The SERENDIP, SEVENDIP, Astropulse, and SPOCK SETI Programs

Slides:



Advertisements
Similar presentations
Ben Barsdell Matthew Bailes Christopher Fluke David Barnes.
Advertisements

Team Presentation July 22, Jodrell Bank is the original arboretum for Manchester University. Immediately after World War II, first radio telescope.
An Optical Receiver for Interplanetary Communications Jeremy Bailey.
1 Hough transform Some Fourier basics: –Nyquist frequency: 1/2 , with  the difference between time samples. If signal is bandwidth limited below Nyquist.
Jim Cordes and Dan Werthimer And Five Milliion Volunteers in 226 countries
The Search for Spock The Scientific Search for Extraterrestrial Life Or Graur Student Seminar
Astronomy190 - Topics in Astronomy Astronomy and Astrobiology Lecture 21: Search for Extraterrestrial Intelligence Ty Robinson.
Life in the Universe. Conditions may be right for primitive life to exist on Mars (or existed in the past) and Europa. Possibly some complex molecules.
The Transient Radio Sky to be Revealed by the SKA Jim Cordes Cornell University AAS Meeting Washington, DC 8 January 2002.
SETI: Search Strategies & Current Plans Jim Cordes 23 September 2002 Motivation for searching we’re here life expected to be common (especially microbial.
Transient SETI Dan Werthimer University of California, Berkeley
What does do? Mini-project for CSE 260 Qian Peng 15 November 2001 Ref.
Jamie Holder School of Physics and Astronomy, University of Leeds, U.K Optical SETI at Leeds Using Cherenkov Light Buckets as Optical SETI Detectors RAS.
10/14/03Prof. Lynn Cominsky1 Class web site: Office: Darwin 329A and NASA E/PO (707) Best way to.
Sunny Gleason COM S 717 November 29, 2001 (Based on the article, Massively Distributed Computing for SETI.”)
Group F – Liam Duffy, Darsh Kodwani and Stuart Keenan.
Extra-terrestrial Civilizations: Interstellar Radio Communications.
1 SKA and the Future of Astrobiology and SETI Claudio Maccone Co-Vice Chair, SETI Permanent Study Group, International Academy of Astronautics, and IASF-INAF.
Abstract Pulsars are highly magnetized, rotating neutron stars that emit a beam of electromagnetic radiation. The radiation can only be observed when the.
SETI on the SKA Dan Werthimer University of California, Berkeley
Radio Astronomy and SETI
NSCI 314 LIFE IN THE COSMOS 15 - THE DRAKE EQUATION: HOW COMMON ARE EXTRATERRESTRIAL CIVILIZATIONS THAT ARE SUFFICIENTLY TECHNOLOGICALLY ADVANCED THAT.
NSCI 314 LIFE IN THE COSMOS 16 - INTERSTELLAR COMUNICATION Dr. Karen Kolehmainen Department of Physics, CSUSB
SETI Search for Extra Terrestrial Intelligence FYOS Lecture 8.
Search for Extraterrestrial Life PHY 100. How life emerged on earth  Amino acids, “building blocks of life” form via chemical reactions  With help of.
Short Time Fourier Transform-based method for fast transients detection Centre for eResearch, University of Auckland, New Zealand,
Medium-Rare Earth. Rare Earth Right distance from star Right mass of star Stable planetary orbits Right planetary mass Jupiter-like neighbor Plate tectonics.
