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Untwinkling the Stars Improving Our View of the Universe with Adaptive Optics 26 August 2011 Elinor Gates UCO/Lick Observatory Center for Adaptive Optics Lick Observatory, Mount Hamilton, CA 9 Telescopes ranging in size from 0.5 m to 3 m "Observing stars through the Earth's atmosphere is like bird watching from the bottom of a swimming pool." -Remington P. S. Stone Why do stars twinkle? Robert Hooke suggested that stars twinkle because there are "small moving regions of the atmosphere having different refracting powers which act like lenses." (1665) Newton wrote that his telescope observations were limited by the fact that "the air through which we look is in perpetual Tremor... The only remedy is a most serene and quiet air, such as may perhaps be found on the tops of the highest mountains above the grosser clouds." Astronomer Horace Babcock, in 1953, proposed using a deformable optical element together with a wavefront sensor to compensate for atmospheric distortions. Only in the last 15 years has technology matured enough to make this possible. Slide Courtesy Claire Max Turbulence in the atmosphere limits the performance of astronomical telescopes • Turbulence is the reason why stars twinkle • More important for astronomy, turbulence spreads out the light from a star; makes it a blob rather than a point Even the largest ground-based astronomical telescopes have no better resolution than an 8" backyard telescope! Slide Courtesy Claire Max Turbulence arises in several places stratosphere tropopause 10-12 km wind flow over dome boundary layer ~ 1 km Heat sources w/in dome Slide Courtesy Claire Max Images of a bright star, Arcturus Lick Observatory, 1 m telescope Long exposure image Short exposure image “Perfect” image: diffraction limit of telescope Distant stars should resemble “points,” if it weren’t for turbulence in Earth’s atmosphere Slide Courtesy Claire Max There are Three ways to eliminate blurring due to the atmosphere 1. Get above the turbulence by going into space (Hubble Space Telescope) 2. Use computer post-processing of ground-based images: Speckle Imaging. Limited to relatively bright objects. 3. Use Adaptive Optics to compensate for turbulence using hardware: - Measure the blurring due to turbulence (up to 1000 times per second) - Then correct for effects of turbulence by changing the shape of a special "deformable mirror" behind the primary mirror of the telescope - Needs a reference star nearby to measure turbulence. Slide Courtesy Claire Max Space vs. Ground Based Telescopes Telescope: HST Shane Mirror Diameter: 2.4 m 3.0 m Resolution at 2.2 microns: 0.23 arcseconds 0.18 arcseconds Lick Observatory's Shane 3m telescope can see smaller structures than the Hubble Space Telescope when using Adaptive Optics. Space vs. Ground Based Telescopes Telescope: Keck JWST Mirror Diameter: 10 m 6.5 m Resolution at 2.2 microns: 0.055 arcseconds 0.085 arcseconds Keck Observatory's 10m telescope can see smaller structures than the planned James Webb Space Telescope when using Adaptive Optics. Schematic of adaptive optics system Feedback loop: next cycle corrects the (small) errors of the last cycle Slide Courtesy Claire Max Most deformable mirrors today have thin glass face-sheets Glass face-sheet Cables leading to mirror’s power supply (where voltage is applied) PZT or PMN actuators: get longer and shorter as voltage is changed Reflective coating (e.g. Aluminum) Slide Courtesy Claire Max Deformable mirrors come in many shapes and sizes Today: mirrors from Xinetics. From 13 to 900 actuators (degrees of freedom); 3 - 15 inches in diameter. Xinetics Inc.Devens, MA Future: very small mirrors (MEMS, LCDs); very large mirrors (replace secondary mirror of the telescope) Slide Courtesy Claire Max Adaptive optics system is usually behind main telescope mirror Example: AO system at Lick Observatory’s 3 m telescope Support for main telescope mirror Adaptive optics package under main mirror Slide Courtesy Claire Max What does a “real” adaptive optics system look like? Light from telescope Wavefront sensor Tip/Tilt Mirror Deformable mirror Infra-red camera Gemini North Adaptive Optics Animation QuickTime™ and a Sorenson Video decompressor are needed to see this picture. Adaptive optics in action Lick Observatory Adaptive Optics System Adaptive optics on 10-m Keck II Telescope: Factor of 10 increase in spatial resolution 9th magnitude star imaged in infrared