| 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 |
|
||
| 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 |
|
||
| 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 |
|
||
| 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 |
|
||
| 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 |
|
||
| 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 |
|
||
| 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 |
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||
| 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 |
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||
| 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 |
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||
| 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 |
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||
| 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 |
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||
| 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 |
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| 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 |
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| 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 |
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| 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 |
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||
| 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 |
|
||
| 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 |
|
||
| 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 |
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||
| 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 |
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||
| 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 |
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||
| 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 |
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||
| 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 |
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||
| 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 |
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||
| 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 |
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| 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 |
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| 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 |
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||
| 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 |
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| 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 |
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| 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 |
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| AF | Jacobs, Kurt
Dowling, Jonathan P. |
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| 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 |
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| 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 |
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| AF | Jacobs, Kurt
Steck, Daniel A. |
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| 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 |
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| 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 |
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| AF | Steck, Daniel A.
Jacobs, Kurt Mabuchi, Hideo Habib, Salman Bhattacharya, Tanmoy |
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| 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 |
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| 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 |
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| AF | Florescu, M
Lee, H Stimpson, AJ Dowling, J |
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| 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 |
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| 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 |
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| AF | Florescu, M
Scheel, S Haffner, HH Lee, H Strekalov, D Knight, PL Dowling, JP |
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| 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 |
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| 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 |