Phasing the GMT with a next generation e-APD dispersed fringe
sensor: design and on-sky prototyping
Derek Kopon a, Brian McLeoda, Antonin Bouchezc, Daniel Catropaa, Marcos A. van Damb, Ken
McCrackena, Stuart McMuldrocha, William Podgorskia, Joseph D’Arcoa, Laird Closed, Jared Malesd,
Katie Morzinskid
∗
a
Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA, 02138
b
Flat Wavefronts, 21 Lascelles St., Christchurch 8022, New Zealand
c
GMTO Corporation, 465 N. Halstead Street, Suite 250, Pasadena, CA 91107
d
Steward Observatory, University of Arizona, Tucson, AZ 85721
ABSTRACT
The GMT will be a 25.4-meter telescope consisting of 7 primary and secondary mirror segments that must be phased to
within a fraction of an imaging wavelength in order to achieve diffraction limited performance. The need to use off-axis
guide stars, coupled with the large (350 mm) segment gaps, makes the task of phasing the GMT uniquely challenging.
To meet these requirements, the Acquisition, Guiding, and Wavefront Sensing system (AGWS) will use four J-band
dispersed fringe sensors (DFS) to measure segment piston at each segment boundary. This DFS will use a novel array of
doublet prisms, instead of grisms, to disperse segment boundary fringes with maximal throughput, minimal stray light,
and no spurious diffractive orders. The DFS will also use a low noise SAPHIRA e-APD array reading out at ~100 Hz in
order to freeze atmospheric turbulence in the segment boundary fringe images. We will test a prototype of this DFS on
the Magellan Clay 6.5 meter telescope using an adaptive optics corrected beam from the MagAO system. We present
the design of the next generation phasing prototype.
Keywords: Active optics, adaptive optics, Giant Magellan Telescope, phasing, dispersed fringe sensor
1. INTRODUCTION
1.1 The GMT AGWS
The Giant Magellan Telescope (GMT) will be a 25.4-meter diameter telescope with a primary mirror consisting of seven
8.4 meter segments. The Acquisition Guiding and Wavefront Sensing system (AGWS) located near the GMT focal plane
will use off-axis guide stars to make the measurements required to keep the optics of the GMT coaligned, phased,
pointing in the correct direction, and conforming to the correct mirror shape1,2,3 (Figure 1). The AGWS will also perform
target acquisition with a 30 arcsec imaging mode and Shack-Hartmann wavefront sensing for ground-layer adaptive
optics (GLAO) operation. When the GMT operates in natural seeing or GLAO mode, the AGWS is the primary
wavefront sensing system for the telescope. When operating in natural guide star AO mode (NGSAO), the AGWS is
responsible for the initial phasing of the seven segment pairs. In laser tomography AO mode (LTAO), the AGWS keeps
the telescope phased over the course of the observations. In LTAO mode, the AGWS also provides high frequency tiptilt correction.
The AGWS consists of four identical movable star probes located in a plane just before the telescope focal plane (Figure
2). Each star probe contains five selectable optical channels: four visible and one IR. The four visible channels are: a 30
arcsec FOV acquisition camera; a Shack-Hartmann wavefront sensor capable both of long time-scale active optics
measurements and ground-layer wavefront sensing at 100 Hz; a fast (~1kHz) guide channel for natural guide star tip/tilt
measurement during LTAO; and a 7-subaperture channel with pupil rotation for segment tip/tilt sensing. The IR channel
is the J-band phasing sensor that is fed by a dichroic beamsplitter.
∗
derek.kopon@cfa.harvard.edu
Figure 1: The AGWS location within the GMT.
Figure 2: View of the AGWS mounted to the GMT Gregorian Instrument Rotator.
1.2 The AGWS dispersed fringe phasing sensor
Dichroic beamsplitters in each AGWS probe will allow visible light to be used for wavefront and fast tip/tilt sensing,
while IR light is used for piston phase sensing. Simulations by van Dam4 show that the highest sky coverage for phasing
the GMT will be achieved by using a J-band dispersed fringe sensor. The DFS operates by taking fringes produced at a
segment boundary and dispersing them with a grism or prism in the direction perpendicular to the diffraction. Because
the locations of the minima and maxima of the fringes of the diffraction pattern are wavelength dependent, the dispersed
fringes will only be straight if the two segments are in phase. A phase shift between the segments will produce a tilt in
the dispersed fringes. A detector reading out faster than the coherence time of the atmospheric seeing is then used to
record images of the fringes. The Fourier transform of the fringes will give a peak whose vertical position is a
measurement of the segment-to-segment phase difference (Figure 3).
