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Test input for an SD-32 sampling head


 

How do you test these? The 7 pS rise time is a pretty difficult spec if you want a 10x margin.

I'm contemplating a mercury wetted reed relay, but even that looks to be 2-3 pS at best.

I just received a couple of SD-22s and at 23 pS those are too fast for my pulser from Leo Bodnar. It's really all Leo's fault for sending plots from his CSA803 with the unit. I managed to get an 11801 with an E5622 error for $185 shipped and a pair of SD-22s for $150 shipped. The latter came today. The 11801 is supposed to arrive Friday.

I don't really need it, but an SD-30 or SD-32 would be kind of neat to have. I plan to get an SD-24 to augment the SD-22s.

Unfortunately no one in the US has fresh NVRAM and won't until June.

Reg


 

On Wed, Mar 13, 2019 at 05:22 PM, Reginald Beardsley wrote:
How do you test these? The 7 pS rise time is a pretty difficult spec if you
want a 10x margin.
With difficulty. I believe there's a method involving three sampling heads looking at each other's kickout pulses and some maths which can be used to evaluate their performance.

The SD-24's pulse generator has a risetime of about 16-17ps, I think, but any faster than that is tricky. The calibrator output on the 11802 (but not the 11801 or 11803/CSA803) has a similarly fast rise time, being made of the same hybrid module.

Chris


 

And if you do get a 2ps rise pulse generator how do you check that that is up to its spec?

Roger


 

LOL With *great* difficulty. That's a large part of the appeal of the project. It's not very expensive and if I succeed serious bragging rights. It would be great fun to take to a Keysight trade show booth and put on their new 110 GHz DSO to check it.

I'll have to give an algebraic solution some thought. That had not occurred to me. I can't justify buying 3 fast heads. Just one is a real stretch to justify. But there may be a useful mathematical subterfuge.

Courtesy of a member of the EEVblog forum who was kind enough to give me the magic phrase, I found Michael Case's 1993 doctoral dissertation at UC Santa Barbara on "non-linear transmission line pulse generators". Very interesting approach. It uses the dispersion produced by reverse biased diodes at appropriate intervals to steepen the leading edge. I've only given it a quick glance. For reading I'll want a paper copy. But starting with a 21 pS edge from the laser diode driver Leo Bodnar is using i might not be too difficult. I'll have to work on the math a bit.

Have Fun!
Reg

I'm hoping that someone involved with the SD-30/32 heads will wander along and tell us how they did it at the factory.


 

Reginald,

To obtain significant NLT compression, you need lots of stages, and a fast and big enough signal to start with - not easily done with conventional electronic and transmission line components. This sort of thing is easier to implement inside an IC made with GaAs or SiGe or such, where you can build many of the same thing, on a tiny scale. I think you'll find that most modern treatises on the subject (at least for very high speeds) are about using them within ICs - the physics is the same, but it does not readily translate to putting up a simple lumped element and transmission line system copy.

With the scale of parts and assemblies we can typically handle and see (with magnification) and build and work with, it may be OK to go from a one nanosecond range, compressing to tens of picoseconds, if you have enough stages - maybe 20-100.

Now, if you happen to have access to microwave/RF IC processes, then that's a different story.

Ed


 

Chris, I think you refer here to the so-called "nose-to-nose" method of characterizing sampling scopes (Rush e.a.).
Albert

On Thu, Mar 14, 2019 at 11:37 AM, cmjones01 wrote:


With difficulty. I believe there's a method involving three sampling heads
looking at each other's kickout pulses and some maths which can be used to
evaluate their performance.


 

I have one of Leo's 100 pS impulse units as a source for initial experiments. If I can narrow that to 10 -20 pS with discrete SMD parts I may be able to get the idea to work. There's a close connection to the Hilbert operator hiding in there somewhere.

I've been reading an excellent book on FPGA implementation of DSP by Roger Woods et al most of the afternoon. So I've not started on the dissertation yet. I can't really say much else until I understand the mathematics and physics of using the reverse biased diodes as capacitors. That should keep me entertained for a few weeks at least.

In any case, failure doesn't matter. It's a hobby project, not a client deliverable. I've been fascinated by the problem of getting a fast rise time edge for a long time. It's a bit of circular logic. My excuse for doing it is I bought an 11801 and my excuse for buying the 11801 is so I could try to do it. If I can narrow the 100 pS pulse by 5x I'll have an excuse to buy an SD-32.

