Radio Telescope Receivers CSIRO ASTRONOMY AND SPACE SCIENCE Alex Dunning 25 th September 2017
Radio Telescope Receivers
CSIRO ASTRONOMY AND SPACE SCIENCE
Alex Dunning
25th September 2017
Receiver Systems for Radio Astronomy | Alex Dunning2 |
“A radio receiver is an electronic device that receives radio waves and converts the information carried by them to a usable form” Wikipedia
Receiver Systems for Radio Astronomy | Alex Dunning3 |
Parkes 10/40cm Receiver
• Captures the signal reflected from the antenna
• Determines the beam shape
• Amplifies the signal
• Conditions the signal for digitisation
Ours look more like this
Receiver Systems for Radio Astronomy| Alex Dunning4 |
Feed Horns
Vacuum Dewar
Control and Monitoring electronics
On the outside…
Receiver Systems for Radio Astronomy| Alex Dunning5 |
On the inside…
Receiver Systems for Radio Astronomy| Alex Dunning6 |
Feed Horn
Receiver Systems for Radio Astronomy| Alex Dunning7 |
Detour: Reciprocity
Microwave Network
A
B
Forward𝑉𝑉𝐵𝐵 = 𝑆𝑆𝐵𝐵𝐵𝐵𝑉𝑉𝐵𝐵
Reverse𝑉𝑉𝐵𝐵 = 𝑆𝑆𝐵𝐵𝐵𝐵𝑉𝑉𝐵𝐵
Reciprocal𝑆𝑆𝐵𝐵𝐵𝐵 = 𝑆𝑆𝐵𝐵𝐵𝐵
Receiver Systems for Radio Astronomy| Alex Dunning8 |
Receiver Systems for Radio Astronomy| Alex Dunning9 |
θ
α
Receiver Systems for Radio Astronomy| Alex Dunning10 |
Receiver Systems for Radio Astronomy| Alex Dunning11 |
-25 -20 -15 -10 -5 0 5 10 15 20 25Theta [deg]
0
50
100
150
200
250
300
Gai
n-25 -20 -15 -10 -5 0 5 10 15 20 25
Theta [deg]
0
50
100
150
200
250
300
Gai
n
Corrugated Smooth Walled
E-Field At Feed mouth
X and Y Feed Patterns
Receiver Systems for Radio Astronomy| Alex Dunning12 |
Feed
Signal
Noise source
Coupler
7mm waveguide couplerNoise coupled in
through small holes
Noise coupled in through vane
21cm waveguide coupler
12mm noise source
Receiver Systems for Radio Astronomy| Alex Dunning13 |
Ortho-mode Transducer
Feed
Signal
Noise source
Coupler
Pol B
Pol A
A output
B output
Input
Receiver Systems for Radio Astronomy| Alex Dunning14 |
Separating the Polarisations: The OMT
Receiver Systems for Radio Astronomy| Alex Dunning15 |
Ortho-mode Transducer
Feed
Signal
Noise source
Coupler LNA
LNAPol B
Pol A
High Electron Mobility Transistor
(HEMT)Low Noise Amplifier
Receiver Systems for Radio Astronomy| Alex Dunning16 |
Noiseless Amplifier
Noise
𝑃𝑃𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜 = 𝐺𝐺𝐺𝐺𝐺𝐺𝐺𝐺 ∆𝑓𝑓 𝑘𝑘𝐵𝐵 𝑇𝑇𝑟𝑟𝑟𝑟𝑟𝑟𝑟𝑟𝑟𝑟𝑜𝑜𝑜𝑜𝑟𝑟
Low Noise Amplifier
Noise
Noise
𝑇𝑇𝑟𝑟𝑒𝑒𝑜𝑜𝑟𝑟𝑒𝑒𝑒𝑒𝑒𝑒𝑟𝑟𝑒𝑒𝑜𝑜 =𝑃𝑃𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜
𝐺𝐺𝐺𝐺𝐺𝐺𝐺𝐺 ∆𝑓𝑓 𝑘𝑘𝐵𝐵
Noiseless Termination
Black body Termination
𝑃𝑃𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜 ∝ 𝐺𝐺𝐺𝐺𝐺𝐺𝐺𝐺 ∆𝑓𝑓
Receiver Systems for Radio Astronomy| Alex Dunning17 |
32
4
2
321 GGGain
TGGain
TGain
TTTLNALNALNA
system ××+
×++=
Feed
Signal
LNA Second Stage
Amplifier
Third Stage Amplifier
