Nyquist barrier - not for all! Jaan Pelt Tartu Observatory

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Nyquist barrier - not for all! Jaan Pelt Tartu Observatory Monday, 7. October 2013 Information and computer science forum

description

Nyquist barrier - not for all! Jaan Pelt Tartu Observatory. Monday, 7. October 2013 Information and computer science forum. Peep Kalv looking through astrophotographic plate (1964-65). http://www.aai.ee/~pelt/. Ilkka Tuominen. Gravitational lenses. Rudy Schild and Sjur Refsdal - PowerPoint PPT Presentation

Transcript of Nyquist barrier - not for all! Jaan Pelt Tartu Observatory

Page 1: Nyquist barrier - not for all! Jaan Pelt Tartu Observatory

Nyquist barrier - not for all!

Jaan Pelt

Tartu Observatory

Monday, 7. October 2013

Information and computer science forum

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Peep Kalv looking through astrophotographic plate (1964-65).

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http://www.aai.ee/~pelt/

Ilkka Tuominen

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Gravitational lenses

Rudy Schild and Sjur Refsdalin wild Estonia

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Four views

• Time (AR, ARMA, etc)

• Frequency (Power spectrum)

• Time-Frequency (Wavelets, Wigner TF etc)

• Phase dispersion

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Phase-process diagram (folding)

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Live demo

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Weights G are larger than zero when phases of two points in pairare similar, or:

G=0

G=1

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How to compute?

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Multiperiodic processes

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An example

???

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Why?

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Carrier fitCarrier frequency

Splines

Function with sparse spectra.

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Harry Nyquist

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Comb function and its Fourier transform

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Fourier transform

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Sampling

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Spectrum replication

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Reconstruction

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Aliasing

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Simple harmonic, regular sampling

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Simple harmonic, irregular sampling

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Frequency to the right from Nyquist limit

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Here it is !

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From “Numerical Recipes”

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They tell us…

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Many possibilities

• Some intervals are shorter (as Press et al).

• Mean sampling step is to be computed.

• Statistical argument, from N data points you can not get more than N/2 spectrum points.

• Every time point set is a subset of some regular grid.

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Phases

Arbitrary trial period (frequency) Correct period (frequency)

Observed magnitudes

Phases

s – frequency, P=1/s - period

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Old story

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Typical “string length spectrum”

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Horse racing argument

For “string length” method maximal return time is N! – number of permutations (N is number of data points).

For other methods return time scales as NN.

This comes from Poincare return theory.

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Noiseless case, simple power spectrum.

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10% noise

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25% noise

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Comments

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More comments

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Left from Nyquist limit

Bandlimited process

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Ohhh…, no….

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But still?

Derivatives of bandlimited functions are also bandlimited! Look at red dots! Zeros are maxima and minima after differentiation.

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First hints

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Aharonov again

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Berry is more explicit

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Abstract

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Kempf is the best seller!

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Another example

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Spectrum of it, no hint of SO-s

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Research programme?

1. Super-resolution using super-oscillations. Already done – using nanohole patterns

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Antenna beamforming

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But sparse and random array?

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Transplanckian frequencies

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Superoscillating particles

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And finally…

Where are the super-oscillations here?

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Gateway to superoscillations:

PROFESSOR SIR MICHAEL VICTOR BERRY, FRS

http://michaelberryphysics.wordpress.com/