I spent 3 years studying sparse L1 pursuits using "A Mathematical Introduction to Compressive Sensing" by Foucart and Rauhut as a text followed by reading the original papers by Donoho, Candes et al. Beats the hell out of watching television. I just wish I could find someone else who was interested in the subject to discuss it with. It's quite amazing what you can do with sparse L1 pursuits and really easy to do in practice. Understanding the math is not easy, but most people use FFTs without really understanding them.

Have Fun!
Reg


 

Picosecond pulse labs used to sell NLTL's for pulse sharpening amonst other applications.
NLTLs are still commercially available.

Bruce

On 15 March 2019 at 14:03 "Reginald Beardsley via Groups.Io" <pulaskite@...> wrote:


I have one of Leo's 100 pS impulse units as a source for initial experiments. If I can narrow that to 10 -20 pS with discrete SMD parts I may be able to get the idea to work. There's a close connection to the Hilbert operator hiding in there somewhere.

I've been reading an excellent book on FPGA implementation of DSP by Roger Woods et al most of the afternoon. So I've not started on the dissertation yet. I can't really say much else until I understand the mathematics and physics of using the reverse biased diodes as capacitors. That should keep me entertained for a few weeks at least.

In any case, failure doesn't matter. It's a hobby project, not a client deliverable. I've been fascinated by the problem of getting a fast rise time edge for a long time. It's a bit of circular logic. My excuse for doing it is I bought an 11801 and my excuse for buying the 11801 is so I could try to do it. If I can narrow the 100 pS pulse by 5x I'll have an excuse to buy an SD-32.

I spent 3 years studying sparse L1 pursuits using "A Mathematical Introduction to Compressive Sensing" by Foucart and Rauhut as a text followed by reading the original papers by Donoho, Candes et al. Beats the hell out of watching television. I just wish I could find someone else who was interested in the subject to discuss it with. It's quite amazing what you can do with sparse L1 pursuits and really easy to do in practice. Understanding the math is not easy, but most people use FFTs without really understanding them.

Have Fun!
Reg



 

Hi, Reg.

Regarding fast pulses and such, there is a wealth of information at Jim
Andrews' page here: He founded
Picosecond Pulse Labs in 1980 and sold it to Tektronix in 2014. I used
PPL products with a CSA803 back in the mid 1990's at Lockheed. I think
the sampling head I used was an SD-24, but since it was about 25 years
ago, my memory is a bit fuzzy.

These days I have a 7904, a 7603, a 7S12, a 7S11, two S-4 sampling
heads, S-53 and S-51 triggering heads, etc in my garage lab. Oh, and a
couple of 10:1 probes I made out of board-edge SMA connectors, 450 ohm
(470 paralleled with 1.8k ohm) 0402 resistors, and 3-pin right-angle 0.1
inch spacing headers. I've not completely characterized the probes, but
at least they pass up to about 12-13 GHz without much attenuation above
the expected 20 dB. Planning to use them to probe some digital RF
boards I'm going to build for work (Raytheon). Too much trouble to try
to get a fast enough sampling scope at work :(

Enjoy the PPL app notes! I've referred to AN-2a through -2e often.

Thanks for the literature references. I'll have to check them out
(someday).

Jim Ford

------ Original Message ------
From: "Reginald Beardsley via Groups.Io" <pulaskite@...>
To: [email protected]
Sent: 3/14/2019 6:03:56 PM
Subject: Re: [TekScopes] Test input for an SD-32 sampling head

I have one of Leo's 100 pS impulse units as a source for initial experiments. If I can narrow that to 10 -20 pS with discrete SMD parts I may be able to get the idea to work. There's a close connection to the Hilbert operator hiding in there somewhere.

I've been reading an excellent book on FPGA implementation of DSP by Roger Woods et al most of the afternoon. So I've not started on the dissertation yet. I can't really say much else until I understand the mathematics and physics of using the reverse biased diodes as capacitors. That should keep me entertained for a few weeks at least.

In any case, failure doesn't matter. It's a hobby project, not a client deliverable. I've been fascinated by the problem of getting a fast rise time edge for a long time. It's a bit of circular logic. My excuse for doing it is I bought an 11801 and my excuse for buying the 11801 is so I could try to do it. If I can narrow the 100 pS pulse by 5x I'll have an excuse to buy an SD-32.

