103/PhysRevA.80.063825
UT WOS:000273233800176
ER

PT J
AU Cable, H
Vyas, R
Singh, S
Dowling, JP
AF Cable, Hugo
Vyas, Reeta
Singh, Surendra
Dowling, Jonathan P.
TI An optical parametric oscillator as a high-flux source of two-mode light for quantum lithography
SO NEW JOURNAL OF PHYSICS
AB We investigate the use of an optical parametric oscillator (OPO), which can generate relatively high-flux light with strong non-classical features, as a source for quantum lithography. This builds on the proposal of Boto et al (2000 Phys. Rev. Lett. 85 2733), for etching simple patterns on multi-photon absorbing materials with sub-Rayleigh resolution, using two-mode entangled states of light. We consider an OPO with two down-converted modes that share the same frequency but differ in field polarization or direction of propagation, and derive analytical expressions for the multi-photon absorption rates when the OPO is operated below, near and above its threshold. Because of strong non-classical correlations between the two modes of the OPO, the interference patterns resulting from the superposition of the two modes are characterized by an effective wavelength that is half of their actual wavelength. The interference patterns resulting when the two modes of the OPO are used for etching are also characterized by an effective wavelength half that for the illuminating modes. We compare our results with those for the case of a high-gain optical amplifier source and discuss the relative merit of the OPO.
RI
Cable, Hugo C-2346-2011 
TC 2
Z9 2
SN 1367-2630
PD NOV 30
PY 2009
VL 11
AR 113055
DI 10.1088/1367-2630/11/11/113055
UT WOS:000272153400006
ER

PT J
AU Wildfeuer, CF
Pearlman, AJ
Chen, J
Fan, JY
Migdall, A
Dowling, JP
AF Wildfeuer, Christoph F.
Pearlman, Aaron J.
Chen, Jun
Fan, Jingyun
Migdall, Alan
Dowling, Jonathan P.
TI Resolution and sensitivity of a Fabry-Perot interferometer with a photon-number-resolving detector
SO PHYSICAL REVIEW A
AB With photon-number resolving detectors, we show compression of interference fringes with increasing photon numbers for a Fabry-Perot interferometer. This feature provides a higher precision in determining the position of the interference maxima compared to a classical detection strategy. We also theoretically show supersensitivity if N-photon states are sent into the interferometer and a photon-number resolving measurement is performed.
TC 13
Z9 13
SN 1050-2947
PD OCT
PY 2009
VL 80
IS 4
AR 043822
DI 10.1103/PhysRevA.80.043822
UT WOS:000271351000178
ER

PT J
AU Wilde, MM
AF Wilde, Mark M.
TI Can classical noise enhance quantum transmission?
SO JOURNAL OF PHYSICS A-MATHEMATICAL AND THEORETICAL
AB A modified quantum teleportation protocol broadens the scope of the classical forbidden-interval theorems for stochastic resonance. The fidelity measures performance of quantum communication. The sender encodes the two classical bits for quantum teleportation as weak bipolar subthreshold signals and sends them over a noisy classical channel. Two forbidden-interval theorems provide a necessary and sufficient condition for the occurrence of the nonmonotone stochastic resonance effect in the fidelity of quantum teleportation. The condition is that the noise mean must fall outside a forbidden interval related to the detection threshold and signal value. An optimal amount of classical noise benefits quantum communication when the sender transmits weak signals, the receiver detects with a high threshold and the noise mean lies outside the forbidden interval. Theorems and simulations demonstrate that both finite-variance and infinite-variance noise benefit the fidelity of quantum teleportation.
TC 1
Z9 1
SN 1751-8113
PD AUG 14
PY 2009
VL 42
IS 32
AR 325301
DI 10.1088/1751-8113/42/32/325301
UT WOS:000268342600013
ER

PT J
AU Jacobs, K
Landahl, AJ
AF Jacobs, Kurt
Landahl, Andrew J.
TI Engineering Giant Nonlinearities in Quantum Nanosystems
SO PHYSICAL REVIEW LETTERS
AB We describe a method to engineer giant nonlinearities in, and probes to measure nonlinear observables of, mesoscopic quantum resonators. This involves tailoring the Hamiltonian of a simple auxiliary system perturbatively coupled to the resonator, and has the potential to engineer a wide range of nonlinearities to high accuracy. We give a number of explicit examples, including a readily realizable two-qubit auxiliary system that creates an x(4) potential and a chi((3)) (Kerr) nonlinearity, valid to fifth order in the perturbative coupling.
RI
Jacobs, Kurt E-7049-2011 
TC 15
Z9 15
SN 0031-9007
PD AUG 7
PY 2009
VL 103
IS 6
AR 067201
DI 10.1103/PhysRevLett.103.067201
UT WOS:000268809300065
ER

PT J
AU Uskov, DB
Kaplan, L
Smith, AM
Huver, SD
Dowling, JP
AF Uskov, Dmitry B.
Kaplan, Lev
Smith, A. Matthew
Huver, Sean D.
Dowling, Jonathan P.
TI Maximal success probabilities of linear-optical quantum gates
SO PHYSICAL REVIEW A
AB Numerical optimization is used to design linear-optical devices that implement a desired quantum gate with perfect fidelity, while maximizing the success rate. For the two-qubit controlled-sign [or controlled NOT (CNOT)] gate, we provide numerical evidence that the maximum success rate is S=2/27 using two unentangled ancilla resources; interestingly, additional ancilla resources do not increase the success rate. For the three-qubit Toffoli gate, we show that perfect fidelity is obtained with only three unentangled ancilla photons-less than in any existing scheme-with a maximum S=0.003 40. This compares well to S=(2/27)(2)/2 approximate to 0.002 74, obtainable by combining two CNOT gates and a passive quantum filter [T. C. Ralph, K. J. Resch, and A. Gilchrist, Phys. Rev. A 75, 022313 (2007)]. The general optimization approach can easily be applied to other areas of interest, such as quantum error correction, cryptography, and metrology [M. M. Wilde and D. B. Uskov, Phys. Rev. A 79, 022305 (2009); G. A. Durkin and J. P. Dowling, Phys. Rev. Lett. 99, 070801 (2007)].
TC 13
Z9 13
SN 1050-2947
PD APR
PY 2009
VL 79
IS 4
AR 042326
DI 10.1103/PhysRevA.79.042326
UT WOS:000265946900058
ER

PT J
AU Jacobs, K
Tian, L
Finn, J
AF Jacobs, Kurt
Tian, Lin
Finn, Justin
TI Engineering Superposition States and Tailored Probes for Nanoresonators via Open-Loop Control
SO PHYSICAL REVIEW LETTERS
AB We show that a nanoresonator can be prepared in mesoscopic superposition states merely by monitoring a qubit coupled to the square of the resonator's position. This works for thermal initial states, and does not require a third-order nonlinearity. The required coupling can be generated using a simple open-loop control protocol, obtained with optimal control theory. We simulate the complete preparation process, including environmental noise. Our results indicate the power of open-loop control for state engineering and measurement in quantum nanosystems.
RI
Jacobs, Kurt E-7049-2011 
TC 13
Z9 13
SN 0031-9007
PD FEB 6
PY 2009
VL 102
IS 5
AR 057208
DI 10.1103/PhysRevLett.102.057208
UT WOS:000263166400061
ER