Figure 3: Left: The GMT pupil overlaid with 1.5 m square apertures at the segment boundaries. Center: Simulated fringes
from one subaperture showing in phase (left) and a 10 micron phase shift (right). The dispersion direction is vertical.
Right: A simulated dispersed fringe image and its FFT. The vertical position of the circled peak is a function of the tilt of
the fringes and thus a measure of the piston error.
1.3 Previous phasing prototypes
SAO has built and tested on sky two previous phasing prototypes. The first was a K-band dispersed Hartmann sensor
that was tested at Magellan in 20125. This instrument operated with a seeing limited beam from the F/11 secondary.
The fringes were tip/tilt stabilized using a fast steering mirror. The advent of the SAPHIRA sub-electron read-noise fast
readout IR array allows us to eliminate the need for tip/tilt stabilization.
The second phasing prototype was a dispersed fringe sensor operating behind the Magellan AO system. The sensor was
tested on sky in December 20156,7. This sensor had two different wavelength channels: an I-band channel that used a
Princeton EMCCD camera and a J-band channel that used a Ninox InGaAs detector. This prototype had a variable
phase shifter and the ability to operate at 6 arcmin off-axis. This sensor verified that our DFS design can achieve our
required 40 micron capture range of piston.
The lessons learned from the previous prototypes have informed the design of our most recent instrument, which will
have a number of key modifications and improvements. The optical design uses custom optics that produce wellcorrected images. Lateral color in particular was carefully controlled, as this aberration produced phase biases in the
previous prototype. A new phase shifter plate will give well qualified phase shifts in each of the three subaperture pairs.
New off-axis lens optics will give us the ability to simulate the GMT off-axis aberrations. A prism doublet array will
allow us to disperse fringes without the stray light and spurious diffractive orders generated by the grism disperser in the
previous prototype. The SAPHIRA e-APD detector (commercially available in First Light Imaging’s C-RED One
camera) with a custom blocking filter should allow us fast sub-electron read-noise performance in the J-band.
2. THE SAPHIRA DFS PROTOTYPE DESIGN
2.1 Prototype goals
Our objective in designing the next generation phasing prototype is to build a sensor that is as similar as possible to the
actual sensor design that we will use at the GMT and then to test it on sky under conditions that most closely mimic the
conditions we expect at GMT. To that end, our optical design is identical to the sensor we have designed for GMT,
which recently passed PDR. The only difference is the focal length of the collimating lens, which matches the F/16
Magellan beam instead of the F/8 beam of GMT. We have mechanically designed the mounts to reach the same
alignment tolerances that we need to meet for the GMT sensor.
The patrol field in which the AGWS will acquire guide stars at GMT is 6-10 arcmin. We have therefore designed the
prototype to operate both on-axis and at 6 arcmin off-axis. At GMT, the phasing sensors will be operated while AO is
being performed with the on-axis science instrument. Therefore, the off-axis sensor will see the atmospheric structure
produced by an on-axis AO-corrected beam. This beam will see disproportionately higher high order turbulence due to
the isoplanatic error in the off-axis beam. The Magellan AO system will correct the beam using an on-axis guide star.
The MagAO system uses a thin-shell adaptive secondary and a pyramid wavefront sensor. It is one of the closest AO
analogues to the GMT design that is currently operational.
At an off-axis position, the Magellan and GMT telescopes produce different static aberrations. As described later, we
will statically correct the Magellan aberrations and introduce the GMT aberrations. By adjusting the Magellan
instrument rotator, we will also be able to change the direction of the parallactic angle relative to the aperture mask and
prism dispersion in order to measure the effects of atmospheric dispersion on the phase measurements.
2.2 Optical design
The prototype optical design is an almost identical copy of the baseline GMT design (Figure 4), the only difference
being the focal length of the first lens element (Figure 5). A collimating lens reimages the Magellan pupil onto a lasercut mask containing pairs of segment boundary apertures (Figure 6). The aperture pairs simulate a 1.5 meter square
overlaid on the segment boundaries of the Magellan pupil for three different guide star off-axis distances: 6, 8, and 10
arcmin. Because the GMT primary and secondary segments are critically sized relative to each other, an increase in offaxis distance causes vignetting that effectively increases the inter-segment spacing.
