Gravitational field around blackhole induces photonic spin-orbit interaction that twists light

The spin-orbit interaction (SOI) of light has been intensively studied in nanophotonics because it enables sensitive control of photons' spin degree of freedom and thereby the trajectory of the photons, which is useful for applications such as signal encoding and routing. A recent study showed that the SOI of photons manifests in the presence of a gradient in the permittivity of the medium through which the photons propagate; this enhances the scattering of circularly polarized light and results in the photons propagating along twisted trajectories. Here we theoretically predict that, because of the equivalence between an inhomogeneous dielectric medium and a gravitational field demonstrated in transformation optics, a significant SOI is induced onto circularly polarized light passing by the gravitational lens of a black hole. This leads to: i) the photons to propagate along chiral trajectories if the size of the blackhole is smaller than the wavelength of the incident photons, ii) the resulting image of the gravitational lens to manifest an azimuthal rotation because of these chiral trajectories. The findings open for a way to probe for and discover subwavelength-size black holes using circularly polarized light.


Introduction
The spin-orbit interaction (SOI) is a fundamental phenomenon for the realization of various exotic spin dynamics and matters of nontrivial topological phases [2,3]. The SOI also occurs for photons when circularly polarized light propagates in an inhomogeneous dielectric medium. The inhomogeneity of the medium forces photons to move along curved trajectories and couples their spin angular momentum (AM) with their orbital AM because of the conservation of total AM [4].
As a result of the SOI, circularly polarized photons acquire a transverse component of anomalous velocity, which shifts the trajectories of the light beam away from those given by ordinary geometric optics. The SOI-induced spin-dependent motion can be used to realize the splitting and routing of photons with different spins; recently, this has been intensively investigated in nanophotonics [5][6][7][8][9][10][11][12][13].
It has been shown that the SOI in light results in the presence of a gradient in permittivity of the medium [1]. Recent developments in transformation optics [14,15] have also demonstrated the equivalence between an inhomogeneous dielectric medium and a gravitational field described in by the theory of general relativity. This equivalence has been utilized to mimic celestial phenomena such as black hole [ 16 , 17 ] and gravitational lensing [ 18 , 19 ] using photonic nanostructures. Conversely, it was also predicted that optical phenomena such as the SOI of light, which can be observed in the photonic nanostructures, can be realized in the presence of a gravitational field [20]. Motivated by these advancements we wondered how circularly polarized light would propagate through the gravitational lens of black holes that have a size similar or smaller to the wavelength of the incident light.
Here we show that the gravitational lens of a sub-wavelength black hole produces a significant SOI effect that leads to chiral trajectories of incident circularly polarized photons and a resulting rotation of the image of the black hole obtained by these photons. The findings predict SOI-induced signatures in circularly polarized light could be used to probe for and discover small blackholes.

Result
The motion of circularly polarized light in the gravitational field of a black hole is described by r p r (2) where r and p are the position and momentum vectors of the photons in the light beam, Eq. (1) and the first term on the right of Eq. In addition to the focusing effect, an intriguing phenomenon emerges as a result of the anomalous velocity in Eq. (1). For wavelengths that are much smaller than the size of the black hole, the trajectories are well focused to a single point [ Fig. 1(a) and Fig. 2(a)], but for wavelengths larger than the black hole the streamlines remain separated near the focus. This arrangement of the streamlines can be more clearly seen in Fig. 2(b), which shows an enlargement of the region near the focus in Fig. 1(b). The trajectories are chirally alignedthey still preserve the rotational symmetry, while the mirror symmetry is lost. For an incident beam of opposite circular polarizations, the distribution of the trajectories is similar but show different chiralities [ Fig. 2(c)].
The chiral distributions of the trajectories clearly demonstrate that the gravitational field induces SOI onto the photons. Because the initial momentum of the incident plane wave is parallel with the z-direction, the photons initially carry no orbital AM, only spin AM, because of their circular polarization. When the photons propagate past the black hole, the gravitational lens effect leads to a redirection of the momentum along the  direction (defined in Fig. 1) and leads to the focusing of the light. This focusing behavior does not contribute to an orbital AM. The deviation of the spin AM implies that the total AM momentum changes in the z-direction. However, since this process is elastic, the total AM is conserved and thus, spin AM is transferred to orbital AM via the SOI effect. According to Eq. (2) the anomalous velocity resulting from the SOI is along the azimuthal direction  and thus leads to a transverse shift of the trajectories, as revealed by the chiral distribution in Fig. 1(b). This transverse shift in turn leads to an azimuthal component of momentum in Eq. (1) and an orbital AM in the z-direction. This orbital AM is the result of SOI of photons in the gravitational field which convert the spin AM to the orbital part. The effect of the SOI is determined by the anomalous velocity, which is proportional to the ratio between the wavelength and the smallest distance of the photon from the center of the black hole as shown in Eq. (2). Therefore, the chiral trajectories resulting from gravitational-field-induced SOI only occur for wavelengths of the incident light that are larger than the Schwarzschild radius [ Figs. 1(a) and

Discussion and conclusion
The above theoretical analysis shows that: i) the gravitational field around black holes of