367 lines
20 KiB
TeX
367 lines
20 KiB
TeX
\documentclass{article}
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\title{Final Project Report}
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\author{Danila Fedorin}
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\begin{document}
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\maketitle
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\tableofcontents
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\pagebreak
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\section{General Design and Considerations}
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The goal of this assignment was to create a 256-byte SRAM memory unit. In order
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to minimize wire delays, I chose to split each bit into \textbf{4 columns of 64 SRAM cells
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each}. This was motivated by the following factors:
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\begin{itemize}
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\item \emph{Larger} columns were eliminated due to the high cost of interconnect.
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Even large write blocks were not able to charge the ``far ends'' of the wire
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at shorter clock cycles. Increasing wire width did not help; although resistance
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decreased, the capacitance increased, leading to small net gains. Thus, I made
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the decision to shrink the columns as much as possible. However...
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\item \emph{Smaller} columns became a routing challenge. Even with a 4-column split,
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to properly connect each cell of the SRAM column, the SRAM cells themselves need
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to accommodate an additional three \textsc{Wl} lines. Due to the pitch requirements
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on metals three and four, this is the upper limit (for reasonably sized cells).
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Alternatives included splitting the decoder into pieces, but for large numbers
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of columns, this meant that the decoder signal traveled through significant amounts
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of wire, and was thus slower.
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\end{itemize}
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For each of the 4 64-bit columns, I attached separate read and write blocks. However,
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my placement of the write block was unorthodox. I observed that, although the write block
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is perfectly capable of quickly manipulating the bitlines close to it, the changes
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to the wires take too long to propagate through to the end. I addressed this with two separate
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changes:
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\begin{itemize}
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\item I added \textbf{additional precharge transistors} along the column, a total of 4.
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Each was sized at $10\lambda$, much like the SRAM transistors themselves. When the clock
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was low, these PMOS transistors became transparent, and helped precharge the bitlines faster.
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Doing so helped avid hysteresis. However, this did not help with writing during high clock,
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so...
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\item I also \textbf{placed the write block in the middle of the column}. This increased the distance
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between my furthest SRAM cell and the read block (since the write block now contributed to wire
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length). However, this made it significantly easier to drive the entire length of the wire,
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which was my main bottleneck. This was because the maximum distance from the write
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block to any cell in the column was halved. Since my read circuit continued to work in this
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configuration, I did not place it in the middle of the column, as that would needlessly
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increase the length of the wires.
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\end{itemize}
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%
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This led to the configuration shown in Figure \ref{fig:top-design}. To simulate this design, I \textbf{tested three configurations}:
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\begin{enumerate}
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\item A memory cell at the very top of my column, which is the furthest spot from both the read and write.
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This is the simulation in the figure.
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\item A memory cell in the middle of my column, in the same place as the write block. Since the write block
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has brief ``false starts'', this test was to ensure that the read block can still pick up data
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despite the write block's misfires.
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\item A memory cell at the very bottom of my column. This area has additional capacitance from the read block;
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it thus takes longer to charge up, and tends to be the first spot where writes fail.
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circuit.
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%
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\end{enumerate}
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I also split the wire into 4 equally-sized fragments, each with resistance $\frac{R}{4}$ and
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capacitance $\frac{C}{4}$. Between each fragment, I added the aforementioned $10\lambda$ precharge
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transistors, as well as 16 always-off $5\lambda$ transistors, which simulated the remaining memory cells.
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I also placed \textsc{Din}, \textsc{Ad0}, and \textsc{Rwt} behind the default-sized flip-flops
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attached to the clock to simulate something like a pipeline stage. My overall design is shown
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in Figure \ref{fig:top-design-sim}.
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\pagebreak
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\begin{figure}[h]
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\centering
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\includegraphics[width=\linewidth]{toplevel_design.png}
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\caption{Top-level design for a single bit.}
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\label{fig:top-design}
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\end{figure}
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My SRAM cell ended up being $30\lambda$ units tall when arrayed. With
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a total of 64 cells in a single column, this led to a wire length of $1920\lambda$.
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However, since my write block was now included in the column, I added another $300\lambda$
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of length to this number, to a total of roughly $2200\lambda$.
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\begin{figure}
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\centering
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\includegraphics[width=0.6\linewidth]{toplevel.png}
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\caption{Architecture of top-level simulation.}
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\label{fig:top-design-sim}
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\end{figure}
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\pagebreak
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\section{Performance Results}
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I was able to clock my design at \textbf{$1.3\textit{ns}$}.
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%
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I realize that this isn't as fast as everyone else, but I ask that you take
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into consideration the fact that \textbf{I was working with the old wire model}
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until about an hour before the final due date (since I didn't know the wire model changed).
