The Effects of Passive Probe Ground Leads
This article explains how the inductance of passive probe ground leads can dramatically reduce effective bandwidth, distort measurements, and introduce resonance and frequency-response errors.
RF pickup can introduce misleading noise into power-rail measurements, but proper shielding and coaxial connections can dramatically reduce interference and reveal true signal behavior.
Channel equalization uses transmitter and receiver techniques to counteract losses, reduce ISI, and improve signal quality in high-speed data links.
Transmit de-emphasis enhances eye diagrams by reducing inter-symbol interference, improving signal clarity at the cost of lower overall amplitude.
Continuous Time Linear Equalization (CTLE) enhances high-speed serial signals by compensating for channel loss, improving eye openings while balancing noise performance.
S-parameters allow engineers to model, remove, or simulate channel effects in high-speed serial links, helping diagnose signal degradation and improve performance.
This practical walkthrough shows how to measure and diagnose ground bounce using oscilloscope techniques, quiet-low sense lines, and controlled I/O switching scenarios.
Ground bounce occurs when simultaneous switching currents flow through shared inductance in IC packages, creating voltage noise that can lead to digital bit errors.
Quiet-low and quiet-high I/O drivers can act as on-die sense lines, helping engineers observe and analyze ground bounce in digital systems.
Ground bounce occurs when multiple switching signals share a high-inductance return path, creating voltage noise that can disrupt digital I/O performance.
Broad dips in S-parameter plots typically result from stub resonances, where reflected signals interfere with the main signal path and reduce transmission at specific frequencies.
A monotonic drop-off in S21 indicates increasing signal attenuation with frequency, typically caused by dielectric and conductor losses in the interconnect.
Ripple patterns in S-parameters are caused by reflections from impedance discontinuities, with ripple spacing determined by interconnect length and ripple magnitude driven by impedance mismatch.