Analog-to-digital converter
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Search complete. 83 mentions across 17 episodes found for "Analog-to-digital converter".
Oct 30, 2026
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46:10BenjaminHOST
Go ahead.
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46:10FabioHOST
Yeah, this is actually a triplet of Shield, but I wanted to pick the AD5593R ADC DAC.
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46:16FabioHOST
How do they call it? The...
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46:19FabioHOST
ADAC.
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46:37FabioHOST
Yeah, this is a chip that does...
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46:39BenjaminHOST
So now there's a shield.
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46:40FabioHOST
Yeah, eight pins, and you can do ADC, DAC, or GPIO.
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46:45FabioHOST
Simple.
Renesas GreenPAK Without Code: Inside the Go Configure Software Hub
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11:43Roman YankevychGUEST
family or search by whatever you want to search.
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11:47Roman YankevychGUEST
ADC, I2C, motor, driver, anything, just type here in search and we'll show you the results.
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11:55Roman YankevychGUEST
And last but not least here is the resources.
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11:59Roman YankevychGUEST
So we tried also to make it as a central place for the knowledge for the engineer that would work with our software.
19 MINS LATER
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31:24Roman YankevychGUEST
So we have the special pieces of the software tools built in for that as well.
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31:30Roman YankevychGUEST
Then there's an interesting device in an analog pack, a product subfamily, SLG47011.
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31:39Roman YankevychGUEST
It has a 14-bit ADC and also an interesting plot called a memory table.
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31:44Roman YankevychGUEST
It's a huge 12-bit memory table with each word being 12 bits as well.
Stanford EE259 I Lenses, image sensors, image signal processing I 2023 I Lecture 20
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69:48Reza Nasiri MahalatiHOST
We will use silicon, but same physics, right? So we're not going to talk more about the principles of PIN because it's exactly the same as what was covered in LIDAR.
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70:00Reza Nasiri MahalatiHOST
Then the other two components in every pixel of a CMOS APS is the readout circuitry And the readout circuitry, what it does is that it kind of sends the signal, the electrical signal that you get out of the PD or the photodiode, and it sends it to the ADCs to be digitized.
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70:17Reza Nasiri MahalatiHOST
So that's the readout circuitry.
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70:19Reza Nasiri MahalatiHOST
And it needs to be architected and designed such that you can read out every pixel in this APS array.
Stanford EE259 I Waveform orthogonality in MIMO radar, radar noise and interference I 2023 I Lec. 14
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1:40Reza Nasiri MahalatiHOST
And then here, basically, this picture shows how we process one frame of data that we have collected.
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1:50Reza Nasiri MahalatiHOST
So, a frame has M chirps and each chirp or actually the down-converted version of each chirp after, you know, mixing the received echo with the transmitted waveform and passing it through the ADC, each chirp would have N samples.
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2:08Reza Nasiri MahalatiHOST
and complex samples.
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2:11Reza Nasiri MahalatiHOST
So one frame of data overall, we can think of it or we can rearrange it as a m by n data matrix.
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2:20Reza Nasiri MahalatiHOST
And this is all in DSP.
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2:21Reza Nasiri MahalatiHOST
So that's a raw data matrix, one frame.
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2:26Reza Nasiri MahalatiHOST
horizontal axis you can think of it as index n which is the ADC samples and vertically so each row is one down converted chirp.
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2:36Reza Nasiri MahalatiHOST
So the row index gives you the chirp index and then the column index gives you the ADC sample number.
Stanford EE259 I Lidar range and direction of arrival estimation I 2023 I Lecture 18
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19:29Reza Nasiri MahalatiHOST
Also, nicely converts current to voltage for us.
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19:33Reza Nasiri MahalatiHOST
So, this voltage can now, you can feed it to an ADC if you like and digitize it and then do DSP on it.
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19:43Reza Nasiri MahalatiHOST
Okay, so this circuit is basically photons in and electrons out.
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19:54Reza Nasiri MahalatiHOST
And the output, it's a voltage type output, so it's very compatible with ADCs for digitization.
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20:01Reza Nasiri MahalatiHOST
Now, this was the ideal circuit.
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20:04Reza Nasiri MahalatiHOST
In reality, it's a little more complex than this.
19 MINS LATER
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38:48Reza Nasiri MahalatiHOST
Then a lens system basically focuses the received light into a photo detector.
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38:53Reza Nasiri MahalatiHOST
And the photo detector gives you an electrical signal, which we call SPD, PD for Photo Detector, SPD of T.
Stanford EE259 I Camera principle of operation and architectures, image formation I 2023 I Lec. 19
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40:29Reza Nasiri MahalatiHOST
There's a lot of very interesting research being done on it.
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40:33Reza Nasiri MahalatiHOST
for, you know, some technological reasons, mainly because it requires, you know, ADCs with very high sampling rate and the DSP gets a little more complicated, it has not been commercially deployed.
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40:45Reza Nasiri MahalatiHOST
Now, that's today.
