Are there smooth bodies of constant width? The standard Reuleaux triangle is not smooth, but the three
points of tangential discontinuity can be smoothed as
in the figure below (left), from the Wikipedia article.
However, it is unclear (to me) from this diagram
whether the curve is $C^2$ or $C^\infty$.
Meissner’s tetrahedron is a 3D body of constant width,
but it is not smooth, as is evident in the right figure
below.
   
My question is:

Are there $C^\infty$ constant-width bodies in $\mathbb{R}^d$ (other than the spheres)?

The image of Meissner’s tetrahedron above is taken
from the impressive work of
Thomas Lachand–Robert and Edouard Oudet,
"Bodies of constant width in arbitrary dimension"
(Math. Nachr. 280, No. 7, 740-750 (2007); pre-publication PDF here). Here is a link to Wayback Machine.)
I suspect the answer to my question is known, in which case a reference would suffice.  Thanks!
Addendum.
Thanks to the knowledgeable (and rapid!) answers by Gerry, Anton, and Andrey,
my question is completely answered—I am grateful!!
 A: Take any odd smooth function h on the unit (d-1)-sphere and take a constant r>0 large enough to ensure that h+r is the support function of a convex body K
(the condition for h+r to be the support function of a smooth convex body whose boundary has positive Gaussian curvature is that the eigenvalues of Hess(h)+(h+r).Id be positive).
This convex body K is of constant width 2r.
Moreover, any smooth convex body with constant width 2r whose boundary has positive Gaussian curvature can be constructed in this way :
If S is a closed convex hypersurface of constant width 2r, then S is the sum of a sphere of radius r with a "projective hedgehog" H whose support function h is the odd part of the support function of S (and which can be regarded as the locus of the middles of S's diameters)." ;
See for instance:
Y. Martinez-Maure, Arch. Math., Vol. 67, 156-163 (1996), page 157.
A: This relevant paper was just released:

Howard Resnikoff. "On Curves and Surfaces of Constant Width." Apr. 2015.
(arXiv abstract.)


"...we provide a Fourier series-based construction that produces arbitrarily many new surfaces of constant width."


     
![ConstWidth][1]

A: Michael Kallay characterized the set of all planar sets with a given width functions: See
M. Kallay, Reconstruction of a plane convex body from the curvature of its boundary. Israel J. Math. 17 (1974), 149–161. and M. Kallay, The extreme bodies in the set of plane convex bodies with a given width function. Israel J. Math. 22 (1975), no. 3-4, 203–207.
A: Fillmore showed that there are sets of constant width in $\mathbb R^d$ with analytic boundaries which have a trivial symmetry group (so these are very different from spheres;
see "Symmetries of surfaces of constant width",  J. Differential Geom., Vol 3, (1969),  pp. 103-110).
Moreover, the set of bodies of constant width with analytic boundaries is dense in the space of all convex bodies of constant width in $\mathbb R^d$ with respect to the Hausdorff metric (see e.g. "Smooth approximation of convex bodies" by Schneider).
A: Take any odd $C^\infty$-function $f$ on the sphere.
Consider the convex set 
$$R_\epsilon=\{\,x\in\mathbb R^n\mid\langle x,u\rangle\le 1+\epsilon{\cdot}f(u)\ \ \text{for any}\ \ u\in\mathbb{S}^{n-1}\,\}.$$
Note that for all sufficiently small $\epsilon>0$, $R_\epsilon$ is a smooth body of constant width.
A: Jay P Fillmore, Symmetries of surfaces of constant width, J Differential Geometry 5 (1969) 103-110, says: the curve $$x_1=h\cos\theta-{dh\over d\theta}\sin\theta,\qquad x_2=h\sin\theta+{dh\over d\theta}\cos\theta$$ where $h=a+b\cos3\theta$, $0\lt8b\lt a$, is analytic and of constant width. If we rotate this curve in Euclidean space ${\bf E}^n$ about an $(n-2)$-dimensional axis perpendicular to the line $\theta=0$, we obtain an analytic surface, not a sphere, of constant width in ${\bf E}^n$.
The paper may be available at https://mathweb.ucsd.edu/~fillmore/papers/a.html,
https://doi.org/10.4310/jdg/1214428822,
https://projecteuclid.org/euclid.jdg/1214428822
