The Giant Magellan Telescope (GMT) consists of seven 8.365 m segments, with
gaps of 0.345 m between adjacent segments. A unique challenge for GMT lies
in phasing the segments and, in particular, how to measure segment piston
optically while the telescope is in science operation. In this paper, we present
a dispersed fringe sensor (DFS) to make these measurements using a novel
algorithm. We show that using four off-axis DFSs operating at J-band with
10 ms exposures, we are able to measure segment piston to the required
50 nm accuracy every 30 s with over 90% sky coverage.
You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.
You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.
You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.
You do not have subscription access to this journal. Equations are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.
The photometric zero point is for the whole telescope on-axis.
The background at K-short depends on the off-axis distance, as
explained in the text.
Table 4.
Limiting Magnitude as a Function of Sky Coverage at the South Galactic
Pole
Sky coverage (%)
50
80
90
95
99
I-band
12.89
13.67
14.03
14.27
14.81
J-band
12.31
12.98
13.34
13.58
14.01
H-band
11.86
12.44
12.82
13.11
13.50
K-short
11.72
12.32
12.66
13.01
13.36
Table 5.
RMS Segment Piston Error in nm as a Function of Off-Axis and Guide Star
Magnitude Using a J-Band DFS
J-Band Magnitude
Off-Axis Distance (′)
10
11
12
12.5
13
13.5
14
6
30
29
38
49
68
73
126
7
30
32
37
44
52
81
127
8
34
34
43
53
58
86
133
9
31
34
42
41
53
88
146
10
30
34
43
44
64
87
139
Table 6.
Off-Axis Aberrations for the GMT in Narrow-Field Mode as a Function of
Guide Star Location in the Directiona,b
Off-Axis Distance (′)
(nm)
(nm)
(nm)
6
2042
−7
10
8
3632
−47
−18
10
5675
−149
−30
The values are the coefficients of the Zernike polynomials [23] that have significant
power.
Tip-tilt and focus errors are ignored as they are easily corrected by
recentering the probes.
Table 7.
Performance of J-Band DFS Piston Sensor with Segment Tip-Tilt under
Different Wind Shake Scenarios
The photometric zero point is for the whole telescope on-axis.
The background at K-short depends on the off-axis distance, as
explained in the text.
Table 4.
Limiting Magnitude as a Function of Sky Coverage at the South Galactic
Pole
Sky coverage (%)
50
80
90
95
99
I-band
12.89
13.67
14.03
14.27
14.81
J-band
12.31
12.98
13.34
13.58
14.01
H-band
11.86
12.44
12.82
13.11
13.50
K-short
11.72
12.32
12.66
13.01
13.36
Table 5.
RMS Segment Piston Error in nm as a Function of Off-Axis and Guide Star
Magnitude Using a J-Band DFS
J-Band Magnitude
Off-Axis Distance (′)
10
11
12
12.5
13
13.5
14
6
30
29
38
49
68
73
126
7
30
32
37
44
52
81
127
8
34
34
43
53
58
86
133
9
31
34
42
41
53
88
146
10
30
34
43
44
64
87
139
Table 6.
Off-Axis Aberrations for the GMT in Narrow-Field Mode as a Function of
Guide Star Location in the Directiona,b
Off-Axis Distance (′)
(nm)
(nm)
(nm)
6
2042
−7
10
8
3632
−47
−18
10
5675
−149
−30
The values are the coefficients of the Zernike polynomials [23] that have significant
power.
Tip-tilt and focus errors are ignored as they are easily corrected by
recentering the probes.
Table 7.
Performance of J-Band DFS Piston Sensor with Segment Tip-Tilt under
Different Wind Shake Scenarios