PRS Visit to the Lick Observatory, Oct 2004 & Jun 2005

Home | PRS Trips

00-Lick_Obs._Mt_Hamilton_CA_4200ft.jpg
Lick Obs. Mt Hamilton 4,200ft
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01-Shane_3m_observatory.jpg
Shane 3m observatory
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02-Hosts-Remington_Stone_Chung_Pei_Ma_James-Graham.jpg
Hosts: Remington Stone (Lick Obs.), Chung-Pei Ma & James Graham (U.C.Berkeley)
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03-PRS_and_hosts_at_original_safe_door.jpg
PRS and hosts at original safe door
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04-3m_Shane_reflector_with_AO_laser.jpg
3m Shane reflector with AO(*) laser
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AO(*) laser
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06-Shane_3m_with_laser.jpg
Shane 3m with laser
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07-Shane_secondary.jpg
Shane secondary
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08-Shane_cell.jpg
Shane primary mirror cell
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09-Shane_instrument.jpg
Shane Adaptive Optics (AO) package(*)
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Shane laser, detail
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Adaptive optics
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11-In_Nickel_dome.jpg
In Nickel dome
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Instruments on 1m Nickel reflector
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13-Nickel_at_rest.jpg
Nickel at rest
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14-36in_Crossley_reflector.jpg
36in Crossley reflector
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Crossley aperture
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Dinner at Lick before observing
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161-36in_Lick_refractor_1.jpg
36in Lick refractor
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36in Lick refractor 2
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Rem Stone at refractor
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PRS at refractor
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20-Business_end.jpg
Business end
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22-Refractor_wheels.jpg
Refractor wheels
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23-Moon_eyepiece_in_foreground.jpg
Moon eyepiece in foreground
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24-Rem_levitating_an_eyepiece.jpg
Rem levitating an eyepiece
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25-36in_trained_on_the_Moon.jpg
36in trained on the Moon
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26-PRS_at_the_moon_eyepiece.jpg
PRS at the moon eyepiece
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27-James_Lick_tomb.jpg
James Lick tomb
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AO(*) laser firing
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Pierre_and_Vlad_at_Nickel_40
Pierre and Vlad at Nickel 40in.
June 1, 2005

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Rem_Stone_Filling_Dewar_on_Nickel_40.jpg
Rem Stone filling Dewar on Nickel 40in.
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Vlad_and_Rem_filling_Dewar.jpg
Vlad and Rem filling Dewar
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[Top-of-page]
(*)AO: Adaptive Optics Laser Guide Star:

The twinkling and dancing of starlight is due to the deformation of its wavefront as it travels down through the atmosphere to the eye, or the telescope. The AO system used at the Shane telescope projects an intense laser beam - along the telescope axis - where it excites the sodium atoms 90km up in the upper atmosphere. This produces an artificial star whose wavefront can be observed by the AO instrument at the telescope. That wavefront is analyzed to deduce the deformation produced by its travel down through the atmosphere - and that deformation is then applied, in reverse, to the starlight coming through the telescope. That light is bounced a small mirror which is pushed and pulled several times a second by a number of actuators driven by the AO logic so that the wavefront arrives at the final recording instrument as flat as possible.

This idea can be applied by using a normal guide star if there is one close to the object under study. But such a bright star is not always available in the given field of view. Hence the idea of creating an artificial guide star (using the laser) which is always available, close to the object under scrutiny.

(Since the laser is fairly intense, its use is governed by regulations of the US Space Command and the FAA - which, amongst other things, require that several warm-blooded lookouts be posted in the cold night outside the telescope at all times the laser is functioning so that the laser can be immediately turned off if a plane is observed approaching the laser vector. Perfect jobs for undergrads.) [Top-of-page]