PT J
AU Wilde, MM
Uskov, DB
AF Wilde, Mark M.
Uskov, Dmitry B.
TI Linear-optical hyperentanglement-assisted quantum error-correcting code
SO PHYSICAL REVIEW A
AB We propose a linear-optical implementation of a hyperentanglement-assisted quantum error-correcting code. The code is hyperentanglement assisted because the shared entanglement resource is a photonic state hyperentangled in polarization and orbital angular momentum. It is possible to encode, decode, and diagnose channel errors using linear-optical techniques. The code corrects for polarization "flip" errors and is thus suitable only for a proof-of-principle experiment. The encoding and decoding circuits use a Knill-Laflamme-Milburn-like scheme for transforming polarization and orbital angular momentum photonic qubits. A numerical optimization algorithm finds a unit-fidelity encoding circuit that requires only three ancilla modes and has success probability equal to 0.0097.
TC 9
Z9 9
SN 1050-2947
PD FEB
PY 2009
VL 79
IS 2
AR 022305
DI 10.1103/PhysRevA.79.022305
UT WOS:000263815000050
ER

PT J
AU Huver, SD
Wildfeuer, CF
Dowling, JP
AF Huver, Sean D.
Wildfeuer, Christoph F.
Dowling, Jonathan P.
TI Entangled Fock states for robust quantum optical metrology, imaging, and sensing
SO PHYSICAL REVIEW A
AB We propose a class of path-entangled photon Fock states for robust quantum optical metrology, imaging, and sensing in the presence of loss. We model propagation loss with beam splitters and derive a reduced density-matrix formalism from which we examine how photon loss affects coherence. It is shown that particular entangled number states, which contain a special superposition of photons in both arms of a Mach-Zehnder interferometer, are resilient to environmental decoherence. We demonstrate an order of magnitude greater visibility with loss than possible with path-entangled parallel to N,0 >+parallel to 0,N > states. We also show that the effectiveness of a detection scheme is related to super-resolution visibility.
TC 45
Z9 45
SN 1050-2947
PD DEC
PY 2008
VL 78
IS 6
AR 063828
DI 10.1103/PhysRevA.78.063828
UT WOS:000262243500078
ER

PT J
AU Wildfeuer, CF
Dowling, JP
AF Wildfeuer, Christoph F.
Dowling, Jonathan P.
TI Strong violations of Bell-type inequalities for Werner-like states
SO PHYSICAL REVIEW A
AB We investigate the violation of Bell-type inequalities for two-qubit Werner-like states parametrized by the positive parameter 0 <= p <= 1. We use an unbalanced homodyne detection scheme to obtain the quantum mechanical probabilities. A violation of the Bell-Wigner and Janssens inequalities is obtained for a large range of the parameter p. The range given by these inequalities is greater than the one given by the Clauser-Horne inequality. The range in which a violation is attained actually coincides with the range where the Werner-like states are known to be nonseparable, i.e., for p > 1/3. However, the improvement over the Clauser-Horne inequality is achieved at the price of restricting the class of possible local hidden variable theories.
TC 2
Z9 2
SN 1050-2947
PD SEP
PY 2008
VL 78
IS 3
AR 032113
DI 10.1103/PhysRevA.78.032113
UT WOS:000259689400025
ER

PT J
AU Han, MX
Olson, SJ
Dowling, JP
AF Han, Muxin
Olson, S. Jay
Dowling, Jonathan P.
TI Generating entangled photons from the vacuum by accelerated measurements: Quantum-information theory and the Unruh-Davies effect
SO PHYSICAL REVIEW A
AB Building on the well-known Unruh-Davies effect, we examine the effects of projective measurements and quantum communications between accelerated and stationary observers. We find that the projective measurement by a uniformly accelerated observer can excite real particles from the vacuum in the inertial frame, even if no additional particles are created by the measurement process in the accelerating frame. Furthermore, we show that the particles created by this accelerating measurement can be highly entangled in the inertial frame, and it is also possible to use this process to generate even maximally entangled two-qubit states by a certain arrangement of measurements. As a by-product of our analysis, we also show that a single qubit of information can be perfectly transmitted from the accelerating observer to the inertial one. In principle, such an effect could be exploited in designing an entangled-state generator for quantum communication.
TC 6
Z9 6
SN 1050-2947
PD AUG
PY 2008
VL 78
IS 2
AR 022302
DI 10.1103/PhysRevA.78.022302
PN Part a
UT WOS:000259263400038
ER

PT J
AU Glasser, RT
Cable, H
Dowling, JP
De Martini, F
Sciarrino, F
Vitelli, C
AF Glasser, Ryan T.
Cable, Hugo
Dowling, Jonathan P.
De Martini, Francesco
Sciarrino, Fabio
Vitelli, Chiara
TI Entanglement-seeded, dual, optical parametric amplification: Applications to quantum imaging and metrology
SO PHYSICAL REVIEW A
AB The study of optical parametric amplifiers (OPAs) has been successful in describing and creating nonclassical light for use in fields such as quantum metrology and quantum lithography [Agarwal , J. Opt. Soc. Am. B 24, 2 (2007)]. In this paper we present the theory of an OPA scheme utilizing an entangled state input. The scheme involves two identical OPAs seeded with the maximally path-entangled vertical bar N00N > state (vertical bar 2,0 >+vertical bar 0,2 >)/root 2. The stimulated amplification results in output state probability amplitudes that have a dependence on the number of photons in each mode, which differs greatly from two-mode squeezed vacuum. A large family of entangled output states are found. Specific output states allow for the heralded creation of N=4 N00N states, which may be used for quantum lithography, to write sub-Rayleigh fringe patterns, and for quantum interferometry, to achieve Heisenberg-limited phase measurement sensitivity.
RI
Cable, Hugo C-2346-2011 
TC 8
Z9 8
SN 1050-2947
PD JUL
PY 2008
VL 78
IS 1
AR 012339
DI 10.1103/PhysRevA.78.012339
UT WOS:000258180300084
ER