I spent 3 years studying sparse L1 pursuits using "A Mathematical Introduction to Compressive Sensing" by Foucart and Rauhut as a text followed by reading the original papers by Donoho, Candes et al. Beats the hell out of watching television. I just wish I could find someone else who was interested in the subject to discuss it with. It's quite amazing what you can do with sparse L1 pursuits and really easy to do in practice. Understanding the math is not easy, but most people use FFTs without really understanding them.

Have Fun!
Reg


---
This email has been checked for viruses by AVG.


 

I wrote a "tidbit" on NLTL patents for Microwave Magazine. You can find it
here:



There's quite a bit of history in NLTLs, so one can spend days/weeks
wandering and reading. Don't ask me how I know.

On Fri, Mar 15, 2019 at 2:10 AM Jim Ford <james.ford@...> wrote:

Hi, Reg.

Regarding fast pulses and such, there is a wealth of information at Jim
Andrews' page here: He founded
Picosecond Pulse Labs in 1980 and sold it to Tektronix in 2014. I used
PPL products with a CSA803 back in the mid 1990's at Lockheed. I think
the sampling head I used was an SD-24, but since it was about 25 years
ago, my memory is a bit fuzzy.

These days I have a 7904, a 7603, a 7S12, a 7S11, two S-4 sampling
heads, S-53 and S-51 triggering heads, etc in my garage lab. Oh, and a
couple of 10:1 probes I made out of board-edge SMA connectors, 450 ohm
(470 paralleled with 1.8k ohm) 0402 resistors, and 3-pin right-angle 0.1
inch spacing headers. I've not completely characterized the probes, but
at least they pass up to about 12-13 GHz without much attenuation above
the expected 20 dB. Planning to use them to probe some digital RF
boards I'm going to build for work (Raytheon). Too much trouble to try
to get a fast enough sampling scope at work :(

Enjoy the PPL app notes! I've referred to AN-2a through -2e often.

Thanks for the literature references. I'll have to check them out
(someday).

Jim Ford


------ Original Message ------
From: "Reginald Beardsley via Groups.Io" <pulaskite@...>
To: [email protected]
Sent: 3/14/2019 6:03:56 PM
Subject: Re: [TekScopes] Test input for an SD-32 sampling head

I have one of Leo's 100 pS impulse units as a source for initial
experiments. If I can narrow that to 10 -20 pS with discrete SMD parts I
may be able to get the idea to work. There's a close connection to the
Hilbert operator hiding in there somewhere.

I've been reading an excellent book on FPGA implementation of DSP by
Roger Woods et al most of the afternoon. So I've not started on the
dissertation yet. I can't really say much else until I understand the
mathematics and physics of using the reverse biased diodes as capacitors.
That should keep me entertained for a few weeks at least.

In any case, failure doesn't matter. It's a hobby project, not a client
deliverable. I've been fascinated by the problem of getting a fast rise
time edge for a long time. It's a bit of circular logic. My excuse for
doing it is I bought an 11801 and my excuse for buying the 11801 is so I
could try to do it. If I can narrow the 100 pS pulse by 5x I'll have an
excuse to buy an SD-32.

I spent 3 years studying sparse L1 pursuits using "A Mathematical
Introduction to Compressive Sensing" by Foucart and Rauhut as a text
followed by reading the original papers by Donoho, Candes et al. Beats the
hell out of watching television. I just wish I could find someone else who
was interested in the subject to discuss it with. It's quite amazing what
you can do with sparse L1 pursuits and really easy to do in practice.
Understanding the math is not easy, but most people use FFTs without really
understanding them.

Have Fun!
Reg


---
This email has been checked for viruses by AVG.