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If I knew earlier, I'd have more time to optimize my design for the timings associated
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with the new model.
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%
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Two factors lead to this upper limit.
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%
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\begin{itemize}
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\item \textit{Write capacitance} makes it increasingly difficult to overwrite the value
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in the cell. Clocking my design any faster leads my cell to \textit{almost} flip, but not resolve correctly.
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I have found no way to work around these limits once my wire was properly sized, and my
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write block was placed in the middle of the column.
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\item \textit{Flop, decoder, and read delays} are the major limitation when both the inputs
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and the outputs of the circuit are connected to flip flops. The most significant
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instance of this issue is my write block: both \textsc{Din} and \textsc{Rwt} arrive
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around $300\textit{ps}$ into the cycle. This means two things: a) if the previous
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operation was ``read'', then the block does not start writing until halfway into
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the positive phase of the clock and b) if the data being written is different
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from the data in the previous cycle, for half the time, the write block will write
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the old data (until the flip flop switches).
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\end{itemize}
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\section{Components}
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\subsection{Decoder}
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\subsubsection{In My Own Words}
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The decoder in this design is \textit{almost} the exact same one as we were given in lecture.
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It computes all combinations of two consecutive bits using a \textsc{Nand} gate; for
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each combination, there are 4 adjacent two-bit combinations,
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leading to a 4 \textsc{Nor} gates connected to each \textsc{Nand}. There are now
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16 combinations of 4 adjacent bits; each combination of the lower 4 bits
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needs to be compared with each of the 16 combinations of the upper 4 bits,
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leading to 16 \textsc{Nand} gates connected to each \textsc{Nor}. This
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results in 256 unique \textsc{Wl} wires. Finally, these need to be attached
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to the clock, so that cells aren't open randomly. This is done using an \textsc{And}
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gate (a \textsc{Nand} followed by an inverter).
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I adjusted this design to account for the address signals that need to be fed
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into the write blocks. Which of the read/write columns is triggered
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depends on the upper two bits of the address (since we have 4 columns). I modeled
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this by increasing the fanout on the first \textsc{Nand} gate from 1 to 4.
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This is pessimistic; each 2-bit combination would only feed into one write block,
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whose trigger gate is normally sized.
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\begin{figure}[h]
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\centering
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\includegraphics[width=\linewidth]{decoder.png}
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\caption{Decoder model used in project.}
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\label{fig:decoder}
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\end{figure}
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% TODO: Domino logic
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% TODO: More inverters?
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\pagebreak
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\subsection{Read Block}
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\subsubsection{In My Own Words}
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The read block uses a \emph{sense amplifier} to detect small changes on the bitlines,
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which it then translates into a zero-or-one output. The changes in the wires are below
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the threshold of what could be considered digital logic; all the sense amplifier
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designs I've come across rely on metastability, a state in which even tiny fluctuations
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can significantly alter the outcome\footnote{My favorite analogy is a pencil balanced on its tip.
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Technically, it's stable; however, even a small air current -- one you can't feel -- can knock it over.}.
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The \textsc{Trigger} signal, which depends on the clock and \textsc{Rwt}, puts the amplifier
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into a metastable state. From there, the connected bitlines cause it to resolve one way
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or another. Finally, if one of the wires resolves, a value is written into the keeper circuit
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at the end, which ensures that the value that was read continues to be expressed until
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the next read operation.
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\subsubsection{Details}
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For my read block, I used a different sense amplifier design. The design based
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on the two \textsc{Nand3} gates was easy to understand and build, but was less
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sensitive, and tended to behave strangely under pressure. This led to difficulties
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with debugging (the output would, for instance, flip completely at certain
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wire widths), and was seemingly random. Instead, I used
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an \textbf{improved latch-based sense amplifier design} from \cite{210039}. % TODO: cite
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The design I used is shown in Figure \ref{fig:latch-amp}.
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I left it sized at $40\lambda$, since larger amplifiers seem to take longer
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to trigger and exit metastability.
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The read block is not a particular bottleneck in this design. The main concern
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was to handle the \textbf{``false start'' activation of the write block}. Because the \textsc{Rwt}
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input is behind a latch, it takes nearly $300\textit{ps}$ to pull up or down after
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the initial clock. Thus, if a write occurred during a previous cycle, the write block will
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activate for a short period of time before the read block does. The memory cell
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will overpower this initial misfire\footnote{According to my additional simulations, this is true even when the memory cell is close to the write block.}, but in this case, both \textsc{Bt} and \textsc{Bf}
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will be below \textsc{Vdd}. The ``improved sense amplifier'' seems to handle this
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case better than the one based on two \textsc{Nand} gates.
