Roberto Gilmozzi and Philippe Dierickx,
European Southern Observatory
This article has been published in the 100th issue of the ESO Messenger, June 2000.
The challenge and the science potential seemed formidable -and highly stimulating.
Extremely large telescopes are no new idea: studies for 25-m class telescopes2,3 date back to the mid-70s. Although these studies concluded that such telescopes were already technically feasible, the science case was not as strong as that permitted today by adaptive optics, and underlying technologies were far less cost-effective than they are now. In the late 80's, plans for a 25-m class telescope were proposed by Ardeberg, Andersen et al4; by 2000 the concept had evolved into a 50-m class adaptive telescope5. Preliminary ideas for a 50-m concept were presented1 by Mountain et al in 1996; studies for a 30-m scaled-up version of the Hobby-Eberly telescope have been unveiled6,7 by Sebring et al in 1998 and 1999; and plans for the 30-m California Extremely Large Telescope (CELT) have been unveiled by Nelson et al at the March 2000 SPIE conference in Munich8.
As for OWL, initial efforts concentrated on finding suitable optical design and fabrication solutions. The emphasis on optics is evident in the first (1998) publication made about the telescope concept9, where it was shown that proven mass-production solutions for the telescope optics are readily available. From that point on, further studies progressed as rapidly as permitted by scarcity of resources, strengthening confidence in the concept. Several contributions10,11,12,13,14 were made at the June 1999 workshop in Bäckaskog, Sweden, where, in particular, the basic concept of the mechanical structure was presented12. Industry showed astounding support for extremely large telescope concepts, two major suppliers announcing15,16 that they were ready to take orders. Two essential conclusions of this workshop were that, first, extremely large telescopes were indeed feasible, experts arguing about solutions instead of feasibility per se, and that, second, the future of high angular resolution belongs to the ground, thanks to adaptive optics.
Preliminary analyses have confirmed the feasibility of OWL's major components within a cost on the order of 1,000 million Euros and within a competitive time frame. A modular design allows progressive transition between integration and science operation, and the telescope would be able to deliver full resolution and unequalled collecting power 11 to 12 years after project funding.
The concept owes much of its design characteristics to features of existing telescopes, namely the Hobby-Eberly for optical design and fabrication, the Keck for optical segmentation, and the VLT for system aspects and active optics control. The only critical area in terms of needed development seems to be multi-conjugate adaptive optics, but its principles have recently been confirmed experimentally, tremendous pressure is building up to implement adaptive capability into existing telescopes, and rapid progress in the underlying technologies is taking place. Further studies are progressing, confirming initial estimates, and a baseline design is taking shape. The primary objective of these studies is to demonstrate feasibility within proven technologies, but provisions are made for likely technological progress allowing either cost reduction or performance improvement, or both.
The main reason for this trend can be identified in the difficulty of producing the optics (both in terms of casting the primary mirror substrate and of polishing it). The advances in material production and in new control and polishing technologies of the last few decades, fostered in part by the requirements set by the present generation of 8-10 m telescopes, offer now the exciting possibility of considering factors much larger than two for the next generation of telescopes. And unlike in the past, they also offer the promise of achieving this without implying a lengthy (and costly) program of R&D.
At the same time, advances also in adaptive optics (AO) bring the promise of being able to achieve diffraction-limited performance. Though still in its infancy, AO is growing very fast, pushed in part also by customer oriented applications. New low-cost technologies with possible application to adaptive mirrors (MEMs), together with methods like multi-conjugated adaptive optics (MCAO), new wave-front sensors and techniques like turbulence tomography are already being applied to AO modules for the present generation of telescopes. Although the requirements to expand AO technology to correct the wave front of a 100m telescope are clearly very challenging (500,000 active elements, enormous requirements on computing power), there is room for cautious optimism. This would allow a spatial resolution of the order of one milliarcsecond, prompting the claim that high angular resolution belongs to the ground. Of course, this is valid only at wavelengths that make sense (i.e. 0.3 < l < 2.5 mm for imaging, l < 5 mm for spectroscopy).
