Anisotropic Optical Spin Hall Effect in Semiconductor Microcavities

Anisotropic Optical Spin Hall Effect in Semiconductor Microcavities

A Amo Laboratoire Kastler Brossel, Université Pierre et Marie Curie, Ecole Normale Supérieure et CNRS, UPMC Case 74, 4 place Jussieu, 75252 Paris Cedex 05, France    T C H Liew Centre for Quantum Technologies, National University of Singapore, Singapore 117543    C Adrados Laboratoire Kastler Brossel, Université Pierre et Marie Curie, Ecole Normale Supérieure et CNRS, UPMC Case 74, 4 place Jussieu, 75252 Paris Cedex 05, France    E Giacobino Laboratoire Kastler Brossel, Université Pierre et Marie Curie, Ecole Normale Supérieure et CNRS, UPMC Case 74, 4 place Jussieu, 75252 Paris Cedex 05, France    A V Kavokin School of Physics and Astronomy, University of Southampton, Highfield, Southampton SO17 1BJ, UK Marie-Curie Chair of Excellence “Polariton devices”, University of Rome II, 1, via della Ricerca Scientifica, Rome, 00133, Italy    A Bramati Laboratoire Kastler Brossel, Université Pierre et Marie Curie, Ecole Normale Supérieure et CNRS, UPMC Case 74, 4 place Jussieu, 75252 Paris Cedex 05, France
September 16, 2019
Abstract

Propagating, directionally dependent, polarized spin-currents are created in an anisotropic planar semiconductor microcavity, via Rayleigh scattering of optically injected polaritons in the optical spin Hall regime. The influence of anisotropy results in the suppression or enhancement of the pseudospin precession of polaritons scattered into different directions. This is exploited to create intense spin currents by excitation on top of localized defects. A theoretical model considering the influence of the total effective magnetic field on the polariton pseudospin quantitatively reproduces the experimental observations.

pacs:
71.36.+c, 72.25.Fe, 72.25.Dc

Introduction.- The field of spintronics has come a long way since the study of magnetic dependent electron transport Tedrow1971 ; Julliere1975 and magnetic injection of electron spins Johnson1985 that began in the 1970s. The spin of an ensemble of particles, such as electrons, can encode a bit of information and today this is exploited to produce non-volatile memory elements with high read/write speeds, high density and low power consumption Gerrits2002 .

Semiconductors have the potential for lower operating power and smaller size than their metallic counterparts, and semiconductor spintronics Awschalom2007 has been developing in parallel with metallic spintronics, however with some difficulties for the spin injection Hanbicki2003 . An alternative method for the creation of spin currents in semiconductors is provided by the spin Hall effect (SHE) Dyakonov1971 ; Kato2004 ; Wundrlich2005 , which leads to a separation of spin-up and spin-down polarized electrons in both real and momentum space. However, this technique presents the problem of the rapid spin decay and dephasing due to the strong carrier-carrier scattering.

Recently, spin currents were generated in a different system, a semiconductor microcavity, using the so-called optical spin Hall effect (OSHE) Leyder2007 . This optical analogue of the SHE created separated spin currents of polaritons in real and momentum space that traveled a distance of the order of , evidencing the realistic potential applications of polariton spin on the implementation of integrated polarization based optical gates Liew2008 . In this letter we show that we can use anisotropic fields to efficiently generate such spin currents in a preferred direction at engineered points of the sample.

Semiconductor microcavities are planar nanostructures designed to strongly couple light and matter; a pair of highly reflective mirrors confines cavity photons which are resonant with the exciton of a quantum well embedded in the cavity. The normal modes of such a system are exciton-polaritons, neutral particles formed from the superposition of excitons and photons  Kavokin2007 , which do not suffer from the fast dephasing experienced by electrons.

The OSHE originates from the combined influence of the polarization splitting of transverse electric and transverse magnetic modes (TE-TM splitting) and Rayleigh scattering on polaritons that are excited by an optical pump Kavokin2005 . The TE-TM energy splitting arises from the dependence of the polariton energy on the angle between the polariton momentum , and its dipole oscillation direction, determined by the plane of polarization of the linearly polarized excitation. The role of the Rayleigh scattering is to provide the system with polaritons with a pletora of different momenta after pumping with a given . In a generalized form, the effect of the TE-TM splitting on the polarization of exciton-polaritons can be conveniently described within the pseudospin formalism by the introduction of an effective magnetic field whose orientation depends on the polariton wave-vector. The pseudospin depicts the polariton polarization state, while the effective field is an optical analogue of the Rashba-field acting upon electron spins in semiconductor crystals lacking inversion symmetry Dyakonov2007 . The effective field results in a -dependent precession of the polariton pseudospin, which leads to the separation of spin up and spin down polaritons in the Rayleigh ring Leyder2007 .

