chalmers university of technology
TRANSCRIPT
gan-on-Silicon Efficient mm-wave euRopean systEm iNtegration plAtform
The SERENA project has received funding from the European Union’s Horizon 2020 research
and innovation programme under grant agreement No 779305.
Christian Fager
Chalmers University of Technology
• Chalmers (present and past) T. Eriksson, K. Buisman, K. Rasilainen,
K. Hausmair, P. Taghikhani, E. Baptista
• Ericsson U. Gustavsson, P. Landin, K. Andersson
• OMMIC M. Marilier, R. Leblanc, A. Gasmi, M. ElKaamouch
• Fraunhofer IZM I. Ndip, U. Maaß
17 January, 2020 2
Dr. U. Gustavsson Dr. P. Landin
Prof. T. Eriksson Dr. K. Hausmair Dr. K. Buisman E. BaptistaP. Taghikhani Dr. K. Rasilainen
Dr. K. Andersson
Multi-physics simulation of mm-wave systems
• Active antenna arrays
• High integration needed to fit within l/2
3
Chip embedding
(IZM/SERENA)
Millimeter waves
Data
Heat
Energy
Vertical stacking IBM / Ericsson
17 January, 2020 Multi-physics simulation of mm-wave systems
• Multi-physical effects
Electrical
Thermal
Mechanical
…
• Efficient simulations and modeling are crucial
Before: Optimization, reliability, margins, time to market
After: Troubleshooting, performance optimization, reverse engineering
17 January, 2020 4Multi-physics simulation of mm-wave systems
Active antenna arrays
Antenna-circuit interactions
Linearity
5
MIM
O
tran
smitt
er
6
[T. Svensson, Chalmers]
𝐲 = 𝐇𝐱 +𝐰
Transistor Circuit SystemRF Sub-system
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• Traditionally 50W assumed
• Single-input-single-output modeling of RF components
7
PA
RL = 50 W
Vin[n] Vout[n]Vout = fNL(Vin)
SISO model
Vout = f(Vin)
17 January, 2020 Multi-physics simulation of mm-wave systems
• Integrated transmitters
Mismatch and mutual coupling
Non-50W interfaces
• Dual-input models needed:
b2 = f(a1,a2)
8
GL≠50W
17 January, 2020 Multi-physics simulation of mm-wave systems
• “PHD” or “X-parameter®” model
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( ) ( ) ( )
1 2 2
1 2 2
1
1 2 2
22 121 1 22 1
2( 1) 2( 1) 2( 2)2 *
2 1 1 2 1 2 2 1 1 2
1 1 2
P P Pp p p
p p p
p p p
T aS a S a
b a a a a a a a − − −
= = =
= + +
b2 = fNL(a1,a2)a1
b2
a2
MISO PA model
Nonlinear
50W SISO-termsNonlinear mismatch terms
[Verspecht and D. E. Root, “Polyharmonic distortion modeling,” IEEE Microw. Mag., vol. 7, no. 3, pp. 44–57, Jun. 2006.]
• “X-parameters®” with memory
17 January, 2020 10Multi-physics simulation of mm-wave systems
( )
( )
( )
1 11
1 1
21 1
2 1 22
2 1 2
22 1
1 22
2 1 2
22 1
2( 1)
2 1, 1 1 1 1 1
0 1
2( 1)
1, 2, 2 1 1 2 2
0 0 1
2( 2)2
1, 2, 2 1 1 1 1
0 2
M Pp
m p
m p
S a
M M Pp
m m p
m m p
S a
M Pp
m m p
m m p
T a
b n a n m a n m
a n m a n m
a n m a n m
−
= =
−
= = =
−
= = =
= − − +
− − +
− −
2
*
2 2
0
M
a n m−
b2 = fNL(a1,a2)a1
b2
a2
MISO PA model
[C. Fager et al., "Prediction of Smart Antenna Transmitter Characteristics Using a New Behavioral Modeling Approach," Proc. IMS, 2014]
11
[C. Fager et al., "Prediction of Smart Antenna Transmitter Characteristics Using a New Behavioral Modeling Approach," Proc. IMS, 2014]
Input ref. plane
Outputref. plane
PA DUT
Simulation based
PA DUT
Measurement based
[S. Gustafsson et al., "A Novel Active Load-pull System with Multi-Band Capabilities," ARFTG, 2013]
PA DUT
17 January, 2020 Multi-physics simulation of mm-wave systems
User1 data
User2 data
UserK data
Channel state
b2 = f1(a1,a2,T)a1,1
a1,2
a2,1
b2,1
a2,2
b2,2
a2,N
b2,N
a1,N
b2 = f1(a1,a2,T)
b2 = f1(a1,a2,T)
Pre-codingDPD
...