The cost issue is evidently one that needs to be addressed (even if a 50 or 100m telescope is demonstrably feasible from the technical point of view, it will be impossible to build one unless the D2.6 cost law can be broken). A "demonstration" that cost can be kept at low values has been put into practice by HET (admittedly accepting reduced performance). The introduction of modular design and mass-production (telescope optics, mechanics) is also a new and favorable factor. Based on this and on extrapolating the experience of the Keck (segmentation) and of the VLT (active control), the cost estimates range nowadays between 0.3 to 1 $billion (respectively 30m CELT and 100m OWL). These costs are large (though not as large as, say, a space experiment), but possibly within what some large international collaboration can achieve.
From the point of view of "astronomical strategy", therefore, all this would also allow perhaps to optimize the space and ground facilities according to their natural location (e.g. optical/NIR astronomy from the ground, UV or thermal IR astronomy from space, etc), stressing their complementary rather than competitive roles. And this with the possibility of a reduction in "global" costs (the cost of HST would allow to build and operate at least three OWLs…)
The progress both of the science case and of the design concept since the early days allows us to give some answers (albeit incomplete) to the question:
Typically the seeing limit designs go together with wide field (here wide is many arcminutes) and/or high spectral resolution (R>50,000) requirements. Apart from the overwhelming role of the background for seeing-limited imaging (sky counts of thousands of photons per second per pixel for a 50m telescope), source confusion is a major scientific issue. From the technical point of view, building incredibly fast focal reducers, or high-resolution spectrographs with collimators the size of present day telescopes, may pose technical challenges more extreme than building the telescope itself.
On the opposite side, imagers for diffraction limited telescopes need very slow f-numbers (50 or so, although admittedly here the challenge is to have enough detector area to cover a reasonable field, and to avoid severe saturation from ‘bright’ sources). Milliracsecond(s) slits would make the beam size of a high-resolution spectrograph comparable to that of UVES or HIRES (i.e. instrumentation could be considered "comparatively" easy in the diffraction limited case).
In the seeing limited case, a spectroscopic telescope (of say 25-30m and 5,000-20,000 resolution) could occupy an interesting scientific niche. Such a design is being considered as the natural evolution of the HET (Sebring et al), and is the first one to have actually been called ELT (in other words, we have stolen the generic name from them. Another possibility for generic name is Jerry Nelson’s suggestion of calling the future behemoths Giant Optical Devices or GODs. The hint about hubris is quite clear…).
Figure 2 crudely illustrates the effect of increased resolution by showing the same hypothetical 0.6x0.6 arc seconds2 field, as seen by a seeing-limited telescope under best conditions (FWHM~0.2 arc secs), by HST, by an 8-m diffraction-limited telescope and by OWL, respectively. Assuming the pixel size in the rightmost (OWL) image to be ~0.5 mas, the left frames have been convolved with the theoretical Point Spread Functions associated to each case. For the diffraction-limited image the exposure times have been adjusted to provide roughly the same total integrated intensity, taking into account collecting area. A corrective factor has been applied to the seeing-limited image to provide comparable peak intensity (this is due to the oversampling of the seeing-limited image).
Figure 2 also illustrates the fact
that field size is a relative concept and should be evaluated in relation
to its information content: the 0.6 x 0.6 arc seconds2
field shown here becomes ~1,400,000 pixels when seen by OWL.
We have built a simulator of the performance of the OWL, which can be also used for different size telescopes (and compared with similar calculations presented at the March 2000 SPIE conference or at the Bäckaskog 1999 Workshop on Extremely Large Telescopes, e.g. Mountain et al). The simulator uses the PSF produced by the most recent optical design iteration, and includes the typical ingredients (diffusion, sky and telescope background, detector properties, and as complete as possible a list of noise sources). The output is a simulated image or spectrum (see figure 3).