LIGO-G Z GWDAW10, December 16, S3 Final Results Bruce Allen, for the LIGO Scientific Collaboration.
Final Exam Comprehensive –Most questions from Ch , some from Ch. 4-14, few from Ch. E-3 Multiple choice plus few short answer questions Please study:
Real-time Acquisition and Processing of Data from the GMRT Pulsar Back- ends Ramchandra M. Dabade (VNIT, Nagpur) Guided By, Yashwant Gupta.
HOW DO WE SEARCH FOR LIFE IN THE UNIVERSE?. Necessary Assumptions All civilizations follow a certain set of broad universal pathways. There are civilizations.
Pulsar surveys at Arecibo and Green Bank David Champion Gravity Wave Meeting, Marsfield, Dec 2007.
Intrinsic Short Term Variability in W3-OH and W49N Hydroxyl Masers W.M. Goss National Radio Astronomy Observatory Socorro, New Mexico, USA A.A. Deshpande,
LIGO-G D Status of Stochastic Search with LIGO Vuk Mandic on behalf of LIGO Scientific Collaboration Caltech GWDAW-10, 12/15/05.
Observing Strategies at cm wavelengths Making good decisions Jessica Chapman Synthesis Workshop May 2003.
IR, Visible and Radio SETI Andrew Siemion, David Anderson, Bob Bankay, Henry Chen, Jeff Cobb, Griffin Foster, Andrew Howard, Eric Korpela,
SETI. Extra Terrestrial Intelligence Is there intelligent life on other planets? If so, –Can we find them? –Can we try to communicate? SETI is the Search.
LIGO-G Z Peter Shawhan (University of Maryland) for the LIGO Scientific Collaboration Special thanks to Michael Landry and Bruce Allen Eastern.
Exploring the Unknown with CASPER Instrumentation Andrew Siemion CASPER Workshop 2011.
OSETI with MAGIC IntroductionIntroduction Radio SETIRadio SETI Optical SETIOptical SETI OSETI with MAGICOSETI with MAGIC SummarySummary July 2004.
NSCI 314 LIFE IN THE COSMOS 16 - INTERSTELLAR COMMUNICATION II Dr. Karen Kolehmainen Department of Physics, CSUSB
ASTR368 Exoplanet Detections. Kepler.
SETI The search for extraterrestrial Intelligence.
Volunteer Computing: SETI and Beyond David P. Anderson University of California, Berkeley 7 June 2007.
Eyes on the Polarized Sky, Feet on the Ground
Nicolas Fagnoni – Cosmology on Safari – 14th February 2017
Using the GAVRT Radio Telescope: The SETI Project
Finding the next Galactic extragalactic FRB
Goal: To understand life in our universe.
A 2 veto for Continuous Wave Searches
Chem. 133 – 3/14 Lecture.
Searching for pulsars using the Hough transform
Search for Extra-Terrestrial Intelligence
High School Teachers 2006.
David P. Anderson Space Sciences Lab UC Berkeley LASER
Searching FRB with Jiamusi-66m Radio Telescope
Goal: To understand intelligent life in our universe.
Search for Extra-Terrestrial Intelligence
A.M. Sintes for the pulgroup
Grid Computing Colton Lewis.
Gravitational Waves and Pulsar Timing
Pulsar Timing with ASKAP Simon Johnston ATNF, CSIRO
An Arecibo HI 21-cm Absorption Survey of Rich Abell Clusters
Pulsar and Transient Science with the 12m Antenna
Class 10: Water/Life on Other Planets.
Coherent Coincident Analysis of LIGO Burst Candidates
The Quest for Extraterrestrial Intelligence
Pulsar Data II Single-Pulse Plots
Pulsar Data II Single-Pulse Plots
Presentation transcript:

