Evaluating SOLT calibration performance at RF...
Transcript of Evaluating SOLT calibration performance at RF...
Evaluating SOLT calibration performance at RF using an LA Techniques VNA
Presentation by Nick Ridler 1
and Nils Nazoa 2
1National Physical Laboratory, UK2LA Techniques Ltd, UK
25th ANAMET meeting, 13 March 2006, NPL
• LA Techniques VNA
• SOLT with a characterised load
• Ripple plots – residual directivity and test port match
• Uncertainty/Best Measurement Capability (BMC)
• Conclusions
Outline
LA19-13-01 - a new type of VNA:
• PC-driven
• Built-in transmission & reflection test set (3 MHz to 3 GHz)
• Small size/portable
• Low cost
• Precision performance from non-precision cal kits (!)
www.www.latechniqueslatechniques.com.com
LA Techniques VNA
LA19-13-01 VNA
SOLT calibration
• Usually assume ‘perfect’ standards:
Short with |Γ| = 1
Open with |Γ| = 1
Load with |Γ| = 0
• However, for non-precision load, |Γ| ≠ 0
• This causes significant post-calibration errors (directivity, test port match, etc)
Solution:
• Measure complex voltage reflection coefficient (VRC) for a candidate cal load using a ‘reference calibration’reference calibration’
• NPL’s ‘national standard’ - Primary IMpedance Measurement System (PIMMS) - provides the ‘reference calibration’reference calibration’
• PIMMS uses TRL with an air line to provide traceability to SI
• Impedance renormalisation is used to give (50 + j0) ohms as the reference impedance (correcting for LF skin depth effects, etc)
SOLT calibration
Characterised SOLT
For each candidate cal load:
• Fit a curve to:measured complex VRC datameasured DC ‘VRC’ (i.e. resistance)
• Use fit to provide cal load complex VRC values during calibration at all required frequencies
(This procedure follows the method used for NPL’s national standard RF System.)
Residual errors - ripple plots
Let’s look at three different cases
Case 1 – SOLT assuming ‘perfect’ cal load
Case 2 – SOLT using ‘characterised’ cal load
Case 3 – SOLT using ‘characterised’ 2.0 VSWR mismatch (as the cal load)
{Use a 150 mm long ripple line – 2.92 mm connectors throughout}
Case 1 – SOLT assuming ‘perfect’ cal load
Residual directivity ripple plot DD ≈≈ 0.015 0.015 ≡≡ --36 dB36 dB
0
0.005
0.01
0.015
0.02
0.025
0.03
0.035
0.04
0.045
0.05
0 500 1000 1500 2000 2500 3000
Freq (MHz)
Lin
ea
r V
RC
Case 1 – SOLT assuming ‘perfect’ cal load
Residual test port match ripple plot MM ≈≈ 0.021 0.021 ≡≡ --34 dB34 dB
0.92
0.93
0.94
0.95
0.96
0.97
0.98
0.99
1
1.01
1.02
0 500 1000 1500 2000 2500 3000
Freq (MHz)
Lin
ea
r V
RC
Case 2 – SOLT using characterised cal load
Residual directivity ripple plot DD ≈≈ 0.002 5 0.002 5 ≡≡ --52 dB52 dB
0
0.001
0.002
0.003
0.004
0.005
0.006
0.007
0.008
0.009
0.01
0 500 1000 1500 2000 2500 3000
Freq (MHz)
Lin
ear
VR
C
Case 2 – SOLT using characterised cal load
Residual test port match ripple plot MM ≈≈ 0.010 0.010 ≡≡ --40 dB40 dB
0.91
0.92
0.93
0.94
0.95
0.96
0.97
0.98
0.99
1
1.01
0 500 1000 1500 2000 2500 3000
Freq (MHz)
Lin
ear
VR
C m
ag
nit
ud
e
Case 3 – SOLT using characterised mismatch
Residual directivity ripple plot DD ≈≈ 0.006 0.006 ≡≡ --44 dB44 dB
0
0.005
0.01
0.015
0.02
0.025
0 500 1000 1500 2000 2500 3000
Freq (MHz)
Lin
ea
r V
RC
ma
gn
itu
de
Case 3 – SOLT using characterised mismatch
Residual test port match – ripple plot MM ≈≈ 0.016 0.016 ≡≡ --36 dB36 dB
0.93
0.94
0.95
0.96
0.97
0.98
0.99
1
1.01
1.02
0 500 1000 1500 2000 2500 3000
Freq (MHz)
Lin
ea
r V
RC
ma
gn
itu
de
Summary performance
(By comparison, some previously published values for SOLT cals (using fixed high precision loads) in 7 mm to 18 GHz are: D = 0.01 and M = 0.03.)
0.0100.010
((--40 dB)40 dB)
0.016
(-36 dB)
0.021
(-34 dB)
Residual
test port match
0.002 50.002 5
((--52 dB)52 dB)
0.006
(-44 dB)
0.015
(-36 dB)
Residual
Directivity
Characterised Characterised load calload cal
Characterised mismatch cal
(VSWR = 2.0)
Perfect load cal
Uncertainty/BMC
Reflection coefficient – linear magnitude uncertainty
Using the EA Guide
approach with:
D = 0.002 5M = 0.010
0.000
0.002
0.004
0.006
0.008
0.010
0.012
0.014
0.016
0.018
0.020
0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
Measured magnitude VRC
VR
C m
ag
nit
ud
e u
nc
ert
ain
ty
Uncertainty/BMC
Reflection coefficient – phase uncertainty
Using:
U(φ) = sin-1(U(|Γ|)/|Γ|)
0
2
4
6
8
10
12
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Measured magnitude VRC
VR
C p
has
e u
nce
rtai
nty
(d
egs)
Summary
• An assumed ‘perfect’ cal load can be the major source of systematic error in a calibrated VNA
• The cal load can be ‘characterised’ in terms of its measured VRC
• The LA Techniques VNA enables characterised cal load data to be stored for use during calibration
• Residual directivity improvement (from -36 dB to -52 dB)
• Residual Test Port Match improvement (from -34 dB to -40 dB)
Bibliography
Nils Nazoa and Nick Ridler, “LA19-13-01 3 GHz VNA calibration and measurement uncertainty”, LA Techniques Ltd, Technical Note Ref LAP02, 2006.
M G Cox, M P Dainton and N M Ridler, “An interpolation scheme for precision reflection coefficient measurements at intermediate frequencies. Part 1: theoretical development”, IMTC'2001 Proceedings of the 18th IEEE Instrumentation and Measurement Technology Conference, Budapest, Hungary, 21-23 May 2001, pp 1720-1725.
N M Ridler, M J Salter and P R Young, “An interpolation scheme for precision reflection coefficient measurements at intermediate frequencies. Part 2: practical implementation”, IMTC'2001 Proceedings of the 18th IEEE Instrumentation and Measurement Technology Conference, Budapest, Hungary, 21-23 May 2001, pp 1731-1735.
“EA guidelines on the evaluation of vector network analysers (VNA)” European co-operation for Accreditation, EA-10/12, May 2000.
N M Ridler and C Graham, “Some typical values for the residual error terms of a calibrated vector automatic network analyser (ANA)”, BEMC 99, 9th International Conference on Electromagnetic Measurement Conference Digest, Brighton Metropole Hotel, UK, 2-4 November 1999, pp 45/1-45/4.