A magnitude limit for isolated point sources of V=38 in 10 hours can be achieved assuming diffraction limited performance (whether there are such isolated sources is a different question, see below). Comparing this performance with the predicted one for NGST shows that the two instruments would be highly complementary. The NGST would have unmatched performance in the thermal IR, while a ground based 100m would be a better imager at l < 2.5 mm and a better spectrograph (R> 5,000) at l < 5 mm. Sensitivity-wise, the 100m would not compete in the thermal IR, although it would have much higher spatial resolution.
In terms of complementarity, OWL would also have a synergetic role with ALMA (e.g. in finding and/or studying proto-planets) and with VLBI (the radio astronomers have been waiting for us optical/IR people to catch up in spatial resolution for decades!)
In any event, there are a number of questions that the Science Case should pose, and find answers to, which will affect the final set of requirements for telescopes like the OWL. Do we need the angular resolution? Is 1 milliarcsecond too much, too little, enough? Is investing in AO research justified? Could we live with seeing limited? Can we not? Do we need 100m? Are 50m enough? Are 30m? Are 20m? Should we push even further? What is a sensible magnitude limit? Is interferometry a better alternative or a precursor? Do we need the optical and its tighter design tolerances and extremely more complex AO (especially since the faint/far Universe is very redshifted)? Do we have a compelling science case? Is "spectroscopy of the faintest NGST sources" enough? Is "unmatched potential for new discoveries" relevant? Is "search for biospheres" too public-oriented? Indeed, do we need an ELT?
In the following we will discuss some areas where OWL could give unprecedented contributions. This is by no means supposed to be a complete panorama, but rather reflects some personal biases.
Admittedly, there may be a confusion limit somewhere. However, the back-of-the-envelope argument that "all far galaxies are 1" across, there are about 1011galaxies and 1011 arcseconds, therefore there must be a point where everything overlaps" fails when one resolves a square arcsecond in > 106 pixels (crowding may still be an issue, though). The topic however is fascinating (and tightly connected with Olbers’ paradox), and will be the subject of a future paper. For the purpose of this discussion, however, the only thing confusing about confusion is whether it is an issue or not. There is a clear tendency in the community to think that it is not.
The history of stellar formation in the Universe is today one of the ‘hot topics’ in astrophysics. Its goal is to determine which kind of evolution has taken place from the epoch of formation of the first stars to today. To do so, "measurements" of star formation rates are obtained in objects at a variety of look back times, and used to determine a global trend. These measurements are usually obtained by comparing some observed integral quantities of unresolved objects (typically an emission line flux) with predictions made by evolution models. Although the method is crude, results are being obtained and a comprehensive picture is starting to emerge.
With a telescope like OWL, what are today "unresolved objects" would be resolved in their stellar components. For example, one could see O stars out to a redshift z ~ 2, detect individual HII regions at z ~ 3, measure SNe out to z ~ 10 (see below). Determining the star formation rates in individual galaxies would go from relying on the assumptions of theoretical models and their comparison with integrated measurements, to the study of individual stellar components, much in the way it is done for the "nearby" Universe.1 for a 50m telescope to observe the faintest galaxies in the HDFs. The symbiosis with NGST would however not only be of the "finder/spectrometer" variety (though much science would be obtained in this way), but as explained above also in terms of complementarity in the space of parameters (wavelength coverage, angular resolution, spectral resolution, sensitivity, etc). The feeling is that a science case to complement the NGST is a strong one, but cannot be the main case for a 100m telescope.
Figure 5 shows model calculations of supernova rates assuming a 1012M¤elliptical galaxy beginning star formation at z = 10. The rates are several dozen per year (i.e. ~ 0.3 per day!). Even for much less massive galaxies the rates are a few per year. This means that any deep exposure in a field < 1 arcmin2 will contain several new supernovae.
Since these SNe will be at high redshift, the observed light curves will be in the rest UV. This actually makes their identification easier, since Type II light curves last typically 12-24 hours in the UV: time dilation will lengthen the curves by (1+z) making them ideal to discover. (Note that the optical light curves, intrinsically some months long, would last years due to dilation).