The SETI@home, SERENDIP, SEVENDIP, Astropulse, and SPOCK SETI Programs ‘Dan Werthimer, Dave Anderson, Jeff Cobb, Paul Demorest, Eric Korpela, Cecile Kim, Geoff Marcy University of California, Berkeley http://seti.berkeley.edu/

6.jpg

7.jpg

NOT FUNDED 1

8.jpg

NOT FUNDED 1

9.jpg

NOT FUNDED 1

17.jpg Retype captions?

Porno in space: FUNDED! 1

Drake Equation N=R fs fp ne fl fi fc L N = number of communicating civilizations in our galaxy

11.jpg

Planet Detection

13.jpg

15.jpg

19.jpg

18.jpg Retype captions

First Radio SETI Nikola Tesla (1899) Guglielmo Marconi (1920) Announces “coherent signals from Mars” Guglielmo Marconi (1920) Strange signals from ET Frank Drake (1960) Project Ozma one channel, 1420-1420.4 MHz

Signal Types 1. Artifact (radio, radar, ~TV, ????) 2. Deliberate (easy to decode, pictures, language lessons) First civilization we contact is likely to be a billion years ahead of us.

Targeted Search Strategy: Project Phoenix - Seti Institute Sky Survey Strategy: Serendip, SETI@home - UC Berkeley Beta - Harvard Southern Serendip - Australia Meta II - Argentina Seti Italia - Medicina Obser.

Quick History of Berkeley SETI Radio SETI SERENDIP Search for Extraterrestrial Radio Emissions from Nearby Developed Intelligent Populations SERENDIP I-III (1979-1997) SERENDIP IV (1997-) SERENDIP V (2004-)

The Berkeley Radio SETI Family Tree SERENDIP SERENDIP II OSU SERENDIP III SETI Italia SETI@home Data Recorder SETI@home Clients SERENDIP IV Southern SERENDIP SETHI@Berkeley HI Survey AstroPulse Pulse Survey SETI@home II Data Recorder SETI@home II Clients SERENDIP V

SETI Programs at the University of California

22.jpg

23.jpg

24.jpg

25.jpg

26.jpg

SERENDIP IV 168M channels 100 MHz Band centered on 1420 MHz Photos Courtesy NAIC Arecibo Observatory, a facility of the NSF 168M channels 100 MHz Band centered on 1420 MHz Carriage House 1 line feed Operating since 1997

28.jpg

29.jpg

40.jpg

Why SETI@home? Coherent Doppler drift correction Narrower Channel Width->Higher Sensitivity Variable bandwidth/time resolution Search for multiple signal types Gaussian beam fitting Search for repeating pulses Problem: Requires TFLOP/s processing power. Solution: Distributed Computing

35.jpg

36.jpg

37.jpg

The SETI@home Client

SETI@home Statistics TOTAL RATE

34.jpg

Structure of SETI@home Tapes from Arecibo Online Science Database 3.8 Million Volunteers The Internet Work Unit Storage Data splitters Volunteer Statistics Master Result Verification Candidate Identification Web Server Data Server

32.jpg

33.jpg

The Input and Output 1 Work-Unit=9.8 kHz x 220 samples (107 sec.) 256 Workunits across 2.5 MHz band centered on 1420.0 MHz. Workunits overlap in time by ~25 sec. Each workunit sent to multiple computers for result verification Typically 4 TFLOP/workunit. Output=Typically ~5 potential signals.

Spikes Power distribution in the Fourier transformed data is exponential if no RFI. SPIKE: Any bin in the spectrum above 22X the mean power (7.8x10-25 W/m2)

38.jpg

39.jpg

Gaussians Weighted 2 fit to beam profile (vs time). Gaussian must exceed a power and 2 threshold Score inversely proportional to probability of arising due to noise Sensitivity 8.4x10-25 W/m2

Triplets Three evenly spaced spikes above 7.75X the mean power. (5.3X10-25 W/m2)

Pulses Modified Fast folding algorithm w/ dynamic threshold Logarithmically spaced periods from 3ms to 35s Sensitivity as low as 10-26 J/m2

Candidate Identification Candidate: A signal or group of signals Within a positional window (~1 beamwidth typ.) Within a frequency window (variable) Above a score or power threshold (variable) With time separation » typical transient RFI timescale Score: Relative ranking of a candidate’s probability of arising due to random noise. Should be independent of signal type Can also include probability of coincidence /w celestial objects

Gaussian Candidates

AstroPulse Sky survey Good time resolution DM range Sensitivity Covers decs 0 to 30 ~3 years of data recorded so far. Good time resolution Sensitive to 0.4 µs radio pulses at 21 cm DM range -100 to +100 pc/cm3 Sensitivity 10-18 W/m2 peak (Coherent de-dispersion)

Pulsed vs. CW Concentrating power into short bursts can be more efficient than a “constantly on” transmitter. Pulsed signals can be easier to see above background noise.

