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An Analytical Subthreshold Drain Current Model for Pocket Implanted Nano Scale n-MOSFET
Muhibul Haque Bhuyan1, Quazi D. M. Khosru2 Department of Electrical and Electronic Engineering (EEE)
Bangladesh University of Engineering and Technology (BUET), Dhaka 1000, Bangladesh E-mail: [email protected] and [email protected]
Received 8 September 2010, accepted 25 September 2010, online October 2010. Abstract: This paper presents an analytical subthreshold drain current model for pocket implanted nano scale n-MOSFET. The model is developed by using the linear pocket profiles at the source and drain edges and by solving the Poisson's equation in the depletion region at the surface with the appropriate boundary conditions at source and drain for deriving the surface potential. The model includes the effective doping concentration of the two linear pocket profiles. Electron current density is obtained from the conventional drift-diffusion equation. Integration of surface potential is obtained numerically. Effective channel thickness is obtained by applying Gauss's Law at the surface. The simulation results show that the derived subthreshold drain current model has a simple compact form that can be utilized to study and characterize the pocket implanted advanced ULSI MOS devices. Keywords: Linear Pocket Profile, Pocket Implanted MOSFET, Subthreshold Drain Current, Surface Potential, Threshold Voltage
1. INTRODUCTION As the channel length of MOSFETs is scaled down to deep-submicrometer or sub-100 nm regime, we observe the reduction of threshold voltage with the reduction of channel length due to the charge sharing between the drain/source region and the channel [1]. Also, the off-state leakage current increases due to sensitivity of the source/channel barrier to the drain potential or drain induced barrier lowering (DIBL). This effect is known as short-channel effect (SCE). This effect arises as a result of two dimensional potential distribution and high electric fields in the channel region [2]. It can be reduced or can be even reversed (then it is called reverse short channel effect or RSCE in short) by locally raising the channel doping near source and drain junctions. RSCE was originally observed in MOSFETs due to oxidation-enhanced-diffusion [3] or implant-damage-enhanced diffusion [4] which are very difficult to control. Lateral channel engineering utilizing halo or pocket implant [5-9] surrounding drain and source regions is effective in
suppressing short channel effects. The halo or pocket implant can be either symmetrical [10] or asymmetrical [11] with respect to source or drain. Reported circuit applications include a 256 M-bit DRAM [12] and mixed-signal processor [13]. In fact, this pocket implant technology is found to be very promising in the effort to tailor the short-channel performances of deep-submicron as well as sub-100 nm MOSFETs although careful tradeoffs need to be made between minimum channel length and other device electrical parameters [6]. Already few papers have been published focusing on the subthreshold behaviour of pocket implanted MOSFET [14-16]. When the gate voltage is below the threshold voltage and the semiconductor surface is in weak inversion, the corresponding drain current is called the subthreshold current. The subthreshold region is particularly important for low-voltage, low-power applications, such as when the MOSFET is used as a switch in digital logic and memory applications, because the subthreshold region describes how the switch turns on and off. In [9], models for subthreshold and above subthreshold currents in 0.1 μm pocket n-MOSFETs for low-voltage applications have been derived based on the diffusion current transport equation. But this model characterizes the localized pile-up of channel dopants as step profile. The influences of halo implant dose and tilt angle on the off-state current have been investigated by technology computer-aided design (TCAD) simulation in [14]. A channel length independent subthreshold characteristic in submicron MOSFETs has been reported by Shin et al in [15] due to the presence of localized pileup of channel dopants near the source and drain ends of the channel. An analytical subthreshold current model for pocket-implanted n-MOSFETs has been presented in [16]. But this model also characterizes the localized channel dopants as step profile. In this paper, an analytical subthreshold current model for the sub-100 nm pocket implanted n-MOSFET has been derived assuming the linear profiles of pocket doping. Here the 1-D pocket profiles across the channel have been transformed to an effective doping concentration expression, which is used in the 1-D Poisson’s equation to derive the surface potential model applying the
Journal of Electron Devices, Vol. 8, 2010, pp. 263-267
© JED [ISSN: 1682 -3427 ]
Journal of Electron Devices www.jeldev.org
M. H. Bhuyan
appropriate boThe effective claw. Finally, conventional dshow that thewell for variowell as variouusefulness of onext generatio
2. POCKEThe pocket im1 is consideresystem is showdevice dimensinterface. In thThe oxide thifixed oxide chp-type Si subsNsub = 4.2×101
source and concentration oLp = 25 nm, aof Nsd = 9.0×10
Fig. 1 Pocket im The pocket imChannel Effecboth from the the peak pocdecreases liconcentration,source and drpocket profilefrom both the as shown in Fplay importantAt the source s
( )sN x =
At the drain si
n+
n et al, Journal o
oundary conditchannel thicknthe current eqdrift-diffusion
e model predicus device and
us bias conditioour proposed mn ULSI device
T DOPINGmplanted n-MO
ed in this wown at the rightsions are meahe structure, thckness (tox) is
harge density ostrate is used 17 cm-3 with podrain side
of Npm = 1.75×and the source 020 cm-3.
