the direct determination of mosfet parameters from the id ... · * from yannis tsividis, operation...
TRANSCRIPT
The direct determination of The direct determination of MOSFET parameters from the IMOSFET parameters from the IDD
versus Vversus VSS curve at low Vcurve at low VDSDS
Carlos Galup-Montoro, Márcio Bender Machado,
Thiago de Oliveira, Márcio Cherem Schneider Thiago de Oliveira, Márcio Cherem Schneider
Federal University of Santa CatarinaBrazil
MOSMOS--AK Workshop, AK Workshop, DecemberDecember 20102010
ContentsContents
11 - Threshold Voltage definitions
22 - Determination of MOSFET parameters from ID
x VS
curve, (channel_conductance)/Id method
33 - Comparison with gm/Id method
222MOS-AK Workshop, December 2010
44 - Applications of the threshold voltage
determinations
55 - Conclusions
Near the threshold condition ( moderate inversion), both the drift and
diffusion transport mechanisms are important.
Threshold voltage (VT)Threshold voltage (VT)
333MOS-AK Workshop, December 2010
IDS1= Drift component
IDS2= Diffusion component
* from Yannis Tsividis, Operation and Modeling of The MOS transistor, MCGraw-Hill
No critical point can be directly identified
ClassicalClassical threshold voltage (VT) definitionthreshold voltage (VT) definition
Classical (surface potential based) definition of threshold:Classical (surface potential based) definition of threshold:
CFS V+= φφ 2Where :φφφφS - surface potential for VG=VT
φφφφF - Fermi potential in the substrate
VC - channel potential
In principle the direct determination of the threshold voltage
is possible
444MOS-AK Workshop, December 2010
is possible
1)1) calculate the saturation drain current IDTh
for
22)) inject IDTh
in the transistor and measure VG
= VT
DrawbacksDrawbacks
- geometrical (W, L) and technological parameters ( mobility, oxide
thickness,.. ) are needed to calculate IDTh
- the transistor operates in the saturation region where several
secondary effects are relevant
CFS V+= φφ 2
For a MOSFET the current defined threshold corresponds to an
inversion charge density equal to the thermal charge density ( the
effective channel capacitance per unit area times the thermal voltage).
diffdrift II =
Current based threshold definition Current based threshold definition
555MOS-AK Workshop, December 2010
where n is the slope factor
tOXI nCQ φ'' −=For a bulk MOSFET
Relationship between threshold voltages Relationship between threshold voltages
666MOS-AK Workshop, December 2010
‘Ideal’ threshold voltage extraction ‘Ideal’ threshold voltage extraction procedureprocedure
• No parameters are needed to calculate the
threshold current
• The transistor operates at low current levels
and in the linear region to minimize series and in the linear region to minimize series
resistances and short channel effects
gm/Id curve in the linear regiongm/Id curve in the linear region
777MOS-AK Workshop, December 2010
VT determination from gm/Id VT determination from gm/Id curve in the linear regioncurve in the linear region
• Transconductance-to-current ratio for VDS
≅ ϕt/2 and V
S=0.
Threshold gm
/ID
≅≅≅≅ 0.5 (gm
/ID)
max
Drawback (gm/ID)max
has some dependence on VG
888MOS-AK Workshop, December 2010
The new (channel conductance GThe new (channel conductance Gn0n0/Id) /Id) methodologymethodology
Direct determination of MOSFET parameters from the ID
versus VS curve at low VDS
VDS=ϕ
t/2
2
x 10-4
x 10-4
[A]
999MOS-AK Workshop, December 2010
XDS VVV ∆=∆=∆
nomdmsX
D GggV
I=+−=
∂∂
VG
VX
0 0.1 0.2 0.3 0.4 0.5 0.6
0
1
VX [V]
I D [A
]
VX
[V]I D[A]
The Gn0/Id methodologyThe Gn0/Id methodology
Transistor operation:Transistor operation:
• low VDS
• weak and moderate inversion
• fixed VG
Negligible effects of :Negligible effects of :
101010MOS-AK Workshop, December 2010
