great mpifr kosma status and future opportunities mps · pdf filegreat with its modular...

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Power distributor Monitor drawer Ethernet-HUB Obs-computer IF-Power-supply IF Pre-processor IF LO-supply IF-processor Chopper control SOFIA PI-rack AOS-system CTS #1 and #2 FFTS Oscilloscope LO-synthesizer #1 Optics control Instrument computer Mixer-BIAS #1 & #2 Power-supply LO-synthesizer #2 1.9 THz Solid-state LO 1.4 THz Solid-state LO Cryostats SI mounting flange Cold-load First design study of a GREAT 7-pixel array K-mirror (inside the pressure coupler) SI-Flange Cal-Unit LO-beam dual-diplexer setup (dual polarization) polarizer grids roof-top mirrors mirror with f =165mm cold-optics assembly signal-beam GREAT GREAT: status and future opportunities MPIfR 1 KOSMA 2 MPS 3 DLR-Berlin 4 S. Heyminck 1 , R. Güsten 1 , U.U. Graf 2 , J. Stutzki 2 , P. Hartogh 3 , H.-W. Hübers 4 , B. Klein 1 , T. Klein 1 , I. Camara 1 , et al. Best noise- performance measured so far ! GREAT, the German REceiver for Astronomy at THz frequencies, on board of SOFIA will offer unique heterodyne observing capabilities in the frequency range above the highest Herschel/HIFI- bands. In the post-Herschel/HIFI phase it will provide the only opportunity for FIR heterodyne observations at frequencies not accessible from ground. GREAT is planed to be shipped to the NASA Palmdale facilities, the present home of SOFIA, in October this year. First science flights with GREAT are expected in the first half of 2011. GREAT is a far-infrared heterodyne receiver based on a modular receiver concept, developed by a consortium of four German science institutes. In its first incarnation the receiver will offer four independent receiver channels out of which two can be operated simultaneously. The both L-Band channels (operating around 1.4 and at 1.9THz , respectively) are operational and finally tested. The M-Band (2.5 – 2.7 THz) channel is in its final build-up phase and should be ready in time for the first GREAT science flights. The H-Band channel, targeting the [OI] line, is foreseen to be operational at SOFIA FOC. The heterodyne mixing elements in both L-band and the M-band channel are wave guide HEB-mixers made by KOSMA. They show excellent noise performance and stabilities. The IF roll-off is above 3 GHz (see also plot below) and hence allows for a receiver IF-bandwidth of up to 1.5 GHz. 1.9 THz waveguide mixer block T REC -T IF /G MIX spectroscopic Allan- variance minimum times of >100 s are usually measured. TP Allan times are >30 s. Typical measurement of the spectroscopic Allan stability time of the L#1-band channel at 1.4 THz. Best measured noise performance of the L#2 channel so far (at 1.81 THz). The measurement was performed using the old HEB- isolator combination with a limited bandwidth of only 700 MHz. The new wide bandwidth HEB / MMIC combination is undergoing final test and will be used for short science. polarizer grid mirror with f = 165mm flat mirror focal-plane units (7-mixers per polarization) dewar signal + LO -beam GREAT with its modular concept offers the possibility to upgrade to small scale heterodyne focal plane arrays. We are currently working on a design for hexagonal 7 pixel [OI] and/or [CII] mappers. Within the GREAT instrument framework even a dual polarization 2 × 7 pixel [CII] array would be possible. These future upgrades will become possible because of ongoing basic research activities for critical technologies within the GREAT consortium. 1.9THz 2.7THz 4.7THz 158 112 63 14.99 10.63 5.98 Waist size in focal-plane 2.51 1.78 1 Beam-spacing in focal-plane [mm] 7.5 5.32 2.99 Beam-spacing on sky [FWHM] 2.1 2.1 2.1 Beam-spacing in focal-plane [waist] 2.99 2.99 2.99 27.55 19.53 10.99 Wavelength [µm] Beam-size [arcsec] 7-Pixel Footprint in f-plane (5 ω-contur) [mm] GREAT Array Features: arrays act as new GREAT-channel all single pixel channels can be used as before avoids construction & airworthiness overheads possible use of existing LO-systems (output power dependent) K-mirror for >360° image de-rotation 7-pixel hexagonal packing for wave-guide mixers: dual polarization receiver possible 14 times the mapping speed of a single channel no modifications to the GREAT main structure required but cryostat needs to be modified Possible updates: new cryostat with closed cycle refrigerator Draft optics layout for a dual-polarization 7-pixel GREAT receiver. In orange the beam-path of the signal beams is shown. Two Martin-Puplett interferometers act as diplexer for the LO-injection, one for each polarization. Both polarizations are superimposed behind the diplexer- arrangement. Therefore only one cryostat window is required and best possible position matching between the both sub-arrays on sky is guaranteed. Inside the cryostat both polarizations are split-up again and fed onto separate focal-plane mixer arrangements. With a quasi-monolithic cold optics approach we here can avoid difficult adjustments of the cold optics. Optics data of a GREAT array Lab-pictures of GREAT in L-L configuration during the PSR in December 2008. The system is fully tested and ready for shipment.

