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WP Objectives. Investigate innovative linearization schemes and try their application to high-efficiency PA for wireless applicationspredistortion, feedback, feedforward, backoff Develop circuit-oriented active device models accurate in the IMP predictionsuited to the design and optimization of
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1. WP2.1 Design and optimization of high-linearity, high-efficiency power amplifiers and oscillators
Prof. Giovanni Ghione
P. Bianco, M. Biey, F. Bonani, F. Cappelluti,
P. P. Civalleri, S. Donati, M. Gilli, C. U. Naldi
2. WP Objectives Investigate innovative linearization schemes and try their application to high-efficiency PA for wireless applications
predistortion, feedback, feedforward, backoff …
Develop circuit-oriented active device models
accurate in the IMP prediction
suited to the design and optimization of Pas
based on experimental characterization
Develop software tools for the design of high complexity dynamic systems, such as oscillators
based on HB and/or bifurcation analysis techniques.
5. Ka Band MMIC PAtwo-tone simulation
6. RF Hybrid Prototypecharacterization
7. Device nonlinear modeling
8. WP2.2 Experimental characterization of power devices and circuits
Prof. Umberto Pisani
Andrea Ferrero, Valentin Nicolae, Marco Pirola, Valeria Teppati
9. WP Objectives Development of a new time domain load pull set up
Development of innovative calibration technique for time domain load pull
Experimental characterization of devices in the wireless frequency range under different modulation scheme and loading conditions
Comparison of time domain and frequency domain results
10. Load/Source Pull A well-known technique for PA design
12. Wireless applications Wireless-oriented characterization of devices/systems
Broad-band modulated signals
New measurements requirements: ACPR, spectrum regrowth…
Time domain waveform acquisition
Open Problems
Broad-band load calibration
Time-domain Transition Analyzer calibration
Time-domain power calibration
13. Microwave Lab LOAD PULL SYSTEM
.5-18 GHz Harmonic Load Pull system with two independent loops
S-parameters capability up to 18 GHz
On prober Reflectometer to allow for different power handling (up to 30W at the probe tips)
14. Developed research activity Acquisition of Microwave Network Analyzer Wiltron Skorpion (6 GHz)
CERCOM scheduled for the beginning of March
Scattering, power, IM3, noise measurments
Design of integration with
LP system
wireless modulated signals generator (CDMA, …)
Time-domain investigation capabilities using load pull test set and transition analyzer in progress
15. WP2.3 Radio over fibers: systems and devices Prof. Ivo Montrosset
F. Cappelluti, V. Feies, V. Ferrero,
R. Gaudino, G. Ghione, M. Gioannini,
M. Goano, M. Pirola, P. Poggiolini
16. RF photonic systems Advantages of optical fibers:
broadband, low-loss transmission
immune to EMI
light weight, small size
RF signals optical processing
17. Program objectives System-level analysis:
radio-over-fiber applications
40 GHz microwave photonic links issues
system performance requirements and related devices specifications
Device-level modeling and design:
semiconductor lasers operating in self-pulsation or mode locking regime
EO, EA modulators
photodetectors
18. Balanced EA modulator (B-EAM)for high-linearity, low-noise links
19. Self-Pulsating 3-section DFB lasers The laser structure is a 3 section laser: two DFB sections and a passive phase control section. In proper working conditions the laser can generate free SP with pulsations frequency from 5 to 40 GHz (experimentally demonstrated); but SP up to 100 GHz are theoretically possible.
There are two regimes that give SP:
DSQS regime: DFB1 is polarized above threshold, DFB2, polarized at transparency, works as a passive reflector. In this case the SP frequency is the range 5-20 GHz, because it is limited by the carrier density dynamics.
MB regime: both DFB works above threshold and the SP frequency is given by the “beating” of the two modes above threshold. In this case controlling the detuning between the Bragg wavelengths of the two DFB it is possible to achieve SP in a wide frequency range and the generated SP have also an higher Extinction Ratio (about 14 dB).
In both MB and DSQS regimes the phase control current allow to:
turn on the SP
- obtain a fine tuning of the SP frequency
The laser structure is a 3 section laser: two DFB sections and a passive phase control section. In proper working conditions the laser can generate free SP with pulsations frequency from 5 to 40 GHz (experimentally demonstrated); but SP up to 100 GHz are theoretically possible.
There are two regimes that give SP:
DSQS regime: DFB1 is polarized above threshold, DFB2, polarized at transparency, works as a passive reflector. In this case the SP frequency is the range 5-20 GHz, because it is limited by the carrier density dynamics.
MB regime: both DFB works above threshold and the SP frequency is given by the “beating” of the two modes above threshold. In this case controlling the detuning between the Bragg wavelengths of the two DFB it is possible to achieve SP in a wide frequency range and the generated SP have also an higher Extinction Ratio (about 14 dB).
In both MB and DSQS regimes the phase control current allow to:
turn on the SP
- obtain a fine tuning of the SP frequency
20. Theoretical model, numerical analysis and design: It has been implemented some computer programs for the design and analysis of SP-DFB.
The programs allow to:
- through a static analysis, find the proper working conditions that give SP
once the SP conditions are found (e.g. detuning, currents to inject in each section), simulate the characteristics of the SP signal. The model implemented in this case is based on the TDTW equations.
The figures present an example of simulation results.
We show the optical output power (output frequency 30.68 GHz and ER=14 dB) and the corresponding optical spectrum. In the spectrum the two modes that are responsible for the SP are visible.It has been implemented some computer programs for the design and analysis of SP-DFB.
The programs allow to:
- through a static analysis, find the proper working conditions that give SP
once the SP conditions are found (e.g. detuning, currents to inject in each section), simulate the characteristics of the SP signal. The model implemented in this case is based on the TDTW equations.
The figures present an example of simulation results.
We show the optical output power (output frequency 30.68 GHz and ER=14 dB) and the corresponding optical spectrum. In the spectrum the two modes that are responsible for the SP are visible.
21. EO Modulators modeling and design Integrated circuit CAD model for EOM analysis and design:
extraction of AM and chirp in small- and large-signal conditions from the electrode geometry
flexibility in analysis, optimization and tuning of complex structures, also accounting for package and other parasitics
integrated simulation with driver circuitry
22. High-speed TW-EAMs Circuit-oriented modeling
quasi-static frequency-domain model:
bandwidth
large-signal time-domain model:
RF and optical power saturation effects
frequency chirp
23. BEAM link performance