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authorNiels Möller <nisse@lysator.liu.se>2014-07-11 23:05:12 +0200
committerNiels Möller <nisse@lysator.liu.se>2014-07-11 23:05:12 +0200
commit71cdc7784c505994efd72d5168a47e7c5380dcd0 (patch)
tree9772ef7944d1dad6fb1e8eba969355c081c4661e
parent660e482f8df70f6b2aeea3953c0869611aa981d5 (diff)
downloadnettle-71cdc7784c505994efd72d5168a47e7c5380dcd0.tar.gz
Added some ECC notes.
-rw-r--r--ChangeLog2
-rw-r--r--misc/.gitignore4
-rw-r--r--misc/ecc-formulas.tex152
3 files changed, 158 insertions, 0 deletions
diff --git a/ChangeLog b/ChangeLog
index f0909d70..e338f4dc 100644
--- a/ChangeLog
+++ b/ChangeLog
@@ -1,5 +1,7 @@
2014-07-11 Niels Möller <nisse@lysator.liu.se>
+ * misc/ecc-formulas.tex: Some ECC notes.
+
* testsuite/curve25519-dup-test.c: New testcase.
* testsuite/Makefile.in (TS_HOGWEED_SOURCES): Added
curve25519-dup-test.c.
diff --git a/misc/.gitignore b/misc/.gitignore
index 2bd18fa4..81c83739 100644
--- a/misc/.gitignore
+++ b/misc/.gitignore
@@ -1 +1,5 @@
/*.pdf
+/*.dvi
+/*.log
+/*.aux
+/auto
diff --git a/misc/ecc-formulas.tex b/misc/ecc-formulas.tex
new file mode 100644
index 00000000..36c15227
--- /dev/null
+++ b/misc/ecc-formulas.tex
@@ -0,0 +1,152 @@
+\documentclass[a4paper]{article}
+\usepackage[utf8]{inputenc}
+\usepackage{amsmath}
+\usepackage{url}
+
+\author{Niels Möller}
+\title{Notes on ECC formulas}
+
+\begin{document}
+
+\maketitle
+
+\section{Weierstrass curve}
+
+Consider only the special case
+\begin{equation*}
+ y^2 = x^3 - 3x + b (mod p)
+\end{equation*}
+See \url{http://www.hyperelliptic.org/EFD/g1p/auto-shortw.html}.
+
+Affine formulas for duplication, $(x_2, y_2) = 2(x_1, y_1)$:
+\begin{align*}
+ t &= (2y)^{-1} 3 (x_1^2 - 1) \\
+ x_2 &= t^2 - 2 x_1 \\
+ y_2 &= (x_1 - x_2) * t - y_1
+\end{align*}
+Affine formulas for addition, $(x_3, y_3) = (x_1, y_1) + (x_2,
+y_2)$:
+\begin{align}
+ t &= (x_2 - x_1)^{-1} (y_2 - y_1) \\
+ x_3 &= t^2 - x_1 - x_2 \\
+ y_3 &= (x_1 - x_3) t - y_1
+\end{align}
+
+\section{Montgomery curve}
+
+Consider the special case
+\begin{equation*}
+ y^2 = x^3 + b x^2 + x
+\end{equation*}
+See \url{http://www.hyperelliptic.org/EFD/g1p/auto-montgom.html}.
+
+Affine formulas for duplication, $(x_2, y_2) = 2(x_1, y_1)$:
+\begin{align*}
+ t &= (2 y_1)^{-1} (3 x_1^2 + 2b x_1 + 1) \\
+ x_2 &= t^2 - b - 2 x_1 \\
+ y_2 &= (3 x_1 + b) t - t^3 - y_1 \\
+ &= (3 x_1 + b - t^2) t - y_1 \\
+ &= (x_1 - x_2) t - y_1
+\end{align*}
+So the computation is very similar to the Weierstraß case, differing
+only in the formula for $t$, and the $b$ term in $x_2$.