Signal processing Circuit behavioral modeling
Antenna modeling
User1
User2
UserK
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( ) ( ) ( )
1 2
1 1
*
2 21 1 1 22 1 2 22 1 2
2 2
NT
jj j
ant
a e e e =
= + +
=
a
b S a a S a a T a a
a S b
( ) ( ) ( ) * *
2 21 1 1 22 1 2 22 1 2ant ant= + +b S a a S a S b T a S b
Antenna couplingand mismatch effects
Regular 50Wnonlinear distortion
( ) ( )2,
1
, ,N
tot i i
i
E El Az n b n E El Az=
=
Etot(Elevation, Azimuth)
Far field radiationAntenna circuit interactions
Beam steering
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• PA model extracted from IC CAD
• Antenna parameters from EM CAD
• Each PA perfectly linearized for 50W load (a2 = 0)
• Ideal phased array beam steering. No amplitude tapering
IC design 64 element antenna array
[C. Fager et al., "Analysis of Nonlinear Distortion in Phased Array Transmitters," Proc. INMMiC, 2017]
17 January, 2020 Multi-physics simulation of mm-wave systems 14
• Distortion highly direction dependent. Why?
User EVM vs. scan direction
Azimuth
a1(input)
b2
28 GHz Freq.
|a2|
Freq.
|a1|
Freq.
|b2|
28 GHz
28 GHz
WCDMA2BW = 3.84 MHz
a2
28 GHz GaN MMIC PA BW = 30.72 MHz
WCDMA1BW = 3.84 MHz
a1(input)
b2
28 GHz Freq.
|a2|
Freq.
|a1|
Freq.
|b2|
28 GHz
28 GHz
WCDMA2BW = 3.84 MHz
a2
28 GHz GaN MMIC PA BW = 30.72 MHz
WCDMA1BW = 3.84 MHz
a1(input)
b2
28 GHz Freq.|a
2|
Freq.
|a1|
Freq.
|b2|
28 GHz
28 GHz
WCDMA2BW = 3.84 MHz
a2
28 GHz GaN MMIC PA BW = 30.72 MHz
WCDMA1BW = 3.84 MHz
Elevation
Ele
vati
on
Azimuth
User
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• Significant variation of PA load impedance vs. beam steering
Central elementGL Edge element
GL vs. scan direction
17 January, 2020 Multi-physics simulation of mm-wave systems 16
• Distortion averaging effects happening inside the array
Low distortion direction
Ga
in [d
B]
Output power [dBm] ColumnRow
Gain compression/expansionAM/AM for each of the 64 branches
DG
ain
[dB
]
17 January, 2020 Multi-physics simulation of mm-wave systems 17
• Distortion addition for some directions
• Direction dependent user distortion → Direction dependent DPD needed
High distortion direction
Gain compression/expansionAM/AM for each of the 64 branches
Ga
in [d
B]
Output power [dBm] ColumnRow
DG
ain
[dB
]
17 January, 2020 Multi-physics simulation of mm-wave systems 18
• Nonlinear effects observed also in mm-wave measurements
• 30 GHz beamforming chip
RF input
Digital
phase controlAzimuth
Elevation
AM-AM compression measurement
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• Load-pull based nonlinear modeling
• 4 element patch antenna: EM simulation based modeling
• Reasonable modeling accuracy
RF input
Digital
phase controlAzimuth
Elevation
AM-AM compression modeling
17 January, 2020 Multi-physics simulation of mm-wave systems 20
Nonlinear PA–antenna interactions Far field distortion
4×Skyworks PAs
2 channel RF generator
2 channel RF generator Antenna array
1-path TX 4-path TX
[K. Hausmair et al. “Prediction of Nonlinear Distortion in Wideband Active Antenna Arrays,” IEEE T-MTT, 2017]
