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Nonlinear Microwave Oscillators:   Dynamics and Synchronization Hien Dao (Chemical Physics Program) John C. Rodgers (IREAP) Thomas E. Murphy (ECE & IREAP)
Outline ,[object Object],[object Object],[object Object],[object Object]
Motivation ,[object Object],nonlinearity Example: An optoelectronic chaotic oscillator A. B. Cohen, B. Ravoori, T. E. Murphy, and R. Roy, Phys. Rev. Lett.  101 , 154102 (2008)  H (s)  gain delay filter
[object Object],Motivation ,[object Object],[object Object],[object Object],Phase- locked- loop using VCO could exhibit chaotic signal. Sandia report, March 2004
VCO splitter  d mixer   Bias at operating point H ( s ) low pass filter gain delay Experimental setup
Voltage Controlled Oscillator (VCO) is a device that converts an input analog voltage into a signal whose frequency is linearly proportional to the magnitude of voltage VCO Tuning signal  v (t) RF signal and  with    is named tuning sensitivity (VCO gain) and   0  is bias frequency. Slowly varying phase  0 =2.65 GHz  =175 MHz/v
v VCO  d Mixer Splitter delay Nonlinear function is created using delay-line frequency discriminator  output
VCO Splitter  d Mixer bidirectional coupler combiner
VCO splitter  d mixer   Bias at operating point H ( s ) low pass filter gain delay Experimental setup
L=5   H C=1nF  u =0.1   s/unit; ,[object Object],[object Object],Loop feedback delay    is built in with transmission line design L/N L/N L/N C/2N C/2N C/2N C/2N C/2N C/2N N units
Mathematical model for tuning signal system equation  H (s)  nonlinearity gain delay low pass filter v(t) f cutoff  =3 MHz  s  1.2   s  Varying from 0.5-9.5  5 ns   175 MHz/V  Value Parameters
 =1.6  =2.2  =6.5 Experiment Simulation
Phase portrait of system plotting phase of envelope signal versus its derivative can tell us about dynamics of system   =1.6  =2.2  =6.5
Simulation Experiment Bifurcation diagram of system Vtune [V] Vtune [V] -2 -1 2 1 0 -2 -1 2 1 0 1 2 3 4 6 5 7 
Vtune [V] Vtune [V] increasing   decreasing   Historesis  effect 1 2 3 4 6 5 7  -2 -1 2 1 0 -2 -1 2 1 0
Vtune [V] Maximum Lyapunov exponent -2 -1 2 1 0 1 2 3 4 6 5 7  -0.2 0.4 0.2 -0.1 0.1 0 0.3 0.5
Synchronization of coupled microwave oscillators
Chaotic synchronization had been achieved by coupling two optoelectronic systems. How to couple two microwave systems and what kind of synchronization we should observe? x 1 (t): x 1 (t) – x 2 (t): x 2 (t):
Two systems are coupled bi-directionally in microwave band,  VCO Splitter  d Mixer   Bias VCO Splitter  d Mixer   Bias H(s) H(s)    is coupling strength v 1  (t) v 2  (t)  Behavior depends on whether the VCO difference frequency exceeds the filter bandwidth
[object Object],[object Object],VCO Tuning signal RF signal RF signal
RF signal collected from scope Analytic signal Hilbert transform Analytic signal Where  is Hilbert transform of  Using Hilbert transform to estimate phase RF signal Constant   amplitude Phase varies around a bias value    0
VCO Tuning signal RF signal  =1.2 and   =0.1
t (  s) 0 100 50 200 250 150 0 100 200
VCO Tuning signal RF signal  =2.1 and   =0.1
0 3000 6000 0 100 50 200 250 150 t (  s)
Conclusion ,[object Object],[object Object],[object Object],[object Object]

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Muri

  • 1. Nonlinear Microwave Oscillators: Dynamics and Synchronization Hien Dao (Chemical Physics Program) John C. Rodgers (IREAP) Thomas E. Murphy (ECE & IREAP)
  • 2.
  • 3.
  • 4.
  • 5. VCO splitter  d mixer   Bias at operating point H ( s ) low pass filter gain delay Experimental setup
  • 6. Voltage Controlled Oscillator (VCO) is a device that converts an input analog voltage into a signal whose frequency is linearly proportional to the magnitude of voltage VCO Tuning signal v (t) RF signal and with  is named tuning sensitivity (VCO gain) and  0 is bias frequency. Slowly varying phase  0 =2.65 GHz  =175 MHz/v
  • 7. v VCO  d Mixer Splitter delay Nonlinear function is created using delay-line frequency discriminator output
  • 8. VCO Splitter  d Mixer bidirectional coupler combiner
  • 9. VCO splitter  d mixer   Bias at operating point H ( s ) low pass filter gain delay Experimental setup
  • 10.
  • 11. Mathematical model for tuning signal system equation  H (s)  nonlinearity gain delay low pass filter v(t) f cutoff =3 MHz  s  1.2  s  Varying from 0.5-9.5  5 ns   175 MHz/V  Value Parameters
  • 12.  =1.6  =2.2  =6.5 Experiment Simulation
  • 13. Phase portrait of system plotting phase of envelope signal versus its derivative can tell us about dynamics of system  =1.6  =2.2  =6.5
  • 14. Simulation Experiment Bifurcation diagram of system Vtune [V] Vtune [V] -2 -1 2 1 0 -2 -1 2 1 0 1 2 3 4 6 5 7 
  • 15. Vtune [V] Vtune [V] increasing  decreasing  Historesis effect 1 2 3 4 6 5 7  -2 -1 2 1 0 -2 -1 2 1 0
  • 16. Vtune [V] Maximum Lyapunov exponent -2 -1 2 1 0 1 2 3 4 6 5 7  -0.2 0.4 0.2 -0.1 0.1 0 0.3 0.5
  • 17. Synchronization of coupled microwave oscillators
  • 18. Chaotic synchronization had been achieved by coupling two optoelectronic systems. How to couple two microwave systems and what kind of synchronization we should observe? x 1 (t): x 1 (t) – x 2 (t): x 2 (t):
  • 19. Two systems are coupled bi-directionally in microwave band, VCO Splitter  d Mixer   Bias VCO Splitter  d Mixer   Bias H(s) H(s)  is coupling strength v 1 (t) v 2 (t)  Behavior depends on whether the VCO difference frequency exceeds the filter bandwidth
  • 20.
  • 21. RF signal collected from scope Analytic signal Hilbert transform Analytic signal Where is Hilbert transform of Using Hilbert transform to estimate phase RF signal Constant amplitude Phase varies around a bias value  0
  • 22. VCO Tuning signal RF signal  =1.2 and  =0.1
  • 23. t (  s) 0 100 50 200 250 150 0 100 200
  • 24. VCO Tuning signal RF signal  =2.1 and  =0.1
  • 25. 0 3000 6000 0 100 50 200 250 150 t (  s)
  • 26.