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%%       biblex xxx.bib | \
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%% by beebe@sunburst.math.utah.edu on Fri Oct 29 23:16:26 MDT 2010
%%======================================================================

\ifx \NAMECITE \undefined % User can override this definition 
    \def \NAMECITE #1#2{{\bf #1}~\cite{#2}}
\fi



\NAMECITE{${L}^1$}{%
		Shapiro:FAA-89-563%
		}.
\NAMECITE{$n$}{%
		Bjorck:FAA-89-131%
		}.
\NAMECITE{$R^n$}{%
		Gabardo:PSM-91-543,%
		Evans:FAA-89-613%
		}.
\NAMECITE{${Z}_n$}{%
		Bjorck:FAA-89-131%
		}.


\NAMECITE{-roots}{%
		Bjorck:FAA-89-131%
		}.


\NAMECITE{Absolutely}{%
		Artemiadis:FAA-89-311%
		}.
\NAMECITE{accurate}{%
		Sarkar:PSM-91-263%
		}.
\NAMECITE{Acoustics}{%
		Schroeder:FAA-89-101%
		}.
\NAMECITE{{Advanced}}{%
		Byrnes:FAA-89%
		}.
\NAMECITE{Advances}{%
		Byrnes:FAA-89%
		}.
\NAMECITE{analyses}{%
		Madych:PSM-91-233%
		}.
\NAMECITE{Analysis}{%
		Brown:FAA-89-367%
		}.
\NAMECITE{Analytic}{%
		Clunie:FAA-89-623%
		}.
\NAMECITE{Anatomic}{%
		Kennedy:FAA-89-17%
		}.
\NAMECITE{Antenna}{%
		Brown:FAA-89-367%
		}.
\NAMECITE{Application}{%
		Klooster:FAA-89-221%
		}.
\NAMECITE{Applications}{%
		Kovalyov:FAA-89-41%
		}.
\NAMECITE{Applied}{%
		Unsal:FAA-89-59%
		}.
\NAMECITE{Approach}{%
		Grochenig:FAA-89-251%
		}.
\NAMECITE{Approximations}{%
		Seitz:FAA-89-661%
		}.
\NAMECITE{Architectures}{%
		Schempp:FAA-89-507%
		}.
\NAMECITE{Atomic}{%
		Hayman:FAA-89-597%
		}.
\NAMECITE{attractors}{%
		Cabrelli:PSM-91-163%
		}.
\NAMECITE{Auto}{%
		Tuzunalp:FAA-89-261%
		}.
\NAMECITE{Auto-Cross}{%
		Tuzunalp:FAA-89-261%
		}.


\NAMECITE{Band}{%
		Grochenig:FAA-89-251%
		}.
\NAMECITE{Band-Limited}{%
		Grochenig:FAA-89-251%
		}.
\NAMECITE{bandlimited}{%
		Grochenig:PSM-91-323%
		}.
\NAMECITE{{Barrier}}{%
		Cullen:FAA-89-499%
		}.
\NAMECITE{basic}{%
		Blei:PSM-91-649%
		}.
\NAMECITE{behaviour}{%
		Saffari:PSM-91-555%
		}.
\NAMECITE{Bispectra}{%
		Papoulis:FAA-89-377%
		}.
\NAMECITE{broadband}{%
		Sarkar:PSM-91-263%
		}.


\NAMECITE{Carlo}{%
		Korner:PSM-91-593%
		}.
\NAMECITE{{Cauchy}}{%
		Sarkar:PSM-91-263%
		}.
\NAMECITE{Certain}{%
		Benke:FAA-89-83%
		}.
\NAMECITE{characteristic}{%
		Capar:PSM-91-517%
		}.
\NAMECITE{Characterization}{%
		Mallat:PSM-91-47%
		}.
\NAMECITE{Circle}{%
		Newman:FAA-89-79%
		}.
\NAMECITE{Class}{%
		Benke:FAA-89-83%
		}.
\NAMECITE{Classical}{%
		Ingolfsson:FAA-89-29%
		}.
\NAMECITE{Coding}{%
		Schempp:FAA-89-507%
		}.
\NAMECITE{Coefficients}{%
		Newman:FAA-89-79%
		}.
\NAMECITE{Coherent}{%
		Feichtinger:FAA-89-427%
		}.
\NAMECITE{Combinatorial}{%
		Blei:FAA-89-631%
		}.
\NAMECITE{Combined}{%
		Hoop:FAA-89-387%
		}.
\NAMECITE{Comparison}{%
		Gurkanli:FAA-89-643%
		}.
\NAMECITE{Complex}{%
		Unsal:FAA-89-59%
		}.
\NAMECITE{Computations}{%
		Tolimieri:FAA-89-237%
		}.
\NAMECITE{Computer}{%
		Schroeder:FAA-89-101%
		}.
\NAMECITE{Conjugate}{%
		Ponnapalli:FAA-89-201%
		}.
\NAMECITE{Constant}{%
		Bjorck:FAA-89-131%
		}.
\NAMECITE{continuations}{%
		Kahane:PSM-91-481%
		}.
\NAMECITE{control}{%
		Cannarsa:PSM-91-617%
		}.
\NAMECITE{Convergent}{%
		Artemiadis:FAA-89-311%
		}.
\NAMECITE{Correlation}{%
		Tuzunalp:FAA-89-261%
		}.
\NAMECITE{Cross}{%
		Tuzunalp:FAA-89-261%
		}.
\NAMECITE{Crystallography}{%
		Hauptman:FAA-89-3%
		}.
\NAMECITE{Cyclic}{%
		Bjorck:FAA-89-131%
		}.


