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A General Subthreshold MOS Translinear Theorem

Serrano Gotarredona, María Teresa; Linares Barranco, Bernabé; Andreou, Andreas G.

Abstract

This paper outlines the conditions under which the translinear principle can be fully exploited for MOS transistors operating in subthreshold. Due to the exponential nature of subthreshold MOS transistors the translinear principle applies immediately as long as the source-to-bulk voltages are made equal to zero (or constant). This paper addresses the conditions under which subthreshold MOS transistors still satisfy a translinear principle but without imposing this constraint. It is found that the translinear principle results in a more general formulation than the original for BJTs since now multiple translinear loops can be involved. The constraint of even number of transistors is no longer necessary.

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A Gene al Sub h eshold MOS T anslinea Theo em Te esa Se ano-Go a edona’, Be nab6 Lina es-Ba anco’, and And eas G. And eou2 Na ional Mic oelec onics Cen e (CNM), Ed. CICA, AV. Reina Me cedes sln, 41012 Se illa, Spain * The Johns Hopkins Uni e si y, 3400 N. Cha les S ee , Ba on Hall, Bal imo e, MD 21218, USA Abs ac This pape ou lines he condi ions unde which he T anslinea P inciple can be ully exploi ed o MOS ansis o s ope a ing in sub h eshold. Due o he exponen ial na u e o sub h eshold MOS ansis o s he T anslinea p inciple applies immedia ely as long as he Sou ce- o-Bulk ol ages a e made equal o ze o (o cons an ). This pape add esses he condi ions unde which sub h eshold MOS ansis o s s ill sa is y a T anslinea p inciple bu wi hou imposing his cons ain . I is ound ha he T anslinea p inciple esul s in a mo e gene al o mula ion han he o iginal o BJTs since now mul iple T anslinea loops can be in ol ed. The cons ain o e en numbe o ansis o s is no longe necessa y. I. In oduc ion The anslinea p inciple, in oduced by Ba y Gilbe in 1975 [I], is one o he mos impo an ci cui heo y con ibu ions in he elec onics e a. In i s o iginal o mula ion, he anslinea p inciple p o ides a simple and e icien way o analyze and syn hesize nonlinea ci cui s based on bipola junc ion ansis o s (BJTs). Due o hei exponen ial cha ac e is ics, he anslinea p inciple can be ex ended o MOS ansis o s ope a ing in weak in e sion [2], [3] wi hou and wi h loa ing-ga e de ices [4]. Fo MOS ansis o s ope a ing abo e h eshold he e has also been ound a simila way o analyze and syn hesize nonlinea ci cui s [5]. Fo bipola ansis o s one p ac ical p oblem ha may equi e some a en ion when applying he anslinea p inciple is he nonze o base cu en [6]. In con as , he anslinea p inciple holds o MOS sub h eshold ansis o s in an exac manne i sou ce and bulk a e sho -ci cui ed. Howe e , i has been ound ha he p inciple holds as well in an exac manne unde di e en ci cums ances [2]-[3], al hough a gene al sub h eshold MOS anslinea heo em has no been de ised un il now. In his pape we p o ide his gene al heo em and ou line he condi ions unde which sub h eshold MOS ansis o s, iewed as ou e minal de ices, sa is y a gene al anslinea p inciple. The ope a ion o a sub h eshold MOS can be desc ibed by he ollowing equa ion [2], [7]-[9] whe e V h = KTIq is he mal ol age, I, is a posi i e cons an cu en , S is he ansis o size ac o (S = WIL , whe e W is ansis o wid h and L is i s leng h), and K is a echnology dependen posi i e pa ame e . This equa ion holds ue as long as whe e @FB is he de ice’s la band ol age [lo]. Vol age VBs can ake ei he posi i e o nega i e alues as long as he pa allel PN diode junc ion is biased below i s o wa d conduc ion h eshold ol age. Pa ame e K is known o ha e a sligh dependency on ol age VBS [2]. Howe e , in his pape we will assume K o be cons an , which is a easonable assump ion i ca e is aken o make he VBs ol ages simila o all ansis o s. Fo ope a ion in sa u a ion eq. (1) can be simpli