vibraon compensated tcxos and ocxos enable improved … · • specifying an oscillator with...
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Vibra&oncompensatedTCXOsandOCXOsenableimprovedsystem
performanceinvibratoryenvironments
FlavienHeur&erSales&Applica&onsEngineer
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Presenta&onoutline
• Accelera&onsensi&vityofthequartz• Characterizingtheaccelera&onsensi&vity• Improvingtheaccelera&onperformance• Conclusion
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ACCELERATIONSENSITIVITYOFTHEQUARTZCRYSTAL
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Accelera&onSensi&vityofthequartzcrystal
• Accelera&onsensi&vitycommonlyreferredas“g-sensi&vity”• AlsoGreekgamma,Γ
• Accelera&onforcescauseschangeinresonantfrequencyduetomoun&ngstructure• Non-uniformstressonac&veareaofthequartzcrystal• SmallfrequencyshiMs(oMenno-no&cedinmanyapps)
• Linearlypropor&onaltoappliedforce• Upto50g’s(dependingonmount)
• Γisavectorquan&ty• FrequencyshiMishighlydependedonappliedforce
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Accelera&onSensi&vityofthequartzcrystal
f (!a) = f0 (1+!Γ⋅!a)
FrequencyshiMisdirec&onallydependent:
• Maximallyposi&vewhenisparallelto• Maximallynega&vewhenisan&-parallelto• Zerowhenisperpendicularto
!a!a!a
!Γ !
Γ!Γ
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Accelera&onSensi&vityversusdirec&onalappliedforce
Γd =!Γ ⋅!a ⋅cosα
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Accelera&onSensi&vityversusdirec&onofappliedforcein3D
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CHARACTERIZINGTHEACCELERATIONSENSITIVITY
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MeasurementSystems
• ForMeasurementofrela&vesidebandslevelswithsinusoidalvibra&on• ForMeasurementofphasenoiseduringrandomvibra&on
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AxisDefini&onforSC-cutCrystal
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AxisDefini&onforStripCrystal
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ATStripCrystal
• Miniaturesize–assmallas1.5x1.0mm• CanprovideprecisionperformanceforTCXOs• Surfacemountpackage
• Consistentaccelera&onsensi&vity• Somedesignsachieve<1.10-10/g
• Statekisalignedwiththesameaxis• Facilitatesmoun&ngandalignment
Γ
Γ
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MiniatureATStripCrystal
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SphericalCoordinateSystemforDefiningCrystalg-sensi&vityVector
!Γ = Γx
2 +Γy2 +Γz
2
Θ = sin−1 Γz!Γ
⎛
⎝
⎜⎜
⎞
⎠
⎟⎟
Φ= cos−1 ΓxΓ2x +Γ
2y
⎛
⎝
⎜⎜
⎞
⎠
⎟⎟
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SidebandsgeneratedbySingleFrequencyVibra&on
• For20MHzTCXOVib=10gpeak90Hz=>=1.56ppb/g
Γ
SBLevel(dBc) = 20 log!a×!Γ× fnom2 fv
⎛
⎝⎜
⎞
⎠⎟
!Γ=
2 fv!a× fnom⎛
⎝⎜
⎞
⎠⎟×10
SBLevel (dBc)20
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PhaseNoisePlot–RandomVibra&on
£( fv ) = 20 log!Γ× fnom× 2×PSD
2 fv
⎛
⎝⎜
⎞
⎠⎟
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PhaseNoisePlot–RandomVibra&on
1.3x10E-9/g
£( fv ) = 20 log!Γ× fnom× 2×PSD
2 fv
⎛
⎝⎜
⎞
⎠⎟
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PhaseNoisePlot–RandomVibra&on
£( fv ) = 20 log!Γ× fnom× 2×PSD
2 fv
⎛
⎝⎜
⎞
⎠⎟
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Phasenoiseundervibra&onandaccelera&onsensi&vity
• Phasenoiseundervibra&onisprimarilydeterminedbytheaccelera&onsensi&vity
