Electricity: measuring and testing – Fault detecting in electric circuits and of electric components – Of individual circuit component or element
Reexamination Certificate
2003-04-10
2004-06-15
Zarneke, David A. (Department: 2829)
Electricity: measuring and testing
Fault detecting in electric circuits and of electric components
Of individual circuit component or element
C324S765010
Reexamination Certificate
active
06750673
ABSTRACT:
BACKGROUND OF INVENTION
1. Field of the Invention
The present invention relates to a method for measuring an effective channel length of a metal-oxide-semiconductor field effect transistor (MOSFET), and more particularly, to a method for measuring the effective channel length of the MOSFET and by using three compensation factors to accuratelydetermine positions of a drain and a source of the MOSFET.
2. Description of the Prior Art
Measuring the value of an effective channel length (L
effective
) has always been one of the most important issues in the semiconductor industry to infer the characteristics of the MOSFET correctly. Furthermore, the effective channel length of the MOSFET is also one of the most important references for computer aided designing (CAD).
Please refer to 
FIG. 1
 of a cross-sectional diagram of a metal-oxide-semiconductor field effect transistor (MOSFET) 
10
. The transistor 
10
 at least comprises a gate 
12
, a source 
14
, a drain 
16
 and a silicon substrate 
18
. Wherein an effective channel length of the transistor 
10
 is defined as the length of a channel 
22
 between the source 
14
 and the drain 
16
. The value of a threshold voltage V
T 
of the transistor 
10
 is depended on the kind of the transistor 
10
, i.e., NMOS and PMOS etc. As the silicon substrate 
18
 and the source 
14
 are both grounded and a voltage greater than the threshold voltage V
T 
of the transistor 
10
 is applied to the gate 
12
 of the transistor 
10
, the channel 
22
 is formed between the source 
14
 and the drain 
16
. In this case, a 0 volts voltage is applied to the source 
14
. Moreover, if and only if the voltage applied to the gate 
12
 is less than the threshold voltage V
T 
of the transistor 
10
, the channel 
22
 vanishes, and the transistor 
10
 is in a cutoff mode and becomes non-conductive.
Normally, the method for measuring the effective channel length L
effective 
according to prior art regards the carrier mobility in the channel 
22
 as a constant for a group of devices with various channel lengths, or further simplified the carrier mobility in the channel 
22
 as a gate-bias-independent constant based on the assumption that the potential of the gate 
12
 is with a fixed value. However, this is not consistent with the reality that the Inversion carrier mobility Is determined by gate overdrive V
GT
, which is equal to the difference between the voltage of the gate V
GS 
and the threshold voltage of the transistor V
T
, i.e.,V
GT
=V
GS
−V
T 
Some techniques are thus proposed to obtain the effective channel length of the transistor more accurately by using the fixed gate overdrive V
GT 
instead of the fixed gate bias. However, the bias dependence of the drain-and-source series resistance is not taken into account. In the conventional I-V (current-voltage) approach, a channel length loss &Dgr; L and a series resistance R
DS 
are needed to be extracted simultaneously and the R
DS 
is assumed bias-independent so as to derive &Dgr; L from the linear I-V equation. Unfortunately, the R
DS 
is not bias-independent in fact, so that the accuracy of the &Dgr; L obtained is flawed.
Please refer to 
FIG. 2
 of the cross-sectional diagram of the MOSFET 
10
 shown in the 
FIG. 1
 with a corresponding photomask 
20
. The photomask 
20
 is used for forming the gate 
12
 of the transistor 
10
 by lithography and etching processes during the manufacturing of the transistor 
10
. Wherein both the source 
14
 and the drain 
16
 are formed by performing ion implantation processes. During the lithography and etching processes, a polysilicon gate lithography bias L
bias 
is formed between the photomask 
20
 and the gate 
12
 so that a length of the photomask L
mask 
is not equal to a length of the gate L
gate
. For simplicity of description, the length of the photomask 
20
 is assumed to be greater than the length of the gate 
12
 in FIG. 
