Transmission Lines

Coax-to-CPW Transition

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A coax-to-CPW transition converts coaxial TEM mode to coplanar waveguide quasi-TEM mode. Center conductor connects to CPW center strip; outer conductor to ground planes. End-launch designs achieve return loss < -20 dB to 67 GHz (1.85 mm connectors) or 110 GHz (1.0 mm). Critical for on-wafer probing with GSG pitches of 50 to 250 μm, enabling S-parameter accuracy of ±0.1 dB to 110 GHz.
Category: Transmission Lines
Return loss: < -20 dB
Bandwidth: DC to 110+ GHz

Understanding Coax-to-CPW Transitions

Coplanar waveguide is the dominant transmission line for MMICs and high-frequency test fixtures because all conductors (signal and ground) are on the same surface, eliminating the need for via holes to a back-side ground plane and enabling direct probing of circuits. However, test equipment (network analyzers, signal generators, spectrum analyzers) use coaxial cables with standardized connectors (SMA, 2.92 mm, 2.4 mm, 1.85 mm, 1.0 mm). The coax-to-CPW transition bridges this interface, converting the rotationally symmetric TEM mode of coax into the planar quasi-TEM mode of CPW while maintaining impedance continuity.

The electromagnetic challenge is managing the mode conversion in a region where the field distribution changes dramatically. In coax, the electric field is radial between center and outer conductors, uniformly distributed around the circumference. In CPW, the electric field spans the gaps between the center strip and ground planes, concentrated at the strip edges. The transition region must smoothly transform one field distribution into the other without exciting higher-order modes (which cause resonances and radiation) or creating abrupt impedance discontinuities (which cause reflections). The design space includes the connector body geometry, the PCB pad layout, the ground via placement, and any matching structures (stubs, tapers, or stepped impedance sections).

Coax-to-CPW Transition Design

CPW Impedance:
Z0 = (30π/√εeff) × K(k')/K(k)

Where:
k = W/(W + 2G)   ;   k' = √(1-k²)

Via Fence Spacing (GCPW):
p < λeff/4 = c/(4fmax√εr)

W = center strip width, G = gap to ground, K = complete elliptic integral of the first kind. For 50 Ω on 10 mil alumina (εr=9.6): W = 100 μm, G = 60 μm. Via fence at 60 GHz on εr=3.5: p < 670 μm.

Coax-to-CPW Transition Types

TypeOrientationBandwidthReturn LossApplication
End-launch (SMA)HorizontalDC to 18 GHz< -20 dBPCB test fixtures
End-launch (2.92 mm)HorizontalDC to 40 GHz< -20 dBModule testing
End-launch (1.85 mm)HorizontalDC to 67 GHz< -18 dBV-band modules
End-launch (1.0 mm)HorizontalDC to 110 GHz< -15 dBW-band, mmWave
GSG probeVertical (angled)DC to 145 GHz< -15 dBOn-wafer MMIC test
Common Questions

Frequently Asked Questions

How is impedance matched across the transition?

Both coax and CPW support 50 Ω; the challenge is the transition region's parasitic reactance (inductive from current path change + capacitive from exposed dielectric). Compensation: stepped impedance sections, chamfered ground connections, via fences. EM simulation (HFSS/CST) optimizes geometry for < -20 dB return loss over 3:1+ bandwidth.

What is the CPW vs GCPW difference?

CPW has no back-side ground. GCPW adds back-side ground connected by vias, enabling heat sinking and mechanical mounting but introducing parasitic parallel-plate mode. Via fences (< λ/4 spacing) suppress this mode. For 10 mil substrate at 60 GHz: via spacing < 1.25 mm.

How are transitions used for on-wafer probing?

RF probes convert coax (1.0 mm or 0.8 mm) to GSG tips at 50 to 250 μm pitch. Transition occurs in probe body via precision thin-film line. Contact force: 5 to 20 g/tip. Calibration (SOLT/TRL/mTRL) on ISS de-embeds probe parasitics, achieving ±0.1 dB and ±1° accuracy to 110 GHz.

RF Connectors & Transitions

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