17 January, 2020 Multi-physics simulation of mm-wave systems 21
• Framework for efficient simulation of
active antenna systems
• Improved understanding of circuits-
antenna interactions with realistic signals
• New nonlinear effects predicted in phased
array and MIMO systems
17 January, 2020 22Multi-physics simulation of mm-wave systems
Thermal modeling
Power dissipation modeling
mm-wave transmitter example
23
• Heat concentration in active antenna arrays
• Chip level heating effects Thermal coupling Efficient power amplifiers
• System level effects Performance degradation Reliability
2417 January, 2020 Multi-physics simulation of mm-wave systems
• T(t) = TA + Pdiss(t)*zth
• Thermal admittance: Yth = Gth + jwCth
Cth Rth
TA
p(t)
YthT(t)
Pdiss(t)
Pdiss(t) = Pdiss(|a1(t)|,T(t))
Pin Pout
Pdiss
Thermal model RF Model
17 January, 2020 Multi-physics simulation of mm-wave systems 25
• Envelope time-stepped solution for T(t)
Cth Rth
TA
p(t)
YthT(t)
Pdiss(t)
Pdiss(t) = Pdiss(|a1(t)|,T(t))
Pin Pout
Pdiss
Thermal model RF Model
17 January, 2020 Multi-physics simulation of mm-wave systems 26
( ) ( )( )1
1 amb th th diss, th amb2 2n s n s nT f f T −
+ = + + + −T G C P C T
User1 data
User2 data
UserK data
Channel state
27
b2 = f1(a1,a2,T)Pdiss = f2(a1,a2,T)
a1,1
a1,2
a2,1
b2,1
a2,2
b2,2
a2,N
b2,N
a1,N
b2 = f1(a1,a2,T)Pdiss = f2(a1,a2,T)
b2 = f1(a1,a2,T)Pdiss = f2(a1,a2,T)
T1 TN
T = Zth*Pdiss+Tamb
Pre-codingDPD
...
TambHeat
dissipationgeneration dissipation
Thermal coupling
[C. Fager et al. “Analysis of Thermal Effects in Active Antenna Array Transmitters…,” Proc. INMMiC, 2015]
17 January, 2020 Multi-physics simulation of mm-wave systems
( ) ( ) ( )( )1
1 amb th th diss, 1, th amb2 , 2n s n n n s nT f f T −
+ = + + + −T G C P a T C T
1,n n=a Gx
( ) ( ) ( ) * *
2, 21 1, 1, 22 1, 2, 22 1, 2, 1| |, | |, ,n n n n n n ant n n n ant n n−= + + +b S a T a S a T S b T a T S b ρ
( ) ( )2,, ,T
n nE = b E
17 January, 2020 Multi-physics simulation of mm-wave systems 28
17 January, 2020 29Multi-physics simulation of mm-wave systems
17 January, 2020 30Multi-physics simulation of mm-wave systems
Thermal simulation results
• One GaN chip in a simplified package environment
17 January, 2020 31
Chip dissipated
power
Ambient
temperature
Thermal RC constants
Thermal response @ 7W step
Multi-physics simulation of mm-wave systems
• Temperature dependent gain
17 January, 2020 32Multi-physics simulation of mm-wave systems
• Dissipated power vs. temperature
17 January, 2020 33Multi-physics simulation of mm-wave systems
• Mismatch and mutual-
coupling neglected in model
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Simulated S-parameters
• Embedded element patterns
for unity excitations
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Far-field radiation patterns
3617 January, 2020
Thermal modeling RF circuit modeling Antenna modeling
Multi-physics simulation of mm-wave systems
• PA input-/output spectrum
for modulated signals
• PA-to-PA nonlinear
interactions
17 January, 2020 37Multi-physics simulation of mm-wave systems
Power amplifier output
• Thermal transients
• On-off switching, e.g.
