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Frequency tuning loop for VCOs

Linares Barranco, Bernabé; Rodríguez Vázquez, Ángel Benito; Sánchez Sinencio, Edgar; Huertas Díaz, José Luis

Abstract

A frequency tuning circuit is introduced for VCOs (voltage-controlled oscillators) so that the final relationship between oscillating frequency and input control voltage is fixed and independent of nonidealities. This tuning loop is applied to an OTA-C sinusoidal VCO. Such an oscillator has an output frequency-input voltage relationship that depends on temperature, process parameters, and even amplitude of the oscillations. It is shown that, by adding the tuning loop, nonideal dependences will be minimized.

Full text

FREQUENCY TUNING LOOP FOR VCOS B. Lina es-Ba anco’, A. Rod iguez-Vbquez2, E. Shchez-Sinencio’ and J. L. Hue as2 ’ Depa men o Elec ical Enginee ing Texas A&M Uni e si y, College S a ion, TX 77843-USA Dp o. de Diseiio Analbgico, Cen o Nacional de Mic oelec bnica, 41012-Se illa, Spain Abs ac -Fo a Vol age Con olled Oscilla o (VCO) he oscilla ing equency is con olled by an ex e nal inpu . The ela ionship be ween he oscilla ing equency and he inpu con ol ol - age is, in mos cases, expec ed o be linea and independen o pa asi ics, p ocess pa ame e s, empe a u e, and o he non-ideali i es. In his pape we in oduce a equency uning ci cui o VCOs so 4a he Anal ela ionship be ween oscilla ing equency and inpu con ol ol age is Axed and independen o he p e ious men ioned non-ideali ies. This uning loop is applied o an OTA-C sinusoidal VCO. Such an oscilla o has an ou pu equency-inpu ol age ela ionship ha depends on empe a u e, p ocess pa ame- e s, and e en ampli ude o he oscilla ions. I is shown ha by adding he uning loop all hese non-ideal dependences will be minimized. I. INTRODUCTION Vol age Con olled Oscilla o s a e key componen s in many signal p ocessing and communica ion sys ems [l-31, and a e also used o he uning o monoli hic il e s [4-91. They alsomay be used o ins umen a ion applica ions [2]. In many cases i is necessa y ha he ela ionship be ween he ac ual oscilla ing equency o he VCO and i s inpu con ol ol age is e y p ecise and does no change wi h empe a u e, p ocess pa ame e s o pa asi ics. Conside a ce ain VCO (sinusoidal, iangula , o squa e wa e,) ha has an “uncon olled” inpu ol age- ou pu equency cha ac e is ics. We will show ha by adding he equency uning loop desc ibed in his pa- pe he inpu ol ageou pu equency ela ionship can be made e y linea and comple ely independen o sec- onda y pa ame e s ( empe a u e, ampli ude, pa asi ics, and p ocess pa ame e s) wi hin he uning ange o he o iginal VCO. The uning loop p oposed in his pape is alid o any ype o VCO. We a e going o e i y i s ope a ion by applying i o an OTA-C sinusoidal VCO [lo]. Sinusoidal OTA-C VCOs ha e a nonlinea inpu ol ageou pu equency ela ionship ha depends on p ocess pa ame e s, empe a u e, pa asi ic componen s and e en ampli ude o he oscilla ions. By adding he p oposed uning loop we will show ha his ela ionship will become linea and independen o he p e iously men ioned pa ame e s. 11. THE FREQUENCY TUNING LOOP Figu e 1 shows he basic s uc u e o he equency uning loop [11,12]. co “OU? I Squa e- wa e Con e e F equency Di ide by N (Op ional) Fig. 1. Block Diag am o F equency Con ol Loop. The ou pu o he oscilla o (i no squa e) is con- e ed o a squa e wa e, di ided by N (op ional) and applied o a F equency- wVol age (FTV) con e e . Usually he maximum ope a ing equency o an oscil- la o is highe han he maximum possible equency in a F equency- o-Vol age Con e o . Fo his eason he inclusion o he equency di ide in Fig. 1 is many imes manda o y. As we will see in he nex sec ion, he FTV con- e e is a de ice such ha i in is he equency o i s inpu signal, i s ou pu ol age will be gi en by in REF Vz = n VBIAS- Whe e n is a posi i e in ege , VBlAS is a e e ence ol - age and REF he equency o a e e ence squa e wa e CH 30064/91/0000 - 2617 $1.00 C IEEE signal (like a c ys al oscilla o ). I is he ou pu e- quency o he VCO and a equency di ide is used wi h a a e N, hen in = /N. I p-' is he ime cons an o he in eg a o , i s ou pu ol age will be gi en by: V = ~( co - z) (2) On he o he hand, o a CMOS OTA-C sinusoidal os- cilla o we ha e 1131, (3) K = e = -(V - ih) 2* c 2TC whe e K and V h a e gi en by he opology and an- sis o geome ies o he OTAs used as well as by he p ocess pa ame e s. Sol ing equa ions (l), (2) and (3) yields, Vco - VBIAS- N REF which has a s able s a iona y poin (!