ied o (i VDs >> V h) (3) and be ew i en as whe e I (a “no malized cu en ”) is ansis o cu en no malized wi h espec o ansis o size ac o S = WIL, and i,, i, a e dimensionless numbe s called pseudo-cu en s and equal o (5) GS‘ Ih . ‘BSI ‘1 h i, = e iB = e Le us use he symbol in Fig. 1 o ep esen a weak- in e sion MOS in sa u a ion. Le us call he pa h ha goes om he ga e e minal G o he sou ce e minal S he G - b unch (o Ga e-b unch), and he pa h ha goes om he bulk e minal B o e minal S he B - b unch (o Bulk-b unch). We a e using a diode- like symbol o ep esen he exponen ial ela ionship be ween he ol age o he b anch and he cu en lowing ou o he de ice and a capaci i e-like e mina ion o each diode symbol o ep esen he capaci i e coupling na u e o he Ga e and Bulk e minals. I Vss = 0 (o cons an ) he e is an exac exponen ial ela ionship be ween VGs and ZDs (see eq. (3)) and he o iginal BJT anslinea o mula ion can be di ec ly and exac ly applied. 11. Gene alized T anslinea Theo em o Sub h eshold MOS T ansis o s In his sec ion we will conside he condi ions unde which anslinea p inciples can be applied o ci cui s PB S Fig. 1: T anslinea Symbol Rep esen a ion o Sub h eshold MOS Tkansis o in Sa u a ion 0-7803-5471 -0/99/$10.0001999 IEEE 11-302 Fig. 2: Example o Coupled G-loops using anslinea symbol ep esen a ion Fig. 3: Illus a ion o he G-o de concep . De ices ‘1-2-3- 6’ o m a G-loop which is coupled o G-loop o med by de ices ‘2-4-5’, because de ices ‘1-2-3-4’ o m a B-loop. De ices ‘1-2-3-4-5-6’ o m a Closed T anslinea Se , and so do de ices 6 and 7. De ice 2 has a G-o de o nc2 = 2 because i s G-b anch belongs o wo G-loops o he same Closed T anslinea Se . All o he de ices ha e G-o de one. wi h sub h eshold MOS ansis o s bu wi hou imposing he cons ain o making Vss = 0. We will in oduce i s some p elimina y heo ems and de ini ions, and hen s a e and p oo he gene alized anslinea heo em o sub h eshold MOS de ices. The i s concep s o be in oduced a e G-loop and B-loop. A G-loop (o Ga e-loop) is a closed loop o G- b anches, and a B-loop (o Bulk-loop) is a closed loop o B-b anches. Fo hese loops we can s a e anslinea heo ems o hei pseudo-cu en s, whose p oo is iden ical as o he o iginal BJT T anslinea Theo em. Theo em: In a G-loop con aining an a bi a y numbe o G-b anches, he p oduc o pseudo- cu en s o b anches cpnnec ed in he Clock-Wis~G(CW) di ec ion is equal o he co esponding p oduc o b anches connec ed in he Coun e -Clock-Wise (CCW) di ec ion. No e ha since pseudo-cu en s a e dimensionless en i ies we can ha e an a bi a y numbe o b anches o ien ed CW and ano he a bi a y numbe o b anches o ien ed CCW (as opposed o he case o eq. (7)). A comple ely equi alen heo em holds di ec ly o B- Up o now hings a e simila o classical anslinea loops, excep ha an a bi a y numbe o b anches a e allowed. Howe e , he p esence o wo exponen ial b anch ol ages in eq. (3) is wha makes sub h eshold MOS anslinea loops mo e gene al and complica ed han he classical ones. A i s consequence o his ac is he ollowing concep o coupled loops: De ini ion: Two G-loops a e said o be coupled i a leas one MOS de ice o he i s G-loop and a leas one o he di e en de ice o he second G-loop sha e hei espec i e B-b anches in a common B-loop. loops. This is illus a ed in Fig. 3. De ices ‘1-3-5’ o m a G- loop and de ices ‘2-4-6’ o m ano he G-loop. Howe e , de ices ‘1-2-3-4’ o m a B-loop, hus making he p e ious wo G-loops o be coupled h ough he B- b anches o de ices 1,2,3 and 4. An equi alen de ini ion applies o coupled B- loops. No e ha wo loops may ha e a common b anch wi hou being necessa ily coupled loops. In he example o Fig. 3, we can w i e o he wo G-loops ( ‘SS4 + ‘LIS6 - ‘BSZ) = Ioe whe e all pseudo-cu en s i, ha e cancelled ou by applying he abo e Theo em. Howe e , due o B-loop ‘1-2-3-4’, ‘BSI + ‘BS4 = ‘LIS2 + ‘BS3 (7) which in oduces a coupling be ween he wo equa ions in (Il), and makes G-loops ‘1-3-5’ and ‘2-4-6’ o be coupled loops. When de ices o