PT J
AU Thanvanthri, S
Kapale, KT
Dowling, JP
AF Thanvanthri, Sulakshana
Kapale, Kishore T.
Dowling, Jonathan P.
TI Arbitrary coherent superpositions of quantized vortices in Bose-Einstein condensates via orbital angular momentum of light
SO PHYSICAL REVIEW A
AB We recently proposed a scheme for the creation of coherent superpositions of vortex states in Bose-Einstein condensates (BECs) using orbital angular momentum (OAM) states of light [Phys. Rev. Lett. 95, 173601 (200.5)], Here we discuss further technical details of the proposal, provide an alternative, time-reversal-symmetric scheme for transfer of a superposition of OAM states of light to the BEC via a procedure analogous to the traditional stimulated Raman adiabatic passage technique, and discuss an alternative trap configuration conducive for sustaining large charge vortices. Superpositions of OAM states of light, that can be created using the existing experimental techniques, can be transferred to an initially nonrotating BEC via a specially devised Raman coupling scheme. The techniques proposed here open up avenues to study coherent interaction of OAM states of light with matter. The study could also be employed for performing various quantum-information-processing tasks with OAM states of light-including a memory for a quantum state of the initial superposition.
TC 15
Z9 15
SN 1050-2947
PD MAY
PY 2008
VL 77
IS 5
AR 053825
DI 10.1103/PhysRevA.77.053825
PN Part b
UT WOS:000257024100060
ER

PT J
AU Combes, J
Wiseman, HM
Jacobs, K
AF Combes, Joshua
Wiseman, Howard M.
Jacobs, Kurt
TI Rapid measurement of quantum systems using feedback control
SO PHYSICAL REVIEW LETTERS
AB We introduce a feedback control algorithm that increases the speed at which a measurement extracts information about a d-dimensional system by a factor that scales as d(2). Generalizing this algorithm, we apply it to a register of n qubits and show an improvement of O(n). We derive analytical bounds on the benefit provided by the feedback and perform simulations that confirm that this speedup is achieved.
RI
Combes, Joshua D-3790-2009 
Wiseman, Howard A-7266-2008 
Jacobs, Kurt E-7049-2011 
TC 17
Z9 17
SN 0031-9007
PD APR 25
PY 2008
VL 100
IS 16
AR 160503
DI 10.1103/PhysRevLett.100.160503
UT WOS:000255457600009
ER

PT J
AU Jacobs, K
Jordan, AN
Irish, EK
AF Jacobs, K.
Jordan, A. N.
Irish, E. K.
TI Energy measurements and preparation of canonical phase states of a nano-mechanical resonator
SO EPL
AB We show that a continuous quantum non-demolition measurement of the energy of a nanomechanical resonator can be achieved by monitoring the resonator with a single-electron transistor, or a quantum point contact, via a Cooper-pair box. This technique can further be used to prepare highly entangled states of two resonators, such as canonical phase reference states, and so-called noon states. Copyright (c) EPLA, 2008.
RI
Jordan, Andrew E-4558-2011 
Jacobs, Kurt E-7049-2011 
TC 9
Z9 9
SN 0295-5075
PD APR
PY 2008
VL 82
IS 1
AR 18003
DI 10.1209/029-5075/82/18003
UT WOS:000255369300029
ER

PT J
AU Wilde, MM
Brun, TA
Dowling, JP
Lee, H
AF Wilde, Mark M.
Brun, Todd A.
Dowling, Jonathan P.
Lee, Hwang
TI Coherent communication with linear optics
SO PHYSICAL REVIEW A
AB We show how to implement several continuous-variable coherent protocols with linear optics. Noise can accumulate when implementing each coherent protocol with realistic optical devices. Our analysis bounds the level of noise accumulation. We highlight the connection between a coherent channel and a nonlocal quantum nondemolition interaction and give two new protocols that implement a coherent channel. One protocol is superior to a previous method for a nonlocal quantum nondemolition interaction because it requires fewer communication resources. We then show how continuous-variable coherent superdense coding implements two nonlocal quantum nondemolition interactions with a quantum channel and bipartite entanglement. We finally show how to implement continuous-variable coherent teleportation experimentally and provide a way to verify the correctness of its operation.
RI
Brun, Todd C-3943-2008 
TC 2
Z9 2
SN 1050-2947
PD FEB
PY 2008
VL 77
IS 2
AR 022321
DI 10.1103/PhysRevA.77.022321
UT WOS:000253763900048
ER

PT J
AU Dowling, JP
AF Dowling, Jonathan P.
TI Quantum optical metrology - the lowdown on high-N00N states
SO CONTEMPORARY PHYSICS
AB 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.
TC 89
Z9 89
SN 0010-7514
PY 2008
VL 49
IS 2
BP 125
EP 143
DI 10.1080/00107510802091298
UT WOS:000257343400003
ER

PT J
AU Gao, Y
Lee, H
AF Gao, Yang
Lee, Hwang
TI Sub-shot-noise quantum optical interferometry: a comparison of entangled state performance within a unified measurement scheme
SO JOURNAL OF MODERN OPTICS
CT 38th Winter Colloquium on the Physics of Quantum Electronics
CY JAN 06-FEB 10, 2008
CL Snowbird, UT
AB Phase measurement using a lossless Mach-Zehnder interferometer with certain entangled N-photon states can lead to a phase sensitivity of the order of 1/N, the Heisenberg limit. However, previously considered output measurement schemes are different for different input states to achieve this limit. We show that it is possible to achieve this limit just by the parity measurement for all the commonly proposed entangled states. Based on the parity measurement scheme, the reductions of the phase sensitivity in the presence of photon loss are examined for the various input states.
TC 6
Z9 6
SN 0950-0340
PY 2008
VL 55
IS 19-20
BP 3319
EP 3327
DI 10.1080/09500340802428298
UT WOS:000261803300022
ER

PT J
AU Chiruvelli, A
Jacobs, K
AF Chiruvelli, Aravind
Jacobs, Kurt
TI Rapid-purification protocols for optical homodyning
SO PHYSICAL REVIEW A
AB We present a number of rapid-purification feedback protocols for optical homodyne detection of a single optical qubit. We derive first a protocol that speeds up the rate of increase of the average purity of the system, and find that as in the equivalent protocol for a nondissipative measurement, this generates a deterministic evolution for the purity in the limit of strong feedback. We also consider two analogs of the Wiseman-Ralph rapid-purification protocol in this setting, and show that as in that protocol they speed up the average time taken to reach a fixed level of purity. We also examine how the performance of these algorithms changes with detection efficiency, being an important practical consideration.
RI
Jacobs, Kurt E-7049-2011 
TC 5
Z9 5
SN 1050-2947
PD JAN
PY 2008
VL 77
IS 1
AR 012102
DI 10.1103/PhysRevA.77.012102
UT WOS:000252862000017
ER

