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Data Challenges in Astronomy: NASA’s Kepler Mission and the Search for Extrasolar Earths Jon M. Jenkins SETI Institute/NASA Ames Research Center Thursday September 22, 2011 STScI SAO
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The Kepler Mission What fraction of sun-like stars in our galaxy host potentially habitable Earth-size planets?
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How Hard is it to Find Good Planets? Earth or Venus 0.01% area of the Sun (1/10,000)
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Kepler Field Of View Credit: Carter Roberts
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Kepler: Big Data, Big Challenges Big Processing Challenges Instrument effects are large compared to signal of interest Observational noise is non-white and non-stationary ~100×10 6 tests per star for planetary signatures [O(N 2 )] Stellar variations are higher than expected Big Data: >150,000 target stars 6x10 6 pixels collected and stored per ½ hour ~40 GB downlinked each month >40×10 9 points in the time series over 3.5 years
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The Kepler Science Pipeline: From Pixels To Planets CAL Pixel Level Calibrations PA Photometric Analysis Sums Pixels Together/Measures Star Locations TPS Transiting Planet Search PDC Pre-Search Data Conditioning Removes Systematic Errors Raw Data TCEs: Threshold Crossing Events Corrected Light Curves Calibrated Pixels Raw Light Curves/ Centroids DV Data Validation Diagnostic Metrics CAL Pixel Level Calibrations PA Photometric Analysis Sums Pixels Together/Measures Star Locations PDC Pre-Search Data Conditioning Removes Systematic Errors TPS Transiting Planet Search DV Data Validation
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Image Data 0.09x0.09 degrees 80x80 pixels 6400 pixels total HAT-P-7b pixels 6.6x6.6 millidegrees 28 pixels collected Black = no data Scaled to show faint detail 1.13 (h) x1.22 (w) degrees
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Pixel Time Series
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What Do Stars Sound Like? HAT-P-7BAnother Star
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Data Challenge Number 1 Dealing with Instrumental Systematic Errors
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Correcting Systematic Errors CAL Pixel Level Calibrations PA Photometric Analysis Sums Pixels Together/Measures Star Locations TPS Transiting Planet Search PDC Pre-Search Data Conditioning Removes Systematic Errors Raw Data TCEs: Threshold Crossing Events Corrected Light Curves Calibrated Pixels Raw Light Curves/ Centroids DV Data Validation Diagnostic Metrics
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PDC Often Does a Good Job Bayesian approaches look promising!
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PDC Often Over-Fits Variable Stars
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PDC Is Fundamentally Flawed PDC co-trends against instrumental signatures using least squares (LS) approach LS attempts to explain all of a given time series, not just the part the model can explain well There is no way a simple LS fit can “put on the brakes” PDC often trades bulk RMS for increased noise at short time scales
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A Bayesian Solution Examine behavior of ensemble of stars responding to systematics Formulate prior probability distributions for model coefficients Maximize Posterior Distribution: “A Bayesian is one who, vaguely expecting a horse, and catching a glimpse of a donkey, strongly believes he has seen a mule.” Maximum LikelihoodPrior PDF
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A Much Better Result
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PDC MAP Example
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PDC MAP Example 2
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Data Challenge Number 2 Detecting Weak Transits Against Non-White, Non-Stationary Noise
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Detecting Transiting Planets CAL Pixel Level Calibrations PA Photometric Analysis Sums Pixels Together/Measures Star Locations TPS Transiting Planet Search PDC Pre-Search Data Conditioning Removes Systematic Errors Raw Data TCEs: Threshold Crossing Events Corrected Light Curves Calibrated Pixels Raw Light Curves/ Centroids DV Data Validation Diagnostic Metrics
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21 Matched Filtering: What Does This Mean?
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Detection Statistics Define Under H0: Under H1: If T , then choose H1 s w s+w TT
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Detection Statistics For Colored Noise w is (colored) Gaussian noise with autocorrelation matrix R x is the data s is the signal of interest Decide s is present if How do we determine R? If the noise is stationary, we can work in the frequency domain:
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Solar Variability
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PSDs for Solar-Like Variability Is stellar variability stationary? No! We must work in a joint time-frequency domain Wavelets are a natural choice High Solar Activity Low Solar Activity Detectable Energy
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A Wavelet-Based Approach Filter-Bank Implementation of an Overcomplete Wavelet Transform The time series x(n) is partitioned (filtered) into complementary channels: W X (i,n) = {h 1 (n) x(n), h 2 (n) x(n),…, h M (n) x(n)} = {x 1 (n), x 2 (n),…, x m (n)}
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A Wavelet-Based Approach
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Kepler-like Noise + Transits
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Single Transit Statistics
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Folded Transit Statistics
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Folded Statistics at Best-Matched Period
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Data Challenge Number 3 Excess Stellar Variability
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Image by Carter Roberts (1946-2008) Excess Stellar Variability Original Noise Budget (Kp=12): 14 ppm Shot Noise 10 ppm Instrument Noise 10 ppm Stellar Variability => 20 ppm Total Noise Reality (11.5 ≤ Kp ≤ 12.5) 17 ppm Shot Noise 13 ppm Instrument Noise 20 ppm Stellar Variability => ~29 ppm Total Noise
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Original expectations yielded ~65% completeness for Earth analogs at 3.5 years Completeness Vs. Time Expected
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Current expectations yield <5% completeness for Earth analogs at 3.5 years Expected Reality Completeness Vs. Time
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~65% completeness for 1.2-R e planets in same orbits at 3.5 years Expected Reality Completeness Vs. Time
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Kepler will recover >60% completeness for Earth analogs after 8 years Expected Reality Completeness Vs. Time
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20 ppm 30 ppm Kepler will detect virtually all Venus analogs within 8 years
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Kepler is revolutionizing the field of exoplanets Kepler data are in a class of their own with significant data challenges Huge dynamic range for measurements requires sophisticated Bayesian techniques for correcting systematic errors Planet detection requires an efficient, adaptive Conclusions method that accounts for non-white noise: wavelets fit the bill Kepler can reach its goal of detecting Earth-Sun analogs with an extended 8 year mission Each day we are getting closer and closer to finding an Earth-Sun analog
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Image by Carter Roberts (1946-2008) Music From the Stars
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Image by Carter Roberts (1946-2008) Music From the Stars (2) 41
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Image by Carter Roberts (1946-2008) Music From the Stars (3) 42
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Image by Carter Roberts (1946-2008) Music From the Stars (4) 43
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