24,886 research outputs found

    Characterization and computation of canonical tight windows for Gabor frames

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    Let (gnm)n,m∈Z(g_{nm})_{n,m\in Z} be a Gabor frame for L2(R)L_2(R) for given window gg. We show that the window h0=Sβˆ’1/2gh^0=S^{-1/2} g that generates the canonically associated tight Gabor frame minimizes βˆ₯gβˆ’hβˆ₯\|g-h\| among all windows hh generating a normalized tight Gabor frame. We present and prove versions of this result in the time domain, the frequency domain, the time-frequency domain, and the Zak transform domain, where in each domain the canonical h0h^0 is expressed using functional calculus for Gabor frame operators. Furthermore, we derive a Wiener-Levy type theorem for rationally oversampled Gabor frames. Finally, a Newton-type method for a fast numerical calculation of \ho is presented. We analyze the convergence behavior of this method and demonstrate the efficiency of the proposed algorithm by some numerical examples

    On Lerch's transcendent and the Gaussian random walk

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    Let X1,X2,...X_1,X_2,... be independent variables, each having a normal distribution with negative mean βˆ’Ξ²<0-\beta<0 and variance 1. We consider the partial sums Sn=X1+...+XnS_n=X_1+...+X_n, with S0=0S_0=0, and refer to the process {Sn:nβ‰₯0}\{S_n:n\geq0\} as the Gaussian random walk. We present explicit expressions for the mean and variance of the maximum M=max⁑{Sn:nβ‰₯0}.M=\max\{S_n:n\geq0\}. These expressions are in terms of Taylor series about Ξ²=0\beta=0 with coefficients that involve the Riemann zeta function. Our results extend Kingman's first-order approximation [Proc. Symp. on Congestion Theory (1965) 137--169] of the mean for β↓0\beta\downarrow0. We build upon the work of Chang and Peres [Ann. Probab. 25 (1997) 787--802], and use Bateman's formulas on Lerch's transcendent and Euler--Maclaurin summation as key ingredients.Comment: Published at http://dx.doi.org/10.1214/105051606000000781 in the Annals of Applied Probability (http://www.imstat.org/aap/) by the Institute of Mathematical Statistics (http://www.imstat.org

    Performance of Hybrid NbTiN-Al Microwave Kinetic Inductance Detectors as Direct Detectors for Sub-millimeter Astronomy

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    In the next decades millimeter and sub-mm astronomy requires large format imaging arrays and broad-band spectrometers to complement the high spatial and spectral resolution of the Atacama Large Millimeter/sub-millimeter Array. The desired sensors for these instruments should have a background limited sensitivity and a high optical efficiency and enable arrays thousands of pixels in size. Hybrid microwave kinetic inductance detectors consisting of NbTiN and Al have shown to satisfy these requirements. We present the second generation hybrid NbTiN-Al MKIDs, which are photon noise limited in both phase and amplitude readout for loading levels P850GHzβ‰₯10P_{850GHz} \geq 10 fW. Thanks to the increased responsivity, the photon noise level achieved in phase allows us to simultaneously read out approximately 8000 pixels using state-of-the-art electronics. In addition, the choice of superconducting materials and the use of a Si lens in combination with a planar antenna gives these resonators the flexibility to operate within the frequency range 0.09<Ξ½<1.10.09 < \nu < 1.1 THz. Given these specifications, hybrid NbTiN-Al MKIDs will enable astronomically usable kilopixel arrays for sub-mm imaging and moderate resolution spectroscopy.Comment: 7 pages, 3 figures. Presented at SPIE Astronomical Telescopes and Instrumentation 2014: Millimeter, Submillimeter, and Far-Infrared Detectors and Instrumentation for Astronomy VI

    Photon noise limited radiation detection with lens-antenna coupled Microwave Kinetic Inductance Detectors

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    Microwave Kinetic Inductance Detectors (MKIDs) have shown great potential for sub-mm instrumentation because of the high scalability of the technology. Here we demonstrate for the first time in the sub-mm band (0.1...2 mm) a photon noise limited performance of a small antenna coupled MKID detector array and we describe the relation between photon noise and MKID intrinsic generation-recombination noise. Additionally we use the observed photon noise to measure the optical efficiency of detectors to be 0.8+-0.2.Comment: The following article has been submitted to AP
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