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Dan Boschen
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The choice of an IF frequency of 100 MHz limits the achievable single-sided bandwidth for a real signal centered on it to be 100 MHz, so any pulse out of the modulator would be limited in rise/fall time as given by that bandwidth, without introducing other distortion effects.

The IF frequency of 100 MHz limits the achievable bandwidth for a real signal centered on it to be 100 MHz, so any pulse out of the modulator would be limited in rise/fall time as given by that bandwidth.

The choice of an IF frequency of 100 MHz limits the achievable single-sided bandwidth for a real signal centered on it to be 100 MHz, so any pulse out of the modulator would be limited in rise/fall time as given by that bandwidth, without introducing other distortion effects.

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Dan Boschen
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As a simplified demonstration of this, consider the baseband equivalent signal as represented below showing a 5 ns duration pulse that changes phase by 180 degrees (we could easily extend this to the I and Q pulses associated with a 90 degree rotation) in the middle of the pulse which is passed through a 100 MHz low pass filter (I did this simulation using a low pass filter that had a single pole at 100 MHz and a higher frequency pole at 400 MHz). This predicts the envelope including the phase transition at the output of a modulator that has similar bandwidth.

IfI created a pre-emphasis compensator that utilized the differential of the driving signal resulting in approximately 12 dB of high frequency gain, which modifies the driving pulse as follows (where the red circles show the actual samples of a 1 GSps sampled signal):

As a simplified demonstration of this, consider the baseband equivalent signal as represented below showing a 5 ns duration pulse that changes phase by 180 degrees (we could easily extend this to the I and Q pulses associated with a 90 degree rotation) in the middle of the pulse which is passed through a 100 MHz low pass filter (I did this simulation using a low pass filter that had a single pole at 100 MHz and a higher frequency pole at 400 MHz). This predicts the envelope including the phase transition at the output of a modulator that has similar bandwidth.

If created a pre-emphasis compensator that utilized the differential of the driving signal resulting in approximately 12 dB of high frequency gain, which modifies the driving pulse as follows (where the red circles show the actual samples of a 1 GSps sampled signal):

As a simplified demonstration of this, consider the baseband equivalent signal as represented below showing a 5 ns duration pulse that changes phase by 180 degrees (we could easily extend this to the I and Q pulses associated with a 90 degree rotation) in the middle of the pulse which is passed through a 100 MHz low pass filter. This predicts the envelope including the phase transition at the output of a modulator that has similar bandwidth.

I created a pre-emphasis compensator resulting in approximately 12 dB of high frequency gain, which modifies the driving pulse as follows (where the red circles show the actual samples of a 1 GSps sampled signal):

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Dan Boschen
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The comparative result for this particular pre-emphasis is shown below. This assumes that we are okhave considered the linearity and noise figure trades with operating the output of the modulator 12 dB below it's maximum linear operating range, as well as the noise enhancement considerations from our driving signal at the higher frequency locations.

The comparative result for this particular pre-emphasis is shown below. This assumes that we are ok with operating the output of the modulator 12 dB below it's maximum linear operating range, as well as the noise enhancement considerations from our driving signal at the higher frequency locations.

The comparative result for this particular pre-emphasis is shown below. This assumes that we have considered the linearity and noise figure trades with operating the output of the modulator 12 dB below it's maximum linear operating range.

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