D. S. Acton’s research while affiliated with University of California, Los Angeles and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (38)


TABLE 1 DISPERSION CALCULATIONS FOR KI 
FIG. 1.-Isometric view of the KI beam line from the Keck I side. Light propagates from the telescope through the AO system, DSM, and the telescope's coude train to a crypt beneath the telescope at the basement level. The crypt houses the final mirror of the coude train, M7, and fold mirror M8, which directs light through the coude tube in the telescope foundation toward the "fore" switchyard in the interferometry basement. Fold mirrors M9 and M10 direct the light to the long delay lines, and their output is reflected toward the fast delay lines via mirrors M14. The output of the fast delay lines is compressed in diameter and directed into the beam combiner area, which includes the "aft" switchyard which feeds the fringe and angle trackers, nuller, and the back-end autoalignment cameras. Inset (a) show the first-light instrumentation, and illustrates the partitioning of space between the environmentally-controlled control room and rest of the beam-combining laboratory; the latter is partitioned with modular cleanrooms into a long delay line and beam transport area, a fast delay line area, and a beam-combiner area. Inset (b) shows the location of the coude mirrors on the telescope structure; the M4, M6 and M7 coude mirrors are 229 mm diameter, and the M5 mirrors, used at a larger angle of incidence, are 305 mm diameter. See the electronic edition of the PASP for a color version of this figure. 
TABLE 2 LIST OF KI MODES AND PERFORMANCE 
FIG. 2.-Plan view of the beam combining laboratory showing the final instrumentation complement, including the three H=K beam combiners feeding two dewars; the L-band combiner and dewar; the 10 um nuller and dewar; the J=H angle tracker and dewar; and the back-end alignment cameras. The aft switchyard contains a number of deployable dichroics to feed the various instruments. See the electronic edition of the PASP for a color version of this figure. 
TABLE 3 SUMMARY K-BAND THROUGHPUT BUDGET 

+18

The Keck Interferometer
  • Article
  • Full-text available

October 2013

·

845 Reads

·

41 Citations

Publications of the Astronomical Society of the Pacific

M. M. Colavita

·

·

R. L. Akeson

·

[...]

·

E. Wetherell

The Keck Interferometer (KI) combined the two 10m W. M. Keck Observatory telescopes on Mauna Kea, Hawaii, as a long-baseline near- and mid-infrared interferometer. Funded by NASA, it operated from 2001 until 2012. KI used adaptive optics on the two Keck telescopes to correct the individual wavefronts, as well as active fringe tracking in all modes for path-length control, including the implementation of cophasing to provide long coherent integration times. KI implemented high sensitivity fringe-visibility measurements at H (1.6m), K (2.2m), and L (3.8m) bands, and nulling measurements at N band (10m), which were used to address a broad range of science topics. Supporting these capabilities was an extensive interferometer infrastructure and unique instrumentation, including some additional functionality added as part of the NSF-funded ASTRA program. This paper provides an overview of the instrument architecture and some of the key design and implementation decisions, as well as a description of all of the key elements and their configuration at the end of the project. The objective is to provide a view of KI as an integrated system, and to provide adequate technical detail to assess the implementation. Included is a discussion of the operational aspects of the system, as well as of the achieved system performance. Finally, details on V-2 calibration in the presence of detector nonlinearities as applied in the data pipeline are provided.

Download

Cloud Structures on Neptune Observed with Keck Telescope Adaptive Optics

December 2007

·

187 Reads

·

25 Citations

The Astronomical Journal

We report on observations obtained with the adaptive optics system at the 10 m Keck II Telescope during engineering validation and early science observing time for the adaptive optics system. We observed Neptune at near-infrared wavelengths. Angular resolution was 005–006, corresponding to a spatial scale of approximately 1000 km at Neptune. We discuss the latitudinal structure of circumferential cloud bands and of compact infrared-bright features seen in the southern hemisphere, as well as their variation with wavelength. We determine the values of I/F (proportional to the ratio of reflected intensity to incident solar flux) in the J and H infrared-wavelength bands, including narrowband filters where there is strong methane absorption. We use the I/F values inside and outside of methane bands to estimate the altitude of clouds responsible for the brightest compact features in the infrared. Our data show that, on two of our four observing dates, the brightest region on Neptune contained highly reflective haze layers located below the tropopause but not deeper than a few bars.


