Tangent Space of the Heisenberg Group Let H$_{3}$(R) denote the Heisenberg group of 3 x 3 real matrices. For any A $\in$ H$_{3}$(R) such that   A = $\left( \begin{array}{ccc}
1 & a & b \\
0 & 1 & c \\
0 & 0 & 1 \end{array} \right)$ ,  $\exists$ a continuous path A(t), 0 $\leq$ t $\leq$ 1, from I to A given by   A(t) = $ \left( \begin{array}{ccc}
1 & a(t) & b(t) \\
0 & 1 & c(t) \\
0 & 0 & 1 \end{array} \right)$ . 
Let v be the tangent vector of A(t) at identity (t=0), then v= $\frac{d}{dt}$ A(t)|$_{t=o}$.
Then shouldn't   v = A'(0) = $ \left( \begin{array}{ccc}
1 & \frac {d}{dt}0 & \frac{d}{dt}0 \\
0 & 1 & \frac{d}{dt}0 \\
0 & 0 & 1 \end{array} \right)$ = $ \left( \begin{array}{ccc}
1 & 0 & 0 \\
0 & 1 & 0 \\
0 & 0 & 1 \end{array} \right)$ ? 
 If this is correct, then is the tangent space of H$_{3}$(R) the standard, orthonormal basis of R$^3$? 
(Apologies if this is horribly fallacious, I'm new to lie algebra)
 A: The notation $A'(0)$ does not mean "differentiate the constant $A(0)$." Indeed, if you differentiate a constant, you will always get $0$. (In this case, you would get the zero matrix, so even the $1$s on the diagonal wouldn't make sense. Moreover, the identity matrix is not "the standard orthonormal basis of $\mathbb{R}^3$"; its columns are, but that's utterly irrelevant. The tangent space of $H_3(\mathbb{R})$ will consist of of matrices, not of column vectors.)
Rather, $A'(0)$ means "differentiate $A(t)$, then plug in $t=0$."
So if you have a differentiable path $A(t)$, each of $a(t),b(t),c(t)$ must be differentiable, and
$$ A'(t)= \frac{d}{dt} \begin{pmatrix} 1 & a(t) & b(t) \\ 0 & 1 & c(t) \\ 0 & 0 & 1 \end{pmatrix} = \begin{pmatrix} 0 & a'(t) & b'(t) \\ 0 & 0 & c'(t) \\ 0 & 0 & 0 \end{pmatrix}. $$
Then you plug $t=0$ into this.
A: No. Choose a path $\gamma$ made up of matrices and passing through the identity; formally, $\gamma : (-r,r) \to H_3 (\Bbb R)$ with $\gamma (0) = 1$ (the $3 \times 3$ identity matrix, and some $r>0$). Writing in components, $\gamma (t) = \begin{pmatrix} 1 & a(t) & b(t) \\ 0 & 1 & c(t) \\ 0 & 0 & 1 \end{pmatrix}$. Now, the tangent space in $1$ at $H_3 (\Bbb R)$ is made up of the tangent vectors at $t=0$ of all these curves, i.e. the vectors $\gamma ' (0) = \begin{pmatrix} 0 & a'(0) & b'(0) \\ 0 & 0 & c'(0) \\ 0 & 0 & 0 \end{pmatrix}$. Since $a$, $b$ and $c$ are arbitrary, their derivatives in $0$ will be arbitrary too. Therefore, calling them $u,v,w$, it follows that the tangent space that you are after is made up of the matrices $\begin{pmatrix} 0 & u & v \\ 0 & 0 & w \\ 0 & 0 & 0 \end{pmatrix}$ with $u,v,w \in \Bbb R$.
