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Simon Josef Thür
Semiconductors_Summary
Commits
d6056679
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Commit
d6056679
authored
1 year ago
by
Simon Josef Thür
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add SOI
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12_nanometric_mos.tex
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-1
78 additions, 1 deletion
12_nanometric_mos.tex
format.tex
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format.tex
semiconductor_summary.tex
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semiconductor_summary.tex
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12_nanometric_mos.tex
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d6056679
\section
{
Nanometric MOS
}
\ No newline at end of file
\section
{
Nanometric MOS
}
\subsection
{
Strained silicon
}
For N-MOS, increase distance between atoms,
for P-MOS, decrease the distance.
this improves mobility.
\subsection
{
Velocity saturation
}
In the case of high electric fields, the velocity of the electrons saturates (Short-Channel-Effect).
\begin{equation}
I
_
D =
\begin{cases}
W Q
_
I(x)v
_
x(x)
&
: v=
\mu
E
\\
W C
_{
ox
}
\mu
v
_{
sat
}
\left
(V
_{
GS
}
-V
_
T
\right
)
&
:
\text
{
saturation
}
\end{cases}
\end{equation}
With the `new' saturation voltage
\begin{equation}
V
_{
D,sat
}
=
\left
(V
_{
GS
}
-V
_
T
\right
)/m
\to
\sqrt
{
2v
_{
sat
}
L/m
\mu
}
\end{equation}
where
$
m
$
is a non-ideality constant.
Note that we completely lose the dependence on L for the current.
Essentially
$
\alpha
=
1
$
for complete saturation and
$
\alpha
=
2
$
for long channel:
\begin{equation}
I
_
D
\bigg
|
_{
V
_{
DS
}
=V
_{
DD
}}
\sim
(V
_{
GS
}
-V
_
T)
^
\alpha
\qquad
:
\
1<
\alpha
<2
\end{equation}
\subsection
{
Silicon-On-Insulator (SOI)
}
PD SOI:
\begin{itemize}
\item
Body thicker than channel depletion width
\item
Body voltage floating
\item
Depends on charge injected into bulk
\item
History effect changes
$
V
_
T
$
\end{itemize}
FD SOI:
\begin{itemize}
\item
Body thinner than channel depletion width
\item
Fixed body charge
\item
Fixed body voltage
\item
Hard to manufacture
\item
Not used yet
\end{itemize}
\subsubsection
{
Partially depleted SOI
}
\begin{itemize}
\item
[+]
simolar to bulk-Si
\item
[+]
no coupling
\item
[-]
SCE
\item
[-]
floating body
\item
[-]
kink effect
\item
[-]
dynamic over- undershoots
\item
[-]
self heating
\end{itemize}
\paragraph
{
Floating body effect
}
Kink effect because of impact ionization near the drain.
Holes are swept into the neutral body, collecting at the source junction.
\begin{equation}
T
_{
SOI
}
>
\sqrt
{
\frac
{
2
\varepsilon
_{
si
}
\cdot
2
\phi
_
F
}{
qN
_{
Body
}}}
\end{equation}
\subsubsection
{
Fully depleted SOI
}
\begin{itemize}
\item
[+]
Excellent ctrs of SCE
\item
[+]
no floating body
\item
[+]
Less parasitic capacitance
\item
[+]
less junction leakage
\item
[+]
Quasi-ideal subthreshold swing
\item
[-]
$
V
_
T
$
sensitive to SOI thickness
\item
[-]
Self heating
\end{itemize}
\subsubsection
{
Why bother with SOI
}
By reducing the thickness of the channel, we reduce the SCE,
since the gate can better control the channel.
\todo
[inline]
{
Subthreshold swing
}
\ No newline at end of file
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format.tex
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@@ -45,6 +45,11 @@
within=section,
]
{
circuit
}
\usepackage
{
enumitem
}
\setlist
[itemize]
{
noitemsep
}
\usepackage
{
url
}
\usepackage
[pdfusetitle]
{
hyperref
}
\hypersetup
{
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semiconductor_summary.tex
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d6056679
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@@ -31,7 +31,8 @@
The aim of this summary is to provide a denser overview of the course material.
Specifically, it is intended to be used as a reference for the exam,
which is why it has only few remarks and focuses mainly on equations with little regard for how they were derived.
which is why it has only few remarks and focuses mainly on equations with little regard for how they were derived,
unless I found it noteworthy.
\end{titlepage}
...
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