We develop a theory of soliton spiraling in a bulk nonlinear medium and reveal a new physical mechanism: periodic power exchange via induced coherence, which can lead to stable spiraling and the formation of dynamical two-soliton states. Our theory not only explains earlier observations, but provides a number of predictions which are also verified experimentally. Finally, we show theoretically and experimentally that soliton spiraling can be controled by the degree of mutual initial coherence.Self-guided optical beams (or spatial solitons) have attracted substantial research interest in the last three decades [1].Although interactions between twodimensional (2D) solitons in Kerr and non-Kerr media have been studied extensively, only the recent discoveries of stable three-dimensional (3D) solitons in different nonlinear bulk media In this Letter we develop, for the first time to our knowledge, a theory of soliton spiraling in a photorefractive-type nonlinear bulk medium. We derive an analytical model describing stable soliton spiraling and predict a number of new effects in soliton interactions, such as an induced coherence and control over 3D interactions, which we verify here experimentally, using experimental setup similar to that reported earlier [3]. Importantly, our analytical model and numerical simulations show that interacting-spiraling solitons conserve angular momentum. We believe that this result is a core foundation for future research on 3D soliton control, resembling the conservation of linear momentum in the interaction of more conventional (1+1)-dimensional solitons [6].We consider incoherent beam interaction in an isotropic saturable nonlinear medium described by two coupled normalized nonlinear Schrödinger (NLS) equationswhere u and w are the beam envelopes, z is the propagation distance; ∇ 2 ⊥ ≡ ∂ 2 /∂x 2 + ∂ 2 /∂y 2 accounts for the diffraction in the transverse (x, y) plane. This system, in the 2D case (i.e., for ∇ 2 ⊥ ≡ ∂ 2 /∂x 2 ), gives rise to incoherently-coupled soliton pairs [7] and to incoherent collisions [8] which have both been demonstrated with photorefractive screening solitons [9].We look for solitary waves of Eqs. (1) in the form u = U (r) exp (iβ u z), w = W (r) exp (iβ w z), where the envelopes U and W satisfy the equationsHere r ≡ x 2 + y 2 is the radial coordinate, and β u and β w are nonlinearity-induced shifts of the propagation constants. System (2) has two families of soliton solutions: U = G u (β u , r), W = 0 and U = 0, W = G w (β w , r), which can be found numerically by solving the equation, where α = {u, w}. These solutions can be characterised by the soliton powers P (β α ) ≡ 2π ∞ 0 G 2 α (β α , r) rdr. In addition to the one-component solitons, at β u = β v ≡ β there exists a family of two-component (vector) solitons defined as: U = G(β, r) cos θ, W = G(β, r) sin θ, where the variable θ characterises a power distribution between the components. Moving solitons of Eqs. (1) can be obtained by a well-known gauge transformation.