Stella Ugo, Grosjean Thierry, De Leo Natascia, Boarino Luca, Munzert Peter, Lakowicz Joseph R, Descrovi Emiliano
Department of Applied Science and Technology (DISAT), Politecnico di Torino, Corso Duca degli Abruzzi 24, Torino, IT-10129, Italy.
FEMTO-ST Institute, Université Bourgogne Franche-Comté, UMR CNRS 6174 15B Avenue des Montboucons, 25030, Besançon, France.
ACS Photonics. 2020 Mar 18;7(3):774-783. doi: 10.1021/acsphotonics.9b01625. Epub 2020 Feb 10.
Axis-symmetric grooves milled in metallic slabs have been demonstrated to promote the transfer of Orbital Angular Momentum (OAM) from far- to near-field and vice versa, thanks to spin-orbit coupling effects involving Surface Plasmons (SP). However, the high absorption losses and the polarization constraints, which are intrinsic in plasmonic structures, limit their effectiveness for applications in the visible spectrum, particularly if emitters located in close proximity to the metallic surface are concerned. Here, an alternative mechanism for vortex beam generation is presented, wherein a free-space radiation possessing OAM is obtained by diffraction of Bloch Surface Waves (BSWs) on a dielectric multilayer. A circularly polarized laser beam is tightly focused on the multilayer surface by means of an immersion optics, such that TE-polarized BSWs are launched radially from the focused spot. While propagating on the multilayer surface, BSWs exhibit a spiral-like wavefront due to the Spin-Orbit Interaction (SOI). A spiral grating surrounding the illumination area provides for the BSW diffraction out-of-plane and imparts an additional azimuthal geometric phase distribution defined by the topological charge of the spiral structure. At infinity, the constructive interference results into free-space beams with defined combinations of polarization and OAM satisfying the conservation of the Total Angular Momentum, based on the incident polarization handedness and the spiral grating topological charge. As an extension of this concept, chiral diffractive structures for BSWs can be used in combination with surface cavities hosting light sources therein.
已证明,金属板上铣出的轴对称凹槽由于涉及表面等离子体激元(SP)的自旋轨道耦合效应,可促进轨道角动量(OAM)从远场到近场的转换,反之亦然。然而,等离子体结构固有的高吸收损耗和偏振限制,限制了它们在可见光谱中的应用效果,特别是对于靠近金属表面的发射器而言。在此,提出了一种产生涡旋光束的替代机制,其中通过布洛赫表面波(BSW)在介质多层膜上的衍射获得具有OAM的自由空间辐射。通过浸没光学器件将圆偏振激光束紧密聚焦在多层膜表面,使得TE偏振的BSW从聚焦点径向发射。在多层膜表面传播时,由于自旋轨道相互作用(SOI),BSW呈现出螺旋状波前。围绕照明区域的螺旋光栅使BSW发生面外衍射,并赋予由螺旋结构的拓扑电荷定义的附加方位角几何相位分布。在无穷远处,基于入射偏振手性和螺旋光栅拓扑电荷,相长干涉产生具有确定偏振和OAM组合的自由空间光束,满足总角动量守恒。作为这一概念的扩展,用于BSW的手性衍射结构可与其中容纳光源的表面腔结合使用。