Spin and Orbital Rotation of Electrons and Photons via Spin-Orbit Interaction

Spin and Orbital Rotation of Electrons and Photons via Spin-Orbit Interaction

C.C. Leary cleary@uoregon.edu    M.G. Raymer    S.J. van Enk Oregon Center for Optics and Department of Physics, University of Oregon, Eugene, OR USA, 97403
July 15, 2019
Abstract

We show that when an electron or photon propagates in a cylindrically symmetric waveguide, its spin angular momentum (SAM) and its orbital angular momentum (OAM) interact. Remarkably, we find that the dynamics resulting from this spin-orbit interaction are quantitatively described by a single expression applying to both electrons and photons. This leads to the prediction of several novel rotational effects: the spatial or time evolution of either particle’s spin/polarization vector is controlled by its OAM quantum number, or conversely, its spatial wavefunction is controlled by its SAM. We show that the common origin of these effects in electrons and photons is a universal geometric phase. We demonstrate how these phenomena can be used to reversibly transfer entanglement between the SAM and OAM degrees of freedom of two-particle states.

pacs:
42.50.Tx, 03.65.-w, 42.81.Qb, 03.75.-b, 03.65.Ge

It is well known that when an electron propagates in an inhomogeneous potential, its spin angular momentum (SAM) interacts with the orbital angular momentum (OAM) associated with its own curvilinear motion. It is also known that when light propagates in a transparent medium with an inhomogeneous refractive index, an analogous effect can take place: its polarization and OAM can interact and alter the propagation characteristics of the light. Several instances of this have been predicted (cf. Liberman and Zel’dovich (1992); Onoda et al. (2004); Bliokh and Bliokh (2004)), and a few experiments have been done Dooghin et al. (1992); Hosten and Kwiat (2008); Bliokh et al. (2008). What has not yet been made clear is the extent to which a unified wave-picture description of this spin-orbit interaction (SOI) for both photons (electromagnetic fields) and electrons (matter waves) can be reached.

In this work we study the dynamics of the SOI from within such a unified framework. Remarkably, we find that the SOI is quantitatively described by a single expression applying to either an electron or a photon propagating in a straight, cylindrically symmetric waveguide geometry. This leads to the prediction of several novel rotational effects for both particle types, in which the particle’s spin and orbital degrees of freedom influence one another as it propagates down the waveguide. These phenomena allow for the reversible transfer of entanglement between the SAM and OAM degrees of freedom of two-particle states. To provide deeper insight, we show that the common origin of these effects in electrons and photons is a universal geometric (Berry) phase associated with the interplay between either particle’s spin and OAM. This implies that the SOI occurs for any particle with spin, and thereby exists independently of whether or not the particle has mass, charge, or magnetic moment.

Previous authors have examined the connection between the geometric phase and the SOI for both particle types (cf. Bliokh et al. (2008); Berard et al. (2006) and Refs. therein). However, the cylindrical geometry we treat here, which supports transversely stationary waves with well-defined OAM that propagate down a straight waveguide axis, contrasts with the geometry in nearly all other related studies, which consider a transversely localized beam traveling along either a curved or refracted trajectory (cf. Onoda et al. (2004); Bliokh and Bliokh (2004); Hosten and Kwiat (2008); Bliokh et al. (2008); Berard et al. (2006); Tomita and Chiao (1986); Białynicki-Birula and Białynicka-Birula (1987)). Furthermore, these analyses have been limited to the contexts of semi-classical equations of motion in a trajectory (ray) picture, so that a majority of the aforementioned rotational effects, which can be described only via the ‘wavefunction’ picture, have been missed.

Figure 1: (a) An OAM eigenstate with in a balanced superposition of and SAM states (see equation (6a)). The signs contained within the transverse spatial profiles indicate the SAM of the contributing state, while the arrows indicate its OAM handedness. (b) A SAM eigenstate in a balanced superposition of right and left-handed OAM states with (see equation (6b)). When states (a) and (b) propagate down a straight waveguide, the spin (polarization) vector of the state in (a) (see equation (7a)) and the transverse spatial profile of the state in (b) (see equation (7b)) exhibit azimuthal rotation, as shown in (c) and (d), with the sense of rotation controlled by the sign of the OAM and SAM quantum numbers, respectively. The straight arrows in (c) denote the orientation of the state’s spin (polarization) vector, while the white plus signs in (d) represent relative transverse phase.

