We propose a light-structure interaction that utilizes circularly polarized light to deform a slightly bent waveguide. The mechanism allows for flipping the direction of deformation upon changing the binary polarization state of light from to .Radiation pressure has been found to cause mechanical displacement. This fact was used for controlling resonators [1][2][3][4][5] and waveguides [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25]. Such forces by light in optomechanical structures were reported in the past to originate from (i) scattering forces, such as the centrifugal radiation pressure that light applies while circulating in a ring [1][2][3], (ii) gradient forces in resonators and waveguides [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25], and (iii) electrostrictive pressure to excite vibration at high rates [4,5].In waveguide structures [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25], optical forces were suggested for all-optical reconfiguration of integrated optical devices [4], for manipulating the position of integrated optical components [6], for artificial materials [6,7] in which the internal mechanical configuration and resultant optical properties are coupled to incoming light signals [7], for tunable devices [7,8] such as actuators and transducers [8], and for more [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25]. In all of these studies [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25] the gradient forces are independent by the polarization state of light.Here we suggest controlling the position of a bent waveguide with the angular momentum that light applies via its circular polarization. Unlike previous studies [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25], no other dielectrics are needed near the waveguide and changing the polarization will flip the deformation direction.While the linear momentum of a photon, h , associated with gradient or scattering optical forces [1-25] is always along its propagation direction, a photon can also carry a different type of momentum: angular momentum [26] for which a binary vector [27] can be either with-or against-propagation. This corresponds to angular momentum for a righthanded circularly polarized [RCP] photon and angular momentum for a left-handed circularly polarized [LCP] photon. This type of angular momentum is called the intrinsic spin and is related to the fact that the photon is a spin-1 boson. We will refer to the photon in what follows as "spinning" to describe it containing angular momentum.In the past, radiation torque effects originating from optical angular momentum were studied in waveplates [26], optically active medium [28], anisotropic crystals [29] and tweezed particles [30,31]. In more complex geometries, a spin Hall effect [32] associated with the Berry phase [33] was reported when circularly-polarized light was helically propagating in a cylinder while free ...