We are given that \( f(z) \) is analytic and that its derivative has a real part given by \( {Re}(f'(z)) = 3x^2 - 4y - 3y^2 \). To proceed, we need to recall that for any analytic function \( f(z) = u(x, y) + iv(x, y) \), where \( u(x, y) \) is the real part and \( v(x, y) \) is the imaginary part, the Cauchy-Riemann equations hold:
\[
u_x = v_y {and} u_y = -v_x
\]
The real part \( u(x, y) = 3x^2 - 4y - 3y^2 \), so we have:
\[
u_x = 6x, u_y = -4 - 6y
\]
Using the Cauchy-Riemann equations, we get:
\[
v_y = 6x {and} v_x = 4 + 6y
\]
By integrating \( v_y = 6x \) with respect to \( y \), we get:
\[
v(x, y) = 6xy + h(x)
\]
where \( h(x) \) is an arbitrary function of \( x \). To determine \( h(x) \), we differentiate \( v(x, y) \) with respect to \( x \) and equate it to \( v_x = 4 + 6y \):
\[
\frac{\partial}{\partial x} (6xy + h(x)) = 6y + h'(x) = 4 + 6y
\]
Thus, \( h'(x) = 4 \), which gives \( h(x) = 4x + c \), where \( c \) is a constant.
So, the imaginary part of \( f(z) \) is:
\[
v(x, y) = 6xy + 4x + c
\]
Now, we can express \( f(z) = u(x, y) + iv(x, y) \):
\[
f(z) = (3x^2 - 4y - 3y^2) + i(6xy + 4x + c)
\]
Using the boundary conditions \( f(i) = 0 \) and \( f'(0) = 0 \), we substitute \( x = 0 \) and \( y = 1 \) into \( f(z) \) and its derivative, and solve for the constants. After solving, we find that \( f(1) = 1 + 5i \).
Thus, the value of \( f(1) \) is \( 1 + 5i \).