Re the Tek 585 and 585A. The vertical sections of these scopes are more-or-less "one of a kind" and they represent an end point in design in several areas. They are the last high-performance all-tube scopes that Tek made, and one has to consider both the CRT and the vertical amplifier separately. So far as the CRT goes, it is typical of what was used in the first 15 years after WWII, except for the distributed vertical deflection. Essentially, this means a Wehnelt gun, a collimating focus structure, deflection plates, and post-deflection acceleration (PDA). The distributed vertical deflection is laid out such that the vertical wave propagates down the deflection plate structure at the same speed the electron stream passes through it. It is a lumped-constant delay line. There are coils in the CRT between the plate segments, and the plate segments are constant capacitances. This type of delay line has a very definite cutoff frequency. A problem with post-deflection acceleration is that the PDA field is distorted by the deflection plates---higher voltage centered between the four plates than at the plates, which makes it a converging lens. This decreases deflection sentsitivity. The reason for using PDA is plain vanilla quantum fizzicks---more electron volts in the beam where it hits the phosphor, more phosphor activity, which improves the writing rate. In this answer, I'll ignore the effective potential of the phosphor screen, although controlling that is significant when designing CRT's. There are several gimmicks that can be used to control the lens shape of the PDA field. HP, Tek, and Dumont all used a flat Faraday shield screen in front of the deflection plates through the early sixties. This reverses the lens from converging to diverging---at the price of widening the spot, problems with the shield wires intercepting the beam at places, and deflection linearity. The 547 was the first Tek design to use such a Faraday shield, and the effect on deflection sensitivity was dramatic---I've forgotten the numbers, but it is something like 10 volts/CM instead of 30 in the vertical plane. The 585's never had such a tube. Peter Keller's book on CRT's does talk about other methods for improving sensitivity and so forth in the post-deflection electric fields. I don't know of a "comprehensive" text on all this----most of what was published in the forties ends with the type of CRT used in the 530/540 scopes, and I felt Keller was a bit obscure for the casual reader who isn't steeped in New Clear Fizzicks concepts. Modern methods are to slow the signal down with digital methodologies (the early sixties sampling scopes are essentially digital, although they don't convert the signal to digital data). I'll ignore the Tek 519 here---that was pretty much a laboratory exercise with no vertical amplifier, and most certainly not a general purpose bench scope. But it did use CRT technology similar to the 585. The vertical amplifier in the 585 is a fairly conventional distributed amplifier---principals of operation are not much different than the original 514 and 545's. However, the amplifier is double-terminated, not just source-terminated as in the 545. This cuts deflection sensitivity in half. When looking at tubes, one has to consider the transit time through a vacuum tubes, and it is mighty long compared with transit times through the base region of modern semiconductors. You have effects that are somewhat analogous to transistor stored charge and so forth, but you have to pay attention to things like virtual cathode points in the tube, as well as the transit time across distances on the order of a millimeter between grid and plate. I'm oversimplifying a bit here (go read Spangenberg and some of the other later texts) but it boils out that it is difficult to get a tube structure small enough, and with enough electron density to give you a gain-bandwidth product much more than 200 Mhz (I think this is the number for the 955 acorn---a product of 1933 technology). Nuvistors and frame grid toobs of the sixties did a little better, but they don't compare with a 600 Mhz. transistor Ft (those little dimey jobs you can buy anywhere) by a long shot. The crossover in gain-bandwidth performance moved to transistors with etched "mesa" and similar technologies in the early sixties. Once the manufacturers learned how to get yield out of angstrom-sized structures (10E-10 meter, a handy size nobody talks about any more), fundamental physics said that they were going to give peformance---if you could live within the voltage and power constraints that come with teeny tiny and semiconductor lattices. Historically, the 585 was announced as a "100 Megacycle" scope in 1959, using an 80-P80 plugin. This is a cathode follower gets-hot-in-your-hand job that isn't what most people consider "general purpose." As time went by (and a lot of time went by) Tek managed to come up with a general purpose plug-in (the 82) and probe that just plain weren't going to deliver enough bandwith (about 150 Mhz needed) at the vertical amplifier connector to give "a hunnert motorcyles" (as the argot went at Tek when this got discussed) at the CRT. At the same time, CRT yield, production tweaking, etc. pointed to backing off a bit from the original target. By 1963, Tek's razzle dazzle backed off to 85 Mhz for the design. Most 585's will beat that handily. The general philosophy behind backing off was more to control customer expectations. The 547 was presented entirely differently---50 Mhz at the probe tip, not 75 Mhz with a specialty plug-in, degrading the more general-purpose you make it. The real differences between the original 585 and the 585A are not in the vertical section, other than making the delay line termination tweakable. The big changes were the addition of a tunnel diode trigger setup that would work out to some reasonable frequency, and incorporation of a bunch of modification packages for the 585 that were suggested/recommended/mandatory for using the 82 and keeping the scope running for a while. In short, all the backing off from "100 Megacycles" was more like backing off from test stand horsepower to horsepower delivered to the tires. Henry van Cleef