 

Hmm... I've not heard of the tidbits before, although I use IEEEXplore fairly often at work.? ?I will try it tonight from a real computer.? Not so much fun trying to read serious articles on a little smartphone screen...Thanks, Mark!Jim Ford?Sent from my Verizon, Samsung Galaxy smartphone

-------- Original message --------From: Mark Kahrs <mark.kahrs@...> Date: 3/19/19 8:13 AM (GMT-08:00) To: [email protected] Subject: Re: [TekScopes] Test input for an SD-32 sampling head I wrote a "tidbit" on NLTL patents for Microwave Magazine.? You can find ithere:'s quite a bit of history in NLTLs, so one can spend days/weekswandering and reading.? Don't ask me how I know.On Fri, Mar 15, 2019 at 2:10 AM Jim Ford <james.ford@...> wrote:> Hi, Reg.>> Regarding fast pulses and such, there is a wealth of information at Jim> Andrews' page here: He founded> Picosecond Pulse Labs in 1980 and sold it to Tektronix in 2014.? I used> PPL products with a CSA803 back in the mid 1990's at Lockheed.? I think> the sampling head I used was an SD-24, but since it was about 25 years> ago, my memory is a bit fuzzy.>> These days I have a 7904, a 7603, a 7S12, a 7S11, two S-4 sampling> heads, S-53 and S-51 triggering heads, etc in my garage lab.? Oh, and a> couple of 10:1 probes I made out of board-edge SMA connectors, 450 ohm> (470 paralleled with 1.8k ohm) 0402 resistors, and 3-pin right-angle 0.1> inch spacing headers.? I've not completely characterized the probes, but> at least they pass up to about 12-13 GHz without much attenuation above> the expected 20 dB.? Planning to use them to probe some digital RF> boards I'm going to build for work (Raytheon).? Too much trouble to try> to get a fast enough sampling scope at work :(>> Enjoy the PPL app notes!? I've referred to AN-2a through -2e often.>> Thanks for the literature references.? I'll have to check them out> (someday).>> Jim Ford>>> ------ Original Message ------> From: "Reginald Beardsley via Groups.Io" <pulaskite@...>> To: [email protected]> Sent: 3/14/2019 6:03:56 PM> Subject: Re: [TekScopes] Test input for an SD-32 sampling head>> >I have one? of Leo's 100 pS impulse units as a source for initial> experiments.? If I can narrow that to 10 -20 pS with discrete SMD parts I> may be able to get the idea to work.? There's a close connection to the> Hilbert operator hiding in there somewhere.> >> >I've been reading an excellent book on FPGA implementation of DSP by> Roger Woods et al most of the afternoon.? So I've not started on the> dissertation yet.? I can't really say much else until I understand the> mathematics and physics of using the reverse biased diodes as capacitors.> That should keep me entertained for a few weeks at least.> >> >In any case, failure doesn't matter.? It's a hobby project, not a client> deliverable.? I've been fascinated by the problem of getting a fast rise> time edge for a long time.? It's a bit of circular logic.? My excuse for> doing it is I bought an 11801 and my excuse for buying the 11801 is so I> could try to do it.? If I can narrow the 100 pS pulse by 5x I'll have an> excuse to buy an SD-32.> >> >I spent 3 years studying sparse L1 pursuits? using "A Mathematical> Introduction to Compressive Sensing" by Foucart and Rauhut as a text> followed by reading the original papers by Donoho, Candes et al.? Beats the> hell out of watching television.? I just wish I could find someone else who> was interested in the subject to discuss it with.? It's quite amazing what> you can do with sparse L1 pursuits and really easy to do in practice.> Understanding the math is not easy, but most people use FFTs without really> understanding them.> >> >Have Fun!> >Reg> >> >> >>> ---> This email has been checked for viruses by AVG.> >> >>


 

Mark,

Thanks. I have to drive 150 miles round trip to access IEEE papers. I'll be collecting lots of NLTL papers the next time I go to Little Rock.

At the moment I'm working on deriving the equations for a transmission line with impedance steps designed to steepen the leading edge. Purely a passive linear pulse shaper using a coplanar waveguide with an air dielectric with no components if possible. After I have explored that I'll look into the magnitude of the improvement I can get using non-linear elements.

What I have in mind is a coplanar waveguide which starts with a 10 ohm impedance and then in a series of steps rises to 50 ohms. The concept is to apply a phase delay to the low frequencies which is greater than the delay applied to the high frequencies. My biggest concern at the moment is how to make the Q of the low frequency sections low enough to be physically tractable without resorting to coaxial cable.

Each step in impedance produces an infinite impulse response, so the mathematical notation can quickly get out of hand.

I have copied all the stuff from KH4HTV's website and read through most of it. Very nice stuff.

Leo Bodnar uses a Maxim 3949 LED driver in his pulsers. That is specified as 22 ps typical, 36 ps maximum Tr & Tf. That's already quite fast.

