Look at the equation $\mathbf \nabla \times \mathbf H = \mathbf J_\textrm{free}$, and at the same time at $\mathbf \nabla \times\mathbf B = \mu_0 \mathbf J$. Now, $\mathbf J = \mathbf J_\textrm{bound} + \mathbf J_\textrm{free}$, and $\mathbf H = \frac1\mu_o \mathbf B - \mathbf M$, where $\mathbf M$ is called the Magnetisation. $\mathbf H$ allows me to write the Ampere's Law in terms of free current alone, and that is the thing that we control directly.
So for problems having specific symmetry I can immediately write $\mathbf H$, and from there $\mathbf B$.So in the laboratory people will talk more about $\mathbf H$ than $\mathbf B$.
And to answer your question both are fundamental.
P.S. $\mathbf B = \mu \mathbf H$, $\mathbf M = \chi_m \mathbf H$ and $\mu = \mu_0(1+\chi_m)$.