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A dynamic threshold cancellation technique for a high-power conversion efficiency CMOS rectifier

Abstract

Power conversion efficiency (PCE) has been one of the key concerns for power management circuits (PMC) due to the low output power of the vibrational energy harvesters. This work reports a dynamic threshold cancellation technique for a high-power conversion efficiency CMOS rectifier. The proposed rectifier consists of two stages, one passive stage with a negative voltage converter, and another stage with an active diode controlled by a threshold cancellation circuit. The former stage conducts the signal full-wave rectification with a voltage drop of 1 mV, whereas the latter reduces the reverse leakage current, consequently enhancing the output power delivered to the ohmic load. As a result, the rectifier can achieve a voltage and power conversion efficiency of over 99% and 90%, respectively, for an input voltage of 0.45 V and for low ohmic loads. The proposed circuit is designed in a standard 130 nm CMOS process and works for an operating frequency range from 800 Hz to 51.2 kHz, which is promising for practical applications.

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A dynamic threshold cancellation technique for a high-power conversion efficiency CMOS rectifier

Author: Godinho, António; Yang, Zhaochu; Dong, Tao; Gonçalves, L. M.; Mendes, P. M.; Wen, Yumei; Li, Ping; Jiang, Zhuangde
Publisher: Multidisciplinary Digital Publishing Institute (MDPI)
Year: 2021
DOI: 10.3390/s21206883
Source: https://repositorium.uminho.pt/bitstreams/4c241b2a-ab40-43eb-bd23-59aff16ec7e5/download
senso s
A icle
A Dynamic Th eshold Cancella ion Technique o a
High-Powe Con e sion E iciency CMOS Rec i ie
An ónio Godinho 1,†, Zhaochu Yang 1,†, Tao Dong 2,*, Luís Gonçal es 3, Paulo Mendes 3, Yumei Wen 4, Ping Li 4
and Zhuangde Jiang 1


Ci a ion: Godinho, A.; Yang, Z.;
Dong, T.; Gonçal es, L.; Mendes, P.;
Wen, Y.; Li, P.; Jiang, Z. A Dynamic
Th eshold Cancella ion Technique o
a High-Powe Con e sion E iciency
CMOS Rec i ie . Senso s 2021,21, 6883.
h ps://doi.o g/10.3390/s21206883
Academic Edi o s: Jong-Ryul Yang
and Seong-Tae Han
Recei ed: 24 Sep embe 2021
Accep ed: 13 Oc obe 2021
Published: 17 Oc obe 2021
Publishe ’s No e: MDPI s ays neu al
wi h ega d o ju isdic ional claims in
published maps and ins i u ional a il-
ia ions.
Copy igh : © 2021 by he au ho s.
Licensee MDPI, Basel, Swi ze land.
This a icle is an open access a icle
dis ibu ed unde he e ms and
condi ions o he C ea i e Commons
A ibu ion (CC BY) license (h ps://
c ea i ecommons.o g/licenses/by/
4.0/).
1
Chongqing Key Labo a o y o Mic o-Nano Sys ems and Sma T ansduc ion, Collabo a i e Inno a ion Cen e
on Mic o-Nano T ansduc ion and In elligen Eco-In e ne o Things, Chongqing Key Labo a o y o Colleges
and Uni e si ies on Mic o-Nano Sys ems Technology and Sma T ansducing, Na ional Resea ch Base o
In elligen Manu ac u ing Se ice, Chongqing Technology and Business Uni e si y,
Chongqing 400067, China; [email p o ec ed] (A.G.); [email p o ec ed] (Z.Y.);
[email p o ec ed] (Z.J.)
2Depa men o Mic osys ems (IMS), Facul y o Technology Na u al Sciences and Ma i ime Sciences,
Uni e si y o Sou h-Eas e n No way, 3616 Kongsbe g, No way
3Cen e o Mic oElec omechanical Sys ems (CMEMS-UMinho), Uni e si y o Minho, 4800-058 Guima ães,
Po ugal; [email p o ec ed] (L.G.); [email p o ec ed] (P.M.)
4School o Elec onic In o ma ion and Elec ical Enginee ing, Shanghai Jiao Tong Uni e si y,
Shanghai 200240, China; [email p o ec ed] (Y.W.); [email p o ec ed] (P.L.)
*Co espondence: [email p o ec ed]
† Au ho s whom i s au ho ship is sha ed by An ónio Godinho and Zhaochu Yang.
Abs ac :
Powe con e sion e iciency (PCE) has been one o he key conce ns o powe managemen
ci cui s (PMC) due o he low ou pu powe o he ib a ional ene gy ha es e s. This wo k epo s a
dynamic h eshold cancella ion echnique o a high-powe con e sion e iciency CMOS ec i ie . The
p oposed ec i ie consis s o wo s ages, one passi e s age wi h a nega i e ol age con e e , and
ano he s age wi h an ac i e diode con olled by a h eshold cancella ion ci cui . The o me s age
conduc s he signal ull-wa e ec i ica ion wi h a ol age d op o 1 mV, whe eas he la e educes he
e e se leakage cu en , consequen ly enhancing he ou pu powe deli e ed o he ohmic load. As
a esul , he ec i ie can achie e a ol age and powe con e sion e iciency o o e 99% and 90%,
espec i ely, o an inpu ol age o 0.45 V and o low ohmic loads. The p oposed ci cui is designed
in a s anda d 130 nm CMOS p ocess and wo ks o an ope a ing equency ange om 800 Hz o
51.2 kHz, which is p omising o p ac ical applica ions.
