I wouldn't word it that way. The mass centres and c are in a straight line, so a direction 'towards c' is the same as 'towards the other star's centre'. Besides, it is important to remember that centripetal force is a resultant force. Your wording might give the false impression that each star is somehow attracted to the common mass centre.
If two stars are on parallel and opposite courses, at right angles to the line joining them at some instant, each experiences attraction towards the other star so accelerates in that direction. Since that is at right angles to their directions of motion, that results in a change of direction, not a change in speed. That is, it will lead them to start to revolve around some points (not necessarily the same point) on the line joining them.
This situation may be transient; a moment later their arrangement no longer matches those conditions.
If the distance between them, their speeds and their masses are in the right relationship to each other, that point will be, for both, the common mass centre. If so, the arrangement is dynamically stable, i.e. they will continue to satisfy all thes conditions and continue to orbit around that common mass centre. But the attaction is always to the mass centre of the other star.
One more point, just to be clear. That each star is attracted to the mass centre of the other is a special feature of spherically symmetric bodies. In reality, each atom of each star is attracted to each atom of the other. But if each star is made of concentric spherical shells, each of uniform mass density, it turns out that the net attraction of each atom of one star is towards the mass centre of the other. The situation would be far more complex with two amorphous lumps of rock orbiting each other.