Sacramento Peak Observatory to Close?

Science ◽  
1985 ◽  
Vol 228 (4695) ◽  
pp. 36-36 ◽  
Author(s):  
M. M. WALDROP
Solar Physics ◽  
1981 ◽  
Vol 69 (2) ◽  
pp. 411-418 ◽  
Author(s):  
Lawrence E. Cram

1983 ◽  
Vol 66 ◽  
pp. 43-54
Author(s):  
Robin Stebbins ◽  
Christopher Wilson

AbstractA program to measure long-period brightness oscillations at the solar limb has been pursued at Sacramento Peak Observatory for several years. Past improvements in observing technique and data analysis are reviewed. The encouraging results aid in the verification of the reality and the origin of oscillatory signals. However, the main stumbling block to this and other observational programs is the length of observing sequences imposed by the day/night cycle. The South Pole has received considerable attention as a site where extended observations might be possible. Currently, the Sacramento Peak program is developing a South Pole telescope designed for the observing technique and data analysis proven in Sunspot. A review of pertinent South Pole site parameters is given here for other workers who may be considering South Pole observations. Observing sequences longer than 150 hr are possible, though rare. Data sets of this duration are very attractive for solar oscillation studies.


1979 ◽  
Vol 91 ◽  
pp. 857 ◽  
Author(s):  
J. M. Beckers ◽  
W. O. Breedlove ◽  
P. G. N. Devegvar ◽  
E. E. Johansen ◽  
L. B. Gilliam ◽  
...  

1966 ◽  
Vol 71 ◽  
pp. 194 ◽  
Author(s):  
G. Wm. Curtis ◽  
The Sacramento Peak Observatory Staff

1988 ◽  
Vol 123 ◽  
pp. 475-479
Author(s):  
D. M. Rust ◽  
T. Appourchaux ◽  
F. Hill

A unique solar lineshift analyzer described by Rust, Burton and Leistner (1986) has been used at the Sacramento Peak Observatory to study solar oscillations. Operation of this “Stablized Solar Analyzer” (SSA) depends on the electro-optic effect in crystalline lithium niobate, the substrate of the solid Fabry-Perot etalon. Voltage on the etalon shifts the passband by ∼ 4.5 × 10−4 Å/V. The etalon has a passband of 0.175 Å at 6102.7 Å. The stabilization system uses a tunable diode laser to relate the Fabry-Perot passband to the D2 line of atomic Cs 133, at 8521.46 Å. This system reduced instrumental noise to less than Δλ/λ = 10−9 over a six-hour interval.


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