Presented at RFIT-2022
Session info : Advanced Circuit and System Design
Date : Aug 30, 2022
Place : Busan, Korea
Cite with the shortened URL if you like
https://lnkd.in/gBhJmSRa
[ URL/DOI of the paper/preprint ]
DOI) 10.1109/RFIT54256.2022.9882474
URL) https://ieeexplore.ieee.org/document/9882474
https://www.researchgate.net/publication/363510202_A_Refined_Skew_Matrix_Model_of_the_CIM3_in_the_Up-Mixer_Extending_the_Duality_of_IQ_Imbalance
Following(corrective) work of https://lnkd.in/gwJhqgb8
Strategies for Unlocking Knowledge Management in Microsoft 365 in the Copilot...
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A Refined Skew Matrix Model of the CIM3 in the Up-Mixer Extending the Duality of I/Q Imbalance (RFIT-2022)
1. GCT Semiconductor, Inc.
RFIT 2022
A Refined Skew Matrix Model of the CIM3 in the Up-Mixer
Extending the Duality of I/Q Imbalance
Ealwan Lee
GCT Semiconductor, Inc.
Aug 30, 2022
Session T3B.4 (2:30 pm ~ 2: 50 pm)
Advanced Circuit and System Designs
2. 1/16
GCT Semiconductor, Inc.
RFIT 2022
Table of Contents
β Introduction
β Meaning of the study on the CIM3-only DPD model.
β Review of the previous work of joint I/Q-imbalance and CIM3 model.
β Duality between the components of I/Q gain/phase mismatch
β Review of the duality in I/Q imbalance model.
β Extension and application to CIM3 model with conjugate signal representation
β Correction/Enhancement to the CIM3 models introduced in 5 years ago
β Identification of missing terms in prior works.
β Evaluation of the improvement after the correction.
β LMS adaptation revisited and its simplification
β Frequency domain => Time domain : Parsevalβs theorem
β Link to other works already established for I/Q imbalance : circularity
β Conclusion
β Refined version of joint CIM3 + I/Q imbalance model
[ pp. 2 ~ 5 ]
[ pp. 6 ~ 8 ]
[ pp. 9 ~ 10 ]
[ pp. 11 ~ 15 ]
[ p. 16 ]
3. 2/16
GCT Semiconductor, Inc.
RFIT 2022
Introduction
β What is CIM3 and Why it became nuisance ?
β CIM3 = 3rd order Counter Inter-Modulation
β Up-conversion mixer
β One of the key factor in the SAW-less Tx implementation of 4G/5G/6G RF IC solution
ο Violating the out-of-band emission spec from UL band to the DL band of specialty network.
β Lowering the CIM3 inside the channel & band helps still in many ways.
β Straightforward and Simple Approach
β Lowering the signal level solves CIM3 problem at least but in trade-off with other metrics.
β Reduction of signal by x1 dB => reduction of CIM3 by x3 dB.
β A study of simple but plausible/consistent mathematical model of CIM3 helps
β Characterizing, pushing to the limit of the analog circuitry in a systematic way.
β Can be combined with other CIM3 reduction method.
DL of other bands
affected without TX SAW filter
UL in operation
fc fc+fm
fc-3fm
No effects to
DL of other bands
UL in operation
fc
IMD3
CIM3
* UL+DL in XDD or Full-duplex
CIM3
4. 3/16
GCT Semiconductor, Inc.
RFIT 2022
Review of Prior Works in RFIT2017
β Mathematical models of CIM3 + DPD up-mixer
β Same model in cascade with complementary(typically negative) parameters.
β 1st order cancellation as in typical I/Q imbalance compensator
β Joint compensation with a single skew matrix
+
X
X
X
X +
zi
zq
yi
yq
π + πΉπ + ππ β ππ
π β πΉπ β ππ β ππ
πΉπ + ππ β ππ
+
X
X
X
X +
xi
xq
zi
zq
π β πΉπ β ππ β ππ
π + πΉπ + ππ β ππ
βπΉπ β ππ β ππ
CIM3 distortion
model (analog circuit)
Digital Pre-Distortion
model (digital processing)
ππ = ππ β ππ
ππ = ππ β ππ
D/A
D/A
w/o DPD
w/o DPD
ππ + π β ππ
ππ + π β ππ
Image @ -fm
CIM3 @ -3fm
counter 3rd order
intermodulation
5. 4/16
GCT Semiconductor, Inc.