$ < 0) cha ac- e ized by N Vco = REF- ~VBIAS (5) The ela ion be ween (ou pu equency) and V,, (in- pu ol age) is shown in Fig. 2. No e ha i is linea and i depends only on REF, VBIAS, n and N. In he nex Sec ion we will gi e he implemen a ion de ails o he FTV con e e , which is he key compo- nen o he equency uning loop. , Fig. 2. Fkequency s con ol ol age ela ionship o V,, wi h equency uning loop. 111. The FTV Con e e Conside he ci cui eo Fig. 3. I con ains a monos- able ha p oduces a pulse o du a ion o = 1 Du ing his pulse, capaci o C is cha ged by a cu en go (~~VBIAS - z). The es o he ime i is discha ged by goV,. The wa e o m ha esul s a he capaci o u( ) is shown in Fig. 4. Fo each cycle o u( ), Vz( ) is he peak alue o u( ) o he p e ious cycle. Two consecu i e peak alues a e ela ed by 2 REF ' V,( +nT) = V,( )-g"Vz(NT- o)+g"(2n ~~~s- z) , whe e T = 1/ . I is cons an and he FTV con e e C C (6) eaches i s s eady s a e, hen Vz( + NT) = Vz( ), i.e., A s abili y condi ion o he s eady s a e can be ob- ained by w i ing (6) in he Z-domain and making he poles o be inside he uni y ci cle. The esul ing condi- ion is [E], (8) Ngo '2C A con enien IC implemen a ion o his FTV con e e is shown in Fig. 5. To imp o e he ime esponse, he swi ch o Fig. 3 has been eplaced by a di e en ial pai and cu en mi o s. The cu en sou ces a e imple- men ed wi h linea ized OTAs. o = , --I+ MONOSTABLE N I 1 4 De ec o Uj , Peak &- - - Fig. 3. Fkequency- o-Vol age Con e e - u( ) Fig. 4. Time wa e o ms o U( ) inside he FTV Con e e , and o Vx( ), i s ou pu . s 1. --cHc Ju-l- V, I J Fig. 5. CMOS Ci cui Implemen a ion o FTV Con e e 2618 The monos able has o p o ide a pulse o du a ion o = 1/2 REF. such a ci cui is shown in Fig. 6. The du a ion o he ou pu pulse o is gi en by he ime i akes o cha ge capaci o CI om OV o VREF by he cu en IREF. VREF is gi en by he ol age o which Cz is cha ged, s a ing a OV by a cu en IREF du ing a ime o = 1/2 REF. The e o e, i he wo ci cui s enclosed by b oken lines in Fig. 6 a e pe ec ly ma ched, he du a ion o he monos able ou pu pulse will be o = 1/2 REF, independen o IREF and cl = cz = c. I he e is a misma ch be ween he wo ci cui s he wid h o he monos able ou pu pulse will no be equal o hal he pe iod o e e ence signal REF. Howe e , besides his, he ope a ion and cha ac e is ics o he uning loop s ill emain basically in a ian . --------------- _L ICIl I1 I- - - a ____-- M. Chcd ChUi . - c--c I. Fig. 6. Block Diag am o Monos able wi h Ou pu Pulse Wid h Con olled by an Ex e nal Squa e Wa e Signal o P ecise F equency. IV. EXPERIMENTAL RESULTS In o de o es heop oposed equency uning loop s a egy we used a sinusoidal OTA-C oscilla o [10,12]. I s equency dependence is shown in Fig. 7. No e ha he ela ionship be ween ou pu equency and inpu ol age (Bias Vol age) is nonlinea and changes wi h he ampli ude o he oscilla ions. A disc e e equency uning loop was implemen ed a ound he p e ious CMOS OTA-C oscilla o . Since he ou pu equency gdes o e 13MHz, a as compa a- o (CM710C) was used o con e he sinusoid o a squa e wa e signal. Fo he monos able a con en ional 555 ime was used. In his case, he wid h o i s ou pu pulse is no con olled by an ex e nal equency e e - ence, bu by a p ecise RC cons an . Also, since his ci cui has e y bad ime esponse (p opaga ion imes a e a ound lOOns he ou pu o he oscilla o had o be di ided by 32. The esul ing ou pu equency-inpu ol age ela ionship o he VCO wi h equency uning loop is shown in Fig. 8. This cha ac e is ic is he same o di e en alues o he oscilla ing ampli udes, o di - .O Bias Vd og. ( ol s) Fig. 7. F equency s Bias Vol age o sinusoidal OTA-C Oscilla o wi hou equency uning loop. e en empe a u es and o di e en IC chips. A his ime we do no ha e a ailable a comple e IC p o o ype o quan i y he deg ee o linea i y, which is highly de- penden on he implemen a ion. 14.0' 13.0. 12.0, 11.0 CI Y E" '"5 8. ;:5 1 6.0 5.0- 4.0. 3.0. 2.0 + 1:O 1:1 1:2 1.3 114 115 1.6 1.7 F oquoncy Con ol V&ap (Vdb) Fig. 8. Measu ed Oscilla ion F equency s F equency Con ol Vol age o VCO wi h F equency Tuning Loop. V. CONCLUSIONS A equency uning loop o VCOs is p esen ed ha compensa es o empe a u e, p ocess pa ame e s, am- pli ude, and pa asi ics in luence in he o iginal ou pu equency-inpu ol age ela ionship. This uning loop can be applied o any ype o VCO. I s iabili y has been demons a ed, by applying i o a sinusoidal OTA-C VCO. The uning loop was cons uc ed using a b ead- boa d p o o ype, bu i can be in eg a ed oge he wi h he oscilla o in he same IC die [14]. 2619 VI. REFERENCES [ 11 K.K. Cla ke and D.J. Hess, “Communica ion Ci - cui s: Analysis and Design”, Addison Wesley 1978. 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