PT J
AU Sciarrino, F
Vitelli, C
De Martini, F
Glasser, R
Cable, H
Dowling, JP
AF Sciarrino, Fabio
Vitelli, Chiara
De Martini, Francesco
Glasser, Ryan
Cable, Hugo
Dowling, Jonathan P.
TI Experimental sub-Rayleigh resolution by an unseeded high-gain optical parametric amplifier for quantum lithography
SO PHYSICAL REVIEW A
AB Quantum lithography proposes to adopt entangled quantum states in order to increase resolution in interferometry. In the present paper we experimentally demonstrate that the output of a high-gain optical parametric amplifier can be intense yet exhibits quantum features, namely, sub-Rayleigh fringes, as proposed by [Agarwal , Phys. Rev. Lett. 86, 1389 (2001)]. We investigate multiphoton states generated by a high-gain optical parametric amplifier operating with a quantum vacuum input for gain values up to 2.5. The visibility has then been increased by means of three-photon absorption. The present paper opens interesting perspectives for the implementation of such an advanced interferometrical setup.
RI
Cable, Hugo C-2346-2011 
TC 13
Z9 13
SN 1050-2947
PD JAN
PY 2008
VL 77
IS 1
AR 012324
DI 10.1103/PhysRevA.77.012324
UT WOS:000252862000056
ER

PT J
AU VanMeter, NM
Lougovski, P
Uskov, DB
Kieling, K
Eisert, J
Dowling, JP
AF VanMeter, N. M.
Lougovski, P.
Uskov, D. B.
Kieling, K.
Eisert, J.
Dowling, Jonathan P.
TI General linear-optical quantum state generation scheme: Applications to maximally path-entangled states
SO PHYSICAL REVIEW A
AB We introduce schemes for linear-optical quantum state generation. A quantum state generator is a device that prepares a desired quantum state using product inputs from photon sources, linear-optical networks, and postselection using photon counters. We show that this device can be concisely described in terms of polynomial equations and unitary constraints. We illustrate the power of this language by applying the Grobner-basis technique along with the notion of vacuum extensions to solve the problem of how to construct a quantum state generator analytically for any desired state, and use methods of convex optimization to identify bounds to success probabilities. In particular, we disprove a conjecture concerning the preparation of the maximally path-entangled vertical bar n,0 >+vertical bar 0,n > (NOON) state by providing a counterexample using these methods, and we derive a new upper bound on the resources required for NOON-state generation.
RI
Quantum, CQD at IMS D-2115-2010 
TC 11
Z9 11
SN 1050-2947
PD DEC
PY 2007
VL 76
IS 6
AR 063808
DI 10.1103/PhysRevA.76.063808
UT WOS:000251985900108
ER

PT J
AU Jacobs, K
Lougovski, P
AF Jacobs, Kurt
Lougovski, Pavel
TI Emergent quantum jumps in a nano-electro-mechanical system
SO JOURNAL OF PHYSICS A-MATHEMATICAL AND THEORETICAL
AB We describe a nano-electro-mechanical system that exhibits the 'retroactive' quantum jumps discovered by Mabuchi and Wiseman ( 1998 Phys. Rev. Lett. 81 4620). This system consists of a Cooper-pair box coupled to a nano-mechanical resonator, in which the latter is continuously monitored by a single-electron transistor or quantum point contact. Further, we show that these kinds of jumps, and the jumps that emerge in a continuous quantum non-demolition measurement, are one and the same phenomena. We also consider manipulating the jumps by applying feedback control to the Cooper-pair box.
RI
Jacobs, Kurt E-7049-2011 
TC 0
Z9 0
SN 1751-8113
PD NOV 16
PY 2007
VL 40
IS 46
BP F987
EP F993
DI 10.1088/1751-8113/40/46/F02
UT WOS:000250687700002
ER

PT J
AU Dowling, JP
AF Dowling, Jonathan P.
TI Quantum optics - Kittens catch phase
SO NATURE
TC 2
Z9 2
SN 0028-0836
PD NOV 15
PY 2007
VL 450
IS 7168
BP 362
EP 363
DI 10.1038/450362b
UT WOS:000250918600036
ER

PT J
AU Wildfeuer, CF
Lund, AP
Dowling, JP
AF Wildfeuer, Christoph F.
Lund, Austin P.
Dowling, Jonathan P.
TI Strong violations of Bell-type inequalities for path-entangled number states
SO PHYSICAL REVIEW A
AB We show that nonlocal correlation experiments on the two spatially separated modes of a maximally path-entangled number state may be performed. They lead to a violation of a Clauser-Horne Bell inequality for any finite photon number N. We also present an analytical expression for the two-mode Wigner function of a maximally path-entangled number state and investigate a Clauser-Horne-Shimony-Holt Bell inequality for such a state. We test other Bell-type inequalities. Some are violated by a constant amount for any N.
RI
Lund, Austin A-3623-2011 
TC 14
Z9 14
SN 1050-2947
PD NOV
PY 2007
VL 76
IS 5
AR 052101
DI 10.1103/PhysRevA.76.052101
UT WOS:000251326400013
ER

PT J
AU Cable, H
Dowling, JP
AF Cable, Hugo
Dowling, Jonathan P.
TI Efficient generation of large number-path entanglement using only linear optics and feed-forward
SO PHYSICAL REVIEW LETTERS
AB We show how an idealized measurement procedure can condense photons from two modes into one and how, by feeding forward the results of the measurement, it is possible to generate efficiently superposition states commonly called N00N states. For the basic procedure sources of number states leak onto a beam splitter, and the output ports are monitored by photodetectors. We find that detecting a fixed fraction of the input at one output port suffices to direct the remainder to the same port, with high probability, however large the initial state. When instead photons are detected at both ports, macroscopic quantum superposition states are produced. We describe a linear-optical circuit for making the components of such a state orthogonal, and another to convert the output to a N00N state. Our approach scales exponentially better than existing proposals. Important applications include quantum imaging and metrology.
RI
Cable, Hugo C-2346-2011 
TC 23
Z9 23
SN 0031-9007
PD OCT 19
PY 2007
VL 99
IS 16
AR 163604
DI 10.1103/PhysRevLett.99.163604
UT WOS:000250296000030
ER

PT J
AU Florescu, M
Lee, H
Puscasu, I
Pralle, M
Florescu, L
Ting, DZ
Dowling, JP
AF Florescu, Marian
Lee, Hwang
Puscasu, Irina
Pralle, Martin
Florescu, Lucia
Ting, David Z.
Dowling, Jonathan P.
TI Improving solar cell efficiency using photonic band-gap materials
SO SOLAR ENERGY MATERIALS AND SOLAR CELLS
AB The potential of using photonic crystal structures for realizing highly efficient and reliable solar-cell devices is presented. We show that due their ability to modify the spectral and angular characteristics of thermal radiation, photonic crystals emerge as one of the leading candidates for frequency- and angular-selective radiating elements in thermophotovoltaic devices. We show that employing photonic crystal-based angle- and frequency-selective absorbers facilitates a strong enhancement of the conversion efficiency of solar cell devices without using concentrators. (c) 2007 Elsevier B.V. All rights reserved.
RI
Florescu, Marian E-9009-2010 
TC 23
Z9 24
SN 0927-0248
PD OCT 15
PY 2007
VL 91
IS 17
BP 1599
EP 1610
DI 10.1016/j.solmat.2007.05.001
UT WOS:000249835800002
ER

