ALMA – The Push for the High Site A Status Report
Transcript of ALMA – The Push for the High Site A Status Report
ALMA engineering and Solar Filters
Presented by P. YagoubovTechnical department
ALMA European Support CenterEuropean Southern Observatory
High thermal load on Front End receivers High radio flux High dynamic range required Wide field imaging
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Solar observations with ALMA –Challenges:
Problem Thermal load on Front End receivers, irradiance of sunlight –
~130kW per 12m diameter collecting areaSolution Antenna panels scalloped to diffuse visible and near infrared
radiation Implemented and proven to work, ALMA can be pointed at
the Sun safely, also without solar filters Drawbacks None
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Solar observations with ALMA –Challenges: high thermal load
Problem ALMA receivers are designed for the maximum RF signal
~800K (effective brightness temperature) at the receiver input (=cryostat vacuum window)
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Solar observations with ALMA –Challenges: high radio flux
ALMA: signal path
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Front End dynamic range
• Mostly determined by the SIS mixers gain compression, in Bands 3-10 (Bands 1-2 will use HEMT amplifiers with higher saturation level)
• Tsat of SIS mixers is ~5000K, so the receivers are in “soft” (quadratic) saturation already with ambient load at the input, few % gain compression
• FE IF components designed to stay 20dB below 1dB compression point
• FE attenuator can be adjusted to deliver nominal power level to the Back End, however its dynamic range of 15 dB is used to cope with sub-assemblies gain variations and cover range of 40K<Tsys<800K
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Back End dynamic range
• BE analog components designed to stay 20dB below 1dB compression point for the nominal input power level
• IF gain and thus power level of signal fed to the digitizer can be adjusted by the BE basebands attenuators
• However, there is no automatic gain control!• BE dynamic range mostly limited by the digitizers, +/-2dB. This
sets the fundamental limit for the IF total power dynamic range, within one observation scan
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Problem ALMA receivers are designed for the maximum RF signal
~800K (effective brightness temperature) at the receiver input (=cryostat vacuum window)
Solution Optical attenuator in the receiver optical path, between
antenna and Front End: Solar Filter
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Solar observations with ALMA –Challenges: high radio flux
Solar filter as part of the Amplitude Calibration Device
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Amplitude calibration device
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WVR pick up mirror
Calibration wheelSolar filter
Front End cryostat
Calibration load
Solar Filter Requirements:
Nominal RF attenuation (dB) = 4 + 2λ, where λ is the wavelength in millimetres. Deviation from this nominal attenuation level no more than +4/-2dB;
Return Loss <–25dB below 400GHz and <–20dB above 400GHz
Cross polarization induced by the Solar Filter<–15 dB relative to the co-polar component, goal of <–20db
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Solar filter core
Absorber
Optical path
Solar filter core design
Three layers:- Inner layer is a Frequency Selective Surface, acting as a low pass filter;- Outer layers are dielectric films
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Solar Filter attenuation
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Frequency, cm-1
Atten new spec (dB)low limit (-2db)upper limit (+4db)ALMA Solar Blocker SFC-061 inclined at 15 degrees ALMA Solar Blocker SFC-062 inclined at 15 degrees ALMA Solar Blocker SFC-063 inclined at 15 degrees ALMA Solar Blocker SFC-064 inclined at 15 degrees ALMA Solar Blocker SFC-065 inclined at 15 degrees ALMA Solar Blocker SFC-066 inclined at 15 degrees ALMA Solar Blocker SFC-067 inclined at 15 degrees ALMA Solar Blocker SFC-068 inclined at 15 degrees ALMA Solar Blocker SFC-069 inclined at 15 degrees ALMA Solar Blocker SFC-070 inclined at 15 degrees ALMA Solar Blocker SFC-071 inclined at 15 degrees ALMA Solar Blocker SFC-072 inclined at 15 degrees ALMA Solar Blocker SFC-073 inclined at 15 degrees ALMA Solar Blocker SFC-074 inclined at 15 degrees ALMA Solar Blocker SFC-075 inclined at 15 degrees ALMA Solar Blocker SFC-076 inclined at 15 degrees ALMA Solar Blocker SFC-077 inclined at 15 degrees ALMA Solar Blocker SFC-078 inclined at 15 degrees ALMA Solar Blocker SFC-079 inclined at 15 degrees ALMA Solar Blocker SFC-080 inclined at 15 degrees
Problem ALMA receivers are designed for the maximum RF input signal with
800K effective brightness temperature Solution Optical attenuator in the receiver optical path: Solar FilterDrawbacks (also potential) Reduced SNR – all calibrations are more difficult Complex gain introduced, frequency and maybe time dependent.