\NAMECITE{Data}{%
		Jakimovski:FAA-89-73%
		}.
\NAMECITE{decomposition}{%
		Suter:PSM-91-217%
		}.
\NAMECITE{Decompositions}{%
		Hayman:FAA-89-597%
		}.
\NAMECITE{definite}{%
		Gabardo:PSM-91-543%
		}.
\NAMECITE{Density}{%
		Cabrelli:PSM-91-163%
		}.
\NAMECITE{Derivatives}{%
		Clunie:FAA-89-623%
		}.
\NAMECITE{differential}{%
		Jaffard:PSM-91-3%
		}.
\NAMECITE{dilation}{%
		Heil:PSM-91-15%
		}.
\NAMECITE{Dimension}{%
		Blei:FAA-89-631%
		}.
\NAMECITE{dimensions}{%
		Cannarsa:PSM-91-617%
		}.
\NAMECITE{Diodes}{%
		Cullen:FAA-89-499%
		}.
\NAMECITE{Diophantine}{%
		Dodson:FAA-89-483%
		}.
\NAMECITE{Direct}{%
		Hauptman:FAA-89-3%
		}.
\NAMECITE{Distributions}{%
		Artemiadis:FAA-89-311%
		}.
\NAMECITE{divisibility}{%
		Carasso:PSM-91-273%
		}.
\NAMECITE{Domain}{%
		Tijhuis:FAA-89-273%
		}.
\NAMECITE{dynamical}{%
		Brown:PSM-91-207%
		}.


\NAMECITE{Effects}{%
		Cullen:FAA-89-499%
		}.
\NAMECITE{Electromagnetic}{%
		Tijhuis:FAA-89-273%
		}.
\NAMECITE{Electromagnetics}{%
		Ponnapalli:FAA-89-201%
		}.
\NAMECITE{Empirical}{%
		Capar:PSM-91-517%
		}.
\NAMECITE{Energy}{%
		Unsal:FAA-89-59%
		}.
\NAMECITE{entropy}{%
		Bisbas:PSM-91-663%
		}.
\NAMECITE{environmental}{%
		Christakos:PSM-91-287%
		}.
\NAMECITE{equations}{%
		Cannarsa:PSM-91-617%
		}.
\NAMECITE{equivalent}{%
		Koumandos:PSM-91-605%
		}.
\NAMECITE{Estimate}{%
		Shapiro:FAA-89-563%
		}.
\NAMECITE{Estimation}{%
		Benedetto:FAA-89-143%
		}.
\NAMECITE{{Eu}{}clid{}ean}{%
		Kovalyov:FAA-89-41%
		}.
\NAMECITE{Even}{%
		Tuzunalp:FAA-89-261%
		}.
\NAMECITE{Expansions}{%
		Heil:FAA-89-441%
		}.
\NAMECITE{Extension}{%
		Gabardo:PSM-91-543%
		}.
\NAMECITE{Extensions}{%
		Carton-Lebrun:FAA-89-579%
		}.
\NAMECITE{Extracting}{%
		Hua:FAA-89-183%
		}.


