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Noise-figure meter

A noise-figure meter is an instrument for measuring the noise figure of an amplifier, mixer, or similar device. An example instrument is the 1983-era Agilent 8970A. 8970A Noise Figure Meter is a Keysight product numbers that were formerly part of Agilent.[1]

Measurement methods edit

One way to perform the measurement is described on the Y-factor page. A noise-figure meter could automate that procedure as follows: A gated broadband noise source (such as an avalanche diode) drives the device under test. A measurement is made with the noise source on; another measurement with the noise source off. From those measurements and the characteristics of the noise source, the noise figure can be calculated.

Noise source edit

Some noise figure meters need a calibrated broadband noise source—a noise generator. Several methods are used to generate broadband noise. Some methods require two sources: a "hot" and "cold" source. For high frequency measurements, the noise source will be embedded in a transmission line.

Thermal noise edit

Noise (electronics)#Thermal noise

Thermal noise in a resistor. Resistor in liquid nitrogen. Resistor in boiling water.

Shot noise edit

Noise (electronics)#Shot noise

Electrons crossing a gap make discrete arrivals. Impulse. White noise. Compare to thermal electrons.

Motchenbacher & Fitchen (1973, p. 292) describe using a forward biased diode as a calibrated noise source. They also describe a generator made from a low-noise amplifier with a shorted input. Its noise voltage is determined by the shot noise of the amplifier's input transistor.

Vacuum tube edit

Random noise generators can be made from temperature-limited vacuum tube diodes. (Motchenbacher & Fitchen 1973, pp. 289–291) The vacuum tube's anode (plate) is high enough to collect all the electrons emitted from the hot cathode. The operating conditions are set to avoid a space charge around the filament/cathode that would affect the electron emission. The anode current exhibits shot noise.

The noise current is set by the filament temperature. The current is an exponential function of filament temperature.

At low frequencies, there is 1/f noise. At high frequencies, the transit time of the electron becomes an issue.

Ott (1976, pp. 218–219) describes using a noise diode to measure noise factor.

Zener and avalanche diodes edit

Voltage breakdown diodes are often used as noise generators. (Motchenbacher & Fitchen 1973, pp. 180–182) There are two breakdown mechanisms: Zener and avalanche. Diodes with the corresponding effects are known as Zener diodes and avalanche diodes. The two mechanisms have different noise behaviors.

The Zener effect (or internal field emission effect) dominates below 7 volts.[2] The junction is thin, and the electric field is large enough that electrons jump the energy gap. The primary noise is shot noise. There is little other noise (excess noise).

Avalanche breakdown is noisier. A carrier traversing the semiconductor junction is accelerated by the reverse-bias field, and it can generate new electron-hole pairs in a collision. Those new carriers can also generate more carriers in a subsequent collisions. The carriers don't arrive singly but rather in bunches. The result is avalanche multiplication of what would have been just shot noise. The spectrum, like shot noise, is white.

Avalanche breakdown can also exhibit multi-state noise. The generated output noise appears to switch between two or more distinct levels. This noise has a 1/f characteristic. The effect can be minimized.

Motchenbacher & Fitchen (1973, pp. 291–292) describe a noise source using a Zener diode (and also suitable for an avalanche diode).

Some commercial microwave noise generators use avalanche diodes to create a large excess noise figure that can be turned off and on. The impedance of the diode is different during the two states, so an output attenuator is used. The attenuator reduces the noise source output, but it minimizes mismatch loss. (Swain & Cox 1983, p. 26)

See also edit

Notes edit

  1. ^ "Keysight | Electronic Measurement Products". Agilent Technologies.
  2. ^ Motchenbacher & Fitchen (1973, p. 182) graphs noise voltage versus diode breakdown voltage at 250 μA for a family of diodes. At 3 V, the noise volage is about 1 μV per root Hz. At 7 V, the noise is about 28 μV per root Hz.

References edit

  • Keysight (June 2009), Keysight 346A/B/C Noise Source (PDF)
  • Hewlett-Packard (May 1985), HP 8970A Noise Figure Meter: Operating & Service Manual (PDF) (29MB download)
  • Motchenbacher, C. D.; Fitchen, F. C. (1973), Low-Noise Electronic Design, New York: John Wiley & Sons, ISBN 0-471-61950-7
  • Ott, Henry W. (1976), Noise Reduction Techniques in Electronic Systems, New York: John Wiley & Sons, ISBN 0-471-65726-3
  • Swain, Howard L.; Cox, Rick M. (April 1983), "Noise Figure Meter Sets Records for Accuracy, Repeatability, and Convenience" (PDF), HP Journal, 34 (4): 23–34