between T/R in TDD systems
• Heat spreading in arrays
17 January, 2020 38
Power amplifier temperature
Multi-physics simulation of mm-wave systems
17 January, 2020 39Multi-physics simulation of mm-wave systems
[ = 90°, = 0°] [ = 90°, = -25°]
• Modulated fields in both polarizations
considering both PA, thermal, antenna and beam-
forming settings
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• Thermal effects at circuit- and package
levels
• Framework for electro-thermal
transmitter simulations
• Prediction of joint electrical- and thermal
effects in mm-wave antenna arrays
17 January, 2020 41Multi-physics simulation of mm-wave systems
42
• mm-wave transmitter design is cross-disciplinary Co-design between signals, circuits & antennas
• New nonlinear distortion phenomena Both circuit and array level linearization needed
Low complexity MIMO linearization proposed
• Power dissipation a great challenge Thermal coupling effects
• Understanding linearity and power dissipation effects through accurate multi-physicssimulations is critical for successful 5G system design
17 January, 2020 43Multi-physics simulation of mm-wave systems
C E N T R E
Acknowledgments
Simulation of RF Systems
[1] C. Fager, X. Bland, K. Hausmair, J. Chani Cahuana, and T. Eriksson, "Prediction of Smart Antenna Transmitter Characteristics Using a New Behavioral Modeling Approach,"
Proc. IEEE International Microwave Symposium, Tampa, FL, 2014.
[2] K. Hausmair, S. Gustafsson, C. Sanchez-Perez, P. Landin, U. Gustavsson, T. Eriksson, C. Fager, "Prediction of Nonlinear Distortion in Wideband Active Antenna Arrays,"
IEEE Trans. Microwave Theory Tech., vol. 65, pp. 4550-4563, 2017.
[3] C. Fager, K. Hausmair, K. Buisman, D. Gustafsson, K. Andersson, and E. Sienkiewicz,
"Analysis of Nonlinear Distortion in Phased Array Transmitters," Proc. INMMIC, Graz, Austria, 2017.
[4] C. Fager, T. Eriksson, F. Barradas, K. Hausmair, T. Cunha, and J. C. Pedro, “Linearity and Efficiency in 5G Transmitters: New Techniques for Analyzing Efficiency, Linearity,
and Linearization in a 5G Active Antenna Transmitter Context,” IEEE Microw. Mag., vol. 20, no. 5, pp. 35–49, 2019.
Electro-thermal simulations
[5] C. Fager et al., "Analysis of Thermal Effects in Active Antenna Array Transmitters …," Proc. INMMiC, Oct. 2015]
[6] E. Baptista et al., "Analysis of Thermal Coupling Effects in Integrated MIMO Transmitters," Proc. IMS2017
[7] F. Besombes et al., “Electro-thermal Behavioral Modeling of RF Power Amplifier taking into account Load-pull Effects for Narrow Band Radar Application,” Microw.
Integr. Circuits Conf. (EuMIC), 2011 Eur., no. October, pp. 264–267, 2011.
[8] V. D’Alessandro, M. De Magistris, A. Magnani, N. Rinaldi, and S. Russo, “Dynamic electrothermal macromodeling: An application to signal integrity analysis in highly
integrated electronic systems,” IEEE Trans. Components, Packag. Manuf. Technol., vol. 3, no. 7, pp. 1237–1243, 2013.
[9] SERENA (gan-on-Silicon Efficient mm-wave euRopean system iNtegration platform), https://serena-h2020.eu/
17 January, 2020 Multi-physics simulation of mm-wave systems 4444
“The SERENA project has received funding from the European Union’s Horizon 2020 research and innovation programme
under grant agreement No 779305.”
If you need further information, please contact the coordinator:TECHNIKON Forschungs- und Planungsgesellschaft mbH
Burgplatz 3a, 9500 Villach, AUSTRIATel: +43 4242 233 55 Fax: +43 4242 233 55 77
E-Mail: [email protected]
17 January, 2020 45Multi-physics simulation of mm-wave systems
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