mplanted n-MOS
mplantation, whct (RSCE), is d
source and drcket doping cinearly towa Nsub with a porain edges. The is to assume
source and drFig. 2. The pot role in determside, the pocke
sub pmp
xN NL
= +
de, the pocket
p-type S
of Electron De
tions at the soness is found apquation is obt
equation. Simcts subthresho
pocket profileons. It proves tmodel for circues.
G PROFILEOSFET structurork and assumt side of the stasured from the junction dept2.5 nm, and
of 1011 cm-2. Uwith doping c
ocket implantawith peak p
×1018 cm-3 and por drain dopin
SFET structure.
hich causes theone by adding rain edges. It iconcentration, ards the suocket length, Lhe basis of thee two linear drain edges acro
ocket parametemining the RSCet profile is giv
11 mp
xL
⎛ ⎞−⎜ ⎟⎜ ⎟
⎝ ⎠
profile is given
Si
n+
evices, Vol. 8, 2
ource and drainpplying Gausstained from thmulation resultld current vere parameters athe validity an
uit simulation o
E re shown in Figmed co-ordinattructure. All thhe oxide-silicoth (rj) is 25 nmit is SiO2 wit
Uniformly dopeconcentration oation both at thpocket dopinpocket length o
ng concentratio
e Reverse Shorimpurity atomis assumed thaNpm graduall
ubstrate leveLp from both the model of thdoping profileoss the channe
ers, Npm and LpCE. ven as:
( 1
n as:
2010, pp. 263-
264
n. 's
he ts ry as nd of
g. te he on m. th ed of he ng of on
rt ms at ly el he he es el p,
)
( )dN x N=
,where x rsource to direct pocassumed s
Fig. 2 Simpocket lenconcentrati The conce(2) are theand then average eequation (
effN =
When Lp <has no effcomparabpocket pro
3. SUBTBased on density Jn
,where ψselectron charge. Vt
267
1sub
p p
LN xL L
⎛−⎜⎜
⎝represents the drain. Since
cket implant asymmetric at b
mulated pocket ngths, Lp = 2ion, Npm = 1.75×
eptual pocket pen integrated mdivided by t
effective chan(3).
1 psub
LN
L⎛ ⎞− +⎜ ⎟
⎝ ⎠
<< L for long cfect on the suble with L forofile affects the
THRESHOthe drift-diffusin an n-MOSF
-n
n
J q
qD
⎛= ⎜⎝
=
ψs(x), n, Dn andensity, diffuth is the therma
thV =
1pmp
Lx NL
⎞ ⎛+ −⎟ ⎜⎟ ⎜
⎠ ⎝distance acrosthe pile-up pr
at the source aoth sides.
profiles at the 20, 25 and 301018 cm-3.
profiles given imathematicallythe channel lennel doping c
pm pN LL
+
channel devicebthreshold currr short channe subthreshold
OLD CURREsion equation, FET can be wri
-
-
sn n
sn
th
d dn Ddx d
dn dnV dx dx
ψμ
ψ
+
⎛+⎜
⎝
nd q is are thusion co-efficial and is given a
n
nDkTq μ
=
1 p p
L xL
⎞+ ⎟⎟
⎠ss the channel rofile is due tand drain side
surface for dif0 nm. Peak p
in equations (1y along the chength to derivconcentration
e then pocket prent, but when
nel device thecurrent.