\NAMECITE{factorization}{%
		Papoulis:PSM-91-247%
		}.
\NAMECITE{{FFT}}{%
		Ponnapalli:FAA-89-201%
		}.
\NAMECITE{fields}{%
		Chou:PSM-91-343%
		}.
\NAMECITE{Finite}{%
		Unsal:FAA-89-59%
		}.
\NAMECITE{Fixed}{%
		Kedem:PSM-91-573%
		}.
\NAMECITE{{Fourier}}{%
		Bjorck:FAA-89-131%
		}.
\NAMECITE{fractals}{%
		Cabrelli:PSM-91-163%
		}.
\NAMECITE{Frames}{%
		Feichtinger:FAA-89-427%
		}.
\NAMECITE{Function}{%
		Hua:FAA-89-183%
		}.
\NAMECITE{Functional}{%
		Gurkanli:FAA-89-643%
		}.
\NAMECITE{Functions}{%
		Artemiadis:FAA-89-311%
		}.
\NAMECITE{fuzzy}{%
		Cabrelli:PSM-91-163%
		}.


\NAMECITE{Gabor}{%
		Heil:FAA-89-441,%
		Suter:PSM-91-217%
		}.
\NAMECITE{Generalized}{%
		Hua:FAA-89-183%
		}.
\NAMECITE{Generation}{%
		Sarkar:PSM-91-263%
		}.
\NAMECITE{geometries}{%
		Keenan:PSM-91-469%
		}.
\NAMECITE{geometry}{%
		Piccioni:PSM-91-669%
		}.
\NAMECITE{Gradient}{%
		Ponnapalli:FAA-89-201%
		}.
\NAMECITE{Groupoids}{%
		Seitz:FAA-89-661%
		}.
\NAMECITE{Groups}{%
		Karanikas:FAA-89-653%
		}.
\NAMECITE{Growth}{%
		Jakimovski:FAA-89-73%
		}.


\NAMECITE{{Hamilton}}{%
		Cannarsa:PSM-91-617%
		}.
\NAMECITE{{Hamilton}-{Jacobi}}{%
		Cannarsa:PSM-91-617%
		}.
\NAMECITE{harmonic}{%
		Cullen:FAA-89-499%
		}.
\NAMECITE{High}{%
		Lahr:FAA-89-463%
		}.
\NAMECITE{High-resolution}{%
		Lahr:FAA-89-463%
		}.
\NAMECITE{Holographic}{%
		Schempp:FAA-89-507%
		}.
\NAMECITE{holography}{%
		Schempp:PSM-91-383%
		}.


\NAMECITE{Identification}{%
		Papoulis:FAA-89-377%
		}.
\NAMECITE{Image}{%
		Schempp:FAA-89-507%
		}.
\NAMECITE{images}{%
		Suter:PSM-91-217%
		}.
\NAMECITE{Inequalities}{%
		Benedetto:FAA-89-143%
		}.
\NAMECITE{inference}{%
		Capar:PSM-91-517%
		}.
\NAMECITE{infinite}{%
		Cannarsa:PSM-91-617%
		}.
\NAMECITE{information}{%
		Sarkar:PSM-91-263%
		}.
\NAMECITE{Innovations}{%
		Papoulis:PSM-91-247%
		}.
\NAMECITE{{Institute}}{%
		Byrnes:FAA-89%
		}.
\NAMECITE{integration}{%
		Blei:PSM-91-649%
		}.
\NAMECITE{Interdependencies}{%
		Blei:FAA-89-631%
		}.
\NAMECITE{Interpolation}{%
		Jakimovski:FAA-89-73%
		}.
\NAMECITE{Invariance}{%
		Roy:FAA-89-317%
		}.
\NAMECITE{Invariant}{%
		Madych:FAA-89-455%
		}.
\NAMECITE{inverse}{%
		Cabrelli:PSM-91-163%
		}.
\NAMECITE{Irregular}{%
		Feichtinger:FAA-89-427%
		}.
\NAMECITE{iterated}{%
		Piccioni:PSM-91-669%
		}.


\NAMECITE{{Jacobi}}{%
		Cannarsa:PSM-91-617%
		}.


\NAMECITE{{Laplace}}{%
		Hoop:FAA-89-387%
		}.
\NAMECITE{Layered}{%
		Hoop:FAA-89-387%
		}.
\NAMECITE{Limit}{%
		Ingolfsson:FAA-89-29%
		}.
\NAMECITE{Limited}{%
		Grochenig:FAA-89-251%
		}.
\NAMECITE{Linear}{%
		Suter:PSM-91-217%
		}.


