Base current noise will eventually be an issue with paralleled bipolars. You could parallel a mess of jfets, too, the penalty then becoming input capacitance.
Noise is a real nuisance.
The circuit is not for public release, but I'll email it to you if you're interested.
--
John Larkin Highland Technology, Inc
picosecond timing laser drivers and controllers
jlarkin att highlandtechnology dott com
http://www.highlandtechnology.com
Actually not, if you choose the Ic current in the first place to get a nice low e_n, but then discover r_bb' is the big problem. Each of n paralleled transistors is operated at Ic' = Ic / n, there's no increase in the base current, only a decrease in r_bb'.
I mean, yes of course, base current can be a problem, but the paralleling trick doesn't exacerbate it.
I sure hope I don't get tired of electronics. It's the only thing that I'm reasonably good at.
--
John Larkin Highland Technology, Inc
picosecond timing laser drivers and controllers
jlarkin att highlandtechnology dott com
http://www.highlandtechnology.com
--
John Larkin Highland Technology, Inc
picosecond timing laser drivers and controllers
jlarkin att highlandtechnology dott com
http://www.highlandtechnology.com
Wow, this sounds interesting. I tried some medium-power BJTs for a low-e_n application some years back, exactly hoping to find a low Rbb', preferably simultaneously with a high hFE. A forget the exact types, they were Zetex, too. It wasn't very successful, however.
Usually, that kind of ohmic emitter character is intentional, as a resistive emitter metallization is effective at preventing thermal runaway (second breakdown). This 140V/5A transistor has a safe operating area that limits to 10V at 100 mA. By comparison, TIP31C (100V/3A) has a safe operating area that limits to 80V at 100 mA. I think that means the emitter degeneration resistance was minimized for the ZX... part.
I also have played that game with 10 pairs of ADA4898-2. That may have advantages wrt pssr, drift and temp. dependence. The improvement in en was testbook-like < 220 pV/sqrtHz from
You can use a jfet as a follower, which automagically bootstraps Cgs, and then you can bootstrap the drain to reduce Cdg. So you can eliminate most of the input capacitance, but get no voltage gain. So, follow the fet with a low-noise bipolar opamp or, better yet, a transformer and more fets, and take care of any DC requirements off to the side.
We're getting into low-noise-no-free-lunch territory.
I wanted the emitter follower in question precisely to bootstrap a jfet drain.
--
John Larkin Highland Technology, Inc
picosecond timing laser drivers and controllers
jlarkin att highlandtechnology dott com
http://www.highlandtechnology.com
A major residual noise source in JFET bootstrapped-bootstraps is the drain bootstrap's noise coupled back via C_DG.
The noise of the current booster (series feedback/Sziklai/PNP wraparound, whatchamacallit) is inside the loop controlled by the JFET(s), so its noise basically goes away. The drain bootstrap isn't in the loop, so its noise doesn't. It doesn't always matter that much, especially if whatever you're bootstrapping has a gross amount of capacitance, so that the FET noise dominates via the omega C_in * e_N mechanism, but it often does at lower capacitance.
I've played with putting the drain bootstrap inside the loop, but it hurts the bandwidth, so the parallelled BJT method is better.
Cheers
Phil Hobbs
--
Dr Philip C D Hobbs
Principal Consultant
ElectroOptical Innovations LLC
Optics, Electro-optics, Photonics, Analog Electronics
160 North State Road #203
Briarcliff Manor NY 10510
hobbs at electrooptical dot net
http://electrooptical.net
Just received the AoE 3rd ed, the story seems to be there, interesting. The ZTX951 hFE is not that wonderful, however, indicating that Tn is not so great - and that's what I'd need with my typically cold generators. The two discontinued classics look better, but they are ..er.. discontinued.
Anyway, I forgot what made me abandon the low Rbb' quest: the fact that there is always cryostat wiring, which must be resistive due to Wiedemann-Franz, and which plays a more significant role that the Rbb'. Cold SiGe transistors are amazing, however. We have a batch of NESG3031's whose hFE peaks at 27000 at 20K. Those can provide gain before the Johnson noise due to wiring adds.
The book looks like a very interesting read, packed with Phil's clever tricks. And those selection tables are truly valuable.
I supplied only a minute fraction of the tricks, and they're nicely acknowledged. I agree about the graphs and tables. There's a _lot_ of information there, and it seems to be pretty up to date, which is amazing considering how long Win and Paul have been working on it. (They must have felt like Sisyphus sometimes.)
Cheers
Phil Hobbs
--
Dr Philip C D Hobbs
Principal Consultant
ElectroOptical Innovations LLC
Optics, Electro-optics, Photonics, Analog Electronics
160 North State Road #203
Briarcliff Manor NY 10510
hobbs at electrooptical dot net
http://electrooptical.net
At 20K. The data-sheets documents the behaviour at room temperature, 298K, or 25C.
With silicon transistors, the current gain usually went up with temperature , rather than down, but Phil will probably be able to explain why SiGe part s might be different.
Bob Widlar at National Semiconductor worked out a way of making super-beta silicon transistors in 1969, and the LM308 depended on their magical proper ties. IIRR the current gain was still only about 3000 and the collector bas e-breakdown voltage was extremely low.
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