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Low-impedance passive probes as an alternative to active probes at GHz frequencies

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Simplified circuit models of an active probe and a low-impedance passive probe connected to a 50 Ω line

Fig. 1. Simplified models of an active and a low-impedance passive probe on a 50 Ω line.

Above a few hundred megahertz a circuit no longer sees the 1 MΩ specified for an active probe. It sees the tip capacitance. A well-designed passive divider into a 50 Ω input is a strong alternative to an active probe in this range, and with low tip capacitance it can even load the circuit less.

Active probes have a buffer amplifier in the probe head. Low-impedance passive probes, also called Z0, 50 Ω or voltage divider probes, have none1. This article explains why the passive type is a strong alternative for GHz work, and when it can outperform an active probe.

What the circuit sees at GHz frequencies

Any probe adds a resistance in parallel with a capacitance from the probed node to ground. As the frequency increases the capacitive reactance falls and takes over1, 2.

Capacitive reactance formula and the impedance of a 1 pF tip at 100 MHz, 1 GHz and 3 GHz

Measured active probes can dip even lower in the upper part of their bandwidth, to between 15 Ω and a few hundred ohms3, 4, 5.

Inside a low-impedance passive probe

The tip feeds a 50 Ω cable terminated by the 50 Ω instrument input. A terminated cable hides its own capacitance, so the circuit sees only the tip network in series with 50 Ω1, 6.

Input resistance and 10:1 division ratio of a low-impedance passive probe

On paper the tip is a single 450 Ω resistor. In a real GHz probe it is a network of components that together behave as 450 Ω. The needle, mechanics, PCB layout and cable transition are tuned together so that the network stays resistive and the response stays flat into the GHz range.

Measured gain versus frequency for SQG60-DC, SQG30-DC and SQG15-DC probes

Fig. 2. Measured gain versus frequency of production SQG60-DC, SQG30-DC and SQG15-DC probes. The level of about −20 dB is the 10:1 division ratio. The response is flat within ±0.5 dB from DC to 5.2 GHz, 2.7 GHz and 1.5 GHz respectively7.

A flat response divides every frequency component by the same factor. Edges, ringing and harmonics reach the instrument in the right proportions.

Comparing the loading

Figure 3 compares the modelled impedance of the two probe types. Below roughly 370 MHz the active probe loads the circuit less. Above it a 500 Ω probe with low tip capacitance presents the higher impedance and outperforms the active probe. At GHz frequencies the tip capacitance decides, not the DC resistance.

Modelled input impedance versus frequency for conventional passive, active and low-impedance passive probes

Fig. 3. Modelled input impedance of a conventional 10:1 passive probe, an active probe and generic low-impedance passive probes with two values of tip capacitance. Calculated as |Z| = |R ∥ 1/(j2πfC)|. The curves illustrate the principle and do not represent a specific product.

On a 50 Ω line the 500 Ω is a light load. A point on a line terminated at both ends behaves like a 25 Ω source2, 5, so the probe leaves 500/525 of the voltage, or −0.42 dB.

Loading of a 500 Ω probe on a 50 Ω line and the effect on 3.3 V, 1.8 V and 1.2 V logic levels

Where passive probes have the advantage

Wide signal range. Typical 1.5 GHz to 3.5 GHz active probes have a linear range of ±8 V, some only ±4 V8, 9, 10, 11. A passive divider has no amplifier that can saturate. Its limit is the voltage and power rating of the front end.

Robustness. Active probes can be damaged by electrostatic discharge1, 12. Passive probes are more robust to overvoltage and ESD6.

Any 50 Ω instrument. An active probe needs power and the manufacturer’s probe interface12. A passive probe works with any oscilloscope, sampling oscilloscope, network analyzer or spectrum analyzer with a 50 Ω input.

Low added noise. A 10:1 probe raises the instrument noise, referred to the tip, by a factor of ten. Most active probes in this class also divide by ten8, 9 and add 1.2 mV to 2.5 mV RMS of amplifier noise on top8, 11. A passive divider adds only a few microvolts of thermal noise.

