Any device used to multiply signals which has a nonlinear response to an electric field.Possible devices include bolometers, photoconductors, classical (Schottky) diodes, and quantum non-linear devices (SIS receivers or Josephson junction mixers).Bolometers and photodetectors have limited response time and therefore limited IF bandwidths. Classical diodes cannot have gain and typically have I-V characteristics whose nonlinearity involves a semiconductor gap of
V. Quantum nonlinear devices can have gain, and have a superconducting gap of a few mV, as well as having low power requirements (Phillips 1988).
Two diodes for which
can be used as multipliers by inputing sums and differences of two voltages and differencing
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Mixers combine a radio frequency [RF] signal and a local oscillator [LO]. The result of the multiplication for two cosinusoidal signals is
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The high frequency term can be removed with a low pass filter.
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The signal is then applied to a filter which only accepts a bandwidth
, so the range of accepted frequencies is
to
, where
is the intermediate frequency. The signals which are accepted satisfy
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and the accepted RFs are
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where LSB denotes the lower sideband,USB the upper sideband, and the LSB has frequencies in the opposite order.
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For
a few 10s of GHz, the signal is applied to low noise amplifiers and then passed through a filter which admits only one sideband (single-sideband mixer). For
GHz, it is difficult to make low-noise amplifiers, so both sidebands are accepted for weak signals (double-sideband mixer).
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Two diodes for which
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(1)
Mixers combine a radio frequency [RF] signal and a local oscillator [LO]. The result of the multiplication for two cosinusoidal signals is
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(2)
The high frequency term can be removed with a low pass filter.
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(3)
The signal is then applied to a filter which only accepts a bandwidth
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(4)
and the accepted RFs are
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(5)
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(6)
where LSB denotes the lower sideband,USB the upper sideband, and the LSB has frequencies in the opposite order.
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For
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