PT J
AU Han, MX
Ma, YG
Huang, WM
AF Han, Muxin
Ma, Yongge
Huang, Weiming
TI Fundamental structure of loop quantum gravity
SO INTERNATIONAL JOURNAL OF MODERN PHYSICS D
AB In the recent twenty years, loop quantum gravity, a background independent approach to unify general relativity and quantum mechanics, has been widely investigated. The aim of loop quantum gravity is to construct a mathematically rigorous, background independent, non-perturbative quantum theory for a Lorentzian gravitational field on a four-dimensional manifold. In the approach, the principles of quantum mechanics are combined with those of general relativity naturally. Such a combination provides us a picture of, so-called, quantum Riemannian geometry, which is discrete on the fundamental scale. Imposing the quantum constraints in analogy from the classical ones, the quantum dynamics of gravity is being studied as one of the most important issues in loop quantum gravity. On the other hand, the semi-classical analysis is being carried out to test the classical limit of the quantum theory.
In this review, the fundamental structure of loop quantum gravity is presented pedagogically. Our main aim is to help non-experts to understand the motivations, basic structures, as well as general results. It may also be beneficial to practitioners to gain insights from different perspectives on the theory. We will focus on the theoretical framework itself, rather than its applications, and do our best to write it in modern and precise langauge while keeping the presentation accessible for beginners. After reviewing the classical connection dynamical formalism of general relativity, as a foundation, the construction of the kinematical Ashtekar-Isham-Lewandowski representation is introduced in the content of quantum kinematics. The algebraic structure of quantum kinematics is also discussed. In the content of quantum dynamics, we mainly introduce the construction of a Hamiltonian constraint operator and the master constraint project. At last, some applications and recent advances are outlined. It should be noted that this strategy of quantizing gravity can also be extended to obtain other background-independent quantum gauge theories. There is no divergence within this background-independent and diffeomorphism-invariant quantization program of matter coupled to gravity.
TC 40
Z9 42
SN 0218-2718
PD SEP
PY 2007
VL 16
IS 9
BP 1397
EP 1474
DI 10.1142/S0218271807010894
UT WOS:000252849400001
ER

PT J
AU Lougovski, P
Casagrande, F
Lulli, A
Solano, E
AF Lougovski, P.
Casagrande, F.
Lulli, A.
Solano, E.
TI Strongly driven one-atom laser and decoherence monitoring
SO PHYSICAL REVIEW A
AB We propose the implementation of a strongly driven one-atom laser, based on the off-resonant interaction of a three-level atom in Lambda configuration with a single cavity mode and three laser fields. We show that the system can be described equivalently by a two-level atom resonantly coupled to the cavity and driven by a strong effective coherent field. The effective dynamics can be solved exactly, including a thermal field bath, allowing an analytical description of field statistics and entanglement properties. We also show the possible generation of quantum superposition (Schrodinger cat) states for the whole atom-field system and for the field alone after atomic measurement. We propose a way to monitor the system decoherence by measuring atomic populations. Finally, we confirm the validity of our model through numerical solutions.
RI
Solano, Enrique C-1132-2013 
TC 28
Z9 28
SN 1050-2947
PD SEP
PY 2007
VL 76
IS 3
AR 033802
DI 10.1103/PhysRevA.76.033802
UT WOS:000249786000143
ER

PT J
AU Durkin, GA
Dowling, JP
AF Durkin, Gabriel A.
Dowling, Jonathan P.
TI Local and global distinguishability in quantum interferometry
SO PHYSICAL REVIEW LETTERS
AB A statistical distinguishability based on relative entropy characterizes the fitness of quantum states for phase estimation. This criterion is employed in the context of a Mach-Zehnder interferometer and used to interpolate between two regimes of local and global phase distinguishability. The scaling of distinguishability in these regimes with photon number is explored for various quantum states. It emerges that local distinguishability is dependent on a discrepancy between quantum and classical rotational energy. Our analysis demonstrates that the Heisenberg limit is the true upper limit for local phase sensitivity. Only the "NOON" states share this bound, but other states exhibit a better trade-off when comparing local and global phase regimes.
TC 36
Z9 36
SN 0031-9007
PD AUG 17
PY 2007
VL 99
IS 7
AR 070801
DI 10.1103/PhysRevLett.99.070801
UT WOS:000248866900007
ER

PT J
AU Kapale, KT
Dowling, JP
AF Kapale, Kishore T.
Dowling, Jonathan P.
TI Bootstrapping approach for generating maximally path-entangled photon states
SO PHYSICAL REVIEW LETTERS
AB We propose a bootstrapping approach to the generation of maximally path-entangled states of photons, so-called "NOON states." The strong atom-light interaction of cavity QED can be employed to generate NOON states with about 100 photons. These can then be used to boost the existing experimental Kerr nonlinearities based on quantum coherence effects, to facilitate NOON generation with an arbitrarily large number of photons. We also offer an alternative scheme that uses an atom-cavity dispersive interaction to obtain a sufficiently high Kerr nonlinearity necessary for arbitrary NOON generation.
TC 24
Z9 24
SN 0031-9007
PD AUG 3
PY 2007
VL 99
IS 5
AR 053602
DI 10.1103/PhysRevLett.99.053602
UT WOS:000248597500019
ER

PT J
AU Wilde, MM
Spedalieri, F
Dowling, JP
Lee, H
AF Wilde, Mark M.
Spedalieri, Federico
Dowling, Jonathan P.
Lee, Hwang
TI Alternate scheme for optical cluster-state generation without number-resolving photon detectors
SO INTERNATIONAL JOURNAL OF QUANTUM INFORMATION
AB We design a controlled-phase gate for linear optical quantum computing by using photodetectors that cannot resolve photon number. An intrinsic error-correction circuit corrects errors introduced by the detectors. Our controlled-phase gate has a 1/4 success probability. Recent development in cluster-state quantum computing has shown that a two-qubit gate with non-zero success probability can build an arbitrarily large cluster state only with polynomial overhead. Hence, it is possible to generate optical cluster states without number-resolving detectors and with polynomial overhead.
TC 1
Z9 1
SN 0219-7499
PD AUG
PY 2007
VL 5
IS 4
BP 617
EP 626
DI 10.1142/S0219749907003080
UT WOS:000251175600012
ER

PT J
AU Jacobs, K
Lund, AP
AF Jacobs, Kurt
Lund, Austin P.
TI Feedback control of nonlinear quantum systems: A rule of thumb
SO PHYSICAL REVIEW LETTERS
AB We show that in the regime in which feedback control is most effective-when measurements are relatively efficient, and feedback is relatively strong-then, in the absence of any sharp inhomogeneity in the noise, it is always best to measure in a basis that does not commute with the system density matrix than one that does. That is, it is optimal to make measurements that disturb the state one is attempting to stabilize.
RI
Lund, Austin A-3623-2011 
Jacobs, Kurt E-7049-2011 
TC 20
Z9 20
SN 0031-9007
PD JUL 13
PY 2007
VL 99
IS 2
AR 020501
DI 10.1103/PhysRevLett.99.020501
UT WOS:000248021000006
ER