light (1.6 mm) Without AO width = 0.34 arc sec With AO width = 0.039 arc sec Slide courtesy of Claire Max Often no bright star where you really need one! Reference Star Science Object Turbulence h Common Atmospheric Path Telescope Slide courtesy of Claire Max If there is no nearby star, make your own “star” using a laser Implementation Concept Lick Obs. Courtesy Laurie Hatch Slide courtesy of Claire Max How does a Sodium Laser make an Artificial Star? 60 miles up is a layer in the mesosphere containing metals, sodium, potassium, calcium. These metals are deposited by meteors burning up in the Earth’s atmosphere. Tune laser to emit 589 nm wavelength light. Sodium atoms absorb and are excited by laser. The atoms quickly de-excite, re-emitting the light, and create an artificial star wherever you need one. Slide courtesy of Claire Max Sodium Laser Guide Star at Keck II Science observations started in 2005. Image of sodium light taken from telescope very close to main telescope Light from Na layer at ~ 90 km Max. altitude of Rayleigh ~ 35 km Rayleigh scattered light Slide courtesy of Claire Max 87 Sylvia with Moonlets Romulus and Remus Franck Marchis, UC-Berkeley Discovery Image, ESO 8.2m VLT 2004 Aug 9 Aug-Sept 2004 Vesta Keck Observatory AO K-band Pyroxene narrow-band filter (1.99 micron wavelength) QuickTime™ and a YUV420 codec decompressor are needed to see this picture. Movie shows rotation over about 20 minutes Image 1.1 x 1.1 arcseconds Jupiter Imke de Pater, UC-Berkeley Left: False Color IR Composite Image (1.29, 1.58 , and 1.65 microns) Right: 5 micron detail of the Great Red Spot and Red Spot Jr. (Keck Observatory) Images of Io UL: Keck, 2.2 microns LL: Keck, 3.5 microns UR: Galileo space orbiter, Visible Light LR: Keck, No AO correction Titan Occultation Titan - Saturn’s largest moon Antonin Bouchez et al. 20 Dec 2001 QuickTime™ and a YUV420 codec decompressor are needed to see this picture. QuickTime™ and a YUV420 codec decompressor are needed to see this picture. Uranus with 3 Moons 17 October 2003, NGS, r0 ~ 18cm Uranus - New Ring Imke de Pater - UC Berkeley Discovered with HST, but imaging from Earth possible with Keck AO! Neptune in Infrared Light With Keck adaptive optics 2.3 arc sec Without adaptive optics May 24, 1999 June 27, 1999 l = 1.65 microns Slide courtesy of Claire Max Lick Ha 225 Laser Guide Star Polarimetry of Herbig Ae/Be Stars Marshall Perrin, James Graham UC-Berkeley Planetary Nebula BD+303639 AO Images from Gemini North June 1999 Campbell’s Hydrogen Star Discovered 1893 by W. W. Campbell at Lick Observatory M13 - Globular Cluster Gemini North, 5”x5” view Left: Visible Light Image, No AO Correction Right: 2.2 micron, AO Corrected (940 second exposure) Galactic Center at 2.2 microns Andrea Ghez, UCLA Galactic Center Andrea Ghez, UCLA Galactic Center - Andrea Ghez, UCLA Quasar Structure QuickTime™ and a TIFF (Uncompressed) decompressor are needed to see this picture. Quasar Host Galaxy: SDSS2323+0040 Elinor Gates, UCO/Lick Mark Lacy, Spitzer Science Center NGS, 120 min, H Band Host Galaxy Luminosity: MV = -21.8 0.15 Host Galaxy r1/2: 0.4 0.1" ~ 3.1 0.5 kpc MBH(Host) = 2.9x108 MO MBH(BLR) = 4.0x107 M L/LE = 0.14-1.0 z = 0.76 1" Companion Galaxy Quasar Host Galaxy: SDSS0244+0028 LGS, 125 min, H Band Host Galaxy Luminosity: MV = -22.7 0.1 Host Galaxy r1/2: 1.3 0.4" ~ 10.7 3.3 kpc MBH(Host) = 1.3x109 MO MBH(BLR) = 3.4x108 M z = 0.84 New developments: tiny deformable mirrors Potential for less cost per degree of freedom Liquid crystal devices Voltage applied to back of each pixel changes index of refraction locally MEMS devices (micro-electro-mechanical systems) Ele ctrostati cal ly Me mbrane actuate d Attachm e nt mi rror diaphragm post Conti nuous mirror Mirror surface map Slide Courtesy Claire Max ViLLaGEs - Visible Light Laser Guide Star Experiment Shane AO Upgrade Uses two deformable mirrors: Woofer - Tweeter System Tweeter is a MEMS device Upgraded Near-IR detector and optics in IRCAL TMT size compared to AT&T Park TMT AO - Coming to a large telescope near you! AO’s potential for expanding our understanding of the Universe is clear! All large telescopes have Adaptive Optics or plans to build an AO system in the near future. More large telescopes are installing Sodium Laser systems now that Lick Observatory has proved real science can be done with this technology. Giant telescopes (30 m diameter or more) of the future require AO and Lasers to realize their full potential.