A fascinating aspect of this is that the mathematics are closely related to the normal incidence plane wave response of a layered medium in reflection seismology, the design of anti-reflection coatings in optics and to ultra wideband antenna design.


Have Fun!
Reg


 

Yes, the math is the same no matter whether it's coplanar waveguide,
seismology, anti-reflection coatings, UWB antennas, or dozens of other
applications. A wave is a wave. About 8 years ago I gave a
presentation on fiber optics to my RF and microwave colleagues. I
explained that fiber is just a roughly 200 terahertz circular dielectric
waveguide. And the quarter wavelength thick anti-reflection coatings on
the facets of a semiconductor optical amplifier operate in the same way
as quarter wave matching transformers at RF or microwave frequencies.

My personal preference is to do engineering for a living but stay close
to the physics and math. Sounds like you're the same way, Reg.

Jim

------ Original Message ------
From: "Reginald Beardsley via Groups.Io" <pulaskite@...>
To: [email protected]
Sent: 3/19/2019 11:06:09 AM
Subject: Re: [TekScopes] Test input for an SD-32 sampling head

Mark,

Thanks. I have to drive 150 miles round trip to access IEEE papers. I'll be collecting lots of NLTL papers the next time I go to Little Rock.

At the moment I'm working on deriving the equations for a transmission line with impedance steps designed to steepen the leading edge. Purely a passive linear pulse shaper using a coplanar waveguide with an air dielectric with no components if possible. After I have explored that I'll look into the magnitude of the improvement I can get using non-linear elements.

What I have in mind is a coplanar waveguide which starts with a 10 ohm impedance and then in a series of steps rises to 50 ohms. The concept is to apply a phase delay to the low frequencies which is greater than the delay applied to the high frequencies. My biggest concern at the moment is how to make the Q of the low frequency sections low enough to be physically tractable without resorting to coaxial cable.

Each step in impedance produces an infinite impulse response, so the mathematical notation can quickly get out of hand.

I have copied all the stuff from KH4HTV's website and read through most of it. Very nice stuff.

Leo Bodnar uses a Maxim 3949 LED driver in his pulsers. That is specified as 22 ps typical, 36 ps maximum Tr & Tf. That's already quite fast.

A fascinating aspect of this is that the mathematics are closely related to the normal incidence plane wave response of a layered medium in reflection seismology, the design of anti-reflection coatings in optics and to ultra wideband antenna design.


Have Fun!
Reg



---
This email has been checked for viruses by AVG.


 

Reg,

This sounds interesting. I have HFSS so I can analyze the kinds of circuits you describe in the frequency domain. It sounds like a high frequency peaking circuit. It may be that HFSS or some part of the suite can do time domain calculations. I don't know. I design rf linear accelerators and waveguide systems for them in the frequency domain.

Jim


 

I'd personally prefer to have unrestricted access to the world wide databases of a super major oil company for about 3 years. But that's unlikely to happen. So I'm contenting myself playing with electronics. And having a blast doing it.

It is a lot more fun if you stay close to the physics and math. Because the payoff is you already know most of the answer when you encounter a new problem. A lot of times you beat on it for a while and then realize, "Oh, I recognize that". I had to teach myself seismology by analogy to optics which I had a very good training in as an igneous petrologist looking through a polarized light microscope all day for many months.

I'd love to know how much math Jim Williams, Widlar and Pease knew. They clearly understood the physics far better than most PhDs.

My current problem is how to delay the lower frequencies of a 10 MHz square wave without killing the higher frequencies. Using tapered steps in a transmission line will let me select the frequencies, but I've still got the problem of resonator length and the associated capacitance. If you can suggest literature references I'd be most grateful. It's a bit of a hassle, but I can circumvent the IEEE paywall by going the the UALR library about 75 miles from me. My current list is all the work by Bode, Nyquist and Shannon and then whatever NLTL papers I find.

The Maxim 3949 should give a 22 ps Tr & Tf typical case. So if I run that through a physical all pass filter, just making it minimum phase will give me a faster edge. Running Octave in a VM is *not* a good idea.

My NVRAM chips for the 11801 are in the post so I'm eager to start doing some physical experiments.