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The latch-induced delay in \textsc{Rwt} also causes a strange \textsc{Trigger} signal during write operations
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directly following read operations. The trigger signal initialy activates, putting the sense
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amplifier into metastability; however, the correct \textsc{Rwt} value arrives before the
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sense amp's outputs are compromised. If this became a problem, I would add an additional,
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delayed clock signal \emph{after} the sense amplifier, and use an \textsc{And} gate
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to delay the read block's output.
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\begin{figure}[h]
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\centering
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\begin{subfigure}{.5\textwidth}
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\centering
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\includegraphics[width=.7\linewidth]{amp.png}
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\caption{The latch-based sense amplifier from \cite{210039}.}
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\label{fig:latch-amp}
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\end{subfigure}%
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\begin{subfigure}{.5\textwidth}
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\centering
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\includegraphics[width=.8\linewidth]{read_select.png}
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\caption{The block gathering signals from the four columns.}
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\label{fig:read-collect}
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\end{subfigure}
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\caption{Read block schematics}
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\label{fig:read}
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\end{figure}
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\pagebreak
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\subsection{Write Block}
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\subsubsection{In My Own Words}
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The write block converts a ``data in'', or \textsc{Din}, signal
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into a one-hot representation. It does so by pulling one of the bitlines high, and the other
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low. Once the memory cell connects to the bitlines, it takes on the charge provided by the
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write block, and is therefore overwritten. In my design, two PMOS transistors for each bitline
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are used to pull down; one of the transistors is triggered by the \textsc{Din} signal (which wire
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we pull down depends on the signal itself!), and the other by a combination of the clock
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and \textsc{Rwt} (we don't want to touch the wires when reading!).
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\subsubsection{Details}
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My write block was not significantly different from the original design. Under the assumption
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that data arrives first, I placed the transistors attached to \textsc{Din} and $\overline{\textsc{Din}}$
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close to \textsc{Gnd}, each followed by a transistor attached to the ``write'' signal.
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I also configured the write block to only precharge when the clock is low.
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I experimented with making the write block pull wires up when writing (during high clock). However,
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I did not find this to be of significant use. Since the wires are initially precharged,
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there is no more time spent on charging them up; furthermore, the memory cell being written to
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does not have enough ``strength'' to pull the wire down enough.
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A curiosity of this design is that reads didn't seem to work with hich clock speeds. When enough
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time is spent reading the wires, the memory cell in question is able to gradually exhaust the amount
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of charge on one of these wires. Since the original, \textsc{Nand}-based sense amplifier required
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all inputs to be high to properly function, this led to it eventually ``flipping'' and producing
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the wrong output. This was only an issue above $5\textit{ns}$, and only with the original sense amplifier
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design, though. I think that both Reed and
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Graham experienced this occurrence -- they seemed to post very similar waveforms
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to the community Discord group chat.
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One thing to note about the write block is that its \textbf{clock input is deliberately delayed} compared
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to the ``actual'' clock. This is because of an issue with \textsc{Din}. Since this
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input is behind a latch, it takes around $300\textit{ps}$ to arrive after the rising clock
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edge. If the previous value of \textsc{Din} was different than its current one, the write
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block will start writing the wrong value. This will typically mean that the block cannot properly
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perform the write. The delay on the clock input serves to mitigate this issue, by giving more
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time for \textsc{Din} to settle before starting to write. To compensate for this delay, I sized
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the write block's pull down transistors quite large ($100\lambda$), so that they can pull
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the wire down, even starting $300\textit{ps}$ into the cycle. This is why the ``clock'' input
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in my diagrams is colored black, unlike every other clocked component. The delay is achieved
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by 6 sequenced inverters, two of which are sized 10x larger than the rest.
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\begin{figure}[h]
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\centering
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\includegraphics[width=0.65\linewidth]{write.png}
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\caption{Write block used in this project.}
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\label{fig:write}
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\end{figure}
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\pagebreak
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\subsection{Memory Cell}
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\subsubsection{In My Own Words}
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The memory cell consists of two cross coupled inverters whose outputs
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are disconnected from the bitlines by two additional nMOS transistors. When disconnected,
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this cell reliably holds its value; one inverter's output turns off the other, and symmetrically,
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the ``off'' output of that other inverter keeps the first one on. However, this cell is pretty
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small; all of its transistors have size $5\lambda$ is the smallest size that can be properly
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connected with a standard $2\lambda\times2\lambda$ via. Thus, when the ``write line'' (signal
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connected to the gates of the two outside transistors) is asserted, the charge from the
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surrounding bitlines can easily overpower the cell, causing it to switch to a different value.
