Projet PEA ICARE sImulation Comportementale d’Antenne Réseau … · 2019. 3. 30. · Keysight...
Transcript of Projet PEA ICARE sImulation Comportementale d’Antenne Réseau … · 2019. 3. 30. · Keysight...
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1This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Systematic Large Signal Stability Analysis
technique for multi-transistor RF Circuit
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2This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
0 200 400 600 800 1000 1200 1400 1600-100
-80
-60
-40
-20
0
Frequency (MHz)
Ou
tpu
t p
ow
er (
dB
m)
0 200 400 600 800 1000 1200 1400 1600-100
-80
-60
-40
-20
0
Frequency (MHz)
Ou
tpu
t p
ow
er
(dB
m)
0 200 400 600 800 1000 1200 1400 1600-100
-80
-60
-40
-20
0
Frequency (MHz)
Ou
tpu
t p
ow
er
(dB
m)0 oscillation
2f
low frequency
oscillation
Oscillations in RF Power Amplifiers
- low-frequency oscillations, often linked to bias networks, can be detected using small-signal simulations
RF Power Amplifiers are prone to (unwanted!) oscillations
- parametric oscillations function of the input drive signal, have to be detected in large signal
Typical ones:
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3This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Linear analysis “small signal”
– K factor
– Normalized Determinant
Function (NDF)
– Stability envelope
Non-linear analysis “large
signal”
– Nyquist criterion
– NDF
– Bolcato, Di Paolo & Leuzzi,
Mochizuki, …
0 200 400 600 800 1000 1200 1400 1600-100
-80
-60
-40
-20
0
Frequency (MHz)
Ou
tpu
t p
ow
er (
dB
m)
0 200 400 600 800 1000 1200 1400 1600-100
-80
-60
-40
-20
0
Frequency (MHz)
Ou
tpu
t p
ow
er
(dB
m)
0 200 400 600 800 1000 1200 1400 1600-100
-80
-60
-40
-20
0
Frequency (MHz)
Ou
tpu
t p
ow
er
(dB
m)0 oscillation
2f
low frequency
oscillation
Existing Methods
Either not complete or too complex !!!
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4This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Existing Methods
Linear analysisWidely used: K factor (also µ and µ’ now)
- K>1 & |∆| <1: unconditional stability of two port network
- K<1: conditional stability → stability circles
Unconditional
stability
Conditional
stability
Unconditional
instability
Only indicates that a stable circuit will continue to be stable when loading it with passive external loads at the input or output
Do not guarantee the internal stability of the circuit !
Limitations:
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5This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Existing Methods
INOUT Gate Drain
So
urc
e
Multi-stage power amplifier Multi-fingers transistor
Linear analysisPotentially instable architectures for which K factor is
not enough (-> see Application Note)
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6This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
-0.3 -0.2 -0.1 0.0 0.1 0.2 0.3-6
-4
-2
0
2
4
6
Re (GHz)
Im (
GH
z)
Pole-Zero Identification
Node ‘n’
in s( i ,f )outv
RG
f0,
Pin
RL
10
30
-10
50
dB
(Zsond)
2.0E9 4.0E9 6.0E9 8.0E9 1.0E100.0 1.2E10
-100
0
100
-200
200
frequency
phase(Z
sond)
Freq (GHz)
|H
| (
dB
)
H (
º)
poles
zeros
Pole-zero plot
( )H j
1
1
( )
( )
( )
n
i
i
p
j
j
s z
H s
s
=
=
−
=
−
Frequency domainidentification
techniques
STAN Tool
CAD Tool
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7This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Suitable for both linear and non-linear stability
analysis
Very easy to use
Very easy to analyze results
Notion of “stability margin”
Oscillation mode knowledge -> Help to find the
suitable stabilization strategy
Parametric Analysis implemented
Monte-Carlo Analysis
Key Elements
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8This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Combining STAN with CAD tools
Keysight ADS
Design Kit of Templates is available
- AC simulation for small-signal stability analysis
- HB simulation (mixer-mode) for large-signal stability analysis
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9This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Combining STAN with CAD tools
Keysight ADS
Step 1:Connect the probe from the template to a node of your circuit
Step 3:Run simulation
Step 2:Set parameters for the simulation
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10This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Combining STAN with CAD tools
Keysight ADS
Step 4:- results are displayed in ADS- Export the results in a text file
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11This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Combining STAN with CAD tools
Keysight ADS
Step 5:- Open the file in STAN tool and launch the identification
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12This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Combining STAN with CAD tools
Keysight ADS
Step 6:- Check
the results
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13This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Wizard
Stability Probe
Step 1:Add stability probes to your schematic
Step 2:Invoke STAN wizard
NI AWR Microwave Office
Combining STAN with CAD tools
Integrated STAN Wizard in MWO v12
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14This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
NI AWR Microwave Office
Combining STAN with CAD tools
Schematic selection
Node(s)
selection
STAN settings
Frequency range
Drive conditions (small
signal / large signal)
Step 3:
Within STAN wizard- Set the parameters for the stability analysis- Launch the analysis
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15This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
NI AWR Microwave Office
Combining STAN with CAD tools
Oscillation detected
at 59,3MHz
Step 4:- Aplac simulation is run – results are
automatically sent to STAN. STAN processes the data and sends results back to MWO
- Check the pole/ zero map results
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16This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Selecting the Node
Where to connect the probe for STAN analysis ?