PT J
AU Zink, B
Stergioulas, N
Hawke, I
Ott, CD
Schnetter, E
Muller, E
AF Zink, Burkhard
Stergioulas, Nikolaos
Hawke, Ian
Ott, Christian D.
Schnetter, Erik
Mueller, Ewald
TI Nonaxisymmetric instability and fragmentation of general relativistic quasitoroidal stars
SO PHYSICAL REVIEW D
AB In a recent publication, we have demonstrated that differentially rotating stars admit new channels of black hole formation via fragmentation instabilities. Since a higher order instability of this kind could potentially transform a differentially rotating supermassive star into a multiple black hole system embedded in a massive accretion disk, we investigate the dependence of the instability on parameters of the equilibrium model. We find that many of the models constructed exhibit nonaxisymmetric instabilities with corotation points, even for low values of T/|W|, which lead to a fission of the stars into one, two, or three fragments, depending on the initial perturbation. At least in the models selected here, an m=1 mode becomes unstable at lower values of T/|W|, which would seem to favor a scenario where one black hole with a massive accretion disk forms. In this case, we have gained evidence that low values of compactness of the initial model can lead to a stabilization of the resulting fragment, thus preventing black hole formation in this scenario.
TC 11
Z9 11
SN 1550-7998
PD JUL
PY 2007
VL 76
IS 2
AR 024019
DI 10.1103/PhysRevD.76.024019
UT WOS:000248545200045
ER

PT J
AU Shizume, K
Jacobs, K
Burgarth, D
Bose, S
AF Shizume, Kosuke
Jacobs, Kurt
Burgarth, Daniel
Bose, Sougato
TI Quantum communication via a continuously monitored dual spin chain
SO PHYSICAL REVIEW A
AB We analyze a recent protocol for the transmission of quantum states via a dual spin chain [Burgarth and Bose, Phys. Rev. A 71, 052315 (2005)] under the constraint that the receiver's measurement strength is finite. That is, we consider the channel where the ideal, instantaneous, and complete von Neumann measurements are replaced with a more realistic continuous measurement. We show that for optimal performance the measurement strength must be "tuned" to the channel spin-spin coupling, and once this is done, one is able to achieve a similar transmission rate to that obtained with ideal measurements. The spin chain protocol thus remains effective under measurement constraints.
RI
Burgarth, Daniel A-5965-2009 
Jacobs, Kurt E-7049-2011 
TC 4
Z9 5
SN 1050-2947
PD JUN
PY 2007
VL 75
IS 6
AR 062328
DI 10.1103/PhysRevA.75.062328
UT WOS:000247624300066
ER

PT J
AU Jacobs, K
Lougovski, P
Blencowe, M
AF Jacobs, Kurt
Lougovski, Pavel
Blencowe, Miles
TI Continuous measurement of the energy eigenstates of a nanomechanical resonator without a nondemolition probe
SO PHYSICAL REVIEW LETTERS
AB We show that it is possible to perform a continuous measurement that continually projects a nanoresonator into its energy eigenstates by employing a linear coupling with a two-state system. This technique makes it possible to perform a measurement that exposes the quantum nature of the resonator by coupling it to a Cooper-pair box and a superconducting transmission line resonator.
RI
Jacobs, Kurt E-7049-2011 
TC 29
Z9 29
SN 0031-9007
PD APR 6
PY 2007
VL 98
IS 14
AR 147201
DI 10.1103/PhysRevLett.98.147201
UT WOS:000245512100058
ER

PT J
AU Agarwal, GS
Chan, KW
Boyd, RW
Cable, H
Dowling, JP
AF Agarwal, Girish S.
Chan, Kam Wai
Boyd, Robert W.
Cable, Hugo
Dowling, Jonathan P.
TI Quantum states of light produced by a high-gain optical parametric amplifier for use in quantum lithography
SO JOURNAL OF THE OPTICAL SOCIETY OF AMERICA B-OPTICAL PHYSICS
AB We present a theoretical analysis of the properties of an unseeded optical parametic amplifier (OPA) used as the source of entangled photons for applications in quantum lithography. We first study the dependence of the excitation rate of a two-photon absorber on the intensity of the light leaving the OPA. We find that the rate depends linearly on intensity only for output beams so weak that they contain fewer than one photon per mode. We also study the use of an N-photon absorber for arbitrary N as the recording medium to be used with such a light source. We find that the contrast of the interference pattern and the sharpness of the fringe maxima tend to increase with increasing values of N, but that the density of fringes and thus the limiting resolution does not increase with N. We conclude that the output of an unseeded OPA exciting an N-photon absorber provides an attractive system in which to perform quantum lithography. (c) 2007 Optical Society of America.
RI
Cable, Hugo C-2346-2011 
TC 14
Z9 14
SN 0740-3224
PD FEB
PY 2007
VL 24
IS 2
BP 270
EP 274
DI 10.1364/JOSAB.24.000270
UT WOS:000244281200016
ER

PT J
AU Kapale, KT
AF Kapale, K. T.
TI Polarization preserving quantum nondemolition photodetector
SO JOURNAL OF MODERN OPTICS
AB A polarization preserving quantum nondemolition photodetector is proposed based on nonlinearities obtainable through quantum coherence effects. An atomic level scheme is devised such that in the presence of strong linearly polarized drive field a coherent weak probe field acquires a phase proportional to the number of photons in the signal mode immaterial of its polarization state. It is also shown that the unavoidable phase-kicks resulting due to the measurement process are insensitive to the polarization state of the incoming signal photon. It is envisioned that such a device would have tremendous applicability in photonic quantum information proposals where quantum information in the polarization qubit is to be protected.
TC 1
Z9 1
SN 0950-0340
PD JAN 20
PY 2007
VL 54
IS 2-3
BP 327
EP 335
DI 10.1080/09500340600753822
UT WOS:000244387900013
ER

PT J
AU Kok, P
Munro, WJ
Nemoto, K
Ralph, TC
Dowling, JP
Milburn, GJ
AF Kok, Pieter
Munro, W. J.
Nemoto, Kae
Ralph, T. C.
Dowling, Jonathan P.
Milburn, G. J.
TI Linear optical quantum computing with photonic qubits
SO REVIEWS OF MODERN PHYSICS
AB Linear optics with photon counting is a prominent candidate for practical quantum computing. The protocol by Knill, Laflamme, and Milburn [2001, Nature (London) 409, 46] 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. The original theory and its improvements are reviewed, and a few examples of experimental two-qubit gates are given. The use of realistic components, the errors they induce in the computation, and how these errors can be corrected is discussed.
RI
MIlburn, Gerard B-6381-2008 
Kok, Pieter B-1658-2010 
Nemoto, Kae A-8833-2011 
Munro, William A-8453-2011 
Ralph, Timothy A-1858-2011 
TC 453
Z9 465
SN 0034-6861
PD JAN-MAR
PY 2007
VL 79
IS 1
BP 135
EP 174
DI 10.1103/RevModPhys.79.135
UT WOS:000244867600004
ER