Keywo ds:
ib a ion ene gy ha es e ; powe managemen ci cui ; CMOS ec i ie ; dynamic h esh-
old cancella ion echnique; high powe con e sion e iciency
1. In oduc ion
P esen ly, ene gy ha es ing appea s as a p omising eliable echnology ha can
p olong he li e ime o ba e ies and powe wi eless senso ne wo ks (WSNs) o en i-
onmen al moni o ing [
1
]. Howe e , in hese WSN applica ions, ambien ib a ions a e
unp edic able, ime- a ying, and low ampli ude, which es ic s he a ailable powe o he
ene gy ha es ing sys em [
2
]. To o e come hese d awbacks, esea ch g oups ha e been
ocusing on using piezoelec ic ha es e s due o hei high powe densi y and capabili y o
in eg a e MEMS and CMOS echnology, making i possible o de elop all he sys ems (en-
e gy ha es e and elec onic sys em) in a single chip [
3
–
5
]. Thus, o maximize he amoun
o ene gy ans e ed unde di e en ambien condi ions, a powe managemen ci cui
(PMC) is c ucial in o de o ex ac , con e , s o e, egula e, and manage he sca enged
ene gy om he piezoelec ic de ice [6,7].
Because he ib a ional ene gy sou ces p oduce AC signals, sca enging such ene gy
equi es a ull-wa e ec i ie as a key ci cui inside he PMC, which allows he AC/DC
Senso s 2021,21, 6883. h ps://doi.o g/10.3390/s21206883 h ps://www.mdpi.com/jou nal/senso s
Senso s 2021,21, 6883 2 o 13
con e sion o p ope ly powe he WSNs. Howe e , because he ou pu powe o he
ib a ional ene gy ha es e is low [
4
], he high o wa d ol age equi ed by s anda d
ull-wa e diode b idges and Scho ky diode ec i ie s limi s hei use on hese low powe
es ic applica ions [
8
]. To su pass hese limi a ions, diode-connec ed MOS ansis o s
ha e been widely used because hey p esen simila I-V cha ac e is ics o he s anda d
diodes. Thus, designing he ec i ie in CMOS echnology is highly desi able o dec ease
he de ice’s o m ac o and easily in eg a e wi h he ene gy ha es e while explo ing new
dynamic echniques o educe he powe consump ion, achie e high PCE, and minimize
leakage cu en [9,10].
Recen wo k has been de eloping dynamic h eshold echniques o educe he h esh-
old ol age e ec [
11
]. Add essing hese echniques allows o he educ ion o o al ol age
d op and mi iga ion o he e e se leakage cu en in he ac i e s age. By a ending o
hese conce ns du ing he design o he ci cui , i is possible o minimize he ci cui ’s
o e all powe and leakage cu en consump ion. Thus, all hese condi ions we e ca e ully
conside ed du ing he design o he p oposed high-powe e iciency CMOS ec i ie o
a end o he demands o his applica ion.
In his wo k, a new CMOS ec i ie s uc u e o piezoelec ic ene gy ha es e s is
p esen ed. I combines a passi e s age nega i e ol age con e e (NVC) wi h an ac i e
diode con olled by a dynamic h eshold cancella ion ci cui o build a new a chi ec u e
ha can educe i s o al ol age d op. Wi h his con igu a ion, a ol age d op lowe han
2 mV can be achie ed in he second s age, which consequen ly enhances ea u es such as
VCE and PCE, as well as educes he e e se leakage cu en ha lows om he load.
2. CMOS Rec i ie s
2.1. Passi e Rec i ie s
The CMOS ga e c oss coupled can eplace he con en ional ull-wa e b idge ec i ie
o o e come he high o wa d ol age d op because i allows a minimum inpu ol age o
ope a e [
10
,
12
,
13
]. Howe e , his opology s ill lacks e iciency due o he h eshold ol age
(VTH) d op ac oss he diode connec ed in each conduc ion pa h [13].
The ully c oss-coupled ec i ie in ends o ul ill he gap o he p e ious con igu a ion
by elimina ing all
VTH
d ops, which educes he ol age d op ac oss his s age [
13
]. Conse-
quen ly, his opology imp o es bo h PCE and VCE o he ci cui [
13
]. Howe e , he e e se
leakage cu en appea s o be he main disad an age o using his single con igu a ion,
which a ec s he powe ans e ed om he ci cui o he load [
10
]. Thus, an ex a ci cui
mus be added o o e come his issue.
2.2. Ac i e Rec i ie s
To p e en he ci cui om e e se leakage cu en , he CMOS passi e ec i ie s
combined wi h an ac i e con igu a ion can mi iga e he e e se leakage cu en o enhance
he DC powe o he load [
14
–
19
]. In hese ac i e con igu a ions, compa a o s a e designed
o con ol he ga e ol age o he ac i e diode (o so-called he main ansis o ) depending
on i s inpu and ou pu ol age condi ions. In wo k done by Pe e s e al. [
15
], an ac i e
ec i ie wi h a bulk-inpu compa a o echnique is p oposed o ul a-low- ol age ene gy
ha es ing sys ems. Howe e , when he inpu ol age is highe han he ou pu ol age,
he PN junc ions be ween he bulk and sou ce e minal o he inpu ansis o will be
u ned on. Consequen ly, he e e se leakage cu en will low om he ca hode e minal
o he anode e minal h ough he body PN junc ions, which comp omises he e iciency
o he ci cui [
8
]. In addi ion, he p oposed ec i ie in [
19
] has a equency ange no
sui able o he applica ion o his esea ch wo k. In con as , in he ollowing esea ch
pape s [
8
,
9
,
20
,
21
], he equency bandwid h co esponds o he desi ed applica ion. The
au ho s use wo ac i e diodes o con ol he e e se cu en ha lows h ough he wo
NMOS in each inpu cycle, and wo PMOS in c oss-coupled o p o ide he conduc ion
pa h. Howe e , he dynamic ange does no mee he equi emen s o achie e a high PCE
o inpu ol ages lowe han 1 V, which is c i ical o ene gy ha es ing applica ions [
8
].