RFIT 2022
CIM3 in spectrum and phasor diagram
β Despite perfect synchronization in digital domain,
β Delay in feed-back path(οt), non-coherency between RF and BB(οο), Tx and Rx(οο±) matters.
β No change in the spectrum of the up-mixer output.
β Any distortion/compensation model should explain the effect of οt.
reference vector (π¦+1)
= y+1,i + jοy+1,q @ +f
CIM3 vector
@ -3f
conjugate of
reference vector (ΰ΄€
π¦+1)
= y+1,i - jοy+1,q
Re
Im
Joint
I/Q imb + CIM3
compensator
tone
generator
accumulator de-rotator
+f
-3f, -f, +f
duration = N/f
Synchronized
with 1/f
Up mixer
{ο€g, ο€p ;Ο΅g, Ο΅p}
RF-PLL
Report
* y-3 = CIM3
* y-1 = Image
* y+1 = Desired
eg, ep
dg, dp
Rx
I/Q imb
compensator
D/A
οt
Variation of the delay
in feed-back path
+ππ πβπ
βππ πβπ
βππ πβπ
+f
-f
-3f
A/D
οο¦
οο±
6. 5/16
GCT Semiconductor, Inc.
RFIT 2022
Just Scribbling to Figure Out Something Else
β Only combination of two terms tried to make (-3 * f) component in previous work.
β 4 terms were able to be combined becoming insensitive to the phase shift.
β cos 2ππ‘ term missed and can complement the missing part of sin 2ππ‘ .
β But, should the number of parameters be increased from 2 to 4, then ?
π¦π = π₯π + 0π₯π
3
+ π2π₯π
2
π₯π
1
+ π1π₯π
1
π₯π
2
+ 0π₯π
3
π¦π = π₯π + 0π₯π
3
β π2π₯π
2
π₯π
1
+ π1π₯π
1
π₯π
2
+ 0π₯π
3
π¦π = π₯π + ΰ·
π=0
3
πππ₯π
π
π₯π
3βπ
π¦π = π₯π + ΰ·
π=0
3
ππ π₯π
3βπ
π₯π
π
Enforcing 0
oversight in prior work
π₯π + 1π β π₯π = cos ππ‘ + 1π β sin ππ‘
π₯π
2
π₯π
1
β 1π β π₯π
1
π₯π
2
= 1
2
β sin 2ππ‘ β cos ππ‘ β 1π β sin ππ‘
Enforcing 0
oversight in prior work
π₯π
1
π₯π
2
+ 1π β π₯π
2
π₯π
1
= 1
2
π β sin 2ππ‘ β cos ππ‘ β 1π β sin ππ‘
π₯π
3
β π₯π
1
π₯π
2
β 1π β π₯π
2
π₯π
1
+ 1π β π₯π
3
= cos 2ππ‘ β cos ππ‘ β 1π β sin ππ‘
βπ₯π
3
+ 1π β π₯π
1
π₯π
2
+ π₯π
2
π₯π
1
β 1π β π₯π
3
= π β cos 2ππ‘ β cos ππ‘ β 1π β sin ππ‘
π3 ?
π0 ?
fIF
-3 fIF
7. 6/16
GCT Semiconductor, Inc.
RFIT 2022
Duality of I/Q imbalance model in the (down)-mixer
β gain mismatch(Ο΅g) and phase mismatch(Ο΅p) are exchangeable under signal rotation.
β explaining the consistency of image signal and IRR in spectrum against co-ordinate rotation.
Another proof by (2nd)
geometric interpretation
Down-mixer [2018]
1. L1-norm based
LMS calibration
2. Completeness of
symmetric skew matrix
Applied to up-mixer
in this paper.
(Ο΅g/2, Ο΅g/2) => (ο€g,ο€g)
Proof by (1st)
simple arithmetic
10. 9/16
GCT Semiconductor, Inc.
RFIT 2022
Donβt be confused
with (Ο΅g, Ο΅g)
Identification of the component missed in our prior work
β Comparison with prior works in matrix representation
β degree of freedom for CIM3 is kept to 2 in spite of added term : (Ο΅g, Ο΅g)
π¦π
π¦π
=
1 0
0 1
+ πΏπ + ππ β ππ + ππ β ππ β
+1 0
0 β1
+ πΏπ + ππ β ππ β ππ β ππ β
0 +1
+1 0
β
π₯π
π₯π
ππ = 2 β π₯π β π₯π
ππ = π₯π
2
β π₯π
2
π = π₯π β π₯π
π¦π
π¦π
=
1 0
0 1
+
+πΏπ πΏπ
πΏπ βπΏπ
+ ππ β
ππ +ππ
+ππ βππ
β
π₯π
π₯π
+ ππ β
ππ βππ
βππ βππ
β
π₯π
π₯π
Terms missed in previous work
and complemented in this work
Terms simplified and merged
in previous work with matrix arithmetic.