Also

  • HP Application notes
  • Newer generation manuals
  • Ailtech fixed IF

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A noise figure meter is an instrument for measuring the noise figure of an amplifier mixer or similar device An example instrument is the 1983 era Agilent 8970A 8970A Noise Figure Meter is a Keysight product numbers that were formerly part of Agilent 1 Contents 1 Measurement methods 2 Noise source 2 1 Thermal noise 2 2 Shot noise 2 3 Vacuum tube 2 4 Zener and avalanche diodes 3 See also 4 Notes 5 ReferencesMeasurement methods editOne way to perform the measurement is described on the Y factor page A noise figure meter could automate that procedure as follows A gated broadband noise source such as an avalanche diode drives the device under test A measurement is made with the noise source on another measurement with the noise source off From those measurements and the characteristics of the noise source the noise figure can be calculated Noise source editSome noise figure meters need a calibrated broadband noise source a noise generator Several methods are used to generate broadband noise Some methods require two sources a hot and cold source For high frequency measurements the noise source will be embedded in a transmission line Thermal noise edit Noise electronics Thermal noiseThermal noise in a resistor Resistor in liquid nitrogen Resistor in boiling water Shot noise edit Noise electronics Shot noiseElectrons crossing a gap make discrete arrivals Impulse White noise Compare to thermal electrons Motchenbacher amp Fitchen 1973 p 292 describe using a forward biased diode as a calibrated noise source They also describe a generator made from a low noise amplifier with a shorted input Its noise voltage is determined by the shot noise of the amplifier s input transistor Vacuum tube edit Main article Noise generator Random noise generators can be made from temperature limited vacuum tube diodes Motchenbacher amp Fitchen 1973 pp 289 291 The vacuum tube s anode plate is high enough to collect all the electrons emitted from the hot cathode The operating conditions are set to avoid a space charge around the filament cathode that would affect the electron emission The anode current exhibits shot noise The noise current is set by the filament temperature The current is an exponential function of filament temperature At low frequencies there is 1 f noise At high frequencies the transit time of the electron becomes an issue Ott 1976 pp 218 219 describes using a noise diode to measure noise factor Zener and avalanche diodes edit Voltage breakdown diodes are often used as noise generators Motchenbacher amp Fitchen 1973 pp 180 182 There are two breakdown mechanisms Zener and avalanche Diodes with the corresponding effects are known as Zener diodes and avalanche diodes The two mechanisms have different noise behaviors The Zener effect or internal field emission effect dominates below 7 volts 2 The junction is thin and the electric field is large enough that electrons jump the energy gap The primary noise is shot noise There is little other noise excess noise Avalanche breakdown is noisier A carrier traversing the semiconductor junction is accelerated by the reverse bias field and it can generate new electron hole pairs in a collision Those new carriers can also generate more carriers in a subsequent collisions The carriers don t arrive singly but rather in bunches The result is avalanche multiplication of what would have been just shot noise The spectrum like shot noise is white Avalanche breakdown can also exhibit multi state noise The generated output noise appears to switch between two or more distinct levels This noise has a 1 f characteristic The effect can be minimized Motchenbacher amp Fitchen 1973 pp 291 292 describe a noise source using a Zener diode and also suitable for an avalanche diode Some commercial microwave noise generators use avalanche diodes to create a large excess noise figure that can be turned off and on The impedance of the diode is different during the two states so an output attenuator is used The attenuator reduces the noise source output but it minimizes mismatch loss Swain amp Cox 1983 p 26 See also editNoise electronics Noise figure Radio noise sourceNotes edit Keysight Electronic Measurement Products Agilent Technologies Motchenbacher amp Fitchen 1973 p 182 graphs noise voltage versus diode breakdown voltage at 250 mA for a family of diodes At 3 V the noise volage is about 1 mV per root Hz At 7 V the noise is about 28 mV per root Hz References editKeysight June 2009 Keysight 346A B C Noise Source PDF Hewlett Packard May 1985 HP 8970A Noise Figure Meter Operating amp Service Manual PDF 29MB download Motchenbacher C D Fitchen F C 1973 Low Noise Electronic Design New York John Wiley amp Sons ISBN 0 471 61950 7 Ott Henry W 1976 Noise Reduction Techniques in Electronic Systems New York John Wiley amp Sons ISBN 0 471 65726 3 Swain Howard L Cox Rick M April 1983 Noise Figure Meter Sets Records for Accuracy Repeatability and Convenience PDF HP Journal 34 4 23 34Also HP Application notes Newer generation manuals Ailtech fixed IF Retrieved from https en wikipedia org w index php title Noise figure meter amp oldid 1177401094, wikipedia, wiki, book, books, library,

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