ENT MODEthe electron cuitten as
dndx
n
⎞⎟⎠
⎞⎟⎠
e surface poteient and electas follows
( ) 2
from to the , it is
fferent pocket
1) and hannel ve an as in
( ) 3
profile n Lp is n the
EL urrent
( ) 4
ential, tronic
( ) 5
M. H. Bhuyan
We assume the1. At x=
potential is sψ2. At x L=
is ( )s biLψ ϕ=
substrate bias,in potential resMultiplying e
/s thVe ψ− , the transformed inboundary cond
n nJ qD= −
After solving above two bosurface potentwill be used density (Jn). The integral inequation (6) itechnique of msurface potentiFinally, the drmultiplying Jnis the multiplicchannel width
The effective cdistance fromdirection wherVth [18]. Whenof the thresholsubthreshold vertical compVth/tch, is equathe effective ch
cht =
,where VGT =factor reflectiinsulator capaand ϕF is the and is given as
n et al, Journal o
e following bo0= , i.e. at th( )0s bi BSVϕ −=
L , i.e. at the d
i BS DSV V− + , w, drain bias anspectively. equation (1) bright hand si
nto an exact deditions, we get
exp bin effN
Vϕ⎛
−⎜⎝
the 2nd order oundary condittial expression
in equation
n the denomins evaluated us
multiple segmenial model given
rain current, Ids and the channcation of effec, W) as given in
dsI J=
channel thicknm the surface
re the electrostn the gate voltald voltage, thecurrent, Isub.
ponent of the al to Qdep/εs in thannel thickne
(2 2Teff
VqN ϕ
=
= VGS – VT, θ ng the gate v
acitance and thFermi potentia
s in equation (1
FkTq
ϕ =
of Electron De
oundary conditihe source sid
S . rain end, the s
where VBS, VDS nd source/drain
by an integraide of equatioerivative and uthe following
0
1 exp
exp
BSL
th
VV
⎛−⎜⎜⎞− ⎝
⎟⎛⎠ −⎜⎝
∫
Poisson's equtions, the comn (ψs) was foun
(6) to calcula
nator of the rigsing the numernts Simpson's n in equation (s in the channenel cross-sectiotive channel thn equation (8).
n chJ Wt
ness, tch can be to the positiotatic potential age VGS is in th drain current By using Gelectric field the subthresho
ess is found as
s
/F BS GTV Vε
ϕ − +
θ is the subthrvoltage divisiohe depletion layal due to pock10).
ln eff
i
NTn
evices, Vol. 8, 2
ions: de, the surfac
urface potentiaS and ϕbi are thn junction built
ating factor oon (4) can busing the abovequation
(p
6
DS
th
s
th
VV
dxVψ
⎞⎛ ⎞⎟⎜ ⎟⎟⎝ ⎠⎠
⎞− ⎟
⎠
uation using thmplete analytica
nd in [17], anate the curren
ght hand side orical integratio1/3 rule and th
(7). el is obtained bonal area (whichickness, tch an.
( 8
obtained as thn along the yhas changed b
he close vicinitIds becomes th
Gauss' law, that the surface
old region. Thuin equation (9)
) ( 9/θ
reshold idealiton between thyer capacitanc
ket implantatio
( 10
2010, pp. 263-
265
ce
al he t-
of be ve
)6
he al
nd nt
of on he
by ch nd
)8
he y-by ty he he e, us ).
)
ty he ce on
)0
Threshold[19]. The is only vainversion
4. RESUIn order model fortypes of siFrom Fig.both RSCEthe drain length becHigher drSince at sand it lowthe adjaceIn Figs. different gbiases witobserved subthreshodrain bias subthreshoincreases.
Fig. 3 Threbiases at ze
267
d voltage, VT feffective chann
alid when –ψ(sand depletion r
ULTS ANDto verify the
r the pocket imulations wer. 3 it is observeE and SCE occinduced barri
comes shorter rain bias makehorter channel
wers the potenent diffused jun
4 (a)-(b) subgate voltages ath channel leng
that for loold current doincreases, but
old current chaThis also occu
eshold voltage vero substrate bias
for this calculnel thickness gs) + VBS < VGTregions.