SISO transfer function → exact
pole/zero cancellations are
possible
Pole/zero cancellations are
associated with the lack of
controllability and/ or observability
in the system
real
imag
d
Pole-zero quasi-cancellation
???
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17This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Physical quasi-cancellations
in s( i ,f )outv
this node has very low sensitivity to
that dynamics (low degree of
observability and/or controllability)
When part of the circuit dynamics is electrically isolated from the node selected for the
analysis, poles representing this dynamics appear quasi-cancelled by zeroes and the effect
of this dynamics on the transfer function is very slight
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18This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
In multistage Circuits
Example of a three-stage PA exhibiting an
oscillation
-0.3 -0.2 -0.1 0.0 0.1 0.2 0.3-6
-4
-2
0
2
4
6
Re (GHz)
Im (
GH
z)
1_biasV _ 2biasV _3biasV
Connecting the probe to a node of the
3rd stage, no instability is detected (we
are electrically isolated from where the
actual oscillation takes place).
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19This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
In multistage Circuits
Connecting the probe to a node
of the 2nd stage → physical
quasi-cancellation (we still have
low sensitivity from the
observation port)
-0.3 -0.2 -0.1 0.0 0.1 0.2 0.3-6
-4
-2
0
2
4
6
Re (GHz)
Im (
GH
z)
Example of a three-stage PA exhibiting an
oscillation
1_biasV _ 2biasV _3biasV
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20This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
In multistage Circuits
Example of a three-stage PA exhibiting an
oscillation1_biasV _ 2biasV _3biasV
Connecting the probe to a node of the 1st
stage → The oscillation is clearly detected,
unstable poles are not quasi-cancelled with
nearby zeros (high sensitivity). We can
conclude that the origin of the oscillation is
located in the 1st stage-0.3 -0.2 -0.1 0.0 0.1 0.2 0.3
-6
-4
-2
0
2
4
6
Re (GHz)
Im (
GH
z)
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21This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Odd mode oscillation in combined amplifiers
Oscillation at f0/2 is very common in amplifiers with parallel
power combining structures
RG
f0,Pin
RL
RL
Q1
Q2
RG
f0,Pin
RL
RL
Q1
Q2
in s( i ,f )
outv
in s( i ,f )
outv
2e9
2e9
2e9
2e9
Odd mode
oscillation is not
detected at the
combining
node. Exact
pole-zero
cancellation
Odd mode
oscillation is
clearly detected
at the gate of
the transistors
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22This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Odd mode oscillation in combined amplifiers
Po
we
r s
pli
tte
r
Po
we
r c
om
bin
er
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
1Q
2Q
3Q
4Q
G
A
B
C
D
E
F
1st step: analysis in nodes A, B and D
A B DOscillation
type
Preferred
strategy
x x x Even mode
- x -Odd mode in
1st stage
- - xOdd mode in
2nd stageSee next slide
- - - No oscillation -
Stabilization networks can be optimized using parametric analysis -> find the best trade-off between stability and RF performances
B,C
or/ and D, E, F, G B
C
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23This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Po
wer
sp
litt
er
Po
wer
co
mb
iner
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
STAN Tool
Odd mode oscillation in combined amplifiers
Test of the 4 branches with 4 probes, changing the phase
Odd mode oscillation
[ + - - +] or [ + - + - ]
→ Q1 oscillates out of
phase with Q2, same for
Q3 and Q4
Po
we
r s
pli
tte
r
Po
we
r c
om
bin
er
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
Q1
Q2
Q3
Q4
Po
we
r s
pli
tte
r
Po
we
r c
om
bin
er
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
Q1
Q2
Q3
Q4
Po
we
r s
pli
tte
r
Po
we
r c
om
bin
er
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
Q1
Q2
Q3
Q4
Po
we
r s
pli
tte
r
Po
we
r c
om
bin
er
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
Q1
Q2
Q3
Q4
Odd mode oscillation
[ + + - - ]
→ Q1 and Q2 oscillates out
of phase with Q3 and Q4
Po
wer
sp
litt
er
Po
we
r co
mb
ine
r
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
Q1
Q2
Q3
Q4
Po
we
r s
pli
tte
r
Po
we
r c
om
bin
er
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
Q1
Q2
Q3
Q4
Po
wer
sp
litt
er
Po
wer
co
mb
iner
Po
wer
sp
litt
er
Po
wer
sp
litt
er
RL
RG
f0 Pin
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24This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
X-band class-E PA
X-band MMIC class-E PA – 0,15µm GaN process
When tested in the lab with RF signal, increasing the input power makesthe middle output interbranch resistance to blow up
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25This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
X-band class-E PA
DC stability analysis
Two STAN probes connectedto the gate of transistor, onefor each stage