m mul iple ouching loops i is no clea which ones o choose o how many o choose. Fo example, in Fig. 4 one can choose G-loops ‘1-2-3-6’, ‘6- 7’, and ‘2-4-5’. Bu why no conside ‘1-3-4-56’, ‘6-7’, and ‘2-4-5’, o ‘1-3-4-5-7’ and ‘1-2-3-6’. One can y all possible op ions as long as one chooses a se o Non- Redundan (NR) loops: De ini ion: A se o loops is said o be Non- Redundan (NR) i he sum o b anch ol ages o any loop canno be exp essed as a linea combina ion o he sum o b anch ol ages o o he loops in he se . Fo example, in Fig. 4, o G-loops ‘1-2-3-6’, ‘2-4- 5’, and ‘1-3-4-5-6’ hei espec i e sum o b anch ol ages is, ‘GS6 + ‘GS, = ‘CS2 + ‘GS3 “GS2 + VGS4 = VGSS VGS6 + VCSl+ VGS4 = VGS3 + VGSS (8) Any o hese h ee equa ions can be exp essed as a linea combina ion o he o he wo. Thus he h ee G- loops do no o m a Non-Redundan se o G-loops. Howe e , any wo o hese h ee G-loops do o m a Non-Redundan se o G-loops. The ac ha sub h eshold MOS ansis o s can o m coupled loops yields na u ally o he ollowing concep o Closed T anslinea Se , De ini ion: Gi en a se o MOS de ices, and once a Non-Redundan se o loops has been chosen, a Closed T anslinea Se (CTS) is a se o de ices such ha all loops hey o m a e only coupled among hem, bu no .o loops 11-303 -I A + L BHCL 8 1V3TH BF l 8T&J T- Fig. 4 Example o Closed 3’5 T anslinea Se s. MOS De ices 7 and 8 o m a Closed T anslinea Se , and so do MOS De ices 1-7. whe e b anches o o he de ices (no belonging o he CTS) a e p esen . This is illus a ed in Fig. 5. Le us selec he NR se o G-loops ‘1-2-3-7’, ‘4-5-6’, and ‘7-8’, and he NR se o B-loops ‘1-2-3-4-56’, ‘7’, and ‘8’. G-loops ‘1-2-3-7’ and ‘4-5-6’ a e coupled because he e is a e B-b anches o de ices o bo h G-loops ha a e sha ed in he common B-loop ‘1-2-3-4-5-6’. The wo G-loops ‘1-2-3- 7’ and ‘4-5-6’, and he wo B-loops ‘1-2-3-4-5-6’ and ‘7’ a e no coupled o o he loops (ei he G-loop ‘7-8’ no B-loop ‘8’), hus ( o he chosen NR se o loops) de ices ‘1-2-3-4-5-6-7’ o m a Closed T anslinea Se . On he o he hand, G-loop ‘7-8’ is no coupled o any o he loop, no a e B-loops ‘7’ and ‘8’. The e o e, de ices ‘7-8’ o m ano he Closed T anslinea Se . When wo king wi h mul iple G-loops and B-loops, wi h some o hem being coupled, i is no e y con enien o classi y each b anch as being CW o CCW o ien ed, as will become appa en la e . Le us ins ead classi y all b anches in o wo o ien a ion g oups, he a-wise o ien ed b anches and he p-wise o ien ed b anches. Two b anches a e classi ied in o he same g oup (ei he he a-wise o he p-wise) i hey appea in he same loop wi h he same o ien a ion. On he con a y, wo b anches a e classi ied each in o a di e en g oup (one in o he a-wise, he o he in o he p- wise) i hey appea in he same loop wi h opposi e o ien a ion. No e ha now a CW b anch in one loop and a CCW b anch in ano he loop can be classi ied in o he same a-wise o p-wise g oup. I a b anch is sho - ci cui ed, i o ms a one b anch loop and can be classi ied as ei he a-wise o p-wise. Ano he concep ha is use ul o s a ing he gene alized anslinea sub h eshold MOS heo em is ha o G-o de and B-o de o a MOS de ice in a Closed T anslinea Se : De ini ion 4: Once a NR se o loops has been chosen, a sub h eshold MOS ansis o which is pa o a Closed T anslinea Se is said o ha e a G-o de o alue nc, i i s G- b anch belongs o nc G-loops o he gi en Closed T anslinea Se . An equi alen de ini ion o B-o de can be s a ed o B- loops. The concep is illus a ed in Fig. 4. Le us choose he NR se o G-loops ‘1-2-3-6’, ‘2-4-5’, and ‘6-7’ and o B-loops ‘1-2-3-4’, ‘5’, ‘6’, and ‘7’. G-loops ‘1-2-3-6’ and ‘2-4-5’ a e coupled because de ices ‘1-2-3-4’ o m a B-loop. The e a e no o he couplings among he chosen loops. Consequen ly, de ices ‘ 1-2-3-4-5-6’ o m a Closed T anslinea Se which consis s o G-loops ‘1- 2-3-6’ and ‘2-4-5’ and B-loops ‘1-2-3-4’, ‘5’, and ‘6’. De ices 6 and 7 o m one G-loop (‘6-7’) and wo B- loops (‘6’ and ‘7’) which a e no coupled o any o he loop. The e o e de ices 6 and 