RF and MW receivers' sensitivity

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Discussion Overview

The discussion revolves around the sensitivity of RF and MW receivers, focusing on current best practices, theoretical limits, and practical implementations. Participants explore various aspects of receiver sensitivity, including bandwidth, noise sources, and the implications of using different sensor technologies.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant seeks papers on the best receiver sensitivity across RF-MW wavelengths, specifically in dBm.
  • Another participant questions the bandwidth of the receiver, suggesting it is crucial for further discussion.
  • A historical reference is made to HF amateur receivers achieving around 20 dB SINAD with a half microvolt input, indicating potential improvements over time.
  • A paper on sensitivity and noise issues for Radio Astronomy receivers is shared, highlighting relevant research.
  • Concerns are raised about real-world noise factors such as cosmic and atmospheric noise, which may dominate receiver performance.
  • Several questions are posed regarding the intended application of the sensor, signal modulation characteristics, and potential noise reduction techniques.
  • One participant mentions working with MW signals at levels around -120 dBm, emphasizing the use of commercially available equipment.
  • A quantum physicist discusses the complexity of comparing their sensor's sensitivity, measured in Tesla/sqrt(Hz), to traditional dBm metrics, noting the variability of bandwidth based on signal intensity.
  • Another participant questions the meaning of "quantum sensor" in this context, suggesting it may relate to SQUIDs or flux qubits.
  • Disagreement arises regarding the interpretation of "MW," with some participants associating it with lower frequencies and others with microwave frequencies.
  • Thermal noise considerations are discussed, with calculations provided for noise temperature based on the sensor's performance.
  • Concerns about the impact of thermal noise on microwave detectors are raised, along with questions about the operational temperature and material properties of the proposed device.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of "MW" and "sensor," leading to confusion and a lack of consensus on terminology. Additionally, there is no clear agreement on the best approaches to improve receiver sensitivity or the implications of thermal noise on performance.

Contextual Notes

Limitations include the ambiguity of terms like "sensor" and "MW," which may lead to misunderstandings. The discussion also highlights the dependence on specific conditions such as bandwidth and temperature, which are not universally defined.

Emperor42
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I'm currently working on a novel RF and MW sensor and I wanted to know whether there is a paper that shows the current very best receiver sensitivity for a range of wavelengths in the RF-MW range in dBm preferably so I can directly compare to my device.
 
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Some years ago I think you could expect a half a microvolt at the antenna connector could get you about 20 db sinad on an HF amateur receiver. Likely has improved since.
-
https://en.m.wikipedia.org/wiki/SINAD
 
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In a screened room the sensitivity is limited by the noise floor of the front-end RF preamplifier, probably a MOSFET. But in the real world the cosmic and atmospheric noise = QRN, and noise from switching power supplies etc = QRM, will dominate the receiver noise.
https://en.wikipedia.org/wiki/Atmospheric_noise

There are ways of digging signals out of the spectrum analyser grass.
1. What is the intended application where you need a very high sensitivity?
2. What are the characteristics of the signal modulation?
3. Will you have a narrow band synchronous detector to reduce noise?
4. Could you use an A to D converter followed by an FFT to get 24 dB of conversion gain?
5. Could you power-spectrum-accumulation to stack maybe another 20 dB deeper?
 
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Emperor42 said:
I'm currently working on a novel RF and MW sensor .
skeptic2 said:
What is the bandwidth of your receiver?
The use of the word "sensor" could imply something other than an audio receiver so the Bandwidth has to be known before any answer can be given.
Perhaps the OP could reply with that necessary piece of information.
However, the question may have just been posted out of 'curiosity', in which case the "half microvolt" figure for an audio MF receiver could be near enough.
 
sophiecentaur said:
The use of the word "sensor" could imply something other than an audio receiver so the Bandwidth has to be known before any answer can be given.
Perhaps the OP could reply with that necessary piece of information.
However, the question may have just been posted out of 'curiosity', in which case the "half microvolt" figure for an audio MF receiver could be near enough.

The bandwidth is roughly sub-kilohertz so around 500Hz.
 
At which frequency?
There are sensors with single photon sensitivity for frequencies above about 4 GHz, but of course these only work at very low temperatures..
Also, the word "sensor" is a bit ambiguous. In applications where you need good sensitivity the easiest thing to do is (usually) to put a good low noise amplifier before he actual detector; that way you can even use standard square-law detector diodes with very small signals.

I routinely work with MW signals (2-8 GHz) with a level of about -120 dBm (and sometimes way below that) and most of our setup is made up of commercially available equipment.
 
