Example: tourism industry

A precision CMOS bandgap reference

1014 IEEEJOURNALOFSOLID-STATECIRCUITS, , , , ,threep-tubresistors,andoneop-amparenece ssarytoproduceareferencewithfixedvoltage of than2percent,whilekeepingthermaldriftbel ow40ppm/ ~ Cto125 ,atmodestcostincircuitcomplexity, ,thevoltagereferenceisoftenapotentiallym osttroublesomecomponentsinceitmustproduc eatemperaturestable,processinvariant, , ;however,theabsolutemagnitudeofoutputisp oorlycontrolledbecauseitdependsontheaccu racyofdepletionandenhancementimplants[1] .Inthebandgapreferences,wheretheoutputis derivedfromthevoltagedifferenceoftwodiod esforwardbiasedbyratioedcur-rents,bothth ethermaldriftandtheabsolutevalueoftheout putcanbecontrolledwithprecision[2] [4].

1014 IEEE JOURNAL OF SOLID-STATE CIRCUITS, VOL. SC-19, NO. 6, DECEMBER 1984 A Precision CMOS Bandgap Reference JOHN MICHEJDA AND SUK K. KIM Abstract — This paper describes the design of a precision on-chip band- gap voltage reference for applications with CMOS analog circuits.

Tags:

  Design, Reference, Precision, Cmos, Bandgap, A precision cmos bandgap reference

Information

Domain:

Source:

Link to this page:

Please notify us if you found a problem with this document:

Other abuse

Advertisement

Transcription of A precision CMOS bandgap reference

1 1014 IEEEJOURNALOFSOLID-STATECIRCUITS, , , , ,threep-tubresistors,andoneop-amparenece ssarytoproduceareferencewithfixedvoltage of than2percent,whilekeepingthermaldriftbel ow40ppm/ ~ Cto125 ,atmodestcostincircuitcomplexity, ,thevoltagereferenceisoftenapotentiallym osttroublesomecomponentsinceitmustproduc eatemperaturestable,processinvariant, , ;however,theabsolutemagnitudeofoutputisp oorlycontrolledbecauseitdependsontheaccu racyofdepletionandenhancementimplants[1] .Inthebandgapreferences,wheretheoutputis derivedfromthevoltagedifferenceoftwodiod esforwardbiasedbyratioedcur-rents,bothth ethermaldriftandtheabsolutevalueoftheout putcanbecontrolledwithprecision[2] [4].

2 ACIVfOSbandgapvoltagereferencewhichusesb ipolar-likesource-to-draintransfercharac teristicsofMOStran-sistorinweakinversion wasreported[5],[6]. [7] , ,1983;revisedJuly13, ,MurrayHI1l, ,Honeywell, [8]usestemperaturedependentp-tubresistor stoprovidebiascurrentstothereferencediod es,whicharetheemitter-basejunctionsofthe bipolartran-sistorsformedbythen+ ,thebasiccircuitandthecriteriafortempera turecompensa-tionarepresented, , , , (7 )andacrossdiode2isV2(T),thentheoutputcan beexpressedasvout=A(vl(T)-v2(T))+B(v2(T) )=avl(T) bv2(T)(1) [4].Thesearederivedfordevicesbiasedbyeit hertemperatureindependentconstantcurrent 1,orcurrentswhichvarywithtemperatureasT , (1) ,andresistorsRl,R2,andR3isthebandgapcirc uitwhichproducesafixedvoltageVOut= , $ :PRSCISIONCMOSBANDGAPREFERENCE1015 DDThevoltagedropattemperatureTisgivenbyT TFig.

3 [9].proposedbyKuijk[8], ,YeandTsividis[9]havedemonstratedthiscon figuration,andaconfigurationpro-ducingap ositiveoutputvoltage, (2)Inladditiontothegainofthecircuit,whic hisde-terminedbytheratioofresistorsR~and R~,themagni-tudeandtheratioofthebiascurr entsisdeterminedbytheratioofresistorsRIa ndR~: (T)=n[vG(T +(?)ln(*) 7)wherenisthenonidealityfactor,VG(T)isth ebandgapvoltageattemperatureT,kistheBolt zmannconstant,qistheelectroncharge,Aisan ormalizingconstantrelatedtothegeometryof thedevice,and~ (T) [10]givestheempiricalexpressionfortheban dgapvalueex-trapolatedfromphysicalmeasur ementovertemperattnx?]

4 (T)=VGO+~T($)whereVGO= ,anddVG/dT= 4 (l),subjecttotheconditionthatthetemperat urecoefficientattempera-tureT=TOiszero,d YOutdT~.~,=o.(9)Thevalueoftheoutputvolta geVOut(TO)isuniqueandgivenby[()kTOvout(T o)=nVGO+ qVOU, Vi(T)II(T)=R1(4)(B-l+T (ZHH=O)) 10)VOut Vi(T)_VOut V(T)12(T)=R R+;.(5)332 Inthisimplementation,however,thebiasingc urrentsII(T)and12(T)aretemperaturedepend entbecauseofthevariationofVI(T)andV2(T), andtoalesserextentbecaluseofthevariation ofVOutwithrespecttotempera-ture,Thecondi tionsforthetemperaturecompensationofthis circuitwithtemperatureindependentRI,Rz,a ndR~are{&enin[8].]}

5 ~= ~followingdifferentialequation:TdVOut--v o~t+%lwdT++W+ vgo=o.(11)Itisimportanttonoticethattheva lueofVOut(TO)asgivenin(10),andthebandgap temperatureresponseasgivenin(11)dependso nlyonphysicaldiodeparametersnand~,andres istortemperaturecoefficient(1/R)(dR/dT). resistorsapproximatelydoubletheirresista nceforatern--peraturein;reaiefrom-Oto100 C. emittervoltageV~eofaShockley sequation,forqV>>nkT, (6)substratecollector,p-tubbase,andn+ , , , ,similartotheonegivenin[6],thereferenced evicecanoperateatlargerbiasingcurrent, ,eachunittransistorwith20pmX20pmemitter, ,werecharacterizedtoobtainthevalueofpara me-tersnand~necessarytopredictthevoltage dropacrossthereferencedeviceasgivenin(7) .

