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[Components]
Technique Trims VCXO Phase Noise
This patented circuit approach can improve the phase-noise performance and frequency stability of even low-cost voltage-controlled crystal oscillators.

Ulrich L. Rohde, Ajay Kumar Poddar  |  ED Online ID #16332 |  August 2007

Frequency reference standards are essential to achieving frequency accuracy and phase stability in electronic systems. Such sources require the chief characteristics of low phase noise and good frequency stability.1-13 The best oscillator performance can be expensive, however. Fortunately, a patented approach has been developed to design and optimize the performance of voltage-controlled crystal oscillators (VCXOs), even those with relative low quality-factor (Q) resonators, to achieve excellent phase noise and frequency stability.

A typical oscillator consists of a tuned circuit and an active device such as a transistor. Ideally, the tuned circuit provides a high loaded Q, generally from less than 100 for simple circuits to more than 1 million for crystal-resonator-based circuits. Noise arises from the active device as well as from resonator losses. Noise from a bipolar transistor, for example, stems from base and collector contributions and from device parasitic elements, such as the base-spreading resistor. The filtering effect of the resonator tends to remove the device noise, with higher Qs delivering greater filtering effects. The Leeson equation relates these noise effects.1 The formula was modified by Rohde for use with VCOs.2

The equation is linear, with many unknowns. Among the more difficult oscillator performance parameters to predict are output power, noise figure, operating Q, and flicker corner frequency. The parameters can not be derived for linear conditions but require large-signal (nonlinear) analysis.3 But by combining Leeson's formula with the contributions of the tuning diode,2 Eq. 3 results, making it possible to calculate oscillator noise based on a linear approach:

where:

£(fm) = the ratio of sideband power in a 1-Hz bandwidth to the total power (in dB) at the frequency offset (fm);
f0 = the center frequency;
fc = the flicker frequency;
QL = the loaded quality factor (Q) of the tuned circuit;
F = the noise factor;
kT = 4.1 10–21 at 300°K (room temperature);
Psav = average power at oscillator output;

R = the equivalent noise resistance of tuning diode (typically 50 Ω to 10 kΩ); and
Ko = the oscillator voltage gain.

Equation 1 is limited by the fact that loaded Q typically must be estimated; the same applies to the noise factor. The following equations, based on this equivalent circuit, are the exact values for Psav, QL, and F, which are required for the Leeson equation. Figure 1 shows the typical simplified Colpitts oscillator giving some insights into the novel noise calculation approach.4

From ref. 3, the noise factor can be calculated by:

After some small approximation,

Figure 2 (left) illustrates the dependency of the noise factor on feedback capacitors C1 and C2. From Eq. 1, the phase noise of the oscillator circuit can be enhanced by optimizing the noise factor terms as given in Eq. 3 with respect to feedback capacitors C1 and C2.

Equation 4 can be found by substituting 1/re for Y21+ (+ sign denotes the large-signal Y-parameter).

When an isolating amplifier is added, the noise of an LC oscillator is determined by Eq. 5.

where:

G = the compressed power gain of the loop amplifier;
F = the noise factor of the loop amplifier;
k = Boltzmann's constant;
T = the temperature (in degrees K);
P0 = the carrier power level (in W) at the output of the loop amplifier;
F0 = the carrier frequency (in Hz); fm = carrier offset frequency (in Hz);
QL = (πF0τg) = the loaded Q of the resonator in the feedback loop; and aR and aE = the flicker noise constants for the resonator and loop amplifier, respectively.


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Reader Comments

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Anonymous -March 24, 2008   (Article Rating: )

Looking for another article on Crystal oscillator by Authors !!!

Jacob -September 13, 2007   (Article Rating: )

After reading this article, I consoled myself in way that mystery behind ultra low phase noise performance of Crystal oscillator is resolved and no longer exist in the form of cut and try method till we get frustrated and ended with prototype lab model without repeatability. Indeed, Leeson formula gave good direction to begin with but new formula described in this article can be used optimization of the performances for high end signal sources. Author's other book "Design of Modern Microwave Oscillators for Wireless Applications" explains most of the oscillator design methodology and worth reading for understanding this article in depth. Prof Rohde should write another book on oscillator for removing the shadow of mystery behind oscillator design otherwise we are going to make same mistake while designing integrated oscillator in Si/GaAs/CMOS foundry.

Lius Suzane, Post Doctorate (Univ of Sydney, Australlia) -September 12, 2007   (Article Rating: )

According to the book “RF/Microwave Circuit Design for Wireless Applications” by U. Rohde and D. Newkirk (ch 5, pg 736), the Flicker Noise corner was introduced for the first time into Leeson formula by Dieter Scherer from HP in 1978.

I am asking myself why when introducing this new parameter which makes a big impact on the final phase noise prediction, there are so many RF engineers that still use in their modeling the basic Leeson formula.

JR -September 10, 2007   (Article Rating: )

Lot of info. but too complex to understand the circuit as shown in Figure 7.

Julia Mercedes -September 05, 2007   (Article Rating: )

Your online article is unprintable. Attempting to print directly from the webpage or from the "Printer-friendly" view results in the page extending beyond the margins of the paper, even when print margins are set to zero.

