Phase-locked loop with multiple degrees of freedom and its design and fabrication method

Patent metadata

Field	Value
Publication number	US-9602114-B2
Application number	US-201514853247-A
Country	US
Kind code	B2
Filing date	Sep 14, 2015
Priority date	Sep 15, 2014
Publication date	Mar 21, 2017
Grant date	Mar 21, 2017

Abstract

A design method for a phase-locked loop comprises: a controlled-frequency oscillator; a phase comparator, to determine a phase difference between an output signal of the controlled-frequency oscillator and a reference signal; a corrector to receive as input a signal representative of the phase difference and to generate at its output a first correction signal; at least one second corrector, to receive as input a signal representative of or affected by a phase noise of the reference signal or of the output signal of the controlled-frequency oscillator and to generate at its output a second correction signal; and a circuit for generating a slaving signal for the controlled-frequency oscillator on the basis of the first and second correction signals; the method using the H-infinity method. Method for fabricating such a loop comprising a design step implementing this method. Phase-locked loop thus obtained.

First claim

The invention claimed is:

1. A method of designing a phase-locked loop, the phase-looked loop being of the type comprising:
a controlled-frequency oscillator;
a phase comparator, configured to determine a phase difference between an output signal of the said controlled-frequency oscillator and a reference signal;
a first corrector, configured to receive as input a signal representative of the said phase difference and to generate at its output a first correction signal;
at least one second corrector, configured to receive as input a signal representative of or affected by a phase noise of the said reference signal or of the said output signal of the said controlled-frequency oscillator and to generate at its output a second correction signal; and
a circuit for generating a slaving signal for the said controlled-frequency oscillator from the said first and second correction signals;
the said method comprising a step of determining transfer functions of the said correctors allowing rejection, in one and the same frequency band, the phase noise of
the said reference signal and the phase noise of the said output signal of the said controlled-frequency oscillator, and wherein said step is implemented, by means of a computer, by applying the H-infinity (H∞) method utilizing:
at input, a first weighting function for a phase noise of the said controlled-frequency oscillator and a second weighting function for a phase noise of a reference signal, and which are determined on the basis of nominal power spectral densities of the said noise; and
at output, at least one third weighting function for a phase noise of an output signal of the phase-lock loop or of an error in tracking the said reference signal, determined on the basis of a phase noise power spectral density template of the said output signal having to be complied with.

2. The method of claim 1 , wherein the said step of determining transfer functions of the said correctors comprises the following sub-steps:
a) determining a nominal power spectral density of the said reference signal;
b) determining a nominal power spectral density of the phase noise of the said controlled-frequency oscillator;
c) determining a phase noise power spectral density template of the said output signal having to be complied with;
d) determining, on the basis of the said nominal power spectral densities and of the said power spectral density template, at least the said first, second and third weighting functions;
e) constructing an augmented system through the said weightings; and
f) applying the H-infinity (H∞) method to the said augmented system so as to synthesize the transfer functions of the said correctors.

3. The method of claim 2 , wherein the said step d) also comprises the determination of a fourth weighting function at output for the power spectral density of the said slaving signal on the basis of a power spectral density template of the said slaving signal to be complied with.

4. The method of claim 2 , also comprising a sub-step d′) of simplifying the weighting functions determined during sub-step d), the weighting functions thus simplified being used during the said sub-step e), the said simplification being implemented by approximating the said weighting functions by transfer functions of lower order and of smaller modulus at least over a spectral operating span of the phase-locked loop.

5. The method of claim 2 , also comprising a sub-step g) of simplifying the transfer functions synthesized during the said sub-step f), the said simplification being implemented by approximating the said transfer functions by transfer functions of lower order.

6. The method of claim 2 , wherein the said step f) is implemented with an extra constraint, according to which the modulus of the transfer function going from the said output signal of the said controlled-frequency oscillator to the said reference signal exhibits, in at least one spectral span, a slope of greater than or equal to +20 db/decade and preferably of greater than or equal to 40 dB/decade.

7. The method of claim 1 , wherein the said phase-locked loop comprises at least one third corrector configured to receive as input a signal representative of or affected by a phase noise generated inside the said loop, other than the said phase noise of the said output signal of the said controlled-frequency oscillator, and to generate at its output a third correction signal, the said circuit for generating a slaving signal for the said controlled-frequency oscillator being configured to generate the said slaving signal also on the basis of the said third correction signal, the said step, implemented by the said H-infinity (H∞) method, of determining transfer functions of the said correctors using as input also a weighting function for the said phase noise other than the said phase noise of the said output signal of the said controlled-frequency oscillator, and also determined on the basis of the power spectral density of the said noise.

8. A method for fabricating a phase-locked loop, of the type comprising:
a controlled-frequency oscillator;
a phase comparator for determining a phase difference between an output signal of the said controlled-frequency oscillator and a reference signal;
a first corrector, configured to receive as input a signal representative of the said phase difference and to generate at its output a signal termed the first correction signal;
at least one second corrector, configured to receive as input a signal representative of or affected by a phase noise of the said reference signal or of the said output signal of the said controlled-frequency oscillator and to generate at its output a signal termed the second correction signal; and
a circuit for generating a signal for slaving the said controlled-frequency oscillator on the basis of the said first and second correction signals;

the said method comprising:
a step of design of the said phase-locked loop; and
a step of physical production of the phase-locked loop thus designed;

wherein the said design step is implemented by a method according to claim 1 .

9. A method for fabricating a phase-locked loop, of the type comprising:
a controlled-frequency oscillator;
a phase comparator for determining a phase difference between an output signal of the said controlled-frequency oscillator and a reference signal;
a first corrector, configured to receive as input a signal representative of the said phase difference and to generate at its output a signal termed the first correction signal;
at least one second corrector, configured to receive as input a signal representative of or affected by a phase noise of the said reference signal or of the said output signal of the said controlled-frequency oscillator and to generate at its output a signal termed the second correction signal; and
a circuit for generating a signal for slaving the said controlled-frequency oscillator on the basis of the said first and second correction signals;

the said method comprising:
a step of design of the said phase-locked loop; and
a step of physical production of the phase-locked loop thus designed;

wherein the said phase-locked loop comprises at least one third corrector, configured to receive as input a signal representative of or affected by a phase noise generated inside the said loop, other than the said phase noise of the said output signal of the said controlled-frequency oscillator, and to generate at its output a third correction signal, the said circuit for generating a slaving signal for the said controlled-frequency oscillator being configured to generate the said slaving signal also on the basis of the said third correction signal, the said design

Assignees

• Commissariat Energie Atomique

Inventors

• Pelissier Michael
• Korniienko Anton
• Zarudniev Mykhailo
• Scorletti Gèrard
• Mokrenko Olesia
• Blanco Eric
• Villard Patrick
• Billiot Gèrard

Classifications

• G06F30/30

  Circuit design · CPC title

• H03L7/08 Primary

  Details of the phase-locked loop · CPC title

• H03L2207/50

  All digital phase-locked loop · CPC title

• H04L7/0079

  Receiver details · CPC title

• H03L7/099

  concerning mainly the controlled oscillator of the loop · CPC title