The study of SNe out to z ~ 10 (if indeed stars started forming at or before that redshift, which is not certain by any means) would allow to access ~ 30% of the co-moving volume (i.e. mass) of the Universe (at present, through SNe we can access less than 3%). Star formation rates at such early ages would be a natural byproduct of these studies. Nearer SNe would be bright enough to provide "light bulbs" to study the intergalactic medium on many more lines of sight than those provided by other bright but less common objects, e.g.QSOs. And of course, although with lower rates and at "nearer" distances (their rate peaks at zI ~ zII– 2.5), the brighter Type I SNe will also contribute to the study.
The achievements of recent projects could hardly be summarized in a few lines, but we emphasize three major breakthroughs:
Optical scalability having been solved, other limitations will inevitably apply. Taking only feasibility criteria into account, and modern telescopes being essentially actively controlled opto-mechanical systems, these new limitations may arise either in the area of structural design, control, or a combination of both. Our perception is that the fundamental limitations will be set by structural design, an area where predictability is far higher than with optical fabrication. However, it should be observed that, despite the fact that control technologies are rapidly evolving towards very complex systems, those technologies are also crucial when it comes to ensuring that performance requirements are efficiently and reliably met. Reliability will indeed be a major issue for extremely large telescopes, which will incorporate about one order of magnitude more active degrees of freedom (e.g. position actuators). In this respect, however, the Keck and VLT performances are encouraging.
Although there is still major effort to be accomplished in order to come to a consolidated design, it appears already that OWL is most likely feasible within currently available technologies and industrial capacity. Actually, the successive iterations of the opto-mechanical design indicate that OWL diameter is quite probably below the current feasibility limit for a steerable optical telescope, which we estimate to be in the 130-150 meter range.
Adaptive optics set aside, OWL's actual limitation seems to be cost, which we constrain to 1,000 million Euros, capital investment, including contingency. Such budget is within a scale comparable to that of space-based projects and spread over a longer time scale. Additionally, it can reasonably be argued that progress in ground-based telescopes is broadly beneficial in terms of cost and efficiency as it allows space-based projects to concentrate on and be optimized for specific applications which cannot be undertaken from the ground -because of physical rather than technological reasons.
It is obviously essential that the concept allows a competitive schedule, which should be the case as the telescope could, according to tentative estimates, deliver unmatched resolution and collecting power well before full completion.
Collecting power is set to ~6,000 m2, with
a goal of 7,000.
The optical quality requirement is set to Strehl Ratio > 20% (goal ³ 40%) at l=500 nm and above, over the entire science field of view and after adaptive correction of atmospheric turbulence with a seeing angle of 0.5 arc seconds or better. We tentatively split this requirement into telescope and atmospheric contributions:
It is quite logical to distinguish between atmospheric and telescope disturbances for their very different spatial and dynamic properties, the former being arguably the most difficult to compensate. Therefore, we incorporate into the telescope concept dedicated adaptive modules, to be designed and optimized for correction of atmospheric turbulence at specified wave bands, and we request that the telescope contribution to the wavefront error delivered to the adaptive module(s) be small with respect to the wavefront error associated with atmospheric turbulence. In brief, we request the telescope itself to be seeing-limited. It should be noted that, in purely seeing-limited mode where the relevant wavefront quality parameter is slope, the aperture size implies that fairly large wavefront amplitudes can be tolerated. For example, a wavefront tilt of 0.1 arc seconds over the total aperture corresponds to a wavefront amplitude of 48 microns peak-to-valley with OWL whereas it would correspond to 3.9 microns with the 8-m VLT.
Taking into account the telescope size and some implied technology solutions (e.g. optical segmentation), we come to the unsurprising conclusion that the telescope itself should provide the following functions: phasing, field stabilization, and active optics, including active alignment. The case for field stabilization is very strong, as a "closed" co-rotating enclosure would be very costly and anyway inefficient in protecting the telescope from wind.
