Mauna Kea ground-layer characterization campaign

We present the results of an 18-month study to characterize the optical turbulence in the boundary layer and in the free atmosphere above the summit of Mauna Kea in Hawaii. This survey combined the Slope-Detection and Ranging (SLODAR) and Low-Layer SCIntillation Detection And Ranging (SCIDAR) (LOLAS) instruments into a single manually operated instrument capable of measuring the integrated seeing and the optical turbulence profile within the first kilometre with spatial and temporal resolutions of 40–80 m and 1 min (SLODAR) or 10–20 m and 5 min (LOLAS). The campaign began in the fall of 2006 and observed for roughly 50–60 h per month. The optical turbulence within the boundary layer is found to be confined within an extremely thin layer (≤80 m), and the optical turbulence arising within the region from 80 to 650 m is normally very weak. Exponential fits to the SLODAR profiles give an upper limit on the exponential scaleheight of between 25 and 40 m. The thickness of this layer shows a dependence on the turbulence strength near the ground, and under median conditions the scaleheight is <28 m. The LOLAS profiles show a multiplicity of layers very close to the ground but all within the first 40 m. The free-atmosphere seeing measured by the SLODAR is 0.42 arcsec (median) at 0.5 μm and is, importantly, significantly better than the typical delivered image quality at the larger telescopes on the mountain. This suggests that the current suite of telescopes on Mauna Kea is largely dominated by a very local seeing either from internal seeing, seeing induced by the flow in/around the enclosures, or from an atmospheric layer very close to the ground. The results from our campaign suggest that groundlayer adaptive optics can be very effective in correcting this turbulence and, in principle, can provide very large corrected fields of view on Mauna Kea.

[1]  Michel Tallon,et al.  Focusing on a Turbulent Layer: Principle of the “Generalized SCIDAR” , 1998 .

[2]  Victor Kornilov,et al.  MASS: a monitor of the vertical turbulence distribution , 2003, SPIE Astronomical Telescopes + Instrumentation.

[3]  G. Daigne,et al.  SCIDAR measurements at Pic du Midi , 2001 .

[4]  Richard W. Wilson,et al.  Determination of the profile of atmospheric optical turbulence strength from SLODAR data , 2006 .

[5]  Leonardo J. Sanchez,et al.  Atmospheric turbulence and wind profiles monitoring with generalized scidar , 2001 .

[6]  Marc S. Sarazin,et al.  Development of a portable SLODAR turbulence profiler , 2004, SPIE Astronomical Telescopes + Instrumentation.

[7]  A. Lambert,et al.  Improved detection of atmospheric turbulence with SLODAR. , 2007, Optics express.

[8]  J. Vernin,et al.  Whole atmospheric-turbulence profiling with generalized scidar. , 1997, Applied optics.

[9]  R. W. Wilson,et al.  LOLAS: an optical turbulence profiler in the atmospheric boundary layer with extreme altitude resolution , 2008 .

[10]  Andrei Tokovinin,et al.  Seeing Improvement with Ground‐Layer Adaptive Optics , 2004 .

[11]  Richard W. Wilson,et al.  SLODAR: measuring optical turbulence altitude with a Shack–Hartmann wavefront sensor , 2002 .

[12]  B. Krauskopf,et al.  Proc of SPIE , 2003 .

[13]  Robert K. Tyson,et al.  Adaptive Optical System Technologies , 1998 .

[14]  Per Capita,et al.  About the authors , 1995, Machine Vision and Applications.

[15]  Jean Vernin,et al.  Automatic Determination of Wind Profiles with Generalized SCIDAR , 2004 .

[16]  David L. Fried Time-delay-induced mean-square error in adaptive optics , 1990 .