In order to summarize these SOI phenomena, we introduce the following terminology: we speak of an electron (photon) as being in a SAM eigenstate if its corresponding quantum state (transverse electric field) is an eigenstate of the SAM z-component (helicity) operator with eigenvalue . Similarly, an eigenstate of the OAM z-component operator with eigenvalue is in an OAM eigenstate. Here, is the particle spin, while is the diagonal Pauli matrix, and and are the SAM and OAM quantum numbers, respectively.

The first of the aforementioned effects involves an OAM eigenstate in a balanced superposition of SAM states as shown in Fig. 1(a). As we will show, when an electron (photon) in this state propagates down the z axis of a cylindrical waveguide (see Fig. 1(c)), it exhibits a cyclic azimuthal rotation of its spin (polarization) vector in the transverse plane, with the direction of this rotation being controlled by the sign of its OAM quantum number , denoted by . Conversely to this, a second effect involves the directional control of the azimuthal rotation of either particle’s transverse spatial wavefunction (i.e., its ‘orbital’ state) by the sign of its SAM quantum number , which occurs when a SAM eigenstate in a balanced superposition of OAM states (see Fig. 1(b)) propagates in the waveguide as shown in Fig. 1(d). One may think of the former phenomenon as orbit-controlled spin rotation, and the latter as spin-controlled orbital rotation. As we discuss later, both of these rotation effects may occur either as a function of space (distance traveled down the guide) or of time, so that combining the above possibilities then yields four distinct, complementary manifestations of the SOI for each particle type.

We note that the spin/polarization rotation of Fig. 1(c) is reminiscent of a well-known polarization rotation effect for light first predicted by Rytov Rytov (1938) and observed by Tomita and Chiao Tomita and Chiao (1986), in whose experiment a single-mode optical fiber was wound into a helical shape so that light propagating in the fiber traced out a closed momentum-space path, thereby giving rise to a polarization rotation induced by a Berry phase. However, we stress that the effect predicted in Fig. 1(c) has fundamental differences with the Rytov-Chiao rotation, as the former case involves an OAM eigenstate traveling along the z axis, while the latter involves the lowest-order fiber mode (which has zero OAM) traveling along a helical trajectory and predicts the absence of any polarization rotation if the fiber is made perfectly straight. As we will show, the reason that rotation still occurs for a straight waveguide in the former case is that the OAM states assume the role played by the helical fiber geometry.

The orbital rotation of Fig. 1(d) has been previously predicted and observed indirectly for photons in a multi-mode fiber by Zel’dovich et al. Liberman and Zel’dovich (1992); Dooghin et al. (1992) (although the aforementioned temporal manifestation was not discussed by them). Aspects of the electron case have been treated previously by us Leary et al. (2008). Here we present a single expression, valid for both electrons and photons, which provides a unified description of this orbital rotation effect with the three additional complementary effects discussed above.

Consider first an electron with mass and charge guided at a non-relativistic velocity by an inhomogeneous but cylindrically symmetric potential with an effective radius . After normalizing the electron’s potential energy by its rest energy , we may express the resulting quantity as , where . In order to ensure transversely bound states, we assume that is zero at the origin and increases monotonically to one at radius , becoming constant thereafter. Due to the z-axis translational invariance of the waveguide geometry, a monoenergetic wavefunction in the coordinate basis assumes the traveling-wave form , and the Dirac equation for the electron’s wavefunction in the Foldy-Wouthuysen representation assumes the form of a time-independent Schrödinger-type equation with a perturbation (c.f. Greiner (1997)),

(1)

Here, the unperturbed operator has the well-known Schrödinger form , where is the transverse Laplacian, and . The solutions of the unperturbed, separable, scalar equation are eigenstates of both SAM and OAM, and have the general form

(2)

where is a normalization constant, is the transverse wavenumber, and the spinor denotes the spin state of the electron as determined by .

The perturbation in (1) consists of three well-known contributions: a relativistic kinetic energy correction, a spin-orbit interaction correction, and the so-called Darwin term. We are concerned only with the spin-orbit contribution, which for an external electrostatic potential takes the general form , where . In Leary et al. (2008), we showed that for , in first-order perturbation theory assumes the form

(3)

under quasi-paraxial conditions.

