Surface crossing of bound (S 1 , ππ*) and continuum (S 2 , πσ*) states has been observed in the ultrafast S−D bond dissociation reaction of thiophenol-d 1 . It is manifested by an unanticipated variation of fragment angular distribution as a function of the excitation energy. The anisotropy parameter (β) of +0.25 at the S 1 origin decreases to −0.60 at ∼600 cm −1 above the S 1 zero-point level, giving a broad peak in β with a bandwidth of ∼200 cm −1 . The peak in β is ascribed to the in-plane S-D bending mode excitation by which the nuclear configuration in the proximity of the S 1 /S 2 conical intersection seam is directly accessed, showing a mixed character of parallel (S 1 −S 0 ) and perpendicular (S 2 −S 0 ) transition dipole moments at the same time. As a result, the dynamic aspect of the conical intersection is experimentally revealed here through direct access to the nuclear configuration on the multidimensional conical intersection seam. C hemical reactions are often described as nuclear movements of which directions and speeds are determined by shapes of multidimensional electronic potential energy surfaces. This adiabatic picture is based on the seminal Born− Oppenheimer approximation that assumes that the nuclear motion is separable in time from the much faster electronic motion. 1 The Born−Oppenheimer approximation has been enormously successful in describing chemical reactions on the ground electronic state. For chemical reactions on the electronically excited states, however, coupling of electronic and nuclear motions becomes nontrivial, and significant nonadiabatic transitions where nuclear motions induce surface-hopping (and vice versa) occur in many circumstances. 2 Nonadiabatic transitions are ubiquitous in nature and even essential in a number of important chemical and biological processes. 3−6 Notably, for polyatomic molecules, the noncrossing rule does not strictly apply and a conical intersection point is generated by intersection of two potential curves on the 2D branching plane. In general, the conical intersection lies on the (3N−8) dimensional seam, where (3N−6) is the number of internal degrees of freedom of N atomic molecular system. 7−9 As the energy gap between two adiabatic potential surfaces becomes infinitesimally small in the proximity of conical intersections, nonadiabatic transitions are facilitated when the reactive flux or wavepacket reaches the conical intersection region during the chemical reaction process. Most dynamic outputs of nonadiabatic transitions are then dictated by the nature of the conical intersections, and it would be extremely valuable if one could figure out the structure and dynamic role of conical intersections.In this regard, there have been numerous theoretical and experimental studies on conical intersection dynamics in recent decades. Theoretical descriptions of conical intersections have been very successful in explaining many important nonadiabatic chemical processes. These include photochemical organic reactions, 10 photoisomerization, 11,12 the ra...