As pointed out earlier, we consider modern telescopes to be controlled opto-mechanical assemblies. The sheer size of OWL only emphasizes the need for a coherent system approach, with rational trade-offs and compromises between different areas, e.g. optical and structural designs. It is also essential that from the earliest stages the design incorporates integration, maintenance and operation considerations. Besides cost, the two essential reasons are construction schedule and operational reliability, the latter playing a critical role when it comes to telescope efficiency.
It does however not appear possible to provide the necessary telescope functions with two optical surfaces; field stabilization, in particular, would require a relatively small, low inertia secondary mirror (in the 2 to 3-m range for effective correction with typical wind frequency spectra) and therefore imply horrendous sensitivity to decenters. In order to minimize structure height a small secondary also implies a very fast primary mirror design, thereby exacerbating fabrication and centering issues, and increasing field aberrations. A possible way around these constraints would be to allow a large secondary mirror and to re-image the pupil of the telescope to perform field stabilization with a conveniently sized surface. Unless the secondary mirror would be concave -which implies a longer telescope structure- such solution, however, raises considerable concerns as to the feasibility of this mirror. It also implies a larger number of surfaces, thereby eliminating the prime argument in favor of an aspheric primary mirror design.
The cost argument is particularly interesting, as it shows how much progress has been realized in optical fabrication over the last decade. There is rather consistent agreement that current technology -polishing of warped segments on planetary machines combined with ion-beam finishing- could lead to an increase of polishing costs for aspheric segments by about 50% -down from 300 to 500%- with respect to all-identical, spherical segments. This figure is however incomplete, as it does not take into account more stringent requirements on substrate homogeneity and residual stresses, which would lead to a cost overshoot far exceeding that of the pure figuring activities. Additionally, polishing of warped segments is intrinsically less deterministic hence less adapted to mass-production, and this solution leads to undesirable schedule risks.
Any trade-off must also incorporate mechanical constraints, and in particular the inevitable difficulty to provide high structural rigidity at the level of the secondary mirror. As will become evident later, this aspect has played a crucial role in the selection of the OWL baseline design.
The considerations outlined above point towards spherical primary and secondary mirror solutions. It should be noted that the trade-off is dependent on telescope diameter; cost considerations set aside, aspheric solutions are probably still superior as long as field stabilization does not require pupil re-imaging. The limit is probably in the 20 to 30 meter range, possibly more with active mechanics and suitable shielding from wind, but certainly well below 100-m.
We have selected a 6-mirror configuration11,17 with spherical primary and flat secondary mirrors (figure 7). Spherical and field aberrations are compensated by a 4-mirror corrector, which includes two 8-m class active, aspheric mirrors, a focusing 4.3-m aspheric mirror and a flat tip-tilt conveniently located for field stabilization. Primary-secondary mirror separation is 95-m, down from 136-m of the first design iteration.
The diffraction-limited (Strehl Ratio ³ 80%) field of view in the visible is close to 3 arc minutes and the total field is ~11 arc minutes. The latter, called technical field, provides for guide stars for tracking, active optics, and possibly phasing and adaptive correction with natural guide stars. A laser guide star solution would require a smaller technical field of view (~6-7 arc minutes) and lead to some design simplification.
The primary mirror would be made of ~1600 hexagonal segments, ~2.0-m flat-to-flat i.e. about the maximum size allowed for cost-effective transport in standard containers. No extensive trade-off has been made so far but we rule out very large segments as those would lead to unacceptably high material, figuring, and transport costs and require substantial investment in production facilities in order to comply with a reasonable schedule. There are, indeed, strong engineering arguments in favor of relatively small segments, such as the 1-m ones proposed by Nelson et al at the March 2000 SPIE conference in Munich. A certain relaxation is however possible with spherical segments, as the added complexity implied by the aspheric deviation -which increases quadratically with the aspheric segment size- disappears. Handling and maintenance would also benefit from a reduced segment size, although auxiliary equipment for automated procedures will be mandatory anyway.