+
+Affine formulas for addition, $(x_3, y_3) = (x_1, y_1) + (x_2,
+y_2)$:
+\begin{align*}
+ t &= (x_2 - x_1)^{-1} (y_2 - y_1) \\
+ x_3 &= t^2 - b - x_1 - x_2 \\
+ y_3 &= (2 x_1 + x_2 + b) t - t^3 - y_1 \\
+ &= (2 x_1 + x_2 + b - t^2) t - y_1 \\
+ &= (x_1 - x_3) t - y_1
+\end{align*}
+Again, very similar to the Weierstraß formulas, with only an
+additional $b$ term in the formula for $x_3$.
+
+\section{Edwards curve}
+
+For an Edwards curve, we consider the special case
+\begin{equation*}
+ x^2 + y^2 = 1 + d x^2 y^2
+\end{equation*}
+See \url{http://cr.yp.to/papers.html#newelliptic}.
+
+Affine formulas for addition, $(x_3, y_3) = (x_1, y_1) + (x_2,
+y_2)$:
+\begin{align*}
+ t &= d x_1 x_2 y_1 y_2 \\
+ x_3 &= (1 + t)^{-1} (x_1 y_2 + y_1 x_2) \\
+ y_3 &= (1 - t)^{-1} (y_1 y_2 - x_1 x_2)
+\end{align*}
+With homogeneous coordinates $(X_1, Y_1, Z_1)$ etc., D.~J.~Bernstein
+suggests the formulas
+\begin{align*}
+ A &= Z_1 Z_2 \\
+ B &= A^2 \\
+ C &= X_1 X_2 \\
+ D &= Y_1 Y_2 \\
+ E &= d C D \\
+ F &= B - E \\
+ G &= B + E \\
+ X_3 &= A F [(X_1 + Y_1)(X_2 + Y_2) - C - D] \\
+ Y_3 &= A G (D - C) \\
+ Z_3 &= F G
+\end{align*}
+This works also for doubling, but a more efficient variant is
+\begin{align*}
+ B &= (X_1 + Y_1)^2 \\
+ C &= X_1^2 \\
+ D &= Y_1^2 \\
+ E &= C + D \\
+ H &= Z_1^2 \\
+ J &= E - 2H \\
+ X_3 &= (B - E) J \\
+ Y_3 &= E (C - D) \\
+ Z_3 &= E J
+\end{align*}
+
+\section{Curve25519}
+
+Curve25519 is defined as the Montgomery curve
+\begin{equation*}
+ y^2 = x^3 + b x^2 + x \pmod p
+\end{equation*}
+with $b = 486662$ and $p = 2^{255} -19$. It is equivalent to the
+Edwards curve
+\begin{equation*}
+ u^2 + v^2 = 1 + d u^2 v^2 \pmod p
+\end{equation*}
+with $d = (121665/121666) \bmod p$. The equivalence is given by
+mapping $P = (x,y)$ to $P' = (u, v)$, as follows.
+\begin{itemize}
+\item $P = \infty$ corresponds to $P' = (0, 1)$
+\item $P = (0, 0)$ corresponds to $P' = (0, -1)$
+\item Otherwise, for all other points on the curve. First note that $x
+ \neq -1$ (since then the right hand side is a not a quadratic
+ residue), and that $y \neq 0$ (since $y = 0$ and $x \neq 0$ implies
+ that $x^2 + bx + 1 = 0$, or $(x + b/2)^2 = (b/2)^2 - 1$, which also
+ isn't a quadratic residue). The correspondence is then given by
+ \begin{align*}
+ u &= \sqrt{b} \, x / y \\
+ v &= (x-1) / (x+1)
+ \end{align*}
+\end{itemize}
+
+The inverse transformation is
+\begin{align*}
+ x &= (1+v) / (1-v) \\
+ y &= \sqrt{b} x / u
+\end{align*}
+If the Edwards coordinates are represented using homogeneous
+coordinates, $u = U/W$ and $v = V/W$, then
+\begin{align*}
+ x &= \frac{W+V}{W-V} \\
+ y &= \sqrt{b} \frac{(W+V) W}{(W-V) U}
+\end{align*}
+so we need to invert the value $(W-V) U$.
+\end{document}
+
+%%% Local Variables:
+%%% mode: latex
+%%% TeX-master: t
+%%% End: