Adaptive Secondary Mirrors

Science Drivers for ASMs

Currently implemented astronomical AO systems operate like auxiliary instruments separate from the main telescope optics. Additional relay optics are used to form an image of the telescope pupil, or an image conjugated with a nominal turbulent layer in the atmosphere, on an adaptive optical element mounted downstream from the telescope focus. Further re-imaging optics are then required to bring the light to a focus on the wavefront sensing camera and science instrument. A separate mirror for removing the tip/tilt of the atmospheric wavefront is also usually included in such systems. Beckers [1] in 1989 proposed the use of the existing secondary mirror in a telescope as a wavefront correction device for correcting atmospheric distortions. Since this approach introduces no extra relay optics it provides several advantages over conventional astronomical AO systems.

 These advantages are:

  1. Greater optical throughput both to the wavefront sensor, allowing fainter guide stars thus increasing sky coverage, and to the science instrument increasing sensitivity. An ASM can have up to a ~20% greater throughput compared to a conventional AO system and this difference can increase as coatings deteriorate with time.
  2. No degradation of telescope IR emissivity, which is a crucial advantage for a system with strong science drivers in the infrared. The naked Gemini telescope (and therefore Gemini with an adaptive secondary) is predicted to produce 2.5% emissivity, whereas the Altair adaptive optics system is predicted to degrade this to 14%.
  3. Less scattered light, stray light arises from both scattering and specular reflections at optical surfaces. The fewer optical surfaces in an ASM system will lead to lower stray light levels, particularly relevant in imaging or spectroscopy of faint structures near bright sources using coronagraphy, where stray light is of crucial importance.
  4. No extra polarisation of the light is introduced. A conventional AO system, due the reflection off various flat relay mirrors, introduces extra polarisation that is of the order of a few percent. This level of polarisation can be a problem especially with extra galactic objects where the degree of polarisation is of a similar magnitude.

Since adaptive secondary mirrors can in principle provide corrections at any necessary frequency and degree of motion, this may obviate the need for expensive support mechanisms associated with conventional secondary mirrors, such as high-speed chopping drives and focus drives.

  Current Adaptive Secondary work at OSL

 

The OSL adaptive secondary prototype

OSL has been at the forefront of the development of adaptive secondary technology. In recent years OSL has undertaken a series of commissioned studies [2][3][4], that have demonstrated the optical efficiency, and mechanical feasibility of performing the adaptive correction with deformable secondary mirrors. In furtherance of this work OSL has built and tested a prototype adaptive secondary mirror (see figure 1) in order to investigate the performance and technological issues.

 

Schematic of the adaptive secondary prototype

The prototype consists of a 270mm diameter mirror faceplate to the back of which are interfaced 7 magnetostrictive actuators via flexures. These in turn are connected to a rigid aluminium mirror support (or reaction plate) against which the forces react. The faceplate is manufactured from a 10mm thick aluminium sheet. The use of aluminium as a face plate material provides several advantages over the conventional glass-ceramic material. These are:-

  • Ten times the yield strength of polished glass, and fifty times that of ground or damaged glass, so aluminium mirrors are robust. They are therefore ideally suited to surviving the many stress-cycles suffered by deformable (active and especially adaptive) mirrors, particularly at a location above the primary where stress-failure could be catastrophic.
  • Unlike glass, large aluminium substrates can be machined to a few microns precision using standard low-cost industrial engineering facilities. Impacts favourably on schedule as well as cost.
  • Aluminium mirrors and associated aluminium structural components can be machined by normal metal working shops, can be light-weighted by standard milling, and can take tapped holes etc for fixtures.
  • High thermal diffusivity, so temperature changes do not disturb mirror figure despite the high thermal expansion coefficient. Mirror seeing effects are essentially eliminated.

A similar glass-ceramic faceplate would be highly vulnerable to damage when removed from the telescope (e.g. for cleaning, aluminising, or maintenance of the actuators or control electronics). A minor or even possibly microscopic defect could act as a stress-concentration that could lead to catastrophic failure in service at an indeterminate time in the future.

The magnetostrictive actuators used in the demonstrator contain a strain gauge position feedback system, which can be used in a control loop to compensate for the hysteresis properties of the actuators, thus linearizing the mirror response. The actuator spacing and arrangement is the same as that which has been proposed for the Gemini South 8-m telescope [2] so the demonstrator is essentially a subsection of this adaptive secondary design with a sufficient degree of freedom to produce several low-order aberrations.

The demonstrator has been successfully used to validate important technological aspects of the OSL approach to adaptive secondaries. The manufacturing, assembly, disassembly, reassembly and calibration techniques for an adaptive secondary system have been developed and it has given insight into the replacement of actuators and confirmed the previous finite element analysis of the actuator influence functions. This system has been extensively statically tested and the results presented in recent conference proceedings and referred journals [5][6][7][8]. The work has also formed the basis of a PhD thesis by J.H. Lee [9].

Recently initial tip/tilt testing of the current system has been performed with the demonstrator operated in closed loop with a quad-cell sensor. Tip/tilt aberrations were generated with a rotating glass plate and figure 2 shows the resulting quad-cell sensor signal for the demonstrator in open and closed loop. As can be seen the tip/tilt aberration was suppressed by a factor of ~10 in this preliminary experiment. With refurbishment of the actuators, residual hysteresis and thermal effects will be reduced which should improve the tip/tilt result.

 More figures of the ASM can be found here

 

References

  1. J. M. Beckers, A proposal to the National Science Foundation, in the NOAO 8M Telescope Description Vol. II, by the Association for University Research in Astronomy, 1989
  2. B.C. Bigalow, D.D. Walker, R.G.Bingham, P. D'Arrigo, Feasibility of Deformable Secondary Mirrors for Adaptive optics and IR chopping, Report to the Gemini-UK project, 1993
  3. B.C. Bigalow, D.D. Walker, R.G.Bingham, Design of an Adaptive Secondary Mirror, Phase II: Zernike polynomial fitting to Mirror FEA Model and design of a 270mm demonstrator mirror. Report to the Gemini-UK project, 1994
  4. B.C. Bigalow, R.W.Wilson, C.R.Jenkins, D.D.Walker, Analysis, simulation and Performance Comparison of Adaptive Optical Correction with Deformable Secondary Mirrors, Report to the Gemini-UK project, 1994
  5. D.D. Walker, J.H. Lee, R.G. Bingham, D. Brooks, M. Dryborough, G. Nixon, H. Jamshidi, S.W. Kim, B. Bigalow, Rugged adaptive telescope secondaries: experience with a demonstrator mirror, The SPIE International Symposium on Astronomical Telescopes and Instrumentation, Kona, 1998.
  6. J.H. Lee, D.D. Walker, A.P..Doel, An Adaptive Secondary mirror demonstrator: Design and Simulation, Opt. Eng., 38, 9, 1999 [download PDF file]
  7. J.H. Lee, D.D. Walker, A.P. Doel, An Adaptive Secondary mirror demonstrator: Construction and preliminary evaluation, To appear in Opt. Eng.[download PDF file]
  8. J.H. Lee, B. C. Bigalow, D.D. Walker, A.P. Doel, Why Adaptive Secondary Mirrors, To appear in PASP.
  9. J.H. Lee, A Deformable Secondary Demonstrator for adaptive optics, PhD Thesis, 1999