The baseline solution for the mirror substrate is glass-ceramics and, according to suppliers, production within 6-8 years would only require duplication of existing production facilities12. A very promising alternative is Silicon Carbide, which would allow a ~75% mass reduction for the primary mirror with a conservatively simple lightweight design, and a mass saving of ~ 4,000 tons for the telescope structure. This technology is, however, not (yet?) demonstrated for mass-production; further studies will have to take place prior to final selection of the mirror technology.
Figuring would require three to four 8-m class polishing (planetary) machines, complemented with one or two 2-m class ion-beam finishing machines. It should be noted that 1-m class, diffraction-limited laser amplifier windows are currently produced13,15 at a rate fully comparable to that needed for OWL.
Phasing of the primary and secondary mirrors relies conservatively on the same solution as the Keck one, i.e. position sensing combined with sensor calibration. An extensive summary of the mirror phasing techniques applied to the Keck telescopes is presented by Chanan19. Calibration is however more complex with OWL as the primary and secondary mirrors must be phased separately. In the worst case scenario, daytime calibration of one of the two mirrors would be required -in practice, interferometric measurements performed on the flat secondary mirror- while the other of the two would be phased on the sky according the scheme described by Chanan. We are also exploring on-sky closed loop phasing techniques, which should provide a more efficient control of phasing errors. Quite a number of on-sky phasing methods have been proposed in the recent past; most are based on curvature sensing or interferometric measurements of one kind or another. These methods are generally sensitive to atmospheric turbulence and require either short exposure or sub-apertures smaller than the atmospheric coherence length, thereby implying use of relatively bright stars -or closing the adaptive loop before the phasing one. The actual limitations are, however, still to be assessed. A particularly attractive method, which should allow to differentiate primary and secondary mirror phasing errors, is the one proposed by Cuevas et al20.21 indicate that multi-conjugate adaptive optics22 (MCAO) should allow for a corrected field of view of at least 20 arc seconds in the visible, assuming a set of three adaptive mirrors conjugated to optimized altitudes. There is ongoing debate on the respective merits of a tomographic-oriented correction strategy, followed by the Gemini team, and a layer-oriented one, proposed by Ragazzoni et al. A European Research and Training Network (RTN) has recently been set up, on ESO's initiative, to address the general issue of adaptive optics for extremely large telescopes.
In the visible, the implied characteristics of adaptive modules (about 500,000 active elements on a 100-m telescope, a corresponding wavefront sampling and commensurate computing power) leaves no doubt as to the technological challenge. Novel ideas about wavefront sensing (e.g. pyramidic wavefront sensors) and spectacularly fast progress in cost-effective technologies which could potentially be applied to adaptive mirrors (MEMs or MOEMs), together with the strong pressure to achieve MCAO correction on existing 8-m class telescopes in a very near future, leaves room for cautious optimism. Prototypes are under development -the Observatory of Marseille, in particular, is working towards a ~5,000 active elements to be tested by 2003-2004 and based on a scalable technology.
Extensive discussions of adaptive optics aspects for OWL and extremely large telescopes are presented elsewhere13,21,22,23,24. Proposals for MCAO demonstrators or even functional instruments to be installed within a fairly short time frame on the VLT and Gemini, respectively, have been made. However promising such developments could be, it is impossible, at this stage, to make any substantiated statement as to their outcomes. Therefore, the telescope design incorporates the most conservative assumptions regarding the eventual technology solutions, which implies, in particular, large field of view for reasonable sky coverage with natural guide star. All attempts are made to avoid constraints on the design and correction range of the adaptive modules, which implies that the telescope be able to deliver seeing-limited performance comparable to that of existing large telescopes without relying on adaptive correction.12 based on fully separate structures for the primary and secondary mirrors. As was -to some extent- expected, the best compromise in terms of cost, performance, and feasibility in a broad sense (i.e. including assembly, integration and maintenance aspects) seems to be an alt-az concept.
