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partity-time_symmetric_wpt [2025/07/07 14:14] – [Output power and efficiency] klpartity-time_symmetric_wpt [2025/07/07 14:27] (current) – [Efficiency] kl
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 For $k<k_c$, the self resonant frequency, $\omega_{o3}=\omega_0$, remains the only resonance frequency in the system. From equation (4), it can be seen that the negative resistor is dependent on the coupling factor $k$ and does not automatically compensates the resistances in the network. For $k<k_c$, the self resonant frequency, $\omega_{o3}=\omega_0$, remains the only resonance frequency in the system. From equation (4), it can be seen that the negative resistor is dependent on the coupling factor $k$ and does not automatically compensates the resistances in the network.
  
-FIGURE k vs frequency (e..g, FIG 3.5) HERE?+{{ :0:pt-symmetric_frequency.png?600 |}} 
 + 
  
 The same conclusions can be drawn for the PP compensated circuit. The same conclusions can be drawn for the PP compensated circuit.
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 We can see that now both the output power and efficiency are NOT constant; they change with varying coupling factor $k$. We can see that now both the output power and efficiency are NOT constant; they change with varying coupling factor $k$.
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-FIGUUR 3.6 HIER? 
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 In the broken PT-symmetric region, the eigenstate amplitude increases or decays exponentially, i.e., no stable region is obtained. In the broken PT-symmetric region, the eigenstate amplitude increases or decays exponentially, i.e., no stable region is obtained.
  
 +{{ :0:pt-symmetric_power_and_efficiency.png?600 |}}
  
-====Efficiency==== 
  
  
partity-time_symmetric_wpt.1751897684.txt.gz · Last modified: by kl