Laudied -August 31, 2007

RF MEMS based low cost oscillator may replace expensive crystal oscillator for the applications where high performance ref. source is very critical. This paper describes techniques to lower the phase noise but author did not elaborate in details about the degree of freedom for selecting lower Q resonator. Readers like us may not figure out the ratio of the Q factor and impact on performances.

Rixioylu -August 30, 2007   (Article Rating: )

What compromise we have to make for low Q crystal oscillator versus high Q crystal oscillator? In general, phase noise performance will be influenced with greater degree but this paper describes the way to overcome this problems but at what price? Whether price is to compensate by circuit complexities or other performance such as tuning range, puliiling/pushing, output power, power consumption, size, and thermal drift. I like this paper because of clear mathematical derivation that allows reserach scholar to test and verify the experimental results. Regards, Tiazurelio, PhD. Student (UK)

Tiazurelio, Ph.D student -August 28, 2007   (Article Rating: )

Can we extend the operating frequency of the VCXO based on discussed techniques in the paper ? Author may like to address this issue and comments about the higher order overtone mode for the realization of oscillation in 1.2/2.4 GHz range.

Gemmy -August 28, 2007   (Article Rating: )

Crystal resonator vibrates due to the piezoelectric effect,and by default we get overtone frequency modes in addition to the fundamental. The mystery of undesired mode jumping is a major drawback in overtone mode VCXO circuit. Not much detailed explanation is given about how to suppress the undesired jumping modes, authors perhaps would like to address this problems/solutions in next issue of journal based on referred patented approach in the cover page of the journals (August Issue).

Dr. Nioyazika G. -August 26, 2007   (Article Rating: )

Yes, there is too much math but the article seems to address in the good way the solution versu phase noise. Congratulations

Gian

Giancarlo "Gian" Moda, I7SWX -August 25, 2007   (Article Rating: )

To all:

While this paper does not give all the details of the patented approach, i would like to add that here we really addressing a VCXO, a voltage controlled VHF crystal oscillator. Certainly we ha in realty a isolating buffer amplifier and the control voltage corrects aging and thermal drifting.

However the same principle applies to a frequency standard like a 10 MHZ oscillator.

If you send me an e-email at ulr@synergymwave.com I can supply you with information on the VHF/UHF VCO technique.

Ulrich L. Rohde PhD, ScD -August 25, 2007

Can't think of better article than this about Crystal oscillators.I'm concern about the pulling/pushing and thermal drift but it seems that patented techniques explained in the Figure 7 will minimize the drift. We will be ordering few crystal oscillators for our reference signal source in space applications.

Dr. Sandyal Shekhawat -August 24, 2007   (Article Rating: )

Good paper. We always find articles on oscillators based on cut & try approach or experimental results without proper explanations that leaves behind mystrey about autonomous systems. I'm amazed by reading this article and convey my regards to authors for giving good insights about crystal oscillators. I will be teachning crystal oscillator based on this paper to graduate students and will add some of the examples as a minor projects.

Prof. M. Sundarrajan, India -August 24, 2007   (Article Rating: )

We seldom find paper on oscillator like this. After reading this article, I am developing keen interest in designing low noise crystal oscillator by using higher order overtone modes as a cost-effective alternative.

D. Szuoiakaina -August 23, 2007   (Article Rating: )

To: Dr. Hoogle V.

We have submitted a paper to IEEE Transactions on Circuits and Systems, titled : " A Novel Grounded Base Oscillator Design for VHF/UHF Frequencies"

which gives a long derivation as well as a "magical" scalable very simple solution suited for 2 min calculation. It covers the general Oscillator optimization problem.

Let us hope is has the right mix of math, practical details and measurements for the IEEE standard. These things are so specialized that finding a good place for a presentation is difficult. Conference proceedings are not readily available and the IEEE papers can have a turnaround time of up to 2 years !!!

Ulrich L. Rohde, PhD, ScD, August 21 , 2007

Ulrich L. Rohde, PhD, ScD -August 21, 2007   (Article Rating: )

Excellent article by a pair of the leading engineers in this area. The mathematical treatment is excellent.

Dr. Bob McGwier -August 21, 2007   (Article Rating: )

I am a PhD student, found this article good for my reference.

Linda -August 21, 2007   (Article Rating: )

Linear approach for oscillator's performance analysis is just a starting condition and does not lead to any specific design goal due to many unknown time varying parameters. Among the more difficult oscillator performance parameters to predict are output power, noise figure, operating Q, and flicker corner frequency. Authors did show the way to overcome the above problems but do require complex large-signal time dependent noise dynamics. It would be appreciated if there is quick and short-cut formulation of the phase noise model based on predominant noise generating sources such as base current, collector current, base spreading resistance, tank loss resistance, flicker noise etc. Authors describe individual contribution of noise sources and finally total phase noise at different offset frequency, however, this exercise is rigorous and practically not feasible for design engineers. The better approach would be if individual noise sources automatically set for optimization and minimization depending upon their magnitudes for a given operating frequency and ratio for a given noise sources in the oscillators and perhaps connected with the linear phase noise model.

Dr. Hoogle V. -August 19, 2007   (Article Rating: )

Article is too mathematical but gives state-of-the art design techniques to achieve low phase noise without using expensive very high Q crystal resonator.

Vario Duglas -August 18, 2007   (Article Rating: )

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