Frequency range from 0.1 to30 GHz
1st stage
2nd stage
Perform identification in several sub-bandwidths
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26This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
X-band class-E PA
DC stability analysis
Perform parametric analyses (sweeping parameters such as gatevoltage) and focus around the frequencies for which there is aresonance
Evolution of the poles at 1,5 GHz while sweeping the gate biasvoltage
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27This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
X-band class-E PA
Large-signal stability analysis
STAN probe connected to the gate of a transistor of the first stage, fin=10GHz and
the input power is swept from 10 to 20dBm, the frequency of the small currentprobe is swept from 0.1 to 10.1GHz (with avoiding exact overlap with fin=10GHz) →
no oscillation detected
Same analysis with STAN probe connected to the gate of a transistor of the secondstage → clear instability is detected around fin=10GHz
Identification results for Fin=10GHz andPin=18dBm
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28This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
X-band class-E PA
Large-signal stability analysis
Oscillation appears for certain power levels, between ~14 and 17dBm,
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29This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
X-band class-E PA
Detection of the oscillation mode
Test of the 4 branches with 4 probes, changing the phaseEven mode (++++): unstable poles are quasi-cancelled, there is not an even mode
Odd mode (+-+-): poles are clear and isolated, observability is high, instability can be [+-+-]Odd mode (++--): again poles are clear and isolated. Instability can also be [++--]
Odd mode (+--+): poles are quasi-cancelled, poor observability. Instability cannot be [+--+]
Instable dynamics involves an odd mode in which transistors 2 and 3 of the second stage are out-of-phase
Arriving at Pin=14,7dBm, the signal switches from an even mode to an odd-mode. We suddenly have signal at fin in the transistor 2 that is 180-out of phase with the signal in transistor 3. This means lot of current flowing through the middle stabilization resistor at fin
→ Coherent with what was observed in the lab!
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30This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
X-band class-E PA
Circuit stabilization
The instability involving transistors 2 and 3 of the second stage, a parallelresistance between the gates of these two transistors is added
Value of this inter-branchresistance is swept in order to findone which can guarantee thestability of the PA for all the inputrange
A value between 25 and 30Ohms seems to be a goodchoice
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31This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
X-band class-E PA
Circuit stabilization
The instability involving transistors 2 and 3 of the second stage, a parallelresistance between the gates of these two transistors is added
Evolution of the polesaround 10GHz versus Pin
with inter-branchstabilization resistance of30 Ohms
2nd run gave stable PA → Now a commercial product
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32This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Performances Optimization
Example: Ku-Band MMIC PA for active space antenna
Stable original circuit
RF in RF out
RC stabilization
networks
Inter-branch
stabilization
resistances
Natanael Ayllón Rozas
“Développement des méthodes
de stabilisation pour la
conception des circuits
hyperfréquences : Application à
l’optimisation d’un amplificateur
de puissance spatial.”, PhD Thesis,
February 2011.
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33This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Performances Optimization
Example: Ku-Band MMIC PA for active space antenna
All stabilization networks removed
Parametric frequency
division /2 instability
RF in RF out
resistances
maintained for
topological reasons
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34This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Performances Optimization
Example: Ku-Band MMIC PA for active space antenna
Optimized version
No oscillation detected,
especially around F0/2
RF in RF out
resistances
maintained for
topological reasons
Stabilization
resistances
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35This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
STAN Tool
Performances Optimization
Example: Ku-Band MMIC PA for active space antennaResults comparison
OptimizedOriginal
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36This document may not be reproduced, modified, adapted, published, translated, in any way, in whole or in part, or disclosed to a third party
without the prior written consent of AMCAD engineering - © Amcad 2018 .
Thank you
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