Stellar Companions to Stars with Planets

July 2002

A combination of high-resolution and wide-field imaging reveals two binary stars and one triple star system among the sample of the first 11 stars with planets detected by radial velocity variations. High resolution speckle or adaptive optics (AO) data probe subarcsecond scales down to the diffraction limit of the Keck 10-m or Lick 3-m, and direct images or AO images are sensitive to a wider field, extending to 10" or 38", depending upon the camera. One of the binary systems -- HD 114762 -- was not previously known to be a spatially resolved multiple system; additional data taken with the combination of Keck adaptive optics and NIRSPEC are used to characterize the new companion. The second binary system -- Tau Boo -- was a known multiple with two conflicting orbital solutions; the current data will help constrain the discrepant estimates of periastron time and separation. Another target -- 16 Cyg B -- was a known common proper motion binary, but the current data resolve a new third component, close to the wide companion 16 Cyg A. Both the HD 114762 and 16 Cyg B systems harbor planets in eccentric orbits, while the Tau Boo binary contains an extremely close planet in a tidally-circularized orbit. Although the sample is currently small, the proportion of binary systems is comparable to that measured in the field over a similar separation range. Incorporating the null result from another companion search project lowers the overall fraction of planets in binary systems, but the detections in our survey reveal that planets can form in binaries separated by less than 50 AU.


Table 1. Results of Disk Modelling 
Table 4: HD 98800 Dust Parameters 
Keck Diffraction-Limited Imaging of the Young Quadruple Star System HD 98800

November 2000

·

48 Reads

·

61 Citations

The Astrophysical Journal

This paper presents diffraction-limited 1-18 micron images of the young quadruple star system HD 98800 obtained with the W. M. Keck 10-m telescopes using speckle and adaptive optics imaging at near-IR wavelengths and direct imaging at mid-IR wavelengths. The two components of the visual binary, A and B, both themselves spectroscopic binaries, were separable at all wavelengths, allowing us to determine their stellar and circumstellar properties. Combining these observations with spectroscopic data from the literature, we derive an age of 10 Myr, masses of 0.93 and 0.64 M_sun and an inclination angle of 58 deg for the spectroscopic components of HD 98800 B, and an age of 10 Myr and a mass of 1.1 M_sun for HD 98800 Aa. Our data confirm that the large mid-IR excess is entirely associated with HD 98800 B. This excess exhibits a black body temperature of 150 K and a strong 10 micron silicate emission feature. The theoretical equilibrium radius of large, perfectly absorbing, 150 K grains around HD 98800 B is 2.4 AU, suggesting a circum-spectroscopic binary distribution. Our observations set important upper limits on the size of the inner dust radius of ~2 AU (mid-IR data) and on the quantity of scattered light of <10% (H-band data). For an inner radius of 2 AU, the dust distribution must have a height of at least 1 AU to account for the fractional dust luminosity of \~20% L_B. Based on the scattered light limit, the dust grains responsible for the excess emission must have an albedo of <0.33. The presence of the prominent silicate emission feature at 10 microns implies dust grain radii of >2 microns. The total mass of the dust, located in a circumbinary disk around the HD 98800 B, is >0.002 M_earth. The orbital dynamics of the A-B pair are likely responsible for the disk geometry. Comment: 27 pages, 4 tables, 9 figures; small revisions to section 3.2.4


Figure 1. -Faintest galaxy ever imaged with a high order adaptive optics system (H=19.0 mag). This image of the galaxy PPM 127095- 8+16 has a resolution of 50 milliarcseconds and also represents the highest resolution infrared image ever taken of a faint field galaxy.  
Figure 2. -AO image of a galaxy at the epoch of the formation of the Solar System. This galaxy (PPM 114182+6+27) shows evidence for a disk but perhaps not a true bulge. Instead a central unresolved core is found along with a point source 0. ′′ 6 south of the center.  
Figure 3. -Optical spectrum of PPM 114182+6+27. It has been shifted to match the spectrum of the local elliptical galaxy IC 4889. The best shift corresponds to a redshift of 0.37±0.05 primarily based on the position of the spectral break at 4000Å4000Å. No emission lines are visible.  
Exploring the Structure of Distant Galaxies with Adaptive Optics on the Keck-II Telescope

August 2000

·

47 Reads

·

15 Citations

Publications of the Astronomical Society of the Pacific

We report on the first observation of cosmologically distant field galaxies with an high order Adaptive Optics (AO) system on an 8-10 meter class telescope. Two galaxies were observed at 1.6 microns at an angular resolution as high as 50 milliarcsec using the AO system on the Keck-II telescope. Radial profiles of both objects are consistent with those of local spiral galaxies and are decomposed into a classic exponential disk and a central bulge. A star-forming cluster or companion galaxy as well as a compact core are detected in one of the galaxies at a redshift of 0.37+/-0.05. We discuss possible explanations for the core including a small bulge, a nuclear starburst, or an active nucleus. The same galaxy shows a peak disk surface brightness that is brighter than local disks of comparable size. These observations demonstrate the power of AO to reveal details of the morphology of distant faint galaxies and to explore galaxy evolution. Comment: 5 pages, Latex, 3 figures. Accepted for publication in P.A.S.P