Consider now the analogous case of a photon propagating in an inhomogeneous but cylindrically symmetric medium characterized by permittivity , which can be written in a form similar to that above, , where in the photon case . In this geometry, the Maxwell equations reduce to a Helmholtz-type wave equation for the transverse electric field, which also assumes the form (1) but with and , where is the free-space permeability and denotes the transverse electric field. It follows from this that the photonic solutions to the unperturbed equation also have the form (2), where (here a vector) denotes the circular polarization (helicity) state of the photon as determined by . The perturbation term in (1) for the photon case has the well-known form Snyder and Love (1983) .

A principal result of this paper is that the perturbation for the photon case also contains a spin-orbit term, which for (weakly guided light fields) is given by the same expression (3) as in the electron case, so that the physics of the spin-orbit interaction is completely analogous for electrons and photons in this regime. Specifically, (2) and (3) allow us to use perturbation theory to calculate the first-order corrections to the propagation constants due to the SOI for either particle, as

(4a)
(4b)

where (4b) gives for the special case with being the unit step function, and where is an -order Bessel function of the first kind. It follows directly from (4) that upon traveling a distance along the waveguide, a particle in the state picks up a phase of the form , which acts as a correction of magnitude to the particle’s propagation constant . The sign of this correction is determined by the product , such that the acquiring of the phase may be expressed via the transformation

(5)

Deferring the details of our derivation of the Hamiltonian (3) for the photon case to a future paper, we employ our result (5) to predict the SOI effects shown in Fig. 1. We then proceed to apply an intuitive geometric phase-based approach to the special case of a step-profile for , which allows us to identify the phase factor in (5) as a universal geometric phase associated with the SOI.

As discussed previously, we now consider the following distinct balanced superpositions of the monoenergetic, unperturbed eigenstates ,

(6a)
(6b)

which are represented pictorially in Figs. 1(a) and 1(b). An important similarity between (6a) and (6b) is that for each of these superpositions one of the contributing eigenstates has parallel SAM and OAM vectors (that is, the product is positive), while the other has anti-parallel SAM and OAM vectors ( negative); this allows the -dependent phase accumulation to manifest itself as the particle propagates down the waveguide. According to (5), upon propagating a longitudinal distance z, the respective states (6a) and (6b) evolve into

(7a)
(7b)

For a monoenergetic photon, (7a) describes a linearly polarized OAM eigenstate whose polarization vector rotates with increasing as shown in Fig. 1(c), such that in a Cartesian basis it can be written as . Similarly, the expectation value of a monoenergetic electron’s spin vector, which rotates in an similar manner, is . In contrast to (7a), (7b) describes a SAM eigenstate with a rotating orbital state, which has the same form for both particles (see Fig. 1(d)). These effects may be viewed as a spatial beating between two waves of identical frequency but with slightly different propagation constants which have been split by the SOI.

Figure 2: (a) Helical particle trajectory with constant radius and pitch . (b) The curve traced out by on the momentum-space unit sphere subtends solid angle .

As we have mentioned, each rotational SOI manifestation may also occur as a function of time 111For related free-space effects, see S. J. van Enk and G. Nienhuis, Phys. Rev. A 76, 053825 (2007).. In this case, the spin and orbital rotation effects may be viewed as temporal beating between waves with identical propagation constants but different frequencies , so that (7) still holds provided that the quantity is everywhere replaced by .

Proceeding to the geometric phase approach, we now consider an electron or photon propagating along a well-defined helical trajectory of constant radius and helix pitch as shown in Fig. 2(a), where is the angle that the unit momentum vector makes with the rotation axis of the helix. In Białynicki-Birula and Białynicka-Birula (1987), Białynicki-Birula and Białynicka-Birula studied an arbitrary particle with spin traveling along such a classical trajectory, in which the adiabatically varying vector traces out a closed circular curve on the momentum space unit sphere, as shown in Fig. 2(b). They found that the particle accumulates a geometric phase associated with the parallel transport of its spin due to its curvilinear motion, which after a single helical round trip can be written as . Here, denotes the handedness of the particle helicity, accounts for the handedness of the helical trajectory, is the particle spin as already defined, and is the solid angle subtended by the circle as seen from the origin, which may be expressed as (see Fig. 2(b)). In order to extend this result to an arbitrary number of helical cycles, we multiply by , so that may be written as a function of the axial particle position : .