PT J
AU Jacobs, K
Dowling, JP
AF Jacobs, Kurt
Dowling, Jonathan P.
TI Concatenated beam splitters, optical feed-forward, and the nonlinear sign gate
SO PHYSICAL REVIEW A
AB We consider a nonlinear sign gate implemented using a sequence of two beam splitters, and consider the use of further sequences of beam splitters to implement feed-forward so as to correct an error resulting from the first beam splitter. We obtain similar results to Scheel [Phys. Rev. A 73, 034301 (2006)], in that we also find that our feed-forward procedure is only able to produce a very minor improvement in the success probability of the original gate.
RI
Jacobs, Kurt E-7049-2011 
TC 0
Z9 0
SN 1050-2947
PD DEC
PY 2006
VL 74
IS 6
AR 064304
DI 10.1103/PhysRevA.74.064304
UT WOS:000243166700175
ER

PT J
AU Agarwal, GS
Kapale, KT
AF Agarwal, G. S.
Kapale, K. T.
TI Subwavelength atom localization via coherent population trapping
SO JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS
AB We present an atom localization scheme based on coherent population trapping. We consider atomic transitions in a Lambda configuration where the control field is a standing-wave field. The probe field and the control field produce coherence between the two ground states and prepare the atom in a pure state. We show that the population in one of the ground states has the same fringe pattern as produced by a Fabry-Perot interferometer and thus measurement of this population would localize the atom. Interestingly enough the role of the cavity finesse is played by the ratio of the intensities of the pump and probe. This is in fact the reason for obtaining extreme subwavelength localization.
TC 53
Z9 53
SN 0953-4075
PD SEP 14
PY 2006
VL 39
IS 17
BP 3437
EP 3446
DI 10.1088/0953-4075/39/17/002
UT WOS:000240490700005
ER

PT J
AU Jacobs, K
Steck, DA
AF Jacobs, Kurt
Steck, Daniel A.
TI A straightforward introduction to continuous quantum measurement
SO CONTEMPORARY PHYSICS
AB We present a pedagogical treatment of the formalism of continuous quantum measurement. Our aim is to show the reader how the equations describing such measurements are derived and manipulated in a direct manner. We also give elementary background material for those new to measurement theory, and describe further various aspects of continuous measurements that should be helpful to those wanting to use such measurements in applications. Specifically, we use the simple and direct approach of generalized measurements to derive the stochastic master equation describing the continuous measurements of observables, give a tutorial on stochastic calculus, treat multiple observers and inefficient detection, examine a general form of the measurement master equation.. and show how the master equation leads to information gain and disturbance. To conclude, we give a detailed treatment of imaging the resonance fluorescence from a single atom as a concrete example of how a continuous position measurement arises in a physical system.
RI
Jacobs, Kurt E-7049-2011 
TC 73
Z9 73
SN 0010-7514
PD SEP-OCT
PY 2006
VL 47
IS 5
BP 279
EP 303
DI 10.1080/00107510601101934
UT WOS:000243585400004
ER

PT J
AU Steck, DA
Jacobs, K
Mabuchi, H
Habib, S
Bhattacharya, T
AF Steck, Daniel A.
Jacobs, Kurt
Mabuchi, Hideo
Habib, Salman
Bhattacharya, Tanmoy
TI Feedback cooling of atomic motion in cavity QED
SO PHYSICAL REVIEW A
AB We consider the problem of controlling the motion of an atom trapped in an optical cavity using continuous feedback. In order to realize such a scheme experimentally, one must be able to perform state estimation of the atomic motion in real time. While in theory this estimate may be provided by a stochastic master equation describing the full dynamics of the observed system, integrating this equation in real time is impractical. Here we derive an approximate estimation equation for this purpose, and use it as a drive in a feedback algorithm designed to cool the motion of the atom. We examine the effectiveness of such a procedure using full simulations of the cavity QED system, including the quantized motion of the atom in one dimension.
RI
Jacobs, Kurt E-7049-2011 
TC 22
Z9 23
SN 1050-2947
PD JUL
PY 2006
VL 74
IS 1
AR 012322
DI 10.1103/PhysRevA.74.012322
UT WOS:000239425900039
ER

PT J
AU Han, MX
Ma, YG
AF Han, MX
Ma, YG
TI Master constraint operators in loop quantum gravity
SO PHYSICS LETTERS B
AB We introduce a master constraint operator (M) over cap densely defined in the diffeomorphism invariant Hilbert space in loop quantum gravity, which corresponds classically to the master constraint in the programme. It is shown that (M) over cap is positive and symmetric, and hence has its Friedrichs self-adjoint extension. The same conclusion is tenable for an alternative master operator (M) over cap', whose quadratic form coincides with the one proposed by Thiemann. So the master constraint programme for loop quantum gravity can be carried out in principle by employing either of the two operators. (c) 2006 Elsevier B.V. All rights reserved.
TC 17
Z9 18
SN 0370-2693
PD APR 13
PY 2006
VL 635
IS 4
BP 225
EP 231
DI 10.1016/j.physletb.2006.03.004
UT WOS:000236630600008
ER

PT J
AU Han, MX
Ma, YG
AF Han, MX
Ma, YG
TI Dynamics of a scalar field in a polymer-like representation
SO CLASSICAL AND QUANTUM GRAVITY
AB In the last 20 years, loop quantum gravity, a background- independent approach to unify general relativity and quantum mechanics, has been widely investigated. We consider the quantum dynamics of a real massless scalar field coupled to gravity in this framework. A Hamiltonian operator for the scalar field can be well defined in the coupled diffeomorphism-invariant Hilbert space, which is both self-adjoint and positive. On the other hand, the Hamiltonian constraint operator for the scalar field coupled to gravity can be well defined in the coupled kinematical Hilbert space. There are one-parameter ambiguities due to scalar field in the construction of both operators. The results heighten our confidence that there is no divergence within this background- independent and diffeomorphism-invariant quantization approach of matter coupled to gravity. Moreover, to avoid possible quantum anomaly, the master constraint programme can be carried out in this coupled system by employing a self-adjoint master constraint operator on the diffectmorphism-invariant Hilbert space.
TC 9
Z9 10
SN 0264-9381
PD APR 7
PY 2006
VL 23
IS 7
BP 2741
EP 2760
DI 10.1088/0264-9381/2317/031
UT WOS:000236932700031
ER