I've got paper copies of the user and service manuals on the way and a PDF of the service manual to study while I wait. When I install the NVRAM I'm going to copy all the ROMs and put together an 11801 support kit.

My one concern with the 11801 is the timebase jitter of 1.4 ps. With the ready availability of sub ps jitter clock chips that seems an attractive upgrade. But without schematics potentially very time consuming. However, it would make the 30 year old instrument quite competitive with more recent instruments.

Has anyone made board extenders for the series? The loud sucking sound you hear is Reginald being pulled into another project.

Have Fun!
Reg

--------------------------------------------

On Tue, 3/19/19, Jim Ford <james.ford@...> wrote:

Subject: Re: [TekScopes] Test input for an SD-32 sampling head
To: [email protected]
Date: Tuesday, March 19, 2019, 8:57 PM

Yes, the math is the same no
matter whether it's coplanar waveguide,
seismology, anti-reflection coatings, UWB
antennas, or dozens of other
applications.?
A wave is a wave.? About 8 years ago I gave a
presentation on fiber optics to my RF and
microwave colleagues.? I
explained that
fiber is just a roughly 200 terahertz circular dielectric
waveguide.? And the quarter wavelength thick
anti-reflection coatings on
the facets of a
semiconductor optical amplifier operate in the same way
as quarter wave matching transformers at RF or
microwave frequencies.

My
personal preference is to do engineering for a living but
stay close
to the physics and math.? Sounds
like you're the same way, Reg.

Jim


 

I had a course in linear systems which used Bracewell's "The Fourier Transform and its Applications". Courtesy of the dictionary of transform pairs in the back I can work in both time and frequency just drawing cartoons with pencil and paper. And Octave will take care of the detailed calculations.

My biggest handicap at present is I spent my career working with digital systems in recorded time. So I've familiar with things that can't be done in real time or in the analog domain. Lots of rabbit holes to fall into.

Consider a triangular pulse with symmetric 22 ps slopes. Can that be converted into a sawtooth pulse without significant loss of BW? If so, how? Mathematically it just requires making the pulse minimum phase to get a vertical leading edge. But TANSTAFL. If it were easy, 1 ps rise time pulses would be common.

I keep hoping that a member of the 118xx design team will wander by with schematics from a box in their garage.

Have Fun!
Reg

--------------------------------------------

On Tue, 3/19/19, Jim Potter <jpotter@...> wrote:

Subject: Re: [TekScopes] Test input for an SD-32 sampling head
To: [email protected]
Date: Tuesday, March 19, 2019, 9:36 PM

Reg,

This sounds interesting. I have HFSS so I can
analyze the kinds of circuits you describe in the frequency
domain. It sounds like a high frequency peaking circuit. It
may be that HFSS or some part of the suite can do time
domain calculations. I don't know. I design rf linear
accelerators and waveguide systems for them in the frequency
domain.

Jim


 

Regarding jitter reduction, can you average it out?? I recall somebody here on TekScopes mentioning using a 7854 with an S-4 or S-6 sampling head, I assume in a 7S11 or 7S12 plug-in, to get effectively zero ps jitter.? Of course that comment put the 7854 on my wishlist...Jim?Sent from my Verizon, Samsung Galaxy smartphone