• Specifyinganoscillatorwithultra-lowsta&cphasenoisewillnotguaranteetheperformanceundervibra&on.Itwillbedeterminedbytheaccelera&onsensi&vityoftheofthecrystal/oscillator
• Inmanycases,alowvibra&oncompensatedTCXOcouldprovidelowerphasenoiseundervibra&onthanalownoiseOCXO
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PhaseNoisePlot–RandomVibra&on
10MHzOCXO=0.6ppb/g
10MHzTCXOVib.Compens.=0.03ppb/g
Γ
Γ
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Accelera&onSensi&vityQuartzCrystalscomparison
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IMPROVINGTHEACCELERATIONSENSITIVITYPERFORMANCE
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Improvingtheaccelera&onsensi&vityperformance
• Crystalmanufacturingandmoun&ngtechniques• Aien&ontomoun&ngstress
• Oscillatormoun&ngandorienta&on• Ac&vecompensa&onwithaccelerometer
• Effec&veatlowfrequency• Vibra&onisola&on
• Effec&veabovenaturalfrequencyofisolator• Addssize,weightandcost
• Mul&ple-crystalpassivecancella&onmethods• Aligncrystalswithan¶llel
!Γ
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Improvingtheaccelera&onsensi&vityperformance
Y1
Y2
G1
G2
Dual Crystal Acceleration Sensitivity
Cancellation
Gamma Vectors aligned antiparallel
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Improvingtheaccelera&onsensi&vityperformance
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Finalaccelera&onsensi&vityresults
T1300-1 40MHz
(Crystal Pairs of CT1061-50) Post Seal
Sideband Levels (dBc)* Acceleration Sensitivity (ppb/g)
S/N z y x Γ z Γ y Γ x Γ max 4 -79.1 -88.8 -88.9 0.05 0.02 0.02 0.055 9 -82.9 -86.9 -88.8 0.03 0.02 0.02 0.041
12 -86 -87.3 -88.2 0.02 0.02 0.02 0.035 14 -83.8 -84.2 -85.4 0.03 0.03 0.02 0.047 31 -87.9 -88.1 -87.7 0.02 0.02 0.02 0.031
*(10g's@90Hz)
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Varia&onofathighertemperature
Γ
Temp +25C +85C S/N Γ z (ppb/g) Γ z (ppb/g) Delta (ppb/g) 15 0.0218 0.0223 0.0005 21 0.0228 0.0396 0.0168 8 0.0259 0.0196 -0.0063
19 0.0337 0.0362 0.0024 9 0.0379 0.0326 -0.0053
17 0.0379 0.1407 0.1028 7 0.0511 0.0425 -0.0086
16 0.0511 0.0755 0.0245 1 0.0580 0.0425 -0.0155 3 0.0621 0.0908 0.0287
12 0.0713 0.0791 0.0078
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PhasenoiseunderRandomVibra&on
A=Standard single crystal Γ≈2.5ppb/g
B=Matched dual crystals Γ≈0.05ppb/g
C=Quiescent phase noise
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PhasenoiseunderRandomVibra&on
125MHzTCXOstandard
Γ≈0.95ppb/g
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PhasenoiseunderRandomVibra&on
125MHzTCXOdual-mount
Γ≈0.060ppb/g
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T1300withdualmoun&ngtechnique
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Accelera&onSensi&vityPatent
IntellectualProperty• Althoughpassive
cancella&ontechniqueshavebeenknownforyears,Greenrayhasbeengrantedapatentforthemethodofimplemen&ngitwithstripcrystals
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Conclusion
Althoughitisnotpossibletocompletelyeliminatetheeffectsofaccelera&onontheresonantfrequencyofaquartzcrystal,byunderstandingthevectornatureofthecrystal’sg-sensi&vitycharacteris&c,theimpactinmostapplica&onscanbeminimizedwithcarefuldesignprac&ces.
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Thanksalotforyouraien&on.AnyQues&ons?