Dynamic measurement of amplitude-frequency effect of VHF resonators

Dynamic amplitude-frequency effect measurements made of VHF quartz resonators indicate the presence of two separate mechanisms, the relative contribution of which varies for different cuts. For the SC-cut a step-change in drive level leads to a frequency shift with very short time constant (1 ms) that is presumably the classic direct nonlinear elastic effect. Others such as AT-, BT-, and LD-cuts show only a much longer time constant (200 ms), presumably a thermally related indirect nonlinear elastic effect. Near the SC-cut, resonators exhibit a combination of both short- and long-time-constant frequency changes. In some cases the two mechanisms produce frequency shifts in opposite directions. This behavior is problematic for some amplitude-frequency-effect measurement approaches because the measured shift depends on the timing of those measurements. It is not surprising that the SC-cut response shows only the direct nonlinear elastic effect, but it is unexpected that the AT- and BT-cuts appear riot to show such effect. These results raise a question as to what amplitude-frequency effect criterion is appropriate to use, as well as whether it is proper to determine nonlinear elastic constants from AT-cut resonator measurements that assume the effect is not thermally related.

[1]  Y. Hirose,et al.  Evaluation of nonlinear elastic coefficient causing frequency shifts in AT-cut resonators , 1991, Proceedings of the 45th Annual Symposium on Frequency Control 1991.

[2]  G. Théobald,et al.  Frequency variations in quartz crystal resonators due to internal dissipation , 1979 .

[3]  S. Galliou,et al.  Recent results on quartz crystal LD-cuts operating in oscillators , 2004, Proceedings of the 2004 IEEE International Frequency Control Symposium and Exposition, 2004..

[4]  F. Sthal,et al.  Doubly rotated quartz resonators with a low amplitude-frequency effect: the LD-cut , 2001, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[5]  J. Gagnepain Nonlinear Properties of Quartz Crystal and Quartz Resonators: A Review , 1981 .

[6]  J. Nosek Drive level dependence of the resonant frequency in BAW quartz resonators and his modeling , 1999, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[7]  H. Tiersten,et al.  The Evaluation of the Coefficient of Nonlinear Resonance for SC-Cut Quartz Resonators , 1985, 39th Annual Symposium on Frequency Control.

[8]  M. Mourey,et al.  Phase noise limitation due to amplitude frequency effects in state-of-the-art quartz oscillators , 1996, Proceedings of 1996 IEEE International Frequency Control Symposium.

[9]  H. Tiersten An Analysis of Nonlinear Resonance in Electroded Contoured AT- and SC- Cut Quartz Crystal Resonators , 1984 .

[10]  R. Smythe,et al.  Experimental Evaluation of the Effective Non-Linear Elastic Constant for Trapped Energy and Contoured Resonators , 1985, 39th Annual Symposium on Frequency Control.

[11]  J. J. Gagnepain,et al.  Nonlinear Constants and Their Significance , 1987, 41st Annual Symposium on Frequency Control.

[12]  R. L. Filler,et al.  The Amplitude-Frequency Effect in SC-Cut Resonators , 1985, 39th Annual Symposium on Frequency Control.

[13]  M. Planat,et al.  Non-linear Propagation of Surface Acoustic Waves on Quartz , 1980 .

[14]  D. Hammond,et al.  Precision Crystal Units , 1963 .

[15]  R. Bourquin,et al.  Isochronism defect for various doubly rotated cut quartz resonators , 1999, Proceedings of the 1999 Joint Meeting of the European Frequency and Time Forum and the IEEE International Frequency Control Symposium (Cat. No.99CH36313).

[16]  J. Nosek Drive level dependence of the resonant frequency in BAW quartz resonators and its modeling , 1997, Proceedings of International Frequency Control Symposium.

[17]  J. Valentin Thermal gradient distributions in trapped energy quartz resonators , 1985 .

[18]  J. Gagnepain,et al.  Amplitude - Frequency Behavior of Doubly Rotated Quartz Resonators , 1977 .