-------- Original message --------From: "Reginald Beardsley via Groups.Io" <pulaskite@...> Date: 3/20/19 6:45 AM (GMT-08:00) To: [email protected] Subject: Re: [TekScopes] Test input for an SD-32 sampling head I'd personally prefer to have unrestricted access to the world wide databases of a super major oil company for about 3 years.? But that's unlikely to happen.? So I'm contenting myself playing with electronics.? And having a blast doing it.It is a lot more fun if you stay close to the physics and math.? Because the payoff is you already know most of the answer when you encounter a new problem. A lot of times you beat on it for a while and then realize, "Oh, I recognize that".? I had to teach myself seismology by analogy to optics which I had a very good training in as an igneous petrologist looking through a polarized light microscope all day? for many months.I'd love to know how much math Jim Williams, Widlar and Pease knew.? They clearly understood the physics far better than most PhDs.My current problem is how to delay the lower frequencies of a 10 MHz square wave without killing the higher frequencies.? Using tapered steps in a transmission line will let me select the frequencies, but I've still got the problem of resonator length and the associated capacitance.? If you can suggest literature references I'd be most grateful.? It's a bit of a hassle, but I can circumvent the IEEE paywall by going the the UALR library about 75 miles from me.? My current list is all the work by Bode, Nyquist and Shannon and then whatever NLTL papers I find.The Maxim 3949 should? give a 22 ps Tr & Tf typical case.? So if I run that through a physical? all pass filter, just making it minimum phase will give me a faster edge.? Running Octave in a VM is *not* a good idea.My NVRAM chips for the 11801 are in the post so I'm eager to start doing some physical experiments.I've got paper copies of the user and service manuals on the way and a PDF of the service manual to study while I wait.? When I install the NVRAM I'm going to copy all the ROMs and put together an 11801 support kit.My one concern with the 11801 is the timebase jitter of 1.4 ps.? With the ready availability of sub ps jitter clock chips that seems an attractive upgrade.? But without schematics? potentially very time consuming.? However, it would make the 30 year old instrument quite competitive with more recent instruments.Has anyone made board extenders for the series?? The loud sucking sound you hear is Reginald being pulled into another project.Have Fun!Reg--------------------------------------------On Tue, 3/19/19, Jim Ford <james.ford@...> wrote: Subject: Re: [TekScopes] Test input for an SD-32 sampling head To: [email protected] Date: Tuesday, March 19, 2019, 8:57 PM Yes, the math is the same no matter whether it's coplanar waveguide, seismology, anti-reflection coatings, UWB antennas, or dozens of other applications.? A wave is a wave.? About 8 years ago I gave a presentation on fiber optics to my RF and microwave colleagues.? I explained that fiber is just a roughly 200 terahertz circular dielectric waveguide.? And the quarter wavelength thick anti-reflection coatings on the facets of a semiconductor optical amplifier operate in the same way as quarter wave matching transformers at RF or microwave frequencies. My personal preference is to do engineering for a living but stay close to the physics and math.? Sounds like you're the same way, Reg. Jim


 

There are issues with doing that. It looks better, but is not accurate. KH4HTV of Picosecond Pulse Labs wrote an app note on that giving the mathematical details.

I'm doing battle with creating minimum phase wavelets via the Hilbert transform in Octave :-(

Unfortunately people toss around "Hilbert transform" a bit too casually. So the term may be the same, but the meaning is different.

I think I have found a counter argument to my expectations. But still not sure if I' dealing with software bugs or thinking bugs. Very likely a bit of both.


--------------------------------------------

On Wed, 3/20/19, Jim Ford <james.ford@...> wrote:

Subject: Re: [TekScopes] Test input for an SD-32 sampling head
To: [email protected]
Date: Wednesday, March 20, 2019, 10:08 AM

Regarding jitter reduction, can you average it out?


 

On Wed, Mar 20, 2019 at 04:08 PM, Jim Ford wrote:


Regarding jitter reduction, can you average it out?? I recall somebody here
on TekScopes mentioning using a 7854 with an S-4 or S-6 sampling head, I
assume in a 7S11 or 7S12 plug-in, to get effectively zero ps jitter.? Of
course that comment put the 7854 on my wishlist...
Averaging and accepting the average as the truth is only acceptable if the dataset has a nice, even distribution, without bias to either side.
Still, no reason not to desire a 7854.

Raymond


 

Ah, limitations noted.? Thanks, Reg and Raymond.Someday I will have that 7854.? And someplace to put it!? 7904, 7603, 5110N, and HP 54504A DSO already taking up most of the shelf space over my work bench.? I have made a space for a 19 inch rack at the side of the bench, though.JimSent from my Verizon, Samsung Galaxy smartphone

-------- Original message --------From: Raymond Domp Frank <hewpatek@...> Date: 3/20/19 10:32 AM (GMT-08:00) To: [email protected] Subject: Re: [TekScopes] Test input for an SD-32 sampling head On Wed, Mar 20, 2019 at 04:08 PM, Jim Ford wrote:>> Regarding jitter reduction, can you average it out?? I recall somebody here> on TekScopes mentioning using a 7854 with an S-4 or S-6 sampling head, I> assume in a 7S11 or 7S12 plug-in, to get effectively zero ps jitter.? Of> course that comment put the 7854 on my wishlist...>Averaging and accepting the average as the truth is only acceptable if the dataset has a nice, even distribution, without bias to either side.Still, no reason not to desire a 7854.Raymond