In realistic microcavities, the TE-TM splitting competes with the polarization splitting generated by the in-plane anisotropy of the sample, caused by interface fluctuations, photonic disorder or local strains Klopotowski2006 ; Krizhanovskii2006 ; Kasprzak2006 ; Glazov2007 . Anisotropy results in the appearance of a wave-vector independent linear polarization splitting equivalent to a supplementary uniform effective magnetic field acting upon the polariton pseudospins. In this letter we experimentally study the polarization dynamics of exciton-polaritons in the presence of such a field and of the TE-TM splitting, and demonstrate the appearance of the anisotropic OSHE. Furthermore, the anisotropic field enhances the spin precession of polaritons moving along directions given by the field orientation. This is used to efficiently generate spin currents at engineered points in the sample, where a localized photonic defect, creating an isolated peak in the polariton potential, is present. Our results are in agreement with a theoretical model based on the spinor Schrödinger equation, which accounts for both the TE-TM splitting and anisotropy effective fields.

Theory.- Given their long decoherence time Langbein2007 , polaritons can be described by a two-component wavefunction, , where represents either spin-up () or spin-down () polaritons (here we consider only lower branch polaritons). These two spin components are directly coupled to the circular polarizations of external light, allowing for their optical excitation and polarization resolved detection. The two-dimensional (spinor) wavefunction obeys a Schrödinger equation, which can be written Liew2009 :

(1)

The Hamiltonian can be written:

(2)

where represents the (non-parabolic dispersion) of lower branch polaritons, is the Pauli matrix vector and is an effective magnetic field. is given as the sum of a field representing the TE-TM splitting Kavokin2005 (this field depends on the direction of the polariton wavevector, ) and an effective field arising from the anisotropy in the microcavity heterostructure (this field is wavevector independent). These fields are illustrated in Fig. 1a.

Figure 1: (color online) (a) The TE-TM splitting (grey arrows) and polarization anisotropy (grey dashed arrows) can be represented by effective magnetic fields, which act on the polariton pseudospin vector (Stokes vector). The total effective magnetic field (black arrows) causes the polariton pseudospin vectors to precess. Panels (b-d) illustrate the expected evolution of the pseudospin of polaritons that have elastically (Rayleigh) scattered from the pump state (at ) to a ring in reciprocal space with different planes of linear polarization of excitation. The purple arrow in the center depicts the initial pseudospin. Pseudospins pointing out of the plane give rise to circularly polarized emission.

represents the polariton potential. We will consider two kinds of profile - one representing the disorder, which is generated by a stochastic field Savona2006 characterized by some correlation length and a root mean squared amplitude ; and one representing an isolated peak. The continuous wave optical pump is represented by:

(3)

where the pump is Gaussian shaped with energy , linewidth , spot-size and amplitude and polarization given by . Unlike the experiments in Refs. Leyder2007 ; Liew2009 we are working with a pump oriented at normal incidence (which excites polaritons with zero in-plane wavevector, ). Provided the pump energy is tuned above the energy , Rayleigh scattering still allows the excitation of a ring in reciprocal space (see Fig. 2a), which is important for the OSHE. Note that Rayleigh scattering alone preserves the polariton polarization.

The decay of polaritons caused by exciton recombination and the escape of photons through the Bragg-mirrors of the microcavity is modeled phenomenologically with a lifetime, , which can be related to the exciton and photon lifetimes, and respectively, by , where and are the Hopfield coefficients HaugKoch ; Laussy2004 .

The reason for defining the effective magnetic field is that it allows a qualitative understanding of the combined effects of TE-TM splitting and anisotropy. The polarization state of polaritons can be represented by the pseudospin vector , equivalent to the Stokes vector for light, where , , and . Graphically, in the Poincaré sphere, and are the pseudospin coordinates laying on the equatorial plane, which represent the degree and plane of the linearly polarized component of the polarization, while describes its circularly polarized component Leyder2007 . The field causes the pseudospin vector to precess, giving rise to the appearance of circularly polarized emission even under linearly polarized excitation. Figures 1b-d illustrate the pseudospin precession for different linear polarizations of the pump.