FIG. 1.ÈIntensity vs. image plane position plots, at left, of an uncorrected (small bump) and AO-corrected (high peak) stellar image of a 9th magnitude star taken in H band on 1999 February 6. The FWHM decreased from 340 mas to 40 mas while the peak intensity, or Strehl ratio, increased from 0.6% to 30%. A 1@@ ] 1@@ display of the corrected, 16 s integration, image is shown on the right.
FIG. 4.ÈImage of the Galactic center obtained from a mosaic of 24 images (total integration time of 2 minutes) taken on 1999 May 26. The inset image (90 s exposure) of the central 800 ] 800 mas area will be used to help determine the mass of the possible central black hole located at the position of the radio source Sgr A.
FIG. 5.ÈThe inset shows the highest resolution image of a faint galaxy ever taken. The original 20 minute exposure has a resolution of 50 mas. The displayed image has been binned by 2 ] 2 pixels to give 35 2A .8]2A .8, mas pixel~1. The plot is a radial proÐle of the galaxy and PSF star. The dashed curve is a standard galaxy model Ðtting the bulge and disk separa- tely.  
First Light Adaptive Optics Images from the Keck II Telescope: A New Era of High Angular Resolution Imagery

March 2000

·

292 Reads

·

398 Citations

Publications of the Astronomical Society of the Pacific

Adaptive optics (AO) is a technology that corrects in real time for the blurring effects of atmospheric turbulence, in principle allowing Earth-bound telescopes to achieve their diffraction limit and to ``see'' as clearly as if they were in space. The power of AO using natural guide stars has been amply demonstrated in recent years on telescopes up to 3-4 m in diameter. The next breakthrough in astronomical resolution was expected to occur with the implementation of AO on the new generation of large, 8-10 m diameter telescopes. In this paper we report the initial results from the first of these AO systems, now coming on line on the 10 m diameter Keck II Telescope. The results include the highest angular resolution images ever obtained from a single telescope (0.022" and 0.040" at 0.85 and 1.65 mum wavelengths, respectively), as well as tests of system performance on three astronomical targets.


Warm Circumstellar Dust in the HD 98800 Quadruple Star System

November 1999

·

50 Reads

We present diffraction-limited images of the young quadruple star system HD 98800 obtained with the W. M. Keck 10-m telescopes from 1-18 microns using speckle imaging and adaptive optics imaging in the near-infrared, and direct imaging with OSCIR in the mid-infrared. These measurements are the first to resolve the 0.8'' (38 AU) North-South pair at multiple wavelengths through the silicate feature. The emission from HD 98800 A, a single-lined spectroscopic binary, is consistent with a Kurucz model photosphere of temperature 4500 K and luminosity 0.71 Lsun. In contrast, the emission seen in HD 98800 B, a double-lined spectroscopic binary, is fit by a Kurucz model photosphere of 4000 K with L = 0.58 Lsun, and a large mid-infrared to sub-millimeter excess with L = 0.11 Lsun. A black body fit to the excess emission yields a dust temperature of 150 K; there is also a strong 10 micron silicate emission feature. The equilibrium radius of this dust is 2.6 AU, indicating a circum-spectroscopic binary distribution of grains. The very high fractional luminosity of the dust, 0.2 LB, implies a large vertical component to the distribution, possibly a result of dynamical interactions with the central binary. This research was supported by the NASA Origins of Solar Systems program and the Packard Foundation.


The Keck Natural Guide Star Adaptive Optics Facility: capabilities and early science

January 1999

·

7 Reads

The expected breakthrough in astronomical resolution with the implementation of Adaptive Optics (AO) on the new generation of large, 8-10 m diameter telescopes was clearly demonstrated in February, 1999 with the Natural Guide Star AO facility on the Keck II telescope. These first light images had a full-width-at-half-maximum of 0.04 arcsec at H-band and Strehl ratios up to 30 wavelength. Since first-light we have been engaged in a program to characterize and optimize the system on the sky while carrying out a program to verify the scientific capabilities. The facility is now available to our science community. The purpose of this paper is to provide a brief overview of the facility and its performance. Several science papers in this conference, ranging from planets to galaxies, will further demonstrate the dramatic new scientific capabilities of this facility.



Closed-loop wave-front correction using phase diversity

August 1998

·

13 Reads

·

15 Citations

Proceedings of SPIE - The International Society for Optical Engineering

Closed loop wave front correction of low order Zernike polynomials has been demonstrated using a phase diversity wavefront sensor. The Lockheed-Martin Advanced Technology Center phase diversity brassboard was used to demonstrate low bandwidth correction of aberrations consisting of the Zernike polynomials describing focus, coma and spherical. The method of Lofdahl-Scharmer is used to estimate and correct fixed aberrations in an optical system. The General Regression Neural Network method is used to estimate slowly varying aberrations in the same optical system. Closed loop experimental results from these tests are presented.


