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1 A Low Spur Fractional-N Frequency Synthesizer Architecture 指導教授 : 林志明 教授 學生 : 黃世一 Circuits and Systems, 2005. ISCAS 2005. IEEE International Symposium.

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Presentation on theme: "1 A Low Spur Fractional-N Frequency Synthesizer Architecture 指導教授 : 林志明 教授 學生 : 黃世一 Circuits and Systems, 2005. ISCAS 2005. IEEE International Symposium."— Presentation transcript:

1 1 A Low Spur Fractional-N Frequency Synthesizer Architecture 指導教授 : 林志明 教授 學生 : 黃世一 Circuits and Systems, 2005. ISCAS 2005. IEEE International Symposium on 23-26 May 2005 Page(s):2807 - 2810 Vol. 3

2 2 Outline Abstract Introduction Fractional spurs Blocking of the fractional spurs Simulation results Conclusions References

3 3 Abstract New architecture of a fractional-N PLL frequency synthesizer Loop filter with a discrete time comb filter Loop filter architecture can be efficiently implemented using switched capacitor techniques

4 4 Introduction 1 Fractional-N PLL, Better phase noise performance, faster lock and better spur levels Advantages: larger loop bandwidth, better VCO phase noise suppression, faster lock time and higher PFD update frequencies Fractional spurs and cycle slipping

5 5 Introduction 2 Delta-sigma control in the feedback divider Fractional spurs by the delta-sigma modulator to high frequencies. Delta-sigma modulator can generate spurs Pseudorandom sequences

6 6 Introduction 3 Another way to suppress fractional spurs is to reduce the bandwidth of the PLL Degradation of the noise performance, lock time and jitter

7 7 Introduction 3 Extension of the conventional fractional-N technique A discrete-time loop filter with notches at spur frequencies A low power frequency synthesizer design with low spur levels

8 8 Fractional spurs Fractional-N frequency synthesizers generate spurs at the output of VCO

9 9 ω s = 2πf s fs - frequency of a spur V i - amplitude of the i-th harmonic ϕ i - phase of the i-th harmonic

10 10 ω 0 = 2πf 0 f 0 - frequency of the free running oscillator V A - amplitude of oscillation Φ(t) - phase of the oscillator

11 11

12 12 ω c = 2πf c = 2π(f 0 + K VCO V 0 )

13 13

14 14 Each harmonic at the control line of a VCO will generate an infinite number of spurs at multiple frequencies around the carrier frequency of the VCO The magnitude of a spur depends on the Bessel functions and depends on the K VCO

15 15 Blocking of the fractional spurs

16 16

17 17

18 18 Simulation results

19 19

20 20

21 21 VCO output spectrum of the conventional PLL (zoomed) VCO output spectrum of the PLL with DTF (zoomed).

22 22 Conclusion Fractional-N frequency synthesizers with low fractional spurs Discrete-time comb filter, switched capacitor techniques Simulation results

23 23 References Kratyuk, V.; Hanumolu, P.K.; Un-Ku Moon; Mayaram, K.;Circuits and Systems, 2005. ISCAS 2005. IEEE International Symposium on 23-26 May 2005 Page(s):2807 - 2810 Vol. 3 Digital Object Identifier 10.1109/ISCAS.2005.1465210 Volodymyr Kratyuk, Pavan Kumar Hanumolu, Un-Ku Moon and Kartikeya Mayaram School of Electrical Engineering and Computer Science Oregon State University, Corvallis, Oregon 97331

24 24 Thank You For Your Attention !


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