Martin Brown from EDN Network build this Oscilloscope Probe. In the original article, he describes a lot about this. Below is some excerpt.
Modern power supplies are edging upward in operational frequency. The benefits include a reduction in size and weight, plus an increase in energy density. For these designs, engineers are migrating to high-frequency power switch and rectifier technologies. The traditional planar or trench MOSFET switches with rise/fall times 30 nsec to 60 nsec are giving way to power switches such as superjunction MOSFETs, GaN MOSFETs, SiC MOSFETs and SiC Schottky rectifiers that switch in less than 5 nsec.
To view such fast transitions, you typically need an oscilloscope with at least 1 GHz bandwidth. Unfortunately, most commercially available voltage and current probes are woefully inadequate at these high frequencies. The average oscilloscope probe has a bandwidth of less than 300 MHz. Current probes can have bandwidths of 60 MHz to 100 MHz or less. Furthermore, high-frequency voltage probes often cost over $12,000 and slightly better current probes start at $4,000. For power engineers who work for mid-sized companies, there is only one path: build your own probes.
Designing and building high-frequency voltage and current probes requires a good understanding of RF, parasitics, transmission-line theory, and field theory.
Commercial probe shortcomings
Commercially available oscilloscope voltage and current probes are robust, ergonomically well designed, and accurate. They have served their markets well where the overwhelming number of applications operate at much less than 1 GHz. The operating frequencies and the edges of new-generation switching transistors are exceeding 1 GHz, resulting in rise and fall times in the sub 5 ns range.
A commercial probe’s low bandwidth can create a major limitation to accurate measurements. Engineers often take for granted the slow rise and fall times and they can easily overlook missing information. In addition, the common probe’s connection to the signal source can cause distortions. These connections have a significant length of unshielded connecting leads, particularly the ground lead. A 4–6 in. (10–15 cm) ground lead can pick-up radiated noise from the circuit or other sources and inject it into the coax cable as a common-mode signal. This unrecognized noise adds to the real signal.
Figure 1 shows a typical commercial voltage probe. It contains a length of unshielded signal or ground wire that acts as a loop antenna. The amount of noise it picks up is proportional to the loop size and the amount of noise energy and noise spectrum. You can view this noise by simply clipping the ground lead to the probe tip and hold it near the target circuit board.
Figure 1. Common voltage oscilloscope probe construction has a ground lead that you clip to the circuit under test.
Instead, you can construct your own 50 Ω voltage probe. By constructing custom 50 Ω voltage probes, the you can better define and understand what is really happening within the circuit. The overall goals of constructing 50 Ω voltage probes are:
1:1 Shielded Coax Voltage Probe
For those signals below the maximum input voltage rating of the oscilloscope input, you can use a cut length of a 50 Ω BNC coax cable as your probe. The length of the unshielded center conductor and the shield pigtail should be kept to less than 1 in. (25 cm) to minimize noise pickup. For viewing a signal at a particular node, solder the center conductor directly to that node; the ground lead should be soldered to the closest associated ground. That is, not to a ground that has a long PCB trace length between the probe and the node of interest. This probe only provides high frequency signal shielding from the target circuit to the oscilloscope. The input termination setting of the oscilloscope scope should be 1 MΩ. Figure 2 shows the design of a 1:1 shielded probe.
Figure 2. The 1:1 Shielded voltage probe is based on coax cable. Inductance on the probe tip (LUS) and ground lead (LG) will limit bandwidth but the small size will help minimize noise pickup.
n:1 50 Ω voltage probe
The n:1 probe is intended for signal amplitudes (including any spikes) that exceed the maximum voltage rating of the oscilloscope’s input amplifier. This probe is a bit more complicated to construct. Its simplified schematic is shown in Figure 3.
Figure 3. Simplified schematic of the n:1 voltage probe shows a series resistor RS that requires some calculations to find its value.
You can find more by following the Original Article here