Cost. Distributor prices for 1.5 GHz to 3.5 GHz active probes, checked in October 2026, ranged from about USD 3,000 to USD 8,00013. Low-impedance passive probes for 1.5 GHz to 6 GHz are available from about USD 190 to USD 3907, so an AC-coupled and a DC-coupled probe can both be on the bench for a fraction of the price of one active probe.

AC or DC coupling

A DC-coupled probe shows the complete signal including logic levels and bias. Its 500 Ω also loads the DC level, which is fine on low-impedance outputs, terminated lines and supply rails. An AC-coupled probe adds a DC block, so no DC current flows through the probe. Use it on DC-biased high-speed links such as USB, PCIe, SATA and HDMI, and for ripple on supply rails7.

Low-speed buses and high-impedance nodes

A 500 Ω probe is not meant for high-impedance nodes. On an I²C line with a 10 kΩ pull-up to 5 V it would pull the idle level down to about 0.24 V14. Such measurements are best made with a high-quality conventional 10:1 passive probe, such as the PCBite SQ100 to SQ500. Its 10 MΩ leaves the bias undisturbed, and its tip capacitance of around 10 pF is small next to the 400 pF the I²C specification allows per bus line15.

Active probes fill the gap between the two passive types, with fast signals on high-impedance nodes and instruments that have only 1 MΩ inputs14.

Which probe type to use on 50 Ω lines, DC-biased links and pull-up nodes

Fig. 4. The impedance, DC level and speed of the node decide which probe disturbs the circuit least.

Low-impedance probing with PCBite SQG

The PCBite SQG series offers handsfree low-impedance probes for 1.5 GHz, 3 GHz and 6 GHz, each in AC-coupled and DC-coupled versions7.

See the SQG high-frequency probes.

References

  1. Tektronix, ABCs of Probes, primer 60W-6053-17.
  2. Tektronix, Probing Tips for High Performance Design and Measurement, application note 51W-60631-0.
  3. H. Johnson, Probing High-Speed Digital Designs, Signal Consulting.
  4. D. C. Smith, Active Probe Design Philosophy, Technical Tidbit, October 2004.
  5. Keysight Technologies, Optimizing Oscilloscope Measurement Accuracy on High-Performance Systems with Keysight Active Probes, 5988-5021EN, 2014.
  6. Teledyne LeCroy, Transmission Line Probes, product overview.
  7. Sensepeek, PCBite SQG series high-frequency handsfree probes, data sheet. Prices EUR 169 to EUR 349 (manufacturer’s suggested retail price), converted at 1.12 USD/EUR (2026-10-14) and rounded.
  8. Rohde & Schwarz, R&S RT-Zxx High Bandwidth Probes, data sheet v26.00, 2022 (RT-ZS10, RT-ZS20, RT-ZS30, RT-ZZ80).
  9. Tektronix, TAP1500 1.5 GHz Active Probe, data sheet.
  10. Tektronix, TAP2500 and TAP3500 Active Probes, data sheet 51W-19044-12, 2023.
  11. Keysight Technologies, N2795A, N2796A and N2797A Active Probes, data sheet 5990-6480EN, 2014, and N2796A product page.
  12. Keysight Technologies, Eight Hints for Better Scope Probing, application note 5989-7894EN, 2014.
  13. Distributor prices checked 2026-10-14, excluding sales tax. Transcat (Keysight N2796A 2 GHz USD 3,917, Tektronix TAP1500 1.5 GHz USD 5,490, TAP3500 3.5 GHz USD 7,960), ValueTronics (Teledyne LeCroy ZS1500 1.5 GHz USD 3,060).
  14. A. Zonenberg, AKL-PT1 Operator Manual, Antikernel Labs, 2020.
  15. NXP Semiconductors, UM10204 I²C-bus specification and user manual, capacitive load for each bus line.

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