Dispersion … eventually becoming very weak. However, we can correct for dispersion ...

AstroPulse Only ~1.5 searches for single pulses on µs timescale before (O’Sullivan, Phinney) Pulsar searches: ms time scales, folded SETI@home: 0.8 ms single pulses. With interesting astrophysics as well as SETI applications. Evaporating primordial black holes? Pulsars, Other astrophysical exotica?

Conclusion: We need more computers! Computation … but it takes a lot of CPU time! To search DMs up to 100 pc/cm3 in real time, we need about 500 GigaFLOPs. (This would take ~1000 years of your PC working full time) Conclusion: We need more computers!

BOINC Berkeley Open Infrastructure for Network Computing General-purpose distributed computing framework. Open source. Will make distributed computing accessible to those who need it. (Starting from scratch is hard!)

AstroPulse/BOINC AstroPulse will be the first to use BOINC. It is a good “beta-test” application: Simple data analysis/reduction. “Only” needs a few thousand computers. Other projects which plan to use BOINC: SETI@home II Global climate modeling/prediction (Oxford)

AstroPulse Testing Sample batch of data run through shows expected noise characteristics, and little else … … so (hopefully) little RFI contamination for this type of signal.

50.jpg

HI Column Density

OPTICAL SETI OPTICAL PULSE SEARCH Pulsed laser power output continues to grow. Petawatt pulses achieved at Livermore Labs. (Mjoule in 1nS) can detect at earth technology at 1Kpc little background noise, even from bright stars in whole visible band

45.jpg

46.jpg

OSETI Detector 3-Photomultiplier fast coincidence detector Sensitive to 1ns pulses Low background False alarm rate: 1 per 300 hours (10-6 Hz) Double false alarm rate: 1 per 600 years! Good sensitivity 10-8 W/m2 peak 10-19 W/m2 average

Optical SETI Uses Leuschner Observatory (UCB) Targeted Search Automated 0.8m telescope Targeted Search Nearby F,G,K,M stars ~2,000 stars observed so far Soon to include galaxies

44.jpg

Amy Reines and Geoff Marcy 47.jpg

10-meter Keck Telescope Survey: 650 F8 – M5 V, IV Hipparcos V < 8.5 B-V > 0.55 (F8V) Sep > 2 arcsec Age > 2 Gyr

Doppler Instruments Echelle Spectrometer Resolution: 60,000 Iodine Abs. Cell. Superimpose I2 lines Wavelength Calib.

43.jpg

42.jpg

Piggyback ALFA Sky Survey SETI Instruments Dedicated spectrometer (SERENDIP V) 300 MHz bandwidth, 2 pols, 7 beams 5 * 109 channels, 0.8 Hz resolution SETI@home II data recorder 10 MHz, 1 pol, 7 beams Steps across 300 MHz band

Piggyback ALFA Sky Survey Improved sensitivity Tsys, integration time Uniform sky sampling galactic plane concentration Multibeam RFI rejection Larger Bandwidth

5.jpg

41.jpg

Our Generous Sponsors The Planetary Society The University of California Sun Microsystems Friends of SETI@home Network Appliance Fujifilm IBM Quantum HP Xilinx The SETI Institute Informix EDT Netscreen Intel O’Reilly & Associates SpaceSounds Dillon Engineering NAIC, Arecibo Observatory ~4 million volunteers Maybe, someday, the U.S. Government

SETI HAIKU

Seti.berkeley.edu