2
. However, the length of the photomask L
mask 
is occasionally less than the length of the gate L
gate 
during different manufacturing processes. Alternatively, a metallurgical channel 
23
, the length of the metallurgical channel 
23
 being defined as the distance between the source 
14
 and the drain 
16
,exists in the transistor 
10
. Normally the effective channel length L
effective 
is greater than the length of the metallurgical channel 
23
.
The method for measuring the effective channel length of the transistor 
10
 according to the prior art is by way of measuring the voltage and the current between the source 
14
 and the drain 
16
. 
FIG.2
 represents a current-voltage (I-V) approach method for measuring the effective channel length. By using the flowing equation below, the effective channel equivalent resistance R
channel 
of the transistor 
10
 is obtained: 
R
channel
=
L
effective
μ
eff
⁢
C
ox
⁢
W
⁡
(
V
gate
-
V
t
)
=
V
ds
I
ds
(
1
)
wherein &mgr;
aff 
is the effective mobility of the inversion carries;
C
ox 
is the gate oxide capacitance per unit area;
W is the width of the transistor 
10
:
V
gate 
is the voltage applied to the gate 
12
;
V
t 
is the threshold voltage of the transistor 
10
;
V
ds 
is the voltage between the source 
14
 and the drain 
16
; and
I
ds 
is the current flows from the source 
14
 to the drain 
16
.
After the effective channel length L
effective 
is measured, the effective channel equivalent resistance R
channel 
is capable of be calculated according to the equation (1), and the one-dimension model of the transistor 
10
 can be established thereafter. However, the method is merely capable of measuring the effective channel length L
effective 
of the transistor 
10
 and cannot be applied to measure the polysilicon gate lithography bias L
bias
, and the overlap length 
2
L
overlap 
of the gate 
12
 and the source/drain 
14
/
16
. Consequently, the correct junction position of the source/drain 
14
/
16
 is not capable of being determined.
SUMMARY OF INVENTION
It is therefore a primary objective of the present invention to provide a method for measuring an effective channel length, a polysilicon gate lithography bias L
bias
, and an overlap length of a gate and a source/drain 
2
L
overlap
.
According to the claimed invention, a metal-oxide-semiconductor field effect transistor (MOSFET) has a silicon substrate, a gate, a drain, and a source. As the silicon substrate and the source are both grounded and a voltage greater than a threshold voltage of the transistor is applied to the gate of the transistor, a channel is formed between the drain and the source, and the transistor is operated in either an inversion mode or an accumulation mode. The method of measuring an effective channel length of the transistor comprising:
a. measuring a first unit length gate capacitance as the transistor is in the inversion mode, measuring a second unit length gate capacitance as the gate is grounded, and calculating a first compensation factor according to both the first unit length gate capacitance and the second unit length gate capacitance, wherein the first compensation factor is equal to a ratio of the first unit length gate capacitance to the second unit length gate capacitance;
b. measuring a first unit length overlap capacitance between the gate and the source/drain as the transistor is in the accumulation mode, measuring a second unit length overlap capacitance between the gate and the source/drain as the gate is grounded, and calculating a second compensation factor according to the first unit length overlap capacitance and the second unit length overlap capacitance, wherein the second compensation factor is equal to a ratio of the first unit length overlap capacitance to the second unit length overlap capacitance;
c. calculating a third compensation factor, the third compensation factor being equal to a ratio of the second compensation factor to the first compensation factor; and
d. calculating the effective channel length and an overlap length of the gate and the source/drain according to the first, second and third compensation factors.
It is an advantage of the present invention that no
Hong Gary
Huang Heng-Sheng
Lee Yueh-Hsun
Lin Shih-Chieh
Hollington Jermele M.
Hsu Winston
United Microelectronics Corp.
Zarneke David A.
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