Amplitude and phase need to be calibrated Short time scale phase correction with WVR not possible in high
ALMA bands, 7-10 Beam properties, focus, and pointing Polarization purity and polarization calibration
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Solar observations with ALMA –Challenges: high radio flux
SNR is decreased by two factors:- the signal is decreased due by the attenuation in the filter- noise is added due to termination at ambient
Trx(sf) = Trx/t + Tsf(1-t), where
Trx is the receiver noise temperature without solar filterTsf is the solar filter termination load physical temperature (~290K)t is the solar filter transmission
ExamplesBand 3, t=0.1, Trx increases from 40K to ~660KBand 9, t=0.2, Trx increases from 100K to ~730K
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Solar Filter drawbacks: reduced SNR
Solar filter drawbacks: no short time scale phase correction using WVR
ALMA 12m antennas of the main array are equipped with Water VapourRadiometers (WVR)
WVR correct for the excess optical path due to water vapour and thus the phase of each antenna signal
WVR are used to correct phase fluctuation for the short time scale: 1sec < t < fast switching period
Problem Solar filter is installed on the Amplitude Calibration Device. With solar
filter inserted in Bands 7-10 (other tbc) receiver beam, calibration wheel blocks WVR optical path.
Solution None
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Amplitude Calibration Device
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Complex gain calibration- Phase: covered by Shimojo-san presentation- Amplitude: low resolution FTS laboratory data available. High resolution
measured in coherent mode in Band 9, spectral response is flat
Trx with and without solar filter Attenuation level derived from Trx
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Solar Filter drawbacks: gain calibration
600 620 640 660 680 700 7200
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Tnoise pol. 1
FLO (GHz)
T nois
e (K
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600 620 640 660 680 700 7205
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FLO (GHz)
dB
Primary beam properties- Focus and pointing can be done with solar filters- Astrophotography measured with solar filter- Band 9 receiver beam measured with solar filter, sidelobe detected however
terminated at the sky (sub-reflector angular dimensions are shown by dashed lines)
Band 9 receiver far field beam patternWithout solar filter With solar filter
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Solar Filter drawbacks: primary beam
(-1.192, -1.454)
Xangle (deg)
Y angl
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FLO = 670 GHz; dFocus = 120 mmCopolarisation: pol. 1
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Am
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(0.060, -1.185)
Xangle (deg)
Y angl
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FLO = 670 GHz; dFocus = 120 mmCopolarisation: pol. 1
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Polarization purity- Tested by the manufacturer at one unit. Confirmed at Band 9- Polarization calibrations are more difficult due to low SNR
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Solar Filter drawbacks: polarization purity
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Frequency, cm-1
ALMA Solar Blocker SFC042 Longside at 15 deg incidence cross pol
ALMA Solar Blocker SFC042 Longside at 15 deg incidence
Solar Filters installation status
• All solar filters delivered to JAO in 2012• 36 antennas equipped with production SF (32 at the AOS)• 1 antenna with pre-production SF (at the AOS) • 17 antennas w/o SF
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Conclusions High dynamic range needed for solar observations is difficult to achieve with
ALMA:o Quite Sun and solar flares up to10 SFU can be observed with solar filter.
However, ALMA receivers in soft saturation, so amplitude scale not accurate, tbd if needs and can be calibrated
o +/-2dB dynamic range of the digitizers limits total IF power variation within one observation scan
No WVR corrections possible when solar filter is used for Bands 7-10, other Bands tbc
Solar filter reduces SNR, all calibrations are more difficult Solar filters introduce complex gain - need to be calibrated Solar filters have been produced and delivered, most of antennas are
equipped already Bands 1-2 will use HEMT amplifiers instead of SIS mixers, higher radio flux
can be measured22
Schematics of IF processor
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IF switch attenuator BB attenuators
TP detectors BB detectors