Citations (17)


... For instance, the GRAVITY instruments installed at the Very Large Telescope Interferometer (VLTI) [1] with four 8meter telescopes, can reach up to 200 meter squared effective collecting area and hence microarcsecond level astrometric accuracy. Keck Interferometer (KI) with two 10 meter telescope separating 85 meters away from each other, can achieve 5mas resolution in astrophysical observations [2]. Such high resolutinon enables the reevaluation of the super massive black hole mass in the center of active galactic neuclei, resolution of the planetary disc as well as star diameter measurement. ...

Reference:

In-Lab High Resolution Mid-infrared Up-conversion Stellar Interferometer Based on Synthetic Long Base-Line
The Keck Interferometer

Publications of the Astronomical Society of the Pacific

... Based on this, Gonsalves introduced the phase diversity algorithm [14], which recovers the distorted phase information using an objective function that incorporates images from different defocus planes. Since then, the PD method has undergone comprehensive research by institutions such as the University of Central Florida [15], Lockheed Martin Space Systems [16,17], and the Chinese Academy of Sciences [18][19][20], affirming its practicality. This method has already found application in adjusting ground-based telescopes and co-phase detection for segmented mirror telescopes. ...

Closed-loop wave-front correction using phase diversity
  • Citing Article
  • August 1998

Proceedings of SPIE - The International Society for Optical Engineering

... This method is the only one ready to be implemented on a telescope. It was in use at Calar Alto (Davies et al. 2000), and it is at Lick (Olivier et al. 1999), and now at the Keck (Wizinowich et al. 1998). It is planed on the relatively short term for the other large telescope projects. ...

Status of the W.M. Keck Adaptive Optics Facility
  • Citing Article
  • September 1998

Proceedings of SPIE - The International Society for Optical Engineering

... Over the years, several methods of producing atmosphericlike wave-front aberrations in the laboratory have been developed. The most popular method utilizes the forced motion of heated air because it reproduces the same process that occurs in the atmosphere and can be fairly easy to set up. 14,15 However, for air the change in refractive index with temperature dn͞dT is of the order of 10 Ϫ6 ͞°C. 2 To create wavefront distortions of the proper magnitude, the path length through the turbulence must be quite long, or temperature gradients of several degrees must be created. Therefore this approach might not be acceptable if space is limited or if the heat radiated from the device could interfere with nearby optical elements. ...

Laboratory calibration of the W.M. Keck Observatory Adaptive Optics Facility
  • Citing Article
  • January 1998

Proceedings of SPIE - The International Society for Optical Engineering

... In 2020, KPIC utilized the Keck AO system with the R-band Shack-Hartmann wave front sensor (P. Wizinowich et al. 2000), while in 2022, we used the NIR pyramid wave front sensor for our observations (C. Z. ...

First Light Adaptive Optics Images from the Keck II Telescope: A New Era of High Angular Resolution Imagery

Publications of the Astronomical Society of the Pacific

... Images taken with this mirror through the 76-cm telescope at Sacramento Peak in May 1985 show 0.5-sec of arc resolution, although taken in 2-sec of arc seeing conditions. 2 It was this experimental data that led us to investigate the performance of relatively simple active mirrors via computer simulation. ...

Initial Solar Observations at Sacramento Peak Using the Lockheed Active Optics System

... Once these aberrations are reduced, wide-field image restoration becomes possible at an observatory site with very good to excellent seeing conditions. As a side note, image restoration was introduced at the VTT ( de Boer, Kneer, and Nesis 1992;de Boer 1993) much earlier than the first steps towards AO at the VTT (Soltau et al. 1997). The first CCD cameras for speckle-masking imaging had 384 × 286 pixels, 8-or 12-bit digitization, and frame rates of up to 6 Hz. ...

Adaptive Optics at the German VTT on Tenerife

... A classical method to obtain a phase aberration is using a Shack-Hartmann (SH) wavefront sensor [1] (see Fig. 1). This sensor measures the spatial derivatives of the wavefront, and from these measurements, the wavefront aberration itself can be estimated, as for example used in [2,3] for (quasi-)static phase aberrations. To optimally compensate for a dynamic aberration, a prediction of future aberrations has to be made. ...

Full-field wavefront measurements with phase diversity

Astronomy and Astrophysics

... There is evidence for the presence of clouds in super-Earths and mini-Neptunes (e.g. Knutson et al. 2014 ;Kreidberg et al. 2014 ;Lothringer et al. 2018 ;Helling 2019 ) and in our Solar system (Max et al. 2003 ;Coulter, Barnes & F ortne y 2022 ;Yin et al. 2022 ). We use petitRADTRANS to model the effects of clouds by setting a grey cloud deck at 1.0, 0.1, and 0.01 bar (Table 8 ). ...

Cloud Structures on Neptune Observed with Keck Telescope Adaptive Optics

The Astronomical Journal