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\subsubsection{Details}
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There are few notable things about my cell design. Even though it was recommended that we only
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use metals one and two for the internal wiring, I went up to metal three for cross-connecting
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the two internal inverters. This was the only way I found to keep the height of the cell to
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minimum. This limited my routing options somewhat; to compensate, I also used metal three for
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the vertical wires, \textsc{Bt} and \textsc{Bf}. This allowed me to use metal four for the
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\textsc{Wl} (access) signal. Since this was the only use of metal four, I had enough free
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room to route thee additional \textsc{Wl} signals to the remaining three columns.
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My general principle for designing the layout was that, in an 12-bit, 4-column design, \textbf{a single
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unit of height costs as much as 64 units of width}. Thus, I was fairly liberal with my layout's
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width, but made sure to minimize the height of the design. The most significant bottleneck
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was the gate oxide ``poking out'' of the ends of the design. In total, I was able to achieve
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a height of $30\lambda$ when arrayed.
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Other designs with smaller height were possible, but I found them undesirable. For instance,
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Reed's now-famous design used a significant amount of high-level metals to achieve its tiny,
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almost square area. This, however, makes routing \textsc{Wl} signals fairly complicated. They either
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need to go to yet another layer of metal, or the decoder needs to be split into 4 pieces. The former
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is undesirable as per the requirements for this assignment; the latter incurs the cost of additional
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decoder hardware between columns, thereby significantly increasing the wire length and signal
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delays. Since delays incurred by the flip flops and other signals are already becoming
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a significant factor in my design, I thought it would be best to avoid such delays.
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Other ideas I am aware of include putting \textit{all} the transistors in a single, horizontal line.
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While this certainly succeeds at reducing the height, it incurs all the same issues described
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above - it becomes nigh impossible to wire further \textsc{Wl} lines through each column,
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unless the decoder is split into bits, in which case the width of the entire assembly drastically increases,
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slowing down all signals.
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\begin{figure}[h]
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\centering
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\includegraphics[width=0.5\linewidth]{layout_single.png}
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\caption{Electric layout for a single cell.}
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\label{fig:layout-cell}
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\end{figure}
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\pagebreak
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My basic cell is shown in Figure \ref{fig:layout-cell}. The arrayed version (in Figure \ref{fig:layout-arrayed})
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merits additional explanation. In my earlier description of the overall design, I mentioned
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that I have precharge PMOS transistors. I have integrated these into my layout to accurately model
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my design. I also made them $10\lambda$ wide, since this is, at the time of writing,
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the size of my 4 precharge transistors. In the bird's eye view (Figure \ref{fig:layout-arrayed-far}),
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three things can be observed:
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\begin{itemize}
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\item \textit{Additional vertical line:} This line represents the clock signal,
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which must be fed to the precharge transistors. In the full design, there would
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be 5 clock lines (3 shared, and 2 on either side).
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\item \textit{``Empty'' space between nodes:} I left this space because I was not sure
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how wide I would end up making my \textsc{Bt} and \textsc{Bf} wires. I have measured
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the distance to ensure that the design will remain DRC clean with up to \textbf{$8\lambda$-wide bitlines}.
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This appears to be a sweet spot for my design, anyway.
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\item \textit{Moved well contacts:} I have moved my well contacts to the region between
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two columns. By extending the N- and P-wells to this area, I was able to
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share a single contact between two cells, leaving room for prechare transistors
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on both sides of the cell. This was partially inspired by Reed's compact cell design,
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which shared a single contact between two cells\footnote{I am operating based on your
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comment that well contacts for every cell are significantly overkill.}.
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\end{itemize}
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Figure \ref{fig:layout-arrayed-close} shows a closer view of the design. Due to the additional
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space incurred, an entire column is approximately $100\lambda$ wide.
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\begin{figure}[h]
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\centering
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\begin{subfigure}{.5\textwidth}
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\centering
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\includegraphics[width=.7\linewidth]{layout_arrayed.png}
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\caption{Bird's eye view of the arrayed SRAM cells.}
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\label{fig:layout-arrayed-far}
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\end{subfigure}%
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\begin{subfigure}{.5\textwidth}
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\centering
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\includegraphics[width=.8\linewidth]{layout_arrayed_closeup.png}
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\caption{Close up from arrayed SRAM cells.}
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\label{fig:layout-arrayed-close}
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\end{subfigure}
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\caption{Read block schematics}
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\label{fig:layout-arrayed}
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\end{figure}
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\pagebreak
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\bibliographystyle{unsrt}
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\bibliography{bibliography}
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\end{document}
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