After the mask, the prototype prism doublet array follows, which disperses the beam in the direction perpendicular to the
diffraction pattern formed by the segment boundary apertures. After the prism array, a three doublet optical relay
images the dispersed fringes onto the detector.
The prototype will have a pupil viewing channel to allow the aperture mask to be precisely aligned to the telescope pupil
and to ensure that the apertures are uniformly illuminated. There will also be an “unobscured mode” that allows the
prism and mask assembly to be removed from the beam and replaced with a lens assembly in order to allow the full
telescope pupil to be viewed, or an undispersed/undiffracted image to be produced. The unobscured mode will be used
to calibrate the detector using an on board flat field source.
Figure 4: Layout of the phasing camera optics. A collimating lens (not shown) forms a pupil image on an aperture mask
that is directly in front of the prism array. Dispersed light from the prism array is then reimaged onto the SAPHIRA
detector by an optical relay. The UL1 and pupil viewing optics can be swapped into the beam as necessary to aid in
alignment and calibration.
Figure 5: Raytrace of the fringe viewing channel of the phasing prototype. The telescope focus is at the lower left. L1
collimates the beam and forms a pupil on the aperture mask just before the prism array. The downstream optical relay
images the dispersed fringes onto the SAPHIRA detector.
Figure 6: The pupil aperture mask overlaid with the circular Magellan pupil and the hexagonal prism array. Aperture pairs
simulating GMT segment boundaries as seen by guide stars of different off-axis differences can be selected by moving the
prism/mask assembly relative to the beam. Three subaperture pairs can be positioned in the telescope beam at one time.
Figure 7 shows the layout of the phasing prototype, the light path through the instrument, and the location of the
SAPHIRA detector. The Cal sources are located on a stage that can select either a white light point source, a flat field
screen, or a 5 arcsec field stop. The light then continues to a reimaged pupil where the OAL, phase shifter, and prism
select stages are located. Two different selectable optical relays reimage either the fringes or the pupil onto the
SAPHIRA detector.
Figure 7: Layout of the phasing prototype. Light from the telescope comes out of the page through a hole in the plate near
the Cal sources.
2.3 Prism array prototype
The complex pupil geometry of the GMT segment boundaries makes it difficult, if not impossible, to spatially filter the
0th and 2nd order diffraction patterns generated by any kind of grism array (Figure 8). To solve this problem, we have
developed an array of prism doublets that use high dispersion optical glass to disperse the fringes generated by the
segment subaperture pairs. Additionally, we have included a spherical surface on the second element of each doublet in
order to eliminate the need for a separate lenslet with its associated throughput loss, optical registration difficulties, and
expense. Precision Optical in Costa Mesa, CA is fabricating a 7-facet prototype array with the same material, size, and
prism geometry as our GMT design (Figure 9). This array will be tested in the lab as a separate component to verify its
fabrication tolerances and then installed in the phasing prototype for use at Magellan.
Figure 8: I-band laboratory image of the previous phasing prototype showing the extra diffractive orders produced by a
grism. In a complex pupil geometry such as the GMT, these 0th and 2nd orders would overlap 1st order images from other
segment boundaries, creating higher noise and spurious signals. The prism array eliminates this issue.
Figure 9: Left: Raytrace of one prism doublet facet. Light enters from the left and forms a pupil image on the aperture
mask. The light then passes through the tilted front surface of the first element that is used to steer the beam. The last
surface of the second element is a long-radius sphere. Right: Photographs of the array being fabricated in the shop.
2.4 SAPHIRA array performance and blocking filter
The key element in the phasing sensor that gives it high-sky coverage is the electron avalanche photodiode (eAPD)
infrared SAPHIRA array produced by Leonardo (formerly Selex). This sensor operates in a charge multiplication mode
that allows it to have an effective read noise less than 1e-.8 There are two characteristics that must be carefully managed
to take advantage of the low noise.
First, as the gain is increased, the dark current also increases. We compute the optimum gain by considering the total
readnoise+dark signal as a function of gain. Using data from G. Finger and First-Light Imaging, we estimate that the
best performance will be obtained with an avalanche gain of approximately 50, which should yield an effective read
noise of 0.3e-, and dark noise of 0.7e- in a 10ms exposure. Recent work by Finger, presented at this conference, has
shown that the dark current can be reduced by operating the SAPHIRA with reduced bias voltages. With this reduction
we may be able to operate at higher gains.