Senso s 2021,21, 6883 3 o 13
In [
20
], he au ho s designed a ully ac i e con igu a ion using PMOS and NMOS o ensu e
ha he e e se cu en h ough he PMOS inpu sou ce is ze o. The main disad an age
o his con igu a ion occu s when he wo NMOS de ices u n on simul aneously, which
leads o powe losses. Chang e al. [
21
] p oposed a ec i ie wi h a hi d compa a o o
elimina e he oscilla ions o NMOS, which a oids he wo ac i e diodes u ning on/o
simul aneously. Ne e heless, he PCE is only high o an inpu ol age a ound 4.88 V.
Howe e , he main limi a ions o hese con igu a ions a e ha hey canno con ol
he
VG
o he main ansis o o inc ease
VSG
du ing he conduc ion phase. Thus, i is no
possible o educe he in e nal esis ance o his ansis o , which limi s he ou pu powe
o he ec i ie . The e o e, an ex a ci cui is needed o educe he h eshold ol age e ec o
his ansis o o o e come hese d awbacks.
2.3. Th eshold Cancella ion Topologies
Se e al h eshold cancella ion opologies we e p oposed o enhance he ou pu s o ed
ol age by dynamically educing he h eshold ol age e ec o he main ansis o o he
ec i ie [
22
–
25
]. The h eshold ol age is a p ocess pa ame e dependen on he oxide
ype and hickness [
24
]. Low h eshold ol age MOSFETs p esen a high leakage cu en
caused by he low subs a e doping, which leads o an inc ease in powe consump ion
and eliabili y p oblems [
24
,
26
]. Thus, hese h eshold cancella ion echniques a e used o
a oid hose ypes o MOSFETs since i is only needed o educe he h eshold ol age e ec
when he main pass ansis o is ON. In [
25
], a low- ol age CMOS ec i ie is p oposed o
pe o m his echnique by using he boo s ap echnique, which has enhanced he ou pu
ol age s o ed in he load capaci o . Howe e , o he minimum ope a ing ol age o his
con igu a ion (0.8 V), he PCE o his ci cui is a ound 30%, which is no enough o he
equi emen s o his applica ion.
An ac i e boo s apping ec i ie is p esen ed in [
27
] o o e come he issues o he
p e ious wo k. This opology uses wo ac i e diodes o con ol he conduc ion pa h o
each inpu cycle and a boo s ap echnique o educe he h eshold ol age o bo h main
pass PMOS. Addi ionally, an adap i e ol age con e e is se in his wo k o adjus he
ga e ol age o he main pass PMOS, which educes he ol age d op by educing he
on- esis ance. Besides lowe ing he e e se leakage cu en , he PCE o his con igu a ion
can s ill be imp o ed o inpu ol ages smalle han 1 V. To o e come he low PCE alues
o a na ow inpu ol age ange, in [
28
], a dual swi ching echnique eplaced he wo
ac i e diodes. This app oach can main ain a cons an ga e bias on he wo main NMOS
ansis o s, a oid he e e se leakage cu en , educe he a ea on-chip, and enhance he
PCE o low ol age applica ions. Howe e , high alues o PCE can only be ob ained o
inpu equencies a ound 20 kHz, which makes he equency bandwid h na ow.
3. Design Implemen a ion
Rega ding he inhe en ou pu cha ac e is ics o he piezoelec ic ansduce , he
p oposed CMOS ec i ie was mainly designed o achie e a high PCE o wide low inpu
ol age and equency condi ions. The e o e, he ope a ional ol age anges om 0.4 V
o 1 V, and he wo king equency a ies om hund eds o Hz o a ew kHz. In addi ion,
he ou pu impedance o he ene gy ha es e is no conside ed in his design because
he ma ching impedance p ocess is pe o med be o e his ec i ica ion s age in he PMC.
Thus, he main goal o his wo k is o educe he ol age d op ac oss he s uc u e by
applying a h eshold cancella ion echnique ha will u he enhance he powe con e ed
o he ohmic load. These imp o emen s will o e come he d awbacks o p e ious wo k
by mi iga ing he e e se leakage cu en , and hus enhancing he PCE o a low inpu
ol age ange.
Figu e 1shows he simpli ied schema ic o he p oposed ac i e ec i ie . I consis s
o an NVC and an ac i e diode biased by a h eshold cancella ion ci cui . The i s s age
is se o pe o m he signal ull-wa e ec i ica ion. Howe e , because his passi e s age
canno con ol he e e se cu en om he load capaci o when he ou pu ol age is highe
Senso s 2021,21, 6883 4 o 13
han he inpu , a second s age ac i e diode (M5) is needed. This ac i e s age is composed
o a PMOS con olled by a h eshold cancella ion ci cui wi h a boo s apping capaci o
o educe he e ec i e h eshold o he ac i e diode, and an adap i e ol age con olle
(AVC) o adjus he ga e ol age o M5 by con olling he cha ging/discha ging cycle o
he boo s apping capaci o . To pe o m i , a wo-inpu common ga e compa a o and an
NMOS ansis o a e used. Besides hese s ages, a dynamic swi ching bulk (DSB) echnique
was used o con ol he bulk ol age o he ac i e diode PMOS.