We now apply this result to a photon (electron) traveling in a helical path near the interface of a step-index (potential) waveguide with normalized step height , such that the pitch angle approaches the critical angle for total internal reflection. In this case, we have (cf. Snyder and Love (1983)) so that and , which yields . Furthermore, in this paraxial regime we may associate the helicity handedness with the spin direction along the z axis, and the helix handedness with the sign of the OAM quantum number, so that and , respectively. With these replacements, the accumulated geometric phase then gives rise to the effective propagation constant shift ,

(8)

Although the geometric phase result (8) does not coincide exactly with the more accurate perturbative result (4b), their forms are seen to be strikingly similar when it is recognized that the factor in square brackets in (4b) is of order one when is near its maximal allowed value. Furthermore, in the classical limit of large OAM (), corresponding to the above helical path in a large waveguide, and in (4b). Equations (8) and (4b) are therefore in complete agreement for photons, where . For electrons however, , for which (8) yields half of the shift given by the more rigorous perturbative calculation. This apparent discrepancy can be explained by recalling that the result (8) assumed parallel transport of the spin for both particles. Although this assumption is consistent with our result for photons, our SOI Hamiltonian (3) actually causes the electron spin vector to precess at twice the rate of the photon polarization vector (cf. (7a) and subsequent discussion). One therefore expects the accumulated phase due to the electron spin evolution to be precisely double the amount predicted by (8), as we find. We conclude that the spin-orbit interaction dynamics of the electron and photon are identical to first order in perturbation theory and have a common geometric origin, with the role of the electron’s potential energy being played by the permittivity in the photon case.

The effects in Figs. 1(c) and 1(d) allow for the reversible transfer of entanglement between the SAM and OAM degrees of freedom of two-particle states. Denoting the single-particle state in (6b) as (), we consider a purely polarization-entangled Bell state with two photons in spatially separated (Hermite-Gauss-like) spatial modes, . According to (7b), for ° this state will evolve under the SOI (in separate waveguides) to , where the single-photon state denotes a photon whose spatial state has been rotated ° from . By employing wave plates and spatial mode converters, it is possible to transform this state into , where and stand for ‘diagonal’ and ‘anti-diagonal’ (oriented at °) linear polarization, and stands for an OAM (Laguerre-Gauss-like) eigenstate. Finally, a second SOI interaction described by (7a) evolves the state into , where stands for horizontal polarization. This is a purely OAM-entangled Bell state.

This work was supported by NSF grant PHY-0554842.

References

  • Liberman and Zel’dovich (1992) V. S. Liberman and B. Y. Zel’dovich, Phys. Rev. A 46, 5199 (1992).
  • Onoda et al. (2004) M. Onoda, S. Murakami, and N. Nagaosa, Phys. Rev. Lett. 93, 083901 (2004).
  • Bliokh and Bliokh (2004) K. Y. Bliokh and Y. P. Bliokh, Phys. Lett. A 333, 181 (2004).
  • Dooghin et al. (1992) A. V. Dooghin, N. D. Kundikova, V. S. Liberman, and B. Y. Zel’dovich, Phys. Rev. A 45, 8204 (1992).
  • Hosten and Kwiat (2008) O. Hosten and P. Kwiat, Science 319, 787 (2008).
  • Bliokh et al. (2008) K. Y. Bliokh, A. Niv, V. Kleiner, and E. Hasman, Nat. Photonics 2, 748 (2008).
  • Berard et al. (2006) A. Bérard and H. Mohrbach, Phys. Lett. A 352, 190 (2006).
  • Tomita and Chiao (1986) A. Tomita and R. Y. Chiao, Phys. Rev. Lett. 57, 937 (1986).
  • Białynicki-Birula and Białynicka-Birula (1987) I. Białynicki-Birula and Z. Białynicka-Birula, Phys. Rev. D 35, 2383 (1987).
  • Rytov (1938) S. M. Rytov, Dokl. Akad. Nauk SSSR 18, 263 (1938).
  • Leary et al. (2008) C. C. Leary, D. Reeb, and M. G. Raymer, New J. Phys. 10, 103022 (2008).
  • Greiner (1997) W. Greiner, Relativistic Quantum Mechanics: Wave Equations (Springer, 1997).
  • Snyder and Love (1983) A. W. Snyder and J. D. Love, Optical Waveguide Theory (Springer, 1983).
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