\NAMECITE{mathematical}{%
		Newman:PSM-91-535%
		}.
\NAMECITE{Maximum}{%
		Benke:FAA-89-83%
		}.
\NAMECITE{Measurements}{%
		Blei:FAA-89-631%
		}.
\NAMECITE{measures}{%
		Bisbas:PSM-91-663%
		}.
\NAMECITE{Media}{%
		Hoop:FAA-89-387%
		}.
\NAMECITE{Method}{%
		Hua:FAA-89-183%
		}.
\NAMECITE{Methods}{%
		Hauptman:FAA-89-3%
		}.
\NAMECITE{Metrizable}{%
		Karanikas:FAA-89-653%
		}.
\NAMECITE{Minimal}{%
		Hauptman:FAA-89-3%
		}.
\NAMECITE{mixed}{%
		Kedem:PSM-91-573%
		}.
\NAMECITE{Modulus}{%
		Benke:FAA-89-83%
		}.
\NAMECITE{Monte}{%
		Korner:PSM-91-593%
		}.
\NAMECITE{Multiband}{%
		Dodson:FAA-89-483%
		}.
\NAMECITE{Multifractal}{%
		Peyriere:PSM-91-175%
		}.
\NAMECITE{Multiresolution}{%
		Madych:PSM-91-233%
		}.
\NAMECITE{Multiscale}{%
		Madych:FAA-89-455%
		}.


\NAMECITE{narrowband}{%
		Sarkar:PSM-91-263%
		}.
\NAMECITE{{NATO}}{%
		Byrnes:FAA-89%
		}.
\NAMECITE{networks}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{neural}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{Neurocomputer}{%
		Schempp:FAA-89-507%
		}.
\NAMECITE{non}{%
		Kovalyov:FAA-89-41%
		}.
\NAMECITE{non-{Eu}{}clid{}ean}{%
		Kovalyov:FAA-89-41%
		}.
\NAMECITE{non-linear}{%
		Suter:PSM-91-217%
		}.
\NAMECITE{Normal}{%
		Brown:PSM-91-207%
		}.
\NAMECITE{Nuclear}{%
		Kallianpur:PSM-91-631%
		}.
\NAMECITE{Number}{%
		Schroeder:FAA-89-101%
		}.
\NAMECITE{numbers}{%
		Brown:PSM-91-207%
		}.
\NAMECITE{Numerical}{%
		Tijhuis:FAA-89-273%
		}.


\NAMECITE{Odd}{%
		Tuzunalp:FAA-89-261%
		}.
\NAMECITE{Operator}{%
		Shapiro:FAA-89-563%
		}.
\NAMECITE{optimal}{%
		Cannarsa:PSM-91-617%
		}.
\NAMECITE{order}{%
		Cannarsa:PSM-91-617%
		}.
\NAMECITE{organising}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{other}{%
		Cabrelli:PSM-91-163%
		}.


\NAMECITE{{Paley}}{%
		Kahane:PSM-91-481%
		}.
\NAMECITE{paper}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{part}{%
		Newman:PSM-91-535%
		}.
\NAMECITE{partial}{%
		Jaffard:PSM-91-3%
		}.
\NAMECITE{Parts}{%
		Tuzunalp:FAA-89-261%
		}.
\NAMECITE{pattern}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{Pencil}{%
		Hua:FAA-89-183%
		}.
\NAMECITE{Pencil-of-Function}{%
		Hua:FAA-89-183%
		}.
\NAMECITE{periodograms}{%
		Korner:PSM-91-593%
		}.
\NAMECITE{phase}{%
		Saffari:PSM-91-555%
		}.
\NAMECITE{Physics}{%
		Kovalyov:FAA-89-41%
		}.
\NAMECITE{{Plancherel}}{%
		Evans:FAA-89-613%
		}.
\NAMECITE{points}{%
		Kedem:PSM-91-573%
		}.
\NAMECITE{Poles}{%
		Hua:FAA-89-183%
		}.
\NAMECITE{Polynomials}{%
		Benke:FAA-89-83%
		}.
\NAMECITE{positive}{%
		Gabardo:PSM-91-543%
		}.
\NAMECITE{positive-definite}{%
		Gabardo:PSM-91-543%
		}.
\NAMECITE{Power}{%
		Jakimovski:FAA-89-73%
		}.
\NAMECITE{prediction}{%
		Papoulis:PSM-91-247%
		}.
\NAMECITE{Principle}{%
		Benedetto:FAA-89-143%
		}.
\NAMECITE{probabilistic}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{probability}{%
		Newman:PSM-91-535%
		}.
\NAMECITE{problem}{%
		Cabrelli:PSM-91-163%
		}.
\NAMECITE{Problems}{%
		Ponnapalli:FAA-89-201%
		}.
\NAMECITE{Proceedings}{%
		Byrnes:FAA-89%
		}.
\NAMECITE{Processing}{%
		Ponnapalli:FAA-89-201%
		}.
\NAMECITE{Products}{%
		Karanikas:FAA-89-653%
		}.
\NAMECITE{Propagation}{%
		Hoop:FAA-89-387%
		}.
\NAMECITE{Properties}{%
		Newman:FAA-89-79%
		}.


