A fibre-fed echelle spectrograph for a telescope must reach a resolving power with a…

PHYSICS · Multi-part · Fermi University Physics · Optics & Photonics · Geometrical optics and imaging · Geometrical optics and imaging

What an Instrument Can See, Ch Radiance, etendue and a throughput budget that is spent

Problem

A fibre-fed echelle spectrograph for a 4.0 m4.0\ \mathrm{m} telescope must reach a resolving power R=60 000R = 60\,000 with a fibre that subtends 1.51.5 arcseconds on the sky. Its echelle has tan⁡θbl=2.0\tan\theta_{\mathrm{bl}} = 2.0. Assume the fibre carries DtelϕD_{\mathrm{tel}}\phi to the collimator without growth. Take the seeing as Gaussian with a full width at half maximum of 1.01.0 arcsecond, so that a centred fibre of angular diameter dd, in arcseconds, catches a fraction 1−2−d21-2^{-d^2} of a star's light. ((a)) Find the collimated beam diameter DcollD_{\mathrm{coll}} that reaches R=60 000R = 60\,000 with the unsliced fibre. ((b)) The beam can be at most 200 mm200\ \mathrm{mm} across. An image slicer that cuts the fibre image into NN equal strips and stacks them along the slit divides the width the collimator sees by NN. Find the smallest NN that reaches R=60 000R = 60\,000. ((c)) Instead of slicing, the fibre could be narrowed, with the 200 mm200\ \mathrm{mm} beam. Find the angular diameter that reaches R=60 000R = 60\,000, and the fractions of a star's light caught by that fibre and by the 1.51.5 arcsecond fibre.

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