7 o m ano he Closed T anslinea Se . MOS de ice 2 has G-o de nG2 = 2 because i s G-b anch appea s in wo G-loops o he same Closed T anslinea Se . MOS de ice 6 does no ha e G-o de 2 because, al hough i s G-b anch belongs o wo di e en G-loops, hese wo loops do no belong o he same Closed T anslinea Se . All MOS de ices ha e B-o de one because hei B-b anches appea only in one B-loop. When a G-b anch has G-o de g ea e han one i belongs o mo e han one G-loop o he same Closed T anslinea Se . In such cases i is possible ha he b anch be classi ied as a-wise in some G-loops and as p- wise in o he G-loops. Unde hese ci cums ances i is con enien o di ide i s G-o de in o wo pa s (9) nc = na.,+n B, G whe e na (le us call i G-a-o de ) deno es he imes his G-b hnch is classi ied as a-wise in a CTS, and n (le us call i G-p-o de ) deno es he imes i is clhied as p-wise in CTS. Simila ly, o B-b anches, he B-o de can be sepa a ed in o he B-a-o de ( na, ) and he B-p-o de ( nP, B). Using he concep s and p elimina y heo ems in oduced un il now, i is possible o s a e and p oo he gene alized anslinea heo em o sub h eshold MOS ansis o s’: Theo em: Gi en a se o sub h eshold MOS de ices and choosing o hem a se o Non- Redundan G-loops and B-loops, o each Closed T anslinea Se he ollowing can be s a ed: I i is possible o ind an a- and p-wise classi ica ion o hei G-loops and B-loops such ha a) he sum o G-a-o de s equals he sum o G- P-o de s Zna,,, = Cnp,cl (10) J E { a-w se) Is {p-wise} bland, e e y ime a de ice’s G-b anch is classi ied as a-wise in a G-loop i s B-b anch can be classi ied as a-wise in some B-loop, and e e y ime a de ice‘s G-b anch is classi ied as P-wise in a G-loop i s B-b anch can be classi ied as p-wise in some B-loop, hen he p oduc o no malized cu en s aised o he powe o hei G-a-o de o all ansis o s in he CTS whose G-b anches ha e been classi ied a-wise equals he p oduc o no malized cu en s aised o he powe o hei G-P-o de o all ansis o s whose G-b anches ha e been classi ied P-wise. P oo : Fo each G-loop in he Closed T anslinea Se he ollowing holds: 11 iG1 le {p-wise) 1. The heo em will be s a ed using G-b unches as p ima y b anches and making B-b anches o depend on hem. Howe e , because o he symme y be ween G-b unches and B-b unches (due o he symme y be ween V,, and V,, ol ages in eq. (3)), he heo em can be s a ed as well by in e changing G-b unches and B- b unches. 11-304 Since his is ue o e e y single G-loop we can mul iply hese equa ions o he chosen se o Non- Redundan G-loops and hei p oduc will s ill be equal o uni y, Fu he mo e, we can aise i o he powe o K, and i s ill be equal o uni y, No e ha , since he de ices o m a CTS, all b anches will be p esen and no b anch o ano he CTS appea s. Consequen ly, eq. (18) includes all G-b anches o he CTS and only he b anches o his CTS. Equi alen ly, he same can be s a ed o all B-loops, bu aising now o he powe o 1 - IC, o con enience. No e ha , due o s a emen b) in Theo em 3, e e y ime a de ice has i s pseudo-cu en iGj in he nume a o o eq. (1 8), i s pseudo-cu en iBj will also appea in he nume a o o eq. (19), and bo h will appea na, cj imes. And he same holds o pseudo-cu en s in he denomina o s o eqs. (18) and (19). The e o e, le us de ine na, and n such ha 1 Also, since he de ices o m a Closed T anslinea Se , eq. (1 8) includes all de ices o he CTS, and so does eq. (1 9). Consequen ly, we can mul iply eqs. (1 8) and (1 9) and index he iG and i pseudo-cu en s o he same de ice wi h he same su&c ip and use his subsc ip o index he MOS de ice, On he o he hand, due o s a emen a) in he heo em he ollowing is sa is ied By mul iplying eqs. (21) and (22), and using eq. (4) we ob ain which concludes he p oo o he Gene alized Sub h eshold MOS T anslinea Theo em. 0 111. Re e ences B. Gilbe , “T anslinea Ci cui s: A P oposed Classi ica ion,” Elec onics Le e s, ol. 1 I, No. 1, pp. 14-16, 1975; e a a, ol. 11, No. 1. A. G. 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