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40:46Reza Nasiri MahalatiHOST
I'm sure, you know, well, not 100% sure, but I'm fairly confident in a, you know, in a few years we're going to see PMCW LiDARs deployed.
Stanford EE259 I Radar antenna designs and characteristics I 2023 I Lecture 11
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4:04Reza Nasiri MahalatiHOST
It can even be fully implemented in analog.
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4:06Reza Nasiri MahalatiHOST
So you might not even, uh, need to use like a ADC and a DSP.
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4:11Reza Nasiri MahalatiHOST
Uh, um, you can, you can do it much simpler.
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4:13Reza Nasiri MahalatiHOST
But it comes with all, uh, uh, sorts of, uh, uh, you know, um, um, um, uh, caveats in terms of, uh, specifically the error in ranging has, has, has dependency on the amplitude of the received echo and also on the angle of where the target is.
11 MINS LATER
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15:36Reza Nasiri MahalatiHOST
So the signal has instantaneous frequency or c- it's actually just a constant frequency that is proportional to the time of flight, tau.
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15:48Reza Nasiri MahalatiHOST
Right? So basically, at this point, uh, we have a sensor, right? Uh, because that block diagram that, that, uh, we showed, if you build that, the intermediate frequency that we get, if I just, uh, go back to the block diagram real quick so we can look at it together.
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16:07Reza Nasiri MahalatiHOST
So this, uh, intermediate frequency signal that we have, uh, it's gonna get filtered and passed through an ADC.
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16:14Reza Nasiri MahalatiHOST
But then the discretized version that we have, this signal has a frequency that is proportional to the time of flight.
Stanford EE259 I Lidar principle of operation, laser physics I 2023 I Lecture 15
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8:40Reza Nasiri MahalatiHOST
Range estimation, velocity estimation, target detection, and DOA, all the way to...
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8:45Reza Nasiri MahalatiHOST
So from raw signals that you receive from the ADC, ADC samples, to the final image, which is, say, a point cloud, aD 2D or a 3D point cloud.
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8:53Reza Nasiri MahalatiHOST
So you start with, uh, these, um, excuse me, uh, these IF signals, SIF1 to SIFP.
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9:00Reza Nasiri MahalatiHOST
So these are coming from the virtual, uh, elements.
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9:20Reza Nasiri MahalatiHOST
So, so all those combinations, you put them, uh, or, or you collect them, uh, together, and that's one, uh, a r- what we call a raw data frame, okay? So you have, uh, three indices.
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9:30Reza Nasiri MahalatiHOST
You have your virtual antenna index, uh, that's P.
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9:34Reza Nasiri MahalatiHOST
Uh, you have, of course, your ADC sample index that we call N.
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9:37Reza Nasiri MahalatiHOST
And we, we know we use multiple chirps in a frame.
Stanford EE259 I Radar principle of operation and architectures (pulsed, FMCW, PMCW) I 2023 I Lec. 10
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21:22Reza Nasiri MahalatiHOST
And at the bottom, you have all the electronics.
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21:25Reza Nasiri MahalatiHOST
So you have, you know, your waveform generator, your amplifiers, your ADCs, your signal processing.
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21:31Reza Nasiri MahalatiHOST
So this basically, you can co-package everything into a small chip.
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21:37Reza Nasiri MahalatiHOST
And this thing is the full sensor then, not just a transducer.
Stanford EE259 I MIMO imaging radar, direction of arrival est, target detection I 2023 I Lecture 13
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12:02Reza Nasiri MahalatiHOST
And remember, this is the IF signal from one chirp, right? So you have down-converted one chirp You've downconverted that.
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12:12Reza Nasiri MahalatiHOST
That's, that's the SIF that you get, and, uh, the ADC has, has sampled it, so you get endpoints or N samples in it.
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12:22Reza Nasiri MahalatiHOST
So N samples corresponding to one downconverted chirp, then you do an endpoint FFT on it, and here I'm kind of loosely using the term FFT.
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12:30Reza Nasiri MahalatiHOST
I mean, uh, we all know FFT is the actual, uh, algorithm, the implementation of a discrete Fourier transform.
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13:42Reza Nasiri MahalatiHOST
So for example, in the, in the, in the case of the, what I showed you in the previous slide where we had three targets, if you do that, we'll see three peaks in the, in the FFT at indices K hat one, K hat two, and K hat three.
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13:55Reza Nasiri MahalatiHOST
And then, uh, to actually find the range of, of, of the targets, uh, you, you first convert the indices to frequencies, right? Um, so the indices go from zero to N minus one because you are doing an endpoint, uh, FFT here.
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14:10Reza Nasiri MahalatiHOST
Uh, to find the frequencies, you just, uh, do, uh, your index divided by N, which is the total number of points in the FFT, times the sampling rate F sub S. F sub S is your ADC sampling rate.
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14:21Reza Nasiri MahalatiHOST
So that converts your index K to your delta F frequency, and then to, from delta F to range, that's another scaling, right, which, which we just looked at.
7 more episodes mention Analog-to-digital converter.
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