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Thanks for the input guys. I'm trying to get more info, but I'm a quantum Physicist by trade so I'm trying to wrap my head around how to compare the sensitivity of our sensor (which measures it as an oscillating electromagnetic field at a single point in space), which is measured in Tesla/sqrt(Hz). I think that I can convert it into an amplifier by attaching it to a coil or array, which would give me a sensitivity of -164dBm at 12.6GHz and up to -200dBm for RF (around 100MHz). So I wanted to compare, but I guess its a lot more complicated than I thought. As for our bandwidth given that it is a quantum sensor the bandwidth changes depending on the intensity of the signal so it could go down to as low as nHz.
 
  • #10
What does "quantum sensor" mean in this context?
The fact that you measure Tesla/sqrt(Hz) would suggest some sort of SQUID based sensor or perhaps a flux qubit.
If that is the case there are a bunch of articles written about using SQUIDs/qubits as sensors. Just put "microwave quantum optics" into Google scholar.
 
  • #12
Averagesupernova said:
MW to me means lower frequencies:
https://en.m.wikipedia.org/wiki/Medium_wave
So my previous post about HF receivers probably means very little knowing you are interested in microwave.
Me too. I read MW as MF. I wish people would declare all their variables, the first time they use them. MW is not a good term to use when μ Wave is meant. You can't even use μW because that's microWatts.
 
  • #13
Emperor42 said:
Thanks for the input guys. I'm trying to get more info, but I'm a quantum Physicist by trade so I'm trying to wrap my head around how to compare the sensitivity of our sensor (which measures it as an oscillating electromagnetic field at a single point in space), which is measured in Tesla/sqrt(Hz). I think that I can convert it into an amplifier by attaching it to a coil or array, which would give me a sensitivity of -164dBm at 12.6GHz and up to -200dBm for RF (around 100MHz). So I wanted to compare, but I guess its a lot more complicated than I thought. As for our bandwidth given that it is a quantum sensor the bandwidth changes depending on the intensity of the signal so it could go down to as low as nHz.
Thermal Noise Power from a resistor at 300K is -174 dBm/Hz. So for 500Hz you have -174 + 10 log 500 = -147 dBm.
If you have -164dBm in 500Hz, that corresponds to a noise temperature of 6K.
 
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  • #14
Fundamentally, the “sensitivity” of today's microwave detectors is so high that it is swamped by thermal noise. For that reason, it is the ease and degree of cooling possible that makes the difference between detectors.

Bandwidth is not critical so long as it is maintained constant during comparisons, or is corrected per √Hz when applicable.

Frequency conversion mixers are significantly noisier than LNAs. Once received, it is necessary to progressively amplify a signal ahead of the rise in mixer and thermal noise as the signal leaves the cryogenic receiver environment and approaches 300K. How and in what form will your signal climb the steps of that ladder?

FETs have a lower inherent noise than junction transistors. How many, and which parameters determine the fundamental noise floor of your proposed device? How do they compare with other devices and materials?

What is the lowest temperature at which your detector will operate, or when does it cease to operate because part of it becomes superconducting. Does your RF detector need to be superconducting?

What is the shortest operating wavelength of your device? Can it be printed as an array of thermal detectors for FLIR imaging applications?

The critical temperature of materials such as Si or GaAs will decide which must be used to make FETs for use at lower temperatures. The question or competition becomes how cold it can be, not how sensitive it is.
 
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  • #15
Emperor42 said:
Thanks for the input guys. I'm trying to get more info, but I'm a quantum Physicist by trade so I'm trying to wrap my head around how to compare the sensitivity of our sensor (which measures it as an oscillating electromagnetic field at a single point in space), which is measured in Tesla/sqrt(Hz). I think that I can convert it into an amplifier by attaching it to a coil or array, which would give me a sensitivity of -164dBm at 12.6GHz and up to -200dBm for RF (around 100MHz). So I wanted to compare, but I guess its a lot more complicated than I thought. As for our bandwidth given that it is a quantum sensor the bandwidth changes depending on the intensity of the signal so it could go down to as low as nHz.
If you have a SQUID, then you are measuring flux through area (granted it may be a small area) rather than field at a single point in space. How exactly are you planning to convert that to dBm? Sensitivity will depend critically on your conversion equipment (transducer), on impedance matching, and on the noise characteristics of your transducer. At high frequencies, parasitics, skin effect and other phenomena may also be important.
"Flux transformers" are widely used with SQUID's and there is an extensive literature extending over 45 years that you can look at.
 

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