Figure 2: (color online) (a) Lower polariton branch (LPB) luminescence under out of resonance excitation at (indicated by the red spot). Resonant Rayleigh scattering takes place to LPB states marked by arrows. (b) Energy of the photoluminescence peak at under circularly polarized excitation as a function of the angle of the detected linear polarization plane (). (c) Real space transmitted intensity in the presence of the shallow disorder usual in standard microcavities, and (d) in presence of a localized photonic defect in the center of the spot. Each panel has been normalized to show the best visibility.

Experimental results.- The sample used in our experiments is a , InGaAs based microcavity with a Rabi splitting of 5.1 meV. All our experiments were performed at 5 K, at zero exciton-photon detuning, using a linearly polarized single mode laser as the excitation source on a spot of 48 in diameter. Real and momentum space images of the emission (circularly polarized resolved) were collected in transmission geometry in two high-definition CCD cameras. The size and direction of has been obtained by analyzing the linear-polarization resolved photoluminescence emission of the LPB at , where the TE-TM splitting vanishes. A splitting due to the anisotropy-related effective field of about 0.04 meV can be observed, as depicted in Fig. 2b.

Figure 3: (color online) Far-field circular polarization degree detected experimentally (left) compared to theory (right) for the cases of horizontal (a, b), vertical (c, d) and diagonal (e, f) linearly polarized pump excitation. These three cases correspond to Figs. 1b-d, respectively. Parameters: m, meV, meV, meV, m, ps, ps. The polarization splitting arising from anisotropy and TE-TM splitting were each assumed equal to meV. The shadow in panels (a), (c) and (e) is a block of the pump field to avoid saturation of the detector.

We have considered the anisotropic spin Hall effect at two different locations on our sample. At the first location (Fig. 2c) the polariton potential is the typical disordered potential present in microcavities, evidenced via the meshed pattern in the real space image of the transmission intensity. In the second location, just away from the first one, excitation is performed on top of a photonic defect (Fig. 2d). The presence of the defect results in Airy ring-like patterns which arise from the interference of the pumped polaritons and those scattered into the Rayleigh ring. The observed fringe separation is of which corresponds to the momentum of the scattered polaritons ().

Figure 3 shows, for the first location with shallow disorder (Fig. 2c), the measurement of the circular polarization degree (z-component of ) in momentum space for different pump polarizations. The results are quantitatively reproduced by the numerical solutions of Eq. 1.

Under vertical (Fig. 3a-b) and horizontal (c-d) planes of linear polarization of excitation, only two quadrants of circular degree of polarization are visible. This is a direct consequence of the presence of the intrinsic momentum independent effective magnetic field , which is canceled by the TE-TM field in the positive diagonal direction in the far field (as depicted in Fig. 1a). Polaritons scattered into this diagonal direction do not feel the action of any field and their linearly polarized pseudospin does not precess, not giving rise to any circularly polarized component. On the other hand, the total field is enhanced in the opposite diagonal direction, giving rise to an increased degree of circular polarization with respect to the case of .

In the absence of , four alternating circular polarization quadrants would be expected as a consequence of the distribution of the TE-TM related magnetic field in the Rayleigh circle, independently of the polarization plane of the injected polaritons Leyder2007 , as the characteristic signature of the standard OSHE. In the presence of we can recover the four quadrants if we rotate the polarization plane of the excitation with respect to the direction of the intrinsic magnetic field so that they are parallel, as shown in Fig. 3e-f. For such injected pseudospin the composition of and the TE-TM related field are canceled at four points in the Rayleigh circle, which delimit the four quadrants (see Fig.1d).

Figure 4: (color online) Far-field [near field] degree of circular polarization detected experimentally (a) [c] and compared to theory (b) [d] for the case of vertically polarized excitation in the presence of a peak in the polariton potential, in the center of panels (c-d). The parameters were the same as in Fig. 3, except that the disorder potential was replaced by a Gaussian shaped defect of height 1meV and full with at half maximum equal to m. Dotted lines in panel (c) show the region where the spin currents flow, in the direction given by the arrow.

We can take advantage of the enhancement in the spin precession related to the existence of the anisotropic field to observe spin currents. They can be directly generated if excitation is performed at the location where the photonic defect is present (Fig. 2d). Here, under vertically polarized excitation, the anisotropic field gives rise a distribution of the