Negligible effects of :Negligible effects of :
• series resistances
• field dependent mobility
• slope factor variation
• channel length modulation
The Gn0/Id methodology The Gn0/Id methodology –– extract Vextract VTT and Iand ISS
When if =3 → VP=VS=VX
From transistor model
From UICM
( ) ( )rfD
n
rftD
n
iiI
G
iiI
G
+++
=
+++−=
11
2
11
2
min
00
φ
( )112
)()( −+= dft
Sdms i
Ig
φ
( )rfSD iiII −=L
WnCI t
OXS 2'
2φµ=
( )11ln21)( −++−+=− DSP ii
VV
111111MOS-AK Workshop, December 2010
When if =3 → VP=VS=VX
for if = 3 and
VDS = φφφφt /2
we have ir = 2.12 VP = VX
When
min
00 *53.0
=
D
n
D
n
I
G
I
G
andVG
VDS
=ϕt/2
VX
( )11ln21 )()( −++−+= rfrft
iiφ
-30
-25
-20
-15
-10
-5
0
Gno
/I D [1
/V]
min
00 53.0
=
D
n
D
n
I
G
I
G
V = V
The Gn0/Id methodology The Gn0/Id methodology –– extract Vextract VTT and Iand ISS
121212MOS-AK Workshop, December 2010
0 0.1 0.2 0.3 0.4 0.5
-40
-35
VX [V]
VP
= VX
VT0 = - nVP + VG
IS = ID
When
min
00 *53.0
=
D
n
D
n
I
G
I
Gand
The Gn0/Id methodology The Gn0/Id methodology –– extract extract pinchpinch--offoff
voltage voltage VVPP
and and slope factor slope factor nnVP[V]
slopefactor(n)
BSIM simulation
0 0.1 0.2 0.3 0.4 0.50
1
2
x 10-4
vg=0.7V
vg=0.75V
vg=0.8Vvg=0.85V
vg=0.9V
131313MOS-AK Workshop, December 2010
measuring ID x VS for different VG values
VG
[V]VG
[V]
VX[V]
I D[A]
Gn0/Id x gm/Id methodsGn0/Id x gm/Id methods
|Gn0/I
D|
gm/I
Dgm/I
D
|Gn0/I
D||G
n0/I
D|
Transconductance
/ID[1/V]
141414MOS-AK Workshop, December 2010
Transconductance
ID
[A]
Gn0/Id x gm/Id methodsGn0/Id x gm/Id methods
IISS
L mask (W/L=100) 0.2 µm 0.3 µm 0.4 µm 0.5 µm 0.6 µm 0.8 µm 2.0 µm
IS
(µA) gm/ID
23.82 18.21 16.19 15.67 15.54 15.94 16.62
IS
(µA) Gn0/ID 21.47 15.21 13.27 13.53 13.41 13.72 14.65
VVT0T0
L mask (W/L=100) 0.2 µm 0.3 µm 0.4 µm 0.5 µm 0.6 µm 0.8 µm 2.0 µm
VT
(mV) gm/ID
514 499 494 488 484 478 456
VT
(mV) Gn0/ID
515 495 490 486 481 475 455
0.18 µm technology
IS
when VGS
≈VT0
151515MOS-AK Workshop, December 2010
0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2450
460
470
480
490
500
510
520
Lmask
[µm]
VT [m
V]
gm/Id method
Gno/Id method
0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 212
14
16
18
20
22
24
Lmask
[µm]
I S [µ
A]
gm/Id method
Gno/Id method
ApplicationsApplications
•• Transistor aging (or electrical stress)
• Matching assessment
• Temperature drift characterization
Applications using VT extractionApplications using VT extraction
161616MOS-AK Workshop, December 2010
• Temperature drift characterization
• Radiations effects on MOS transistor
ApplicationsApplications
11- Extract IS and VT in a non-noisy environment using an accurate method (gm/Id or Gn0/Id)
VV −22- Extract VT in a real environment considering Id=3*Is (if =3) in a
171717MOS-AK Workshop, December 2010
n
VVVP TG 0−
=
VP
= 0 VG
= VT0
VP
[V]
VG[V]
VG
VS
3IS
considering Id=3*Is (if =3) in a
saturated transistor
From UICM
when if = 3, VP
= VS
Example of HCI stress measurement using VT variation
ApplicationsApplications
[mV]
181818MOS-AK Workshop, December 2010
ΔVT[m
V]
Time [Seconds]
ConclusionsConclusions
• New procedure for direct determination of the threshold voltage and some other important electrical parameters with minimum influence of second order effects.
• The threshold voltage is determined at a constant gate-to-substrate voltage, at a low drain-to-source voltage and with transistor operation in the weak and moderate inversion transistor operation in the weak and moderate inversion regions.
• Under these operating conditions the effects of series resistances, mobility and slope factor variations, and channel length modulation are practically negligible, allowing a direct determination of the threshold voltage and of the DIBL effect.
191919MOS-AK Workshop, December 2010