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Page 1: GREAT MPIfR KOSMA status and future opportunities MPS · PDF fileGREAT with its modular concept offers the possibility to upgrade to small scale heterodyne focal plane arrays. We are

Power distributor

Monitor drawer

Ethernet-HUB

Obs-computer

IF-Power-supply

IF Pre-processor

IF LO-supply

IF-processor

Chopper control

SOFIA PI-rackAOS-system

CTS #1 and #2

FFTS

Oscilloscope

LO-synthesizer #1

Optics control

Instrument computer

Mixer-BIAS #1 & #2

Power-supply

LO-synthesizer #2

1.9 THz Solid-state LO

1.4 THz Solid-state LO

Cryostats

SI mounting flange

Cold-load

First design study of a GREAT 7-pixel array

K-mirror

(inside the pressure

coupler)

SI-Flange

Cal-Unit

LO-beam

dual-diplexer setup

(dual polarization)

polarizer grids

roof-top mirrorsmirror with f =165mm

cold-optics assembly

signal-beam

GREATGREAT:status and future opportunities

MPIfR1

KOSMA2

MPS3

DLR-Berlin4

S. Heyminck1, R. Güsten1, U.U. Graf2, J. Stutzki2, P. Hartogh3, H.-W. Hübers4, B. Klein1, T. Klein1, I. Camara1, et al.

Best noise-

performance

measured so far !

GREAT, the German REceiver for Astronomy at THz frequencies, on board of SOFIA will offer unique heterodyne observing capabilities in the frequency range above the highest Herschel/HIFI-

bands. In the post-Herschel/HIFI phase it will provide the only opportunity for FIR heterodyne

observations at frequencies not accessible from ground. GREAT is planed to be shipped to the

NASA Palmdale facilities, the present home of SOFIA, in October this year. First science flights with

GREAT are expected in the first half of 2011.

GREAT is a far-infrared heterodyne receiver based on a modular receiver concept, developed by a

consortium of four German science institutes. In its first incarnation the receiver will offer four

independent receiver channels out of which two can be operated simultaneously.

The both L-Band channels (operating around 1.4 and at 1.9THz , respectively) are operational and

finally tested. The M-Band (2.5 – 2.7 THz) channel is in its final build-up phase and should be ready in

time for the first GREAT science flights. The H-Band channel, targeting the [OI] line, is foreseen to be

operational at SOFIA FOC.

The heterodyne mixing elements in both L-band and the

M-band channel are wave guide HEB-mixers made by KOSMA.

They show excellent noise performance and stabilities. The IF

roll-off is above 3 GHz (see also plot below) and hence allows

for a receiver IF-bandwidth of up to 1.5 GHz.

1.9 THz waveguide mixer block

TREC - TIF/GMIX

spectroscopic Allan-

variance minimum times

of >100 s are usually

measured.

TP Allan times are >30 s.

Typical measurement of the spectroscopic Allan stability time of

the L#1-band channel at 1.4 THz.

Best measured noise performance of the L#2 channel so far (at

1.81 THz). The measurement was performed using the old HEB-

isolator combination with a limited bandwidth of only 700 MHz.

The new wide bandwidth HEB / MMIC combination is undergoing

final test and will be used for short science.

polarizer grid

mirror with f = 165mm

flat mirror

focal-plane units

(7-mixers per polarization)

dewar

signal + LO -beam

GREAT with its modular concept offers the possibility to upgrade to

small scale heterodyne focal plane arrays. We are currently working on a

design for hexagonal 7 pixel [OI] and/or [CII] mappers. Within the GREAT

instrument framework even a dual polarization 2 × 7 pixel [CII] array

would be possible. These future upgrades will become possible because

of ongoing basic research activities for critical technologies within the

GREAT consortium.

1.9THz 2.7THz 4.7THz

158 112 63

14.99 10.63 5.98

Waist size in focal-plane 2.51 1.78 1

Beam-spacing in focal-plane [mm] 7.5 5.32 2.99

Beam-spacing on sky [FWHM] 2.1 2.1 2.1

Beam-spacing in focal-plane [waist] 2.99 2.99 2.99

27.55 19.53 10.99

Wavelength [µm]

Beam-size [arcsec]

7-Pixel Footprint in f-plane (5 ω-contur) [mm]

GREAT Array Features:

� arrays act as new GREAT-channel

���� all single pixel channels can be used as before

� avoids construction & airworthiness overheads

� possible use of existing LO-systems (output power dependent)

� K-mirror for >360° image de-rotation

� 7-pixel hexagonal packing

� for wave-guide mixers: dual polarization receiver possible

���� 14 times the mapping speed of a single channel

� no modifications to the GREAT main structure required

� but cryostat needs to be modified

Possible updates:

� new cryostat with closed cycle refrigerator

Draft optics layout for a dual-polarization 7-pixel

GREAT receiver. In orange the beam-path of the signal

beams is shown. Two Martin-Puplett interferometers act as

diplexer for the LO-injection, one for each polarization.

Both polarizations are superimposed behind the diplexer-

arrangement. Therefore only one cryostat window is

required and best possible position matching between the

both sub-arrays on sky is guaranteed.

Inside the cryostat both polarizations are split-up again and

fed onto separate focal-plane mixer arrangements. With a

quasi-monolithic cold optics approach we here can avoid

difficult adjustments of the cold optics.

Optics data of a GREAT array

Lab-pictures of GREAT in L-L configuration during the PSR in December 2008. The system is fully tested and ready for shipment.