We will first demonstrate that \(D\) can be embedded in the field \(F_D\text{.}\) Define a map \(\phi : D \rightarrow F_D\) by \(\phi(a) = [a, 1]\text{.}\) Then for \(a\) and \(b\) in \(D\text{,}\)
\begin{equation*}
\phi( a + b ) = [a+b, 1] = [a, 1] + [b, 1] = \phi(a ) + \phi(b)
\end{equation*}
and
\begin{equation*}
\phi( a b ) = [a b, 1] = [a, 1] [b, 1] = \phi(a ) \phi(b);
\end{equation*}
hence, \(\phi\) is a homomorphism. To show that \(\phi\) is one-to-one, suppose that \(\phi(a) = \phi( b)\text{.}\) Then \([a, 1] = [b, 1]\text{,}\) or \(a = a1 = 1b = b\text{.}\) Finally, any element of \(F_D\) can be expressed as the quotient of two elements in \(D\text{,}\) since
\begin{equation*}
\phi(a) [\phi(b)]^{-1} = [a, 1] [b, 1]^{-1} = [a, 1] \cdot [1, b] = [a, b]\text{.}
\end{equation*}
Now let \(E\) be a field containing \(D\) and define a map \(\psi :F_D \rightarrow E\) by \(\psi([a, b]) = a b^{-1}\text{.}\) To show that \(\psi\) is well-defined, let \([a_1, b_1] = [a_2, b_2]\text{.}\) Then \(a_1 b_2 = b_1 a_2\text{.}\) Therefore, \(a_1 b_1^{-1} = a_2 b_2^{-1}\) and \(\psi( [a_1, b_1]) = \psi( [a_2, b_2])\text{.}\)
If \([a, b ]\) and \([c, d]\) are in \(F_D\text{,}\) then
\begin{align*}
\psi( [a, b] + [c, d] ) & = \psi( [ad + b c, b d ] )\\
& = (ad + b c)(b d)^{-1}\\
& = a b^{-1} + c d^{-1}\\
& = \psi( [a, b] ) + \psi( [c, d] )
\end{align*}
and
\begin{align*}
\psi( [a, b] \cdot [c, d] ) & = \psi( [ac, b d ] )\\
& = (ac)(b d)^{-1}\\
& = a b^{-1} c d^{-1}\\
& = \psi( [a, b] ) \psi( [c, d] )\text{.}
\end{align*}
Therefore, \(\psi\) is a homomorphism.
To complete the proof of the theorem, we need to show that \(\psi\) is one-to-one. Suppose that \(\psi( [a, b] ) = ab^{-1} = 0\text{.}\) Then \(a = 0b = 0\) and \([a, b] = [0, b]\text{.}\) Therefore, the kernel of \(\psi\) is the zero element \([ 0, b]\) in \(F_D\text{,}\) and \(\psi\) is injective.