Senso s 2021, 21, x FOR PEER REVIEW 4 o 14
Figu e 1 shows he simpli ied schema ic o he p oposed ac i e ec i ie . I consis s o
an NVC and an ac i e diode biased by a h eshold cancella ion ci cui . The i s s age is
se o pe o m he signal ull-wa e ec i ica ion. Howe e , because his passi e s age can-
no con ol he e e se cu en om he load capaci o when he ou pu ol age is highe
han he inpu , a second s age ac i e diode (M5) is needed. This ac i e s age is composed
o a PMOS con olled by a h eshold cancella ion ci cui wi h a boo s apping capaci o o
educe he e ec i e h eshold o he ac i e diode, and an adap i e ol age con olle
(AVC) o adjus he ga e ol age o M5 by con olling he cha ging/discha ging cycle o
he boo s apping capaci o . To pe o m i , a wo-inpu common ga e compa a o and an
NMOS ansis o a e used. Besides hese s ages, a dynamic swi ching bulk (DSB) ech-
nique was used o con ol he bulk ol age o he ac i e diode PMOS.
Figu e 1. Schema ic o he p oposed ac i e ec i ie composed by a NVC and an ac i e diode con olled by a h eshold
cancella ion ci cui .
3.1. Nega i e Vol age Con e e
The i s s age is ully passi e, and i is used o pe o m he signal ull-wa e ec i i-
ca ion by applying a ully-c oss coupled con igu a ion. Du ing he posi i e hal pe iod o
he inpu signal (𝑉 > 𝑉
), M1 and M3 will be conduc i e as soon as he inpu ol age
ge s la ge han 𝑉 and |𝑉|. In his cycle, node 1 is connec ed o 𝑉 and node 2 o
𝑉. Fo he nega i e pe iod o he sine wa e, M2 and M4 a e conduc ing while he p e-
ious wo ansis o s a e now u ned o (cu -o egion). The e o e, he highe ol age
po en ial is always a 𝑉
, whe eas he lowes po en ial is a 0 V. The ol age d op o he
NVC is gi en by 𝑉 + 𝑉
 in each conduc ion pa h, whe e 𝑉 and 𝑉 a e he ol -
age d op o NMOS ansis o s M2 o M3 and PMOS ansis o s M1 o M4, espec i ely.
To mee all he powe es ic ions ela ed o he piezoelec ic ene gy ha es ing sys-
ems, he ec i ie ci cui mus minimize he ol age d op ac oss he ec i ica ion p ocess.
As less ol age d op occu s, bo h he VCE and he PCE o he ci cui will be highe . Fo
his s age, NVC, he main equi emen is o dec ease he ol age d op associa ed wi h each
MOSFET by educing hei on- esis ance.
3.2. Ac i e Diode
One o he main challenges on he ec i ie ci cui is o a oid he e e se leakage cu -
en by con olling he ope a ion o ansis o M5. The e o e, an ac i e diode con olled
wi h a h eshold cancella ion ci cui can egula e he wo k beha io o his de ice
Figu e 1.
Schema ic o he p oposed ac i e ec i ie composed by a NVC and an ac i e diode con olled by a h eshold
cancella ion ci cui .
3.1. Nega i e Vol age Con e e
The i s s age is ully passi e, and i is used o pe o m he signal ull-wa e ec i ica-
ion by applying a ully-c oss coupled con igu a ion. Du ing he posi i e hal pe iod o he
inpu signal (
Vin+>Vin−
), M1 and M3 will be conduc i e as soon as he inpu ol age ge s
la ge han
VTHn
and

VTHp

. In his cycle, node 1 is connec ed o
Vin+
and node 2 o
Vin−
.
Fo he nega i e pe iod o he sine wa e, M2 and M4 a e conduc ing while he p e ious
wo ansis o s a e now u ned o (cu -o egion). The e o e, he highe ol age po en ial
is always a
Vn c
, whe eas he lowes po en ial is a 0 V. The ol age d op o he NVC is
gi en by
VDSn +VSDp
in each conduc ion pa h, whe e
VDSn
and
VSDp
a e he ol age d op
o NMOS ansis o s M2 o M3 and PMOS ansis o s M1 o M4, espec i ely.
To mee all he powe es ic ions ela ed o he piezoelec ic ene gy ha es ing sys-
ems, he ec i ie ci cui mus minimize he ol age d op ac oss he ec i ica ion p ocess.
As less ol age d op occu s, bo h he VCE and he PCE o he ci cui will be highe . Fo
his s age, NVC, he main equi emen is o dec ease he ol age d op associa ed wi h each
MOSFET by educing hei on- esis ance.
3.2. Ac i e Diode
One o he main challenges on he ec i ie ci cui is o a oid he e e se leakage cu en
by con olling he ope a ion o ansis o M5. The e o e, an ac i e diode con olled wi h a
h eshold cancella ion ci cui can egula e he wo k beha io o his de ice depending on
he ol age po en ial be ween he inpu and ou pu . The deployed h eshold cancella ion
ci cui con ols he ga e po en ial o he MOSFET M5 by compa ing he inpu /ou pu
ol age condi ions. Addi ionally, he wid h o M5 has a la ge in luence on he pe o mance
o his ec i ie because he ol age d op is mainly a ec ed by his pa ame e due o he
Senso s 2021,21, 6883 5 o 13
in e nal on- esis ance. Consequen ly, since he ga e capaci ance o M5 depends on he
wid h, he u n on/o ime o he ansis o will also be a ec ed by his pa ame e . In
addi ion, he DSB echnique, composed o M6 and M8, is deployed o educe he leakage
cu en h ough he bulk e minal o M5 by connec ing i o he highe po en ial (
Vn c
o
V ec
). Ano he ad an age o his echnique is elimina ing he body e ec o M5, which
educes he ec i ie ol age d op. Bo h M6 and M8 can be small in size since only a e y
low cu en lows h ough hem du ing he s a -up phase.
To assu e a sa e s a -up o M5, a bypass PMOS diode (M10) was connec ed in pa allel.
This ansis o makes he ac i e diode mo e obus by p e en ing i om leakage cu en in
he sub ac ion ha induces la ch-up. A e he s a -up phase, he bypass diode always
ope a es in he cu -o egion.
3.3. Th eshold Cancella ion Ci cui
In o de o educe he h eshold ol age e ec on M5, a boo s ap echnique is used
by a aching he capaci o
C1
o he ou pu e minal. When he
VNVC
is highe han he
ou pu ol age
V ec
, M5 is u ned ON, since
VSG5
is no longe lowe han
VTH5
, and hus
i can be de ined in (1). Ne e heless, because M5 is ope a ing in he deep- iode egion
due o
VSD5
2
·(VSG5−|VTH5|)
,
VSG5
can also be de ined acco ding o he on- esis ance
equa ion, see (2).
VSG5=VNVC −VCAP (1)
VSG5=1
µp·Cox·W5/L5·RSD5
+|VTH5|(2)
He e,
µp
is he ca ie mobili y,
Cox
is he oxide capaci ance,
W5/L5
is he aspec a io
o ansis o M5, and VTH5is i s espec i e h eshold ol age.
The boo s apping capaci o (
C1
) is cha ged up h ough an auxilia y diode-connec ed
PMOS ansis o M7, and i main ains a alue when he ec i ie is unde he s eady-s a e
egime. A his ime, because
C1
is discha ging,
VCAP
is one diode o wa d-bias ol age
(
VTH7
) bellow
V ec
due o M7 is being in he sa u a ion egion. Thus, he ol age held on
he boo s apping capaci o can be de ined as:
VCAP =V ec −|VTH7|(3)
VSG5
and
VCAP
om (2) and (3), espec i ely, can be eplaced in (1), which means ha
V ec can now be de ined acco ding o he ollowing equa ion:
V ec =VNVC −(|VTH5|−|VTH7|)−1
µp·Cox·W5/L5·RSD5
(4)
Acco ding o (4), he ec i ied signal is highly in luenced by he size o M5 and he
h eshold ol age o bo h M5 and M7, and hus i is i al o manage hese pa ame e s o
enhance he ou pu signal ol age. The implemen ed h eshold cancella ion ci cui educes
he ol age d op o he main pass ansis o M5 by lowe ing he h eshold ol age e ec .
Addi ionally, he size o he boo s ap capaci o is an impo an design conce n o he
implemen a ion o he p oposed ec i ie . In eg a ed capaci o s consume a la ge a ea on he
chip when s anda d CMOS p ocesses a e used [
24
]. The e o e,
C1
was se a 200 F no only
o educe he co esponden a ea on he die bu also o ha e a as e cha ging/discha ging
ime. Consequen ly, his low boo s ap capaci ance allows a lowe ga e ol age o M5 a he
ON s a e. Due o he educ ion o i s in e nal sou ce o d ain esis ance, he ol age d op is
dec eased. The e e se leakage cu en du ing he OFF s a e will be a oided because
VSG5
is educed. Mo eo e , i is necessa y o ha e an auxilia y ci cui o hold he
VCAP
node
when M5 is OFF, and o discha ge i a he opposi e s a e.
The boo s apping capaci o is used o educe he h eshold ol age e ec o M5.
Howe e , an inc ease in i s on- esis ance can be no iced due o he educ ion o
VSG5
. Thus,
a conduc ion pa h needs o be gene a ed o discha ge he ga e o M5 du ing he ON s a e,

Senso s 2021,21, 6883 6 o 13
which will lead o a u he inc ease o
VSG5
. The p oposed AVC is composed o NMOS M9
and a compa a o CMP ha d i es i s ga e. When
VNVC
is highe han he ou pu ol age
V ec
, he compa a o CMP should immedia ely u n on M9 o p o ide a discha ge pa h
o he
VCAP
node. Consequen ly, i will u n on he main pass ansis o M5 wi h a low
on- esis ance. Because he la ge size o M5 inc eases he ga e capaci ance, he AVC mus
ha e a as e bias signal con ol o swi ch he discha ge pa h o he ga e node (
VCAP
). Thus,
he compa a o mus be designed o a end o hese demands.
Figu e 2shows he p oposed wo-inpu common ga e compa a o . This compa a o
is composed o a cu en mi o s age o make he compa ison, plus an in e e block
o bias he ga e o M9. E en i he ansis o o he cu en mi o should be as small
as possible o educe he cu en consump ion o he compa a o , he size o M12 and
M15 mus be ca e ully chosen o manage he delay, and consequen ly, he e e se leakage
cu en in M5. These wo ansis o s canno ha e he same W/L a io as M11 and M14.
O he wise, his would gene a e a delay caused by he in e e ’s ga e capaci ance’s low
cha ging/discha ging ime. Addi ionally, hey canno be much la ge han he o he
ansis o s because o he educed ime ha M5 would be ON, which would lead o a
PCE educ ion. The e o e, M12 and M15 only need o be sligh ly highe o p o ide he
equi ed cha ging/discha ging ime o educe he delay o he o e all compa a o . Table 1
summa izes he dimension alues o he p oposed ec i ie ci cui .
Senso s 2021, 21, x FOR PEER REVIEW 6 o 14
a oided because 𝑉 is educed. Mo eo e , i is necessa y o ha e an auxilia y ci cui o
hold he 𝑉 node when M5 is OFF, and o discha ge i a he opposi e s a e.
The boo s apping capaci o is used o educe he h eshold ol age e ec o M5.
Howe e , an inc ease in i s on- esis ance can be no iced due o he educ ion o 𝑉. Thus,
a conduc ion pa h needs o be gene a ed o discha ge he ga e o M5 du ing he ON s a e,
which will lead o a u he inc ease o 𝑉. The p oposed AVC is composed o NMOS
M9 and a compa a o CMP ha d i es i s ga e. When 𝑉 is highe han he ou pu ol -
age 𝑉
, he compa a o CMP should immedia ely u n on M9 o p o ide a discha ge
pa h o he 𝑉 node. Consequen ly, i will u n on he main pass ansis o M5 wi h a
low on- esis ance. Because he la ge size o M5 inc eases he ga e capaci ance, he AVC
mus ha e a as e bias signal con ol o swi ch he discha ge pa h o he ga e node (𝑉).
Thus, he compa a o mus be designed o a end o hese demands.
Figu e 2 shows he p oposed wo-inpu common ga e compa a o . This compa a o
is composed o a cu en mi o s age o make he compa ison, plus an in e e block o
bias he ga e o M9. E en i he ansis o o he cu en mi o should be as small as pos-
sible o educe he cu en consump ion o he compa a o , he size o M12 and M15 mus
be ca e ully chosen o manage he delay, and consequen ly, he e e se leakage cu en in
M5. These wo ansis o s canno ha e he same W/L a io as M11 and M14. O he wise,
his would gene a e a delay caused by he in e e ’s ga e capaci ance’s low cha ging/dis-
cha ging ime. Addi ionally, hey canno be much la ge han he o he ansis o s because
o he educed ime ha M5 would be ON, which would lead o a PCE educ ion. The e-
o e, M12 and M15 only need o be sligh ly highe o p o ide he equi ed cha ging/dis-
cha ging ime o educe he delay o he o e all compa a o . Table 1 summa izes he di-
mension alues o he p oposed ec i ie ci cui .
Figu e 2. Schema ic o he wo-inpu common ga e compa a o CMP.
Table 1. Ci cui ansis o sizes.
Uni Size (µm/µm) Mul iply Fac o
M1/2/3/4 100/0.13 100
M5 100/0.13 50
M6/7/10/11/13/14/16 0.28/0.13 1
M7/9 20/0.13 1
M11/12 0.34/0.13 1
Figu e 2. Schema ic o he wo-inpu common ga e compa a o CMP.
Table 1. Ci cui ansis o sizes.
Uni Size (µm/µm) Mul iply Fac o
M1/2/3/4 100/0.13 100
M5 100/0.13 50
M6/7/10/11/13/14/16 0.28/0.13 1
M7/9 20/0.13 1
M11/12 0.34/0.13 1
4. Resul s and Discussion
The simula ion expe imen s we e ca ied ou using Cadence Vi uoso Analog Design
En i onmen wi h a 130 nm CMOS p ocess. The espec i e physical layou o he CMOS
ec i ie is p esen ed in Figu e 3. To eplica e he ou pu beha io o he ene gy ha es e ,
he de aul inpu sinusoidal ol age ampli ude and equency used in he simula ions
we e 600 mV and 3.2 kHz, espec i ely. Th oughou mos o he es s,
CLOAD
and
RLOAD
Senso s 2021,21, 6883 7 o 13
we e se a 2
µ
F and 5.5 k
Ω
o simula e he capaci ance o he s o ing capaci o and he
impedance o he elec onics o be powe ed, espec i ely.
Senso s 2021, 21, x FOR PEER REVIEW 7 o 14
4. Resul s and Discussion
The simula ion expe imen s we e ca ied ou using Cadence Vi uoso Analog Design
En i onmen wi h a 130 nm CMOS p ocess. The espec i e physical layou o he CMOS
ec i ie is p esen ed in Figu e 3. To eplica e he ou pu beha io o he ene gy ha es e ,
he de aul inpu sinusoidal ol age ampli ude and equency used in he simula ions
we e 600 mV and 3.2 kHz, espec i ely. Th oughou mos o he es s, 𝐶 and 𝑅
we e se a 2 µF and 5.5 kΩ o simula e he capaci ance o he s o ing capaci o and he
impedance o he elec onics o be powe ed, espec i ely.
Figu e 3. Physical layou o he p oposed CMOS ec i ie .
4.1. T ansien Beha io
The ansien pe o mance o he ou pu ol age, in bo h s ages, is displayed in Figu e
4. The i s s age pe o ms he ull-wa e ec i ica ion by con e ing he nega i e inpu
ol ages (𝑉) in o posi i e ones (𝑉). The ol age d op on his s age is a ound 1 mV,
whe eas he o al ol age d op on he ci cui is a ound 12 mV, which is possible due o
he educ ion o he in e nal esis ance o he main pass ansis o M5. The achie ed ol -
age d op is c ucial o enhance he ou pu ol age ac oss he load.
Figu e 4. Simula ed wa e o ms o he ec i ie o R =5.5 kΩ and C =2 µF.
Figu e 3. Physical layou o he p oposed CMOS ec i ie .
4.1. T ansien Beha io
The ansien pe o mance o he ou pu ol age, in bo h s ages, is displayed in
Figu e 4
. The i s s age pe o ms he ull-wa e ec i ica ion by con e ing he nega i e
inpu ol ages (
VIN
) in o posi i e ones (
VNVC
). The ol age d op on his s age is a ound
1 mV, whe eas he o al ol age d op on he ci cui is a ound 12 mV, which is possible due
o he educ ion o he in e nal esis ance o he main pass ansis o M5. The achie ed
ol age d op is c ucial o enhance he ou pu ol age ac oss he load.
