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An Analytical Subthreshold Drain Current Model for Pocket Implanted Nano Scale n-MOSFET Muhibul Haque Bhuyan 1 , Quazi D. M. Khosru 2 Department of Electrical and Electronic Engineering (EEE) Bangladesh University of Engineering and Technology (BUET), Dhaka 1000, Bangladesh E-mail: 1 [email protected] and 2 [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

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Page 1: An Analytical Subthreshold Drain Current Model for · PDF fileAn Analytical Subthreshold Drain Current Model for ... low-power applications, such as when the MOSFET is used as a

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

Page 2: An Analytical Subthreshold Drain Current Model for · PDF fileAn Analytical Subthreshold Drain Current Model for ... low-power applications, such as when the MOSFET is used as a

M. H. Bhuyan

appropriate boThe effective claw. Finally, conventional dshow that thewell for variowell as variouusefulness of onext generatio

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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.

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mplantation, whct (RSCE), is d

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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⎛ ⎞− +⎜ ⎟

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profiles at the 20, 25 and 301018 cm-3.

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pm pN LL

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OLD CURREsion equation, FET can be wri

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sn

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d dn Ddx d

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ψμ

ψ

+

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=

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

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e surface poteient and electas follows

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ential, tronic

( ) 5

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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

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=

= 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

Page 4: An Analytical Subthreshold Drain Current Model for · PDF fileAn Analytical Subthreshold Drain Current Model for ... low-power applications, such as when the MOSFET is used as a

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

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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.

REFERENCES [1] S. M. Sze, “Physics of Semiconductor Devices,” 2nd

Edition, John Wiley and Sons, New York, ch. 8, (1981). [2] M. Miura-Mattausch, M. Suetake, H. J. Mattausch, S.

Kumashiro, N. Shigyo, S. Oganaka and N. Nakayama, “Physical modeling of the reverse short channel effect for circuit simulation,” IEEE Transaction on Electron Devices, vol. 48, pp. 2449-2452, Oct. (2001).

[3] M. Orlowski, C. Mazure and F. Lau, “Submicron short channel effects due to gate reoxidation induced lateral interstitial diffusion,” IEEE IEDM Technical Digest, p. 632, (1987).

[4] M. Nishida and H. Onodera, “An anomalous increase of threshold voltage with shortening the channel lengths for deeply boron-implanted n-channel MOSFETs,” IEEE Trans. on Electron Devices, vol. 48, pp. 1101, (1981).

[5] K. Y. Lim and X. Zhou, “Modeling of Threshold Voltage with Non-uniform Substrate Doping,” in Proc. of the IEEE Int’l Conf. on Semiconductor Electronics (ICSE’98), Malaysia, pp. 27-31, (1998).

[6] B. Yu, C. H. Wann, E. D. Nowak, K. Noda and C. Hu, “Short Channel Effect improved by lateral channel engineering in deep-submicrometer MOSFETs,” IEEE Transactions on Electron Devices, vol. 44, pp. 627-633, Apr. (1997).

[7] B. Yu, H. Wang, O. Millic, Q. Xiang, W. Wang, J. X. An and M. R. Lin, “50 nm gate length CMOS transistor with super-halo: Design, process and reliability,” IEDM Technical Digest, pp. 653-656, (1999).

[8] K. M. Cao, W. Liu, X. Jin, K. Vasant, K. Green, J. Krick, T. Vrotsos and C. Hu, “Modeling of pocket implanted MOSFETs for anomalous analog behavior,” IEEE IEDM Technical Digest, pp. 171-174, (1999).

[9] Y. S. Pang and J. R. Brews, “Models for subthreshold and above subthreshold currents in 0.1 μm pocket n-MOSFETs for low voltage applications,” IEEE Transactions on Electron Devices, vol. 49, pp. 832-839, May (2002).

[10] J. Tanaka, S. Kimura, H. Noda, T. Toyabe, and S. Ihara, “A sub-0.1 μm grooved gate MOSFET with high immunity to short channel effects,” IEEE IEDM Technical Digest, p. 537, (1993).

[11] T. N. Buti, S. Ogura, N. Rovedo, K. Tobimatsu, and C. F. Codella, “Asymmetrical halo source GOLD drain (HS-GOLD) deep-half-micron n-MOSFET design for reliability and performance,” IEEE IEDM Technical Digest, pp. 617, (1989).

[12] A. Chatterjee, J. Liu, P. K. Mozumder, M. Rodder and I. C. Chen, “Pass transistor designs using pocket implant to improve manufacturability for 256-Mbit DRAM and beyond,” IEEE IEDM Technical Digest, p. 87, (1994).

[13] H. Chen, J. Zhiao, C. S. Teng, L. Moberly and R. Lahri, “Submicron large-angle-tilt-implanted drain technology for mixed signal applications,” IEEE IEDM Technical Digest, p. 91, (1994).

[14] J.-G. Su, C.-T. Huang, S.-C. Wong, C.-C. Cheng, C.-C. Wang, H.-L. Shiang and B.-Y. Tsui, “Tilt angle effect on optimizing HALO PMOS and NMOS performance,” in Proc. of IEEE IEDM, pp. 11-14, (1997).

[15] H. S. Shin, C. Lee, S. W. Hwang, B. G. Park and H. S. Min, “Channel length independent subthreshold characteristics in submicron MOSFETs,” IEEE Electron Device Letters, vol. 19, pp. 137-139, Apr. (1998).

[16] C. S. Ho, J. J. Liou, K.-Y. Huang and C.-C. Cheng, “An analytical subthreshold current model for pocket implanted NMOSFETs,” IEEE Trans. On Electron Devices, vol. 50, pp. 1475-1479, Jun. (2003).

[17] M. H. Bhuyan and Q. D. M. Khosru, “Linear Profile Based Analytical Surface Potential Model for Pocket Implanted Sub-100 nm n-MOSFET,” Journal of Electron Devices, ISSN 1682-3427, vol. 7, pp 235-240, (2010).

[18] T. A. Fieldly and M. Shur, “Threshold voltage modeling and the subthreshold operation of short-channel MOSFETs,” IEEE Transactions on Electron Devices, vol. 40, pp. 137, Jan. (1993).

[19] M. H. Bhuyan and Q. D. M. Khosru, “Linear Pocket Profile Based Threshold Voltage Model for Sub-100 nm n-MOSFET Incorporating Substrate and Drain Bias Effects,” in Proc. of the 5th International Conference on Electrical and Computer Engineering (ICECE 2008), Dhaka, pp. 447-451, December 20-22, (2008).