6 Thevalueofnwasdeterminedbymeasuring1 ,andthenfittingthemeasuredvoltageusing(7 ), , ~parameterdirectly,theprecise1 ,becauseaminorinaccuracy( C)intemperaturemeasurementofthereference s,canleadtolargeerrorsinestimateof~.When thesemeasurementsaremadeondevicesplacedo nawaferprober,anuncertaintyintemperature betweenthethermo-coupleinthewaferchuck,a ndthewaferitselfcanalsocausesignificante rrorsinthevalueof~.Anewindirectmethodofm easurementwasusedindeterminingthevalue~. Aprecisionop-ampwithlowinputoffsetandhig hopen-loopgain,andasetofprecisiondiscret eresistorswhosevalueswereindividuallymea sured, ,andthevaluesofdiscreteresistorsweresele cted ~ ~= (7),and(8),togeneratethe1 V ,andtheresistancevaluesRI,R~,andR~,thepr ogramsolvesiterativelyforbiaspointsVIand V2,andoutputvoltageV&until,VOU,-V1(R1(T) ,T)_VOU, V2(R3(T),T)R~(T)RI(T) R2(T)+R3(T) RI(T) (12)-4284-1:s88- x ~= ~=4, ,4,700I.

7 ,,,00~8080100120 TEMPERATURE(UC) :~edresistorbandgapcircuittodeterminethe vatueof, ~ ,andmoreprecisedeterminationof~. , ~mtwintubCMOS technologyis-3 , p-typesiliconsamples[11] , , ,forap-tubresistor,R(T)=ROT22(13)MICEIEJ DAANDKIM:PRECISIONCMOSBANDGAPREFERENCE10 17100-90-80 70 R,60 50-R240-30- R= ~o,,lnT( K) ~ ,[l\(dR} (14)andthepropercompensation,accordingto formula(10),occurswhenI&tatTOis[(3P++(H) out(~O) ~ GO+ C,wheretheresistanceofbiasingresistorsva riesasT22,thevalueof/3= ,andthevalueofTois50 (To)is ,andthetemperaturevariationofP&over100 :1yieldingvoltagedifferenc~(Vl-Vz)-80mVa t25 (1)is10and9.))]]

8 P-tubdoping,resistormismatch,referencedi odemismatch, ,whichresultsintheop-ampoffseterror, , ,3006-4, 5> +00 TEMF3 SRATURE( C) , ,.(16)Therefore,forafractionalerrorinimp lantdosedN,/iV,,thefractionalerroronthep -tubresistancedR/Ris;dR dN$ - RN, (17)Forthen-p-nbipolardevicebiasedwithfi xedV~G,thecollectorcurrentisproportional tothenumberofimpuri-ties/unitareaintheba se[12](alsoknownasGurnmelnumber).Forthed evicewithionimplantedp-tubbase,thisnumbe risequaltotheiopimplantdoseN,.Therefore, I-h~qvh,/kT(18)sandtheVbedropacrossthere ferencedeviceisV-~ln(lN~).

9 Be(19)ThechangeinVb~ofthereferencedevice duetothep-tubionimplanterroriskTdN,dVbe= qN~ (20)Thedopingofthep-tubinthetwintubCMOS processcanbecontrolledto+ , , ,DECEMBER1984implantdoseshouldresultina+ ,or+ (19)thevariationofthevoltageacrosstheref er-encedevicebiasedbythep-tubresistorres ultingfromthechangesinV~,andthebiascurre ntis[1kTdNdIdV1=dV2=y@+Fs(21)Forbiascurr ent1inthecircuit,V&t VbgI=R (22)thechangeincurrentdIisdVOut dVbedI=~ (%,-%)dRR2(23)for10%resistancevariation, thefirsttermin(23) ~__IRandusing(17),(21),and(24)(12kTdN,dV 1=dV2= 9% (24)(25)Thebandgapoutputvoltagechangeist hendVOutl=adV1-bdV,=(a-b)dV1=dV1.)]

10 (26)Thetotalvariationoftheoutputvoltaged uetovariationinthep-tubdopingis(27)The+1 0percenterrorinthep-tubimplantwillresult in+ ~ , (28)wherethevalueofa= ~ , ~canbematchedaccuratelybecausetheycanber atioedbyanexactintegerfactor,and- ~.A;~ x x x-x-x-~-x-x~ s> :31-x-x-x-x_x x-x-x-x-x-x-.,,),~020406060100 TEMPERATURE[ C) !0,2MV----P-TUBIMPLANTERRORMO%-X-RESISTO RRATloMISMATCHttOA ,Sensitivityofoutputvoltagetoprocessingv ariationsalsobecauseRIandR~haveanidentic ~ ~andR~ismorelikelytooccursincetheseresis torsareratioedbyanonin-tegernumber,andbe causeRzisbiasedatadifferentpotentialfrom thesubstratethanRIandR~.]


Related search queries