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Shared Cryptographic Bits Via Quantized Quadrature Phase Amplitudes of Light

by Yi Mu, Jennifer Seberry, Yuliang Zheng - PUBLISHED IN OPTICS COMMUNICATIONS 123 , 1996
"... We propose a novel quantum cryptographic protocol without using polarized photons. The protocol consists of an optical coupler and four nonorthogonal coherent states which are analyzed by means of quadrature phase amplitudes of quantized light field. ..."
Abstract - Cited by 1 (1 self) - Add to MetaCart
We propose a novel quantum cryptographic protocol without using polarized photons. The protocol consists of an optical coupler and four nonorthogonal coherent states which are analyzed by means of quadrature phase amplitudes of quantized light field.

Contradiction of Quantum Mechanics with Local Hidden Variables for Continuous Variable Quadrature Phase Amplitude Measurements

by A. Gilchrist, P. Deuar, M. D. Reid , 2008
"... We demonstrate a contradiction of quantum mechanics with local hidden variable theories for continuous variable quadrature phase amplitude (“position” and “momentum”) measurements, by way of a violation of a Bell inequality. For any quantum state, this contradiction is lost for situations where the ..."
Abstract - Cited by 3 (0 self) - Add to MetaCart
We demonstrate a contradiction of quantum mechanics with local hidden variable theories for continuous variable quadrature phase amplitude (“position” and “momentum”) measurements, by way of a violation of a Bell inequality. For any quantum state, this contradiction is lost for situations where

Full length article OPTICS COMMUNICATIONS

by Yi Mu A, Jennifer Seberry B, Yuliang Zheng Blc , 1996
"... Shared cryptographic bits via quantized quadrature phase amplitudes of light ..."
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Shared cryptographic bits via quantized quadrature phase amplitudes of light

How Iris Recognition Works

by John Daugman , 2003
"... Algorithms developed by the author for recogniz-ing persons by their iris patterns have now been tested in six field and laboratory trials, producing no false matches in several million comparison tests. The recognition principle is the failure of a test of statis-tical independence on iris phase st ..."
Abstract - Cited by 509 (4 self) - Add to MetaCart
structure encoded by multi-scale quadrature wavelets. The combinatorial complexity of this phase information across different persons spans about 244 degrees of freedom and gen-erates a discrimination entropy of about 3.2 bits/mm over the iris, enabling real-time decisions about per-sonal identity

Global modeling of tropospheric chemistry with assimilated meteorology: Model description and evaluation

by Isabelle Bey, Daniel J. Jacob, Robert M. Yantosca, Jennifer A. Logan, Brendan D. Field, Afiene M. Fiore, Qinbin Li, Honguy Y. Liu, Loretta J. Mickley, Martin G. Schultz , 2001
"... Abstract. We present a first description and evaluation of GEOS-CHEM, a global threedimensional (3-D) model of tropospheri chemistry driven by assimilated meteorological observations from the Goddard Earth Observing System (GEOS) of the NASA Data Assimilation Office (DAO). The model is applied to a ..."
Abstract - Cited by 459 (132 self) - Add to MetaCart
the seasonal phases and amplitudes of ozone concentrations for different regions and altitudes, but tends to underestimate the seasonal amplitude at northern midlatitudes. Observed concentrations of NO and peroxyacetylnitrate (PAN) observed in aircraft campaigns are generally reproduced to within a factor of 2

Measuring phase-synchrony in brain signals

by Eugenio Rodriguez, Jacques Martinerie, Francisco J. Varela - Hum. Brain Mapp , 1999
"... r r Abstract: This article presents, for the first time, a practical method for the direct quantification of frequency-specific synchronization (i.e., transient phase-locking) between two neuroelectric signals. The motivation for its development is to be able to examine the role of neural synchronie ..."
Abstract - Cited by 346 (6 self) - Add to MetaCart
coherence, PLS separates the phase and amplitude components and can be directly interpreted in the framework of neural integration. To validate synchrony values against background fluctuations, PLS uses surrogate data and thus makes no a priori assumptions on the nature of the experimental data. We also

amplitude

by M. D. Reid , 1999
"... Quantum cryptography using continuous variable Einstein-Podolsky-Rosen correlations and quadrature phase ..."
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Quantum cryptography using continuous variable Einstein-Podolsky-Rosen correlations and quadrature phase

Experimental verification of a negative index of refraction,”

by R A Shelby , D R Smith , S Schultz - Science, , 2001
"... Abstract: We studied a two-dimensional square-lattice photonic crystal with all-angle negative refraction at its first band. Using this photonic crystal, we designed and fabricated a flat lens functioning as a cylindrical lens by increasing the vertical dimension of the photonic crystal. Twodimensi ..."
Abstract - Cited by 377 (9 self) - Add to MetaCart
refraction imaging in both amplitude and phase, and obtained an image with feature size, 0.77λ 0 .

Quadrature Amplitude Modulation (QAM). This work is

by unknown authors
"... Abstract—The ad hoc networks are the future of wireless technology as everyone wants fast and accurate error free information so keeping this in mind Bit Error Rate (BER) and power is optimized in this research paper by using the Genetic Algorithm (GA). The digital modulation techniques used for thi ..."
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for this paper are Binary Phase

Sparse solution of underdetermined linear equations by stagewise orthogonal matching pursuit

by David L. Donoho, Yaakov Tsaig, Iddo Drori, Jean-luc Starck , 2006
"... Finding the sparsest solution to underdetermined systems of linear equations y = Φx is NP-hard in general. We show here that for systems with ‘typical’/‘random ’ Φ, a good approximation to the sparsest solution is obtained by applying a fixed number of standard operations from linear algebra. Our pr ..."
Abstract - Cited by 274 (22 self) - Add to MetaCart
proposal, Stagewise Orthogonal Matching Pursuit (StOMP), successively transforms the signal into a negligible residual. Starting with initial residual r0 = y, at the s-th stage it forms the ‘matched filter ’ Φ T rs−1, identifies all coordinates with amplitudes exceeding a specially-chosen threshold, solves
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