This might be a bit annoying to justify (see below), but I'm quite sure that the surface you're looking for is constructed as follows. (And in any case this is too long for a comment.)
Start with the $d$-braid $\beta = \sigma_1\sigma_2\dots\sigma_{d-1}$, whose closure is the unknot. The torus link $T(d,d)$ (the union of $d$ fibres of the Hopf link, which is the link you're describing) is the closure of the braid $\beta^d$. $\beta^d$ is obtained from $\beta$ by adding $(d-1)^2$ generators.
Now, start with the closure of $\beta$, take the disc it bounds in $S^3$, and push it into the 4-ball. Each addition of a generator $\sigma_i$ to your braid can be viewed as a band attachment in $S^3\times [0,1]$, which gives you a cobordism (with Euler characteristic 1) from the link before-adding and the link after-adding. Do this for each of the $(d-1)^2$ braid generators you need to add to $\beta$ to get to $\beta^d$, and this gives you a cobordism in $S^3\times [0,(d-1)^2]$ from the unknot to $T(d,d)$. Glue in the ball with the disc on the lower boundary component, and you get your desired surface.
As a sanity check: the Euler characteristic of this surface is $1-(d-1)^2 = 2d-d^2$ (the $1$ is from the disc, the $-(d-1)^2$ is from the bands). The Euler characteristic of the surface you were looking for is $(3d-d^2)-d = 2d-d^2$ (the $3d-d^2$ is from the algebraic curve, and the $-d$ is from the $d$ discs you're removing). So, ok, at least this checks.
One piece of justification for why what I'm doing is actually what you want, is that each band attachment corresponds to a plumbing of a positive Hopf band, so what I'm describing is the fibre of a fibration of $T(d,d)$ as a link in $S^3$, which arises as the boundary of a Lefschetz fibration of $B^4$. This is exactly the picture you'd expect, since $T(d,d)$ is the link of the singularity of $\{x^d + y^d = 0\}$, and the piece of algebraic curve you're looking for is a fibre of the Milnor fibration associated to this singularity.