The Triclinic Crystal System
Triclinic is the most general crystal system. All other
crystal systems can be considered special cases of the
triclinic. The primitive vectors are also completely general: their
lengths ($a$, $b$, $c$) and angles ($\alpha$, $\beta$, $\gamma$) may
have arbitrary values. The triclinic system has one Bravais lattice,
which is also the conventional lattice for this system.
There are many choices for the primitive vectors in the triclinic
system. We make the choice
\[
\begin{eqnarray}
\mathbf{a}_1 & = & a \, \mathbf{\hat{x}} \nonumber \\
\mathbf{a}_2 & = & b \, \cos\gamma \, \mathbf{\hat{x}} + b \, \sin\gamma \,\mathbf{\hat{y}}
\nonumber \\
\mathbf{a}_3 & = & c_x \, \mathbf{\hat{x}} + c_y \, \mathbf{\hat{y}} + c_z \, \mathbf{\hat{z}},
\end{eqnarray}
\]
where
\[
\begin{eqnarray*}
c_x & = & c \, \cos\beta \\
c_y & = & \frac{c \, (\cos\alpha - \cos\beta \, \cos\gamma)}{\sin\gamma}
\end{eqnarray*}
\]
and
\[
\begin{eqnarray*}
c_z & = & \sqrt{c^2 - c_x^2 - c_y^2}.
\end{eqnarray*}
\]
The volume of
the triclinic unit cell is
\[
\begin{equation}
V = a \, b \, c_z \, \sin\gamma.
\end{equation}
\]
The space groups associated with the triclinic lattice are
\begin{array}{ll}
1. ~ \mbox{P1} & 2. ~ \mbox{P}\overline{1} \\
\end{array}