D DISCUSSIe analytical suimplanted n-M
re performed. ed that as the dcur at longer chier lowering (DDIBL effect is
es the thresholl length, electrntial barrier thanction. bthreshold cuare shown for gths of 0.25 μmonger channe
oes not changefor shorter ch
anges appreciaburs due to signi
s. gate length cus.
ation is taken given in equatioT/θ, i.e., in the
IONS ubthreshold cuMOSFET, dif
drain bias increhannel length dDIBL). As chs more pronould voltage negric field is veryat separates it
urrent variationtwo different
m and 100 nmel length dee appreciably aannel length debly as the drainificant DIBL e
urves for various
from on (9) weak
urrent fferent
eases, due to hannel unced. gative. y high
from
n for drain
m. It is evice, as the evice, n bias ffect.
s drain
M. H. Bhuyan
Fig. 4 (a) Subthdrain biases of VL = 0.25 μm.
Fig. 4 (b) Subthdrain biases of VL = 100 nm. Fig. 5 shows variation with concentration.implant conceincreases for thto the additiondrain edges. Iimplant consubthreshold diminishes.
n et al, Journal o
hreshold drain cuVDS = 0.1 V and
hreshold drain cuVDS = 0.1 V and
the variation gate voltage f It is observed
entration decrehe same applie
nal doping atomIt is also obsencentration d
slope decrea
of Electron De
urrent versus gatVDS = 2.5 V wit
urrent versus gatVDS = 2.5 V wit
of subthresholfor three differe
that as the peaeases the subthed gate bias. Thms present nearrved that as th
decreases moases. Because
evices, Vol. 8, 2
te voltage for twth channel length
te voltage for twth channel length
ld drain currenent peak pockeak of the pockehreshold currenhis happens dur the source anhe peak pocke
ore then the then RSCE
2010, pp. 263-
266
wo h,
wo h,
nt et et nt ue nd et he E
Fig. 5 Subpeak pockelength, L = Fig. 6 shdifferent subthreshobias in thewith the found in tthe amousubthreshovoltage in
Fig. 6 Sudifferent sulength, L =
5. CONAn analytthin oxidehas been diffusion as the thren-MOSFEdrain biaassuming
267
threshold drain et concentration,100 nm.
hows the variasubstrate bia
old current dee negative diresubstrate bias
the literature. Bunt of currenold slope decrcreases in the s
ubthreshold draiubstrate biases,100 nm.
NCLUSIONStical subthreshe and nano sca
developed bequation and ueshold voltage
ETs incorporatas dependenctwo linear po
current versus , drain bias, VDS
ation of subthases. It is oecreases with iction. The resus effect on suBut it has alsont increment reases more rshorter channel
in current versdrain bias, VDS
S hold drain currale pocket impased on the using the surfae models for thting the effect
cies. The mocket profiles a
gate voltage forS = 2.5 V and ch
hreshold currenobserved thatincreasing subults are in consubthreshold cu
o been observeis less, and
rapidly as thel length device
sus gate voltag= 0.1 V and ch
rent model forplanted n-MOconventional
ace potential ashe pocket implts of substrateodel is devealong the chan
r three hannel
nt for t the bstrate sistent urrent d that d the e gate .
ge for hannel
r ultra SFET drift-
s well lanted e and
eloped nnel at
M. H. Bhuyan et al, Journal of Electron Devices, Vol. 8, 2010, pp. 263-267
267
the surface of the device from the source and drain edges. The effect of changing the device and pocket profiles parameters on the subthreshold current have been studied using the proposed model. The simulated results show that the proposed model predicts the subthreshold current down to 50 nm channel length. It shows similar behaviour as found in the literature. Hence this model efficiently evaluates the subthreshold drain current of scaled pocket n-MOSFETs having channel lengths in the nano scale regime.
ACKNOWLEDGMENT The authors would like to acknowledge the financial support provided by the Committee of Advanced Studies and Research, Bangladesh University of Engineering and Technology (BUET) for conducting the research work.
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