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Page 1: Power Spectrum Estimation in Theory and in Practice

Power Spectrum Estimation in Theory and

in Practice

Adrian Liu, MIT

Page 2: Power Spectrum Estimation in Theory and in Practice

What we would like to do

Inverse noise and foreground covariance

matrix

Vector containing

measurement

Page 3: Power Spectrum Estimation in Theory and in Practice

What we would like to do

Bandpower at k“Geometry” -- Fourier

transform, binningNoise/residual

foreground bias removal

Page 4: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless

CleanedData

RawDataCleaning

Page 5: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars

Page 6: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars

100

0.02 0.04 0.060.08

101

10 mK

1 K100 mK

3.0

2.5

2.0

1.5

1Log10 T(in mK)

Errors using Line of Sight Method

AL, Tegmark, Phys. Rev. D 83, 103006 (2011)

Page 7: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars

100

0.02 0.04 0.060.08

101

<10 mK

130 mK

3.0

2.5

2.0

1.5

1Log10 T(in mK)

Errors using Inverse Variance Method

30 mK

AL, Tegmark, Phys. Rev. D 83, 103006 (2011)

Page 8: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars• Smaller “horizontal” error bars

Page 9: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars• Smaller “horizontal” error bars

100

101

10-210-110010-1

1.0

0.60.50.40.30.20.1

0.70.80.9

AL, Tegm

ark, Phys. Rev. D

83, 103006 (2011)

Page 10: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars• Smaller “horizontal” error bars

100

101

10-210-110010-1

1.0

0.60.50.40.30.20.1

0.70.80.9

AL, Tegm

ark, Phys. Rev. D

83, 103006 (2011)

Page 11: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars• Smaller “horizontal” error bars• No additive noise/foreground bias

Page 12: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars• Smaller “horizontal” error bars• No additive noise/foreground bias• A systematic framework for evaluating

error statistics

Page 13: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars• Smaller “horizontal” error bars• No additive noise/foreground bias• A systematic framework for evaluating

error statistics

BUT

Page 14: Power Spectrum Estimation in Theory and in Practice

Why we like this method• Lossless• Smaller “vertical” error bars• Smaller “horizontal” error bars• No additive noise/foreground bias• A systematic framework for evaluating

error statistics

BUT• Computationally expensive because

matrix inverse scales as O(n3). [Recall C-1x]

• Error statistics for 16 by 16 by 30 dataset takes CPU-months

Page 15: Power Spectrum Estimation in Theory and in Practice

Quicker alternatives

Full inverse variance

AL, Tegmark 2011

O(n log n) versionDillon, AL, Tegmark (in

prep.)

FFT + FKPWilliams, AL,

Hewitt, Tegmark

Page 16: Power Spectrum Estimation in Theory and in Practice

Quicker alternatives

Full inverse variance

AL, Tegmark 2011

O(n log n) versionDillon, AL, Tegmark (in

prep.)

FFT + FKPWilliams, AL,

Hewitt, Tegmark

Page 17: Power Spectrum Estimation in Theory and in Practice

O(n log n) version• Finding the matrix inverse C-1 is the

slowest step.

Page 18: Power Spectrum Estimation in Theory and in Practice

O(n log n) version• Finding the matrix inverse C-1 is the

slowest step.• Use the conjugate gradient method for

finding C-1x, which only requires being able to multiply by Cx.

Page 19: Power Spectrum Estimation in Theory and in Practice

O(n log n) version• Finding the matrix inverse C-1 is the

slowest step.• Use the conjugate gradient method for

finding C-1, which only requires being able to multiply by C.

• Multiplication is quick in basis where matrices are diagonal.

Page 20: Power Spectrum Estimation in Theory and in Practice

O(n log n) version• Finding the matrix inverse C-1 is the

slowest step.• Use the conjugate gradient method for

finding C-1, which only requires being able to multiply by C.

• Multiplication is quick in basis where matrices are diagonal.

• Need to multiply by C = Cnoise + Csync + Cps + …

Page 21: Power Spectrum Estimation in Theory and in Practice

Different components are diagonal in different

combinations of Fourier space

C = Cps + Csync + Cnoise + …

Real spatialFourier spectral

Fourier spatialFourier spectral

Real spatialReal

spectral

Page 22: Power Spectrum Estimation in Theory and in Practice

Comparison of Foreground Models

GSMOur

model

Eig

enva

lue

AL, Pritchard, Loeb, Tegmark, in prep.

Page 23: Power Spectrum Estimation in Theory and in Practice

Quicker alternatives

Full inverse variance

AL, Tegmark 2011

O(n log n) versionDillon, AL, Tegmark (in

prep.)

FFT + FKPWilliams, AL,

Hewitt, Tegmark

Page 24: Power Spectrum Estimation in Theory and in Practice

FKP + FFT version

Bandpower at k“Geometry” -- Fourier

transform, binningNoise/residual

foreground bias removal

Page 25: Power Spectrum Estimation in Theory and in Practice

FKP + FFT version• Foreground avoidance instead of

foreground subtraction.

100

0.02 0.04 0.060.08

101

10 mK

1 K100 mK

Page 26: Power Spectrum Estimation in Theory and in Practice

FKP + FFT version• Foreground avoidance instead of

foreground subtraction.• Use FFTs to get O(n log n) scaling,

adjusting for non-cubic geometry using weightings.

Page 27: Power Spectrum Estimation in Theory and in Practice

FKP + FFT version• Foreground avoidance instead of

foreground subtraction.• Use FFTs to get O(n log n) scaling,

adjusting for non-cubic geometry using weightings.

• Use Feldman-Kaiser-Peacock (FKP) approximation– Power estimates from neighboring k-cells

perfectly correlated and therefore redundant.– Power estimates from far away k-cells

uncorrelated.– Approximation encapsulated by FKP

weighting.– Optimal (same as full inverse variance

method) on scales much smaller than survey volume.

Page 28: Power Spectrum Estimation in Theory and in Practice

FKP + FFT version

100

0.02 0.04 0.060.08

101

10 mK

1 K100 mK

Page 29: Power Spectrum Estimation in Theory and in Practice

Summary

Full inverse variance

AL, Tegmark 2011

O(n log n) versionDillon, AL, Tegmark (in

prep.)

FFT + FKPWilliams, AL,

Hewitt, Tegmark