As in the case of the main optics, the mechanical design26 relies heavily on standardized modules and parts, allowing cost reduction factors which are normally not attainable with classical telescope designs. Manufactured or pre-assembled parts are constrained to having dimensions compatible with cost-effective transport in standard 40 ft containers. It should be pointed out that, in view of the structure dimensions, the standardization does not necessarily impair performance. Particular attention is given to assembly and integration constraints as well as to suitability for maintenance26.
The all-steel structure has a moving mass on the order of 13,500 tons (including mirrors) and does not rely on advanced materials. Iso-static and hyper-static configurations are being evaluated, the former yielding lower dynamic performance and the latter, slightly higher mass, complexity, and cost. First locked rotor frequency is 1.5 Hz for the iso-static and 2.4 Hz for the hyper-static configurations, respectively. Static deformations require the decenters of the secondary mirror and of the corrector to be compensated, but the relevant tolerances, which are set to guarantee that the on-sky correction loop by active optics can be closed, are not particularly stringent17.
Open-air operation is evidently a major issue with respect to tracking and, as mentioned before, full protection from the effect of wind is not a realistic option. Hence the need for field stabilization. The latter is provided by a 2.5-m class flat mirror located in a pupil image, and there is reasonable confidence that a bandwith of 5-7 Hz could be achieved with available mirror technology. It should also be noted that active and passive damping systems have not yet been incorporated into the design.
The kinematics of the structure is comparable to that of the VLT telescopes: 3 minutes for 90º elevation range, 12 minutes for 360º azimuth range, maximum centrifugal acceleration not exceeding 0.1 g at any location of the structure, and 1 degree zenithal blind angle. The number of motor segments would be on the order of 200 for elevation and 400 for azimuth. These figures are based on VLT technology and appear very conservative.
The telescope can point towards horizon, which allows to reduce the dimensions of the sliding enclosure and facilitates maintenance of the secondary mirror unit and extraction of the corrector unit along the axis of the telescope. Mirror covers are foreseen; they would consist of four quadrants sliding into the structure when the telescope is pointing towards zenith. One of these covers would be equipped with segments handling systems and in-situ cleaning facilities allowing periodic cleaning of the primary mirror. Figure 8 shows the telescope pointing towards 60o zenithal distance, mirror covers retracted. The sliding enclosure is not figured.
A preliminary cost model has been assembled and, to some extent, consolidated. The total capital investment remains within the target maximum of 1,000 million Euros, including contingency. It should be pointed out, however, that some of the most determinant cost positions correspond to subsystems involving mass production (primary optics, structure), an area traditionally terra incognita to telescope designers. The full implication of mass-production of the primary optics, of actuators and sensors, and of the structure may be underestimated. Our cost estimate should therefore be consolidated by industrial studies. Our perception is that current estimates are probably conservative.
There is strong indication that a competitive schedule is possible; the critical path is set by the mechanics, and, in contrast to the situation which prevailed at the time the last generation of 8- to 10-m class telescopes was designed, long-lead items such as the main optics do not require time-consuming technology developments. Whereby achieving technical first light within 8-9 years after project go-ahead would be a challenging objective, flexibility in the subsequent integration phases should allow a start of partial science operation at full resolution within 11 and 12 years in the infrared and in the visible, respectively.
The current schedule calls for a completion of phase A, including demonstration of the principle of multi-conjugate adaptive optics on the VLT, by 2003. As ambitious as such objective may seem, it should be recalled that the design of the OWL observatory relies extensively on proven technologies, bar adaptive optics -an approach which has also been adopted for the CELT project. In this respect, it should be pointed out that technology development for long-lead items (primary mirrors) played a determinant role with the current generation of 8-10-m class telescopes. These specific, highly time-consuming technology developments being largely unnecessary for extremely large telescopes such as CELT and OWL, tighter scheduling may become possible.
Further information and publications about the OWL study are available at http://www.eso.org/owl
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Last update: 17 Jan 2002