\NAMECITE{Quantum}{%
		Schempp:PSM-91-383%
		}.


\NAMECITE{radial}{%
		Gabardo:PSM-91-543%
		}.
\NAMECITE{{Radon}}{%
		Walnut:PSM-91-187%
		}.
\NAMECITE{random}{%
		Chou:PSM-91-343%
		}.
\NAMECITE{rate}{%
		Papoulis:PSM-91-247%
		}.
\NAMECITE{Rates}{%
		Dodson:FAA-89-483%
		}.
\NAMECITE{ray}{%
		Hauptman:FAA-89-3%
		}.
\NAMECITE{recognition}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{Recurrence}{%
		Lahr:FAA-89-463%
		}.
\NAMECITE{Reflector}{%
		Brown:FAA-89-367%
		}.
\NAMECITE{Relations}{%
		Lahr:FAA-89-463%
		}.
\NAMECITE{research}{%
		Christakos:PSM-91-287%
		}.
\NAMECITE{resolution}{%
		Lahr:FAA-89-463%
		}.
\NAMECITE{Responses}{%
		Hua:FAA-89-183%
		}.
\NAMECITE{Restriction}{%
		Carton-Lebrun:FAA-89-579%
		}.
\NAMECITE{Results}{%
		Artemiadis:FAA-89-311%
		}.
\NAMECITE{{Riesz}}{%
		Karanikas:FAA-89-653%
		}.
\NAMECITE{roots}{%
		Bjorck:FAA-89-131%
		}.


\NAMECITE{Sampling}{%
		Dodson:FAA-89-483%
		}.
\NAMECITE{scaling}{%
		Madych:PSM-91-233%
		}.
\NAMECITE{Scattering}{%
		Tijhuis:FAA-89-273%
		}.
\NAMECITE{{Schottky}}{%
		Cullen:FAA-89-499%
		}.
\NAMECITE{{Schottky}-{Barrier}}{%
		Cullen:FAA-89-499%
		}.
\NAMECITE{Science}{%
		Schroeder:FAA-89-101%
		}.
\NAMECITE{Second}{%
		Cullen:FAA-89-499%
		}.
\NAMECITE{Second-harmonic}{%
		Cullen:FAA-89-499%
		}.
\NAMECITE{self}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{self-organising}{%
		Nandagopal:PSM-91-369%
		}.
\NAMECITE{Semi}{%
		Ingolfsson:FAA-89-29%
		}.
\NAMECITE{Semi-Classical}{%
		Ingolfsson:FAA-89-29%
		}.
\NAMECITE{sequence}{%
		Capar:PSM-91-517%
		}.
\NAMECITE{Series}{%
		Artemiadis:FAA-89-311%
		}.
\NAMECITE{sets}{%
		Cabrelli:PSM-91-163%
		}.
\NAMECITE{Shape}{%
		Kennedy:FAA-89-17%
		}.
\NAMECITE{Sharp}{%
		Grochenig:PSM-91-323%
		}.
\NAMECITE{Signal}{%
		Ponnapalli:FAA-89-201%
		}.
\NAMECITE{Signals}{%
		Dodson:FAA-89-483%
		}.
\NAMECITE{singular}{%
		Carasso:PSM-91-273%
		}.
\NAMECITE{singularities}{%
		Mallat:PSM-91-47%
		}.
\NAMECITE{Solution}{%
		Tijhuis:FAA-89-273%
		}.
\NAMECITE{solving}{%
		Heil:PSM-91-15%
		}.
\NAMECITE{some}{%
		Gurkanli:FAA-89-643%
		}.
\NAMECITE{Space}{%
		Kovalyov:FAA-89-41%
		}.
\NAMECITE{space-valued}{%
		Kallianpur:PSM-91-631%
		}.
\NAMECITE{Spaces}{%
		Gurkanli:FAA-89-643%
		}.
\NAMECITE{spatiotemporal}{%
		Christakos:PSM-91-287%
		}.
\NAMECITE{Spectral}{%
		Lahr:FAA-89-463%
		}.
\NAMECITE{Spectras}{%
		Gurkanli:FAA-89-643%
		}.
\NAMECITE{Spectrum}{%
		Benedetto:FAA-89-143%
		}.
\NAMECITE{Spline}{%
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\NAMECITE{Wave}{%
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\NAMECITE{{X}}{%
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\NAMECITE{{Zygmund}}{%
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