PT J
AU Guillaume, A
Dowling, JP
AF Guillaume, A
Dowling, JP
TI Heisenberg-limited measurements with superconducting circuits
SO PHYSICAL REVIEW A
AB We describe an assembly of N superconducting qubits contained in a single- mode cavity. In the dispersive regime, the correlation between the cavity field and each qubit results in an effective interaction between qubits that can be used to dynamically generate maximally entangled states. With only collective manipulations, we show how to create maximally entangled quantum states and how to use these states to reach the Heisenberg limit in the determination of the qubit bias control parameter (gate charge for charge qubits, external magnetic flux for rf-superconducting quantum interference devices).
TC 1
Z9 1
SN 1050-2947
PD APR
PY 2006
VL 73
IS 4
AR 040304
DI 10.1103/PhysRevA.73.040304
UT WOS:000237147700004
ER

PT J
AU Dowling, JP
AF Dowling, JP
TI Quantum information - To compute or not to compute?
SO NATURE
TC 6
Z9 6
SN 0028-0836
PD FEB 23
PY 2006
VL 439
IS 7079
BP 919
EP 920
DI 10.1038/439919a
UT WOS:000235486100025
ER

PT J
AU Spedalieri, FM
Lee, H
Dowling, JP
AF Spedalieri, FM
Lee, H
Dowling, JP
TI High-fidelity linear optical quantum computing with polarization encoding
SO PHYSICAL REVIEW A
AB We show that the KLM scheme [Knill, Laflamme, and Milburn, Nature 409, 46 (2001)] can be implemented using polarization encoding, thus reducing the number of path modes required by half. One of the main advantages of this new implementation is that it naturally incorporates a loss detection mechanism that makes the probability of a gate introducing a non-detected error, when non-ideal detectors are considered, dependent only on the detector dark-count rate and independent of its efficiency. Since very low dark-count rate detectors are currently available, a high-fidelity gate (probability of error of order 10(-6) conditional on the gate being successful) can be implemented using polarization encoding. The detector efficiency determines the overall success probability of the gate but does not affect its fidelity. This can be applied to the efficient construction of optical cluster states with very high fidelity for quantum computing.
TC 14
Z9 14
SN 1050-2947
PD JAN
PY 2006
VL 73
IS 1
AR 012334
DI 10.1103/PhysRevA.73.012334
UT WOS:000235008900063
ER

PT J
AU Kapale, KT
Dowling, JP
AF Kapale, KT
Dowling, JP
TI Vortex phase qubit: Generating arbitrary, counterrotating, coherent superpositions in bose-einstein condensates via optical angular momentum beams
SO PHYSICAL REVIEW LETTERS
AB We propose a scheme for the generation of arbitrary coherent superpositions of vortex states in Bose-Einstein condensates (BEC) using the orbital-angular-momentum states of light. We devise a scheme to generate coherent superpositions of two such counterrotating states of light using well-known experimental techniques. We show that a specially designed Raman scheme allows for transfer of the optical vortex-superposition state onto an initially nonrotating BEC. This creates an arbitrary and coherent superposition of a vortex and antivortex pair in the BEC. The ideas presented here could be extended to generate entangled vortex states, design memories for the orbital-angular-momentum states of light, and perform other quantum information tasks. Applications to inertial sensing are also discussed.
TC 60
Z9 60
SN 0031-9007
PD OCT 21
PY 2005
VL 95
IS 17
AR 173601
DI 10.1103/PhysRevLett.95.173601
UT WOS:000232724400031
ER

PT J
AU Florescu, M
Lee, H
Stimpson, AJ
Dowling, J
AF Florescu, M
Lee, H
Stimpson, AJ
Dowling, J
TI Thermal emission and absorption of radiation in finite inverted-opal photonic crystals
SO PHYSICAL REVIEW A
AB We study theoretically the optical properties of a finite inverted-opal photonic crystal. The light-matter interaction is strongly affected by the presence of the three-dimensional photonic crystal and the alterations of the light emission and absorption processes can be used to suppress or enhance the thermal emissivity and absorptivity of the dielectric structure. We investigate the influence of the absorption present in the system on the relevant band edge frequencies that control the optical response of the photonic crystal. Our study reveals that the absorption processes cause spectral broadening and shifting of the band edge optical resonances, and determine a strong reduction of the photonic band gap spectral range. Using the angular and spectral dependence of the band edge frequencies for stop bands along different directions, we argue that by matching the blackbody emission spectrum peak with a prescribed maximum of the absorption coefficient, it is possible to achieve an angle-sensitive enhancement of the thermal emission/absorption of radiation. This result opens a way to realize a frequency-sensitive and angle-sensitive photonic crystal absorbers/emitters.
RI
Florescu, Marian E-9009-2010 
TC 21
Z9 21
SN 1050-2947
PD SEP
PY 2005
VL 72
IS 3
AR 033821
DI 10.1103/PhysRevA.72.033821
UT WOS:000232228300171
ER

PT J
AU Sun, QQ
Rostovtsev, YV
Dowling, JP
Scully, MO
Zubairy, MS
AF Sun, QQ
Rostovtsev, YV
Dowling, JP
Scully, MO
Zubairy, MS
TI Optically controlled delays for broadband pulses
SO PHYSICAL REVIEW A
AB We propose a scheme that provides large controllable delays for broadband optical pulses. The system is based on the steep dispersion of a coherently driven medium, in which the narrow electromagnetically induced transparency (EIT) band is overcome by using spatial and temporal processing.
TC 45
Z9 46
SN 1050-2947
PD SEP
PY 2005
VL 72
IS 3
AR 031802
DI 10.1103/PhysRevA.72.031802
UT WOS:000232228300015
ER

PT J
AU Florescu, M
Scheel, S
Haffner, HH
Lee, H
Strekalov, D
Knight, PL
Dowling, JP
AF Florescu, M
Scheel, S
Haffner, HH
Lee, H
Strekalov, D
Knight, PL
Dowling, JP
TI Single photons on demand from 3D photonic band-gap structures
SO EUROPHYSICS LETTERS
AB We describe a practical implementation of a (semi-deterministic) photon gun based on stimulated Raman adiabatic passage pumping and the strong enhancement of the photonic density of states in a photonic band-gap material. We show that this device allows deterministic and unidirectional production of single photons with a high repetition rate of the order of 100 kHz. We also discuss specific 3D photonic micro-structure architectures in which our model can be realized and the feasibility of implementing such a device using Er(3+) ions that produce single photons at the telecommunication wavelength of 1.55 mu m.
RI
Florescu, Marian E-9009-2010 
Haeffner, Hartmut D-8046-2012 
TC 9
Z9 9
SN 0295-5075
PD MAR
PY 2005
VL 69
IS 6
BP 945
EP 951
DI 10.1209/epl/i2004-10453-5
UT WOS:000228445900014
ER

PT J
AU Ghali, JK
AF Ghali, JK
TI Contemporary issues in heart failure
SO AMERICAN HEART JOURNAL
TC 4
Z9 5
SN 0002-8703
PD JUL
PY 1999
VL 138
IS 1
BP 5
EP 8
DI 10.1016/S0002-8703(99)70235-8
PN Part 1
UT WOS:000081395400003
ER

EF