Senso s 2021, 21, x FOR PEER REVIEW 7 o 14
4. Resul s and Discussion
The simula ion expe imen s we e ca ied ou using Cadence Vi uoso Analog Design
En i onmen wi h a 130 nm CMOS p ocess. The espec i e physical layou o he CMOS
ec i ie is p esen ed in Figu e 3. To eplica e he ou pu beha io o he ene gy ha es e ,
he de aul inpu sinusoidal ol age ampli ude and equency used in he simula ions
we e 600 mV and 3.2 kHz, espec i ely. Th oughou mos o he es s, 𝐶 and 𝑅
we e se a 2 µF and 5.5 kΩ o simula e he capaci ance o he s o ing capaci o and he
impedance o he elec onics o be powe ed, espec i ely.
Figu e 3. Physical layou o he p oposed CMOS ec i ie .
4.1. T ansien Beha io
The ansien pe o mance o he ou pu ol age, in bo h s ages, is displayed in Figu e
4. The i s s age pe o ms he ull-wa e ec i ica ion by con e ing he nega i e inpu
ol ages (𝑉) in o posi i e ones (𝑉). The ol age d op on his s age is a ound 1 mV,
whe eas he o al ol age d op on he ci cui is a ound 12 mV, which is possible due o
he educ ion o he in e nal esis ance o he main pass ansis o M5. The achie ed ol -
age d op is c ucial o enhance he ou pu ol age ac oss he load.
Figu e 4. Simula ed wa e o ms o he ec i ie o R =5.5 kΩ and C =2 µF.
Figu e 4. Simula ed wa e o ms o he ec i ie o RLOAD =5.5 kΩand CLOAD =2µF.
Figu e 5shows he VCE beha io e sus he inpu ol age ampli ude o di e en
RLOAD
alues. I is possible o obse e ha he p oposed ec i ie can wo k e icien ly o
an inpu ol age ange om 0.45 V o 1 V o di e en ohmic loads, wi h a VCE a ying
be ween 96% and 99%. Fo an inpu ol age lowe han 0.4 V, he VCE sha ply dec eases
because he NVC ansis o s will en e he sub h eshold egion o e en cu -o . Mo eo e , i
can be no iced ha he ec i ie VCE is highe o la ge load esis o s, as would be expec ed.
Senso s 2021,21, 6883 8 o 13
Senso s 2021, 21, x FOR PEER REVIEW 8 o 14
Figu e 5 shows he VCE beha io e sus he inpu ol age ampli ude o di e en
𝑅 alues. I is possible o obse e ha he p oposed ec i ie can wo k e icien ly o
an inpu ol age ange om 0.45 V o 1 V o di e en ohmic loads, wi h a VCE a ying
be ween 96% and 99%. Fo an inpu ol age lowe han 0.4 V, he VCE sha ply dec eases
because he NVC ansis o s will en e he sub h eshold egion o e en cu -o . Mo eo e ,
i can be no iced ha he ec i ie VCE is highe o la ge load esis o s, as would be ex-
pec ed.
Figu e 5. VCE e sus inpu ol age ampli ude simula ed o di e en ohmic loads.
4.2. Re e se Leakage Cu en Analysis
The e e se leakage cu en analysis is one o he mos impo an analyses o make
in CMOS ec i ie s because i a ec s he powe e iciency o he o e all sys em. This e-
e se leakage cu en is dependen on he delay o he compa a o and, consequen ly, o
he discha ging pa h o he ac i e diode p o ided by he AVC. The e o e, he analysis o
he ansien pe o mance o he compa a o is shown in Figu e 6. I p esen s he ou pu
ol age o he compa a o (𝑉), he inpu and ou pu ol age o he ac i e diode used o
pe o m he compa ison, he ga e ol age o M5 (𝑉), and he cu en ha lows h ough
he ac i e diode (𝐼). As can be obse ed, he compa a o immedia ely u ns on he ga e
o he AVC ansis o o c ea e he discha ge pa h when 𝑉 exceeds 𝑉
. A his s age,
he cu en is lowing h ough M5, and 𝑉 is low, which leads o a low ol age d op
because 𝑉 is high. When 𝑉 d ops below 𝑉
, he compa a o hen quickly u ns o
he AVC, and consequen ly he ac i e diode. Thus, he p oposed s uc u e does no exhibi
e e se leakage cu en ha would deg ade he PCE o he p oposed ec i ie .
Figu e 5. VCE e sus inpu ol age ampli ude simula ed o di e en ohmic loads.
4.2. Re e se Leakage Cu en Analysis
The e e se leakage cu en analysis is one o he mos impo an analyses o make in
CMOS ec i ie s because i a ec s he powe e iciency o he o e all sys em. This e e se
leakage cu en is dependen on he delay o he compa a o and, consequen ly, o he
discha ging pa h o he ac i e diode p o ided by he AVC. The e o e, he analysis o he
ansien pe o mance o he compa a o is shown in Figu e 6. I p esen s he ou pu
ol age o he compa a o (
VCMP
), he inpu and ou pu ol age o he ac i e diode used o
pe o m he compa ison, he ga e ol age o M5 (
VCAP
), and he cu en ha lows h ough
he ac i e diode (
IM5
). As can be obse ed, he compa a o immedia ely u ns on he ga e
o he AVC ansis o o c ea e he discha ge pa h when
VNVC
exceeds
V ec
. A his s age,
he cu en is lowing h ough M5, and
VCAP
is low, which leads o a low ol age d op
because
VSG
is high. When
VNVC
d ops below
V ec
, he compa a o hen quickly u ns o
he AVC, and consequen ly he ac i e diode. Thus, he p oposed s uc u e does no exhibi
e e se leakage cu en ha would deg ade he PCE o he p oposed ec i ie .
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Figu e 6. Simula ed compa a o beha io in s eady s a e o R = 500 Ω and C =2 µF.