The second effect that must be managed is thermal background. The avalanche effect requires using a low-band gap
layer of HgCdTe which is sensitive to light at thermal wavelengths. So though the detector layer has a cutoff
wavelength λc=2.5µm, longer wavelength photons will pass through the detector layer and be absorbed in the gain layer
which has has λc=3.5µm. At unity-gain the sensor has very high QE out to the cutoff wavelength of the gain layer.
Because these photons may be absorbed part way through the gain layer, they will experience partial amplification,
reducing the effective long-wavelength QE at high gain.8 Absent a blocking filter, our optical design would allow
thermal photons in an f/2 cone to reach the detector. In addition, light coming in at larger angles will be scattered inside
the camera and reach the detector. This light must be blocked by a cold filter inside the camera. Because the 300K
thermal background rises extremely steeply redward of the 3.5µm cutoff wavelength, the filter must block light out to
5µm. We estimate the long wavelength QE of HgCdTe using the Urbach approximation.9 This extrapolation is shown in
Figure 10. We have optimized the design of a baffle inside the C-RED camera using the FRED® scattered light software
package. Multiplying the detector response curve by the black-body spectrum, the scattering function of the baffle, and a
10x reduction in long-wavelength QE for high-gain operation, yields the expected photon rates as a function of angle and
wavelength (Figure 11). We require that the detector see thermal background summed over all wavelengths and incident
angles of less than 10e-/pix/sec. This implies a very stringent blocking function on the filter (Figure 12). We have
ordered a filter meeting this function from VIAVI.
Figure 10: Extrapolation of SAPHIRA QE to longer wavelength using the Urbach approximation.
Figure 11: Photon rate as a function of incident angle that would be detected in the absence of a filter. We require that
the sum of the integrals of all these curves be less than 10e-/sec/pix.
Figure 12: Filter blocking function that meets the 10e-/sec/pix requirement.
2.5 Inter-segment phase shifts
Because the Magellan 6.5 meter primary mirror is monolithic, the phasing prototype should measure zero phase shifts
over each of the three subaperture pairs in the pupil. Once we had verified that the sensor does indeed measure zero
phase, we will use a lithographically produced stepped phase plate to introduce discreet phase shifts into the beam. Our
phase plate is a rectangular fused silica plate that can be translated in the beam to one of four discreet positions to give
200, 400, or 800nm phase shifts in various combinations to each of the three subapertures in the beam.
2.6 Off-axis aberration correction
When operating off-axis, the Magellan telescope produces different aberrations than the GMT. To account for this
difference, we will have two removable custom phase plates that can be introduced to the beam in front of the mask at
the Prototype pupil. The first is the “Magellan OAL” (Off-Axis Lens), which will correct the Magellan telescope coma
and astigmatism aberrations at 6 arcmin. The second is the “GMT OAL”, which will introduce the astigmatism produced
by the GMT at 8 arcmin off-axis. Both phase plates will be lithographically generated on 4 mm thick fused silica. Figure
13 shows the sag maps of the front surface of the two phase plates.
Figure 13: Left: “Magellan OAL” phase plate sag map that consists of coma and astigmatism aberration. Right: “GMT
OAL” sag map that simulates the astigmatism produced by the GMT at 8 arcmin.
3. CONCLUSIONS
We have completed the design and begun fabrication on a prototype dispersed fringe phasing sensor that will verify the
critical technology needed to phase the GMT. This prototype uses several novel enabling technologies, such as a
Saphira e-APD low noise IR detector with a custom cold filter, an array of high index prism doublets, and a custom
optical design. By testing in an off-axis configuration behind an AO corrected beam from the MagAO instrument on
Magellan, we will be able to replicate as closely as possible the conditions we will face at the GMT.
Acknowledgements
This work was supported by the GMTO Corporation, a non-profit organization operated on behalf of an international
consortium of universities and institutions: Astronomy Australia Ltd., the Australian National University, the Carnegie
Institution for Science, Harvard University, the Korea Astronomy and Space Science Institute, The Sao Paolo Research
Foundation, the Smithsonian Institution, The University of Texas at Austin, Texas A&M University, University of
Arizona, and University of Chicago.
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