T1 T2 T3
Receiver Systems for Radio Astronomy| Alex Dunning18 |
10Jy radio source → ~1K additional noise
Your hand → ~300K additional noise
Mobile Phone at 1 km→ ~1 × 1011 K !!(in primary beam)
Zirconicusso Freepik.com
Receiver Systems for Radio Astronomy| Alex Dunning19 |
Part Room Temperature Cryogenic Ratio
Sky + CMB (Tsky) 6K 6K 1
Spillover (Tspill) 3K 3K 1
Feed + OMT 10K 2K 5
LNA (Tlna) 35K 5K 7
Rest of the System 1K 1K 1
Total (Tsys) 55K 17K ~3
Noise contributions of a typical receiver
Receiver Systems for Radio Astronomy| Alex Dunning20 |
15K section
70K section
Helium Lines
Helium Compressor
Helium Refrigerator
Refrigerator in the Parkes 12mm receiver
Cold finger
Receiver Systems for Radio Astronomy| Alex Dunning21 |
CSIRO. Receiver Systems for Radio Astronomy
Copper Radiation Shield 70K
Helium Refrigerator cold finger
Vacuum Dewar
Thermal Isolation waveguide
15K section
Low Noise Amplifiers
Gap
Receiver Systems for Radio Astronomy| Alex Dunning22 |
The RF System
Contains:• More amplification• Band defining filters• Frequency conversion• Level adjustment• Signal detection• Band shaping
Frequency Conversion
Signal
Filter
To Digitiser
AmplifierLevel
Adjustment
Receiver Systems for Radio Astronomy| Alex Dunning23 |
Signal 1
Signal 2
Signal 1 × Signal 2
Mixer (Multiplier)
Frequency
Pow
er
Frequency
Pow
er
cos(ω1t)cos(ω2t)=½[cos((ω1+ω2)t)+ cos((ω1-ω2)t)]
Δf Δf
Receiver Systems for Radio Astronomy| Alex Dunning24 |
Signal 1
Signal 2
Mixer (Multiplier)
Frequency
Pow
er
Frequency
Pow
er
cos(ω1t)cos(ω2t)=½[cos((ω1+ω2)t)+ cos((ω1-ω2)t)]
Δf Δf
Low pass filter
Receiver Systems for Radio Astronomy| Alex Dunning25 |
Signal 1
Mixer (Multiplier)
Frequency
Pow
er
Frequency
Pow
er
Δf Δf
Local Oscillator
flo
cos(ω1t)cos(ωLOt) → ½cos[(ω1-ωLO)t]
Upper Side Band (USB)
Receiver Systems for Radio Astronomy| Alex Dunning26 |
Signal 1
Mixer (Multiplier)
Frequency
Pow
er
Frequency
Pow
er
Δf Δf
Local Oscillator
flo
cos(ω1t)cos(ωLOt) → ½cos[(ωLO-ω1)t]Lower Side Band (LSB)
Receiver Systems for Radio Astronomy| Alex Dunning27 |
Signal 1
Mixer (Multiplier)
Frequency
Pow
er
Frequency
Pow
er
Δf Δf
Local Oscillator
flo
Band pass filter
Receiver Systems for Radio Astronomy| Alex Dunning28 |
The modern radio telescope 0.000001 megapixels
Receiver Systems for Radio Astronomy| Alex Dunning29 |
Photo credit: Wheeler Studios
Receiver Systems for Radio Astronomy| Alex Dunning30 |
Receiver Systems for Radio Astronomy| Alex Dunning31 |
Receiver Systems for Radio Astronomy| Alex Dunning32 |
Digital beamformer
Weighted (complex) sum of inputs
Receiver Systems for Radio Astronomy| Alex Dunning33 |
CSIRO Astronomy and Space ScienceAlex Dunning
t +61 2 9372 4346e [email protected] www.csiro.au/cass
CSIRO ASTRONOMY AND SPACE SCIENCE
Thank you