4.3. Powe E iciency
The simula ed powe e iciency e sus inpu ol age ampli ude o di e en load e-
sis o s is p esen ed in Figu e 7. The de ini ion o PCE is shown in (5):
𝑃𝐶𝐸 = 𝑉(𝑡)∙𝐼
(𝑡)𝑑𝑡
  

𝑉(𝑡)∙𝐼
(𝑡)𝑑𝑡
  

∙ 100% (5)
Figu e 7. PCE e sus inpu ol age ampli ude simula ed o di e en alues o R.
The maximum PCE alue o 94% can be ound a 0.6 V o a R o 500 Ω. When
𝑉 is lowe han his ange, he PCE sha ply dec eases due o he low ol age e iciency,
as no ed in Sec ion 4.1. Thus, he e iciency o he ec i ie is poo in he ul a-low ol age
ange. Addi ionally, he PCE ends o dec ease o highe inpu ol ages because he
powe losses a e mainly concen a ed in he compa a o . Howe e , his case is no signi -
ican o ohmic loads lowe han 15.5 kΩ. Mo eo e , o highe load esis o s, he PCE
ends o dec ease due o he educ ion o he ou pu cu en , whe eas he bias cu en ha
comes om he ol age sou ce keeps almos cons an . Rega dless, om 0.45 V o 1 V, he
Figu e 6. Simula ed compa a o beha io in s eady s a e o RLOAD =500 Ωand CLOAD =2µF.
Senso s 2021,21, 6883 9 o 13
4.3. Powe E iciency
The simula ed powe e iciency e sus inpu ol age ampli ude o di e en load
esis o s is p esen ed in Figu e 7. The de ini ion o PCE is shown in (5):
PCE =R +T
VOUT( )·IOUT( )d
R +T
VIN( )·IIN( )d ·100%. (5)
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Figu e 6. Simula ed compa a o beha io in s eady s a e o R = 500 Ω and C =2 µF.
4.3. Powe E iciency
The simula ed powe e iciency e sus inpu ol age ampli ude o di e en load e-
sis o s is p esen ed in Figu e 7. The de ini ion o PCE is shown in (5):
𝑃𝐶𝐸 = 𝑉(𝑡)∙𝐼
(𝑡)𝑑𝑡
  

𝑉(𝑡)∙𝐼
(𝑡)𝑑𝑡
  

∙ 100% (5)
Figu e 7. PCE e sus inpu ol age ampli ude simula ed o di e en alues o R.
The maximum PCE alue o 94% can be ound a 0.6 V o a R o 500 Ω. When
𝑉 is lowe han his ange, he PCE sha ply dec eases due o he low ol age e iciency,
as no ed in Sec ion 4.1. Thus, he e iciency o he ec i ie is poo in he ul a-low ol age
ange. Addi ionally, he PCE ends o dec ease o highe inpu ol ages because he
powe losses a e mainly concen a ed in he compa a o . Howe e , his case is no signi -
ican o ohmic loads lowe han 15.5 kΩ. Mo eo e , o highe load esis o s, he PCE
ends o dec ease due o he educ ion o he ou pu cu en , whe eas he bias cu en ha
comes om he ol age sou ce keeps almos cons an . Rega dless, om 0.45 V o 1 V, he
Figu e 7. PCE e sus inpu ol age ampli ude simula ed o di e en alues o RLOAD
The maximum PCE alue o 94% can be ound a 0.6 V o a
RLOAD
o 500
Ω
. When
Vin
is lowe han his ange, he PCE sha ply dec eases due o he low ol age e iciency,
as no ed in Sec ion 4.1. Thus, he e iciency o he ec i ie is poo in he ul a-low ol age
ange. Addi ionally, he PCE ends o dec ease o highe inpu ol ages because he powe
losses a e mainly concen a ed in he compa a o . Howe e , his case is no signi ican
o ohmic loads lowe han 15.5 k
Ω
. Mo eo e , o highe load esis o s, he PCE ends o
dec ease due o he educ ion o he ou pu cu en , whe eas he bias cu en ha comes
om he ol age sou ce keeps almos cons an . Rega dless, om 0.45 V o 1 V, he powe
e iciency o low ohmic loads is conside ed as being good o his applica ion. Addi ionally,
he in luence o he wid h o he NVC s age (M1–M4) and o M5 in bo h PCE and VCE can
be obse ed in Figu e 8. Fo his simula ion es , he wid h o each s age was indi idually
a ied while he o he was kep cons an . This igu e shows ha he VCE and PCE ea u es
o bo h s ages a e a hei maximum poin o a wid h o 100
µ
m because he on- esis ance
o his ansis o is di ec ly in luenced by he
W/L
a io o he MOSFET. E en i he ga e
capaci ance o M5 inc eases wi h he size, Figu e 6shows ha he h eshold cancella ion
ci cui can d i e his la ge ansis o .
Figu e 9shows he powe e iciency e sus inpu ol age ampli ude o di e en
inpu equencies. The load capaci o alue was adap ed o keep he ou pu ipple ol age
small depending on he inpu equency. I is possible o obse e ha he p oposed
ec i ie can achie e a high-powe e iciency o low inpu equencies in he ope a ing
ol age ange. Howe e , when he inpu ol age and equency a e high, he powe
e iciency ends o sligh ly dec ease due o he powe losses in he NVC and in he ac i e
diode, which in his case i is caused by he ou pu signal o he compa a o being oo
as . Consequen ly, he wo king ime o ansis o M5 will be oo sho , which educes
he amoun o powe con e ed o he load. None heless, a ypical ene gy ha es ing
equencies, he pe o mance o he CMOS ec i ie o he p esen ed equency ange is
sui able o his applica ion.