Skew matrix for I/Q imbalance
ΰ·€
ππ = 2 β ΰ·€
π₯π β ΰ·€
π₯π = π₯π
2
β π₯π
2
ΰ·€
ππ = ΰ·€
π₯π
2
β ΰ·€
π₯π
2
= 2 β π₯π β π₯π
re-scaled and re-named
for generalization
Rotation by ο°/4
11. 10/16
GCT Semiconductor, Inc.
RFIT 2022
Comparison of two models side-by-side
β Re-plot of previous works by flipping the direction of before/after the DPD for comparison.
β Reflection of the sequential estimation of ο€ and ο
β Scope of the problem has extended.
β All the harmonics at -f, +3f, +5f not just -3f should be suppressed at its best of the given model.
β Cascade of a single skew matrix has its limitation leaving artifact on +3f, +5f.
Before DPD
After DPD
Image @ -9 MHz
-26 => -56 (dBc)
CIM3 @ -27 MHz
-38 => -64 (dBc)
Image @ -9 MHz
-26 => -71 (dBc)
CIM3 @ -27 MHz
-38 => -72 (dBc)
Prior model in RFIT2017 @ Seoul
- Single run applied from for ο€ ,then ο.
Refined model in RFIT2022 @ Busan
- Optimal ο€, ο obtained with iterative joint LMS adaptation.
12. 11/16
GCT Semiconductor, Inc.
RFIT 2022
Derivation of LMS Adaptation Formulae
β Frequency domain
β Obtain the Fourier-transform at each desired frequency, π +π , π(β3π)
β Process only π +π to obtain π +π 3
β Derived measure is insensitive to the rotation caused by the delay of the feed-back path.
+fm +3fm
-3fm -fm 0
π(βπππ) β πβπππ ππβπ π(+π) β π+πππ ππβπ
+fm +3fm
-3fm -fm 0
π(+π)π
β π+πππ ππβπ
π(βπππ) β πβπππ πππ
βπ β Ξ€
π βπππ π +ππ
π
β
π(βπππ) β π(+ππ)π
π +ππ
π β π(+ππ)π
π = π + πΉ β ΰ΄₯
π + π β ΰ΄₯
ππ
Norm of the signal
that can be absorbed into update factor.
13. 12/16
GCT Semiconductor, Inc.
RFIT 2022
Derivation of LMS Adaptation Formulae (contβd)
β Frequency domain
β How to align the desired and distorted component with the same offset from carrier(DC) ?
β Squaring in time-domain => Convolution in freq-domain.
β Previous method did not pre-processed time-domain signal before DFT.
β This measure is also insensitive to the rotation caused by the delay of the feed-back path.
β Frequency domain => Time domain : next page
π[π]π
+fm +2fm
-3fm -fm 0
π(+ππ)π
β π+πππ πππ
-2fm
π(βπππ)βπ(+ππ)βπβπππ πππ
-6fm
+fm +2fm
-3fm -fm 0
π(βπππ) β πβπππ πππ
π(+ππ)βπ+πππ πππ
-2fm
π[π]
βπ β π βπππ β π ππ
π
β π(βπππ) β π(ππ) β π(ππ)π
+π β ππ
βπ β ππ
+π β ππ
βπ β ππ
17. 16/16
GCT Semiconductor, Inc.
RFIT 2022
Conclusion
β A refined model for joint CIM3 and I/Q imbalance model has been proposed.
β Duality similar to that of I/Q imbalance has been also applied to CIM3.
β Missing components identified and complemented.
β Framework for the proposed model unified to get the help from
β Conjugate signal representation
β Circularity of the signal.
β Derivation of the joint LMS adaptation formulae.
β Optimization => LMS
β Frequency domain => Time domain
β Block-wise => Sample-wise
β URL of the slide/presentation
β [4] Duality of the I/Q imbalance : https://lnkd.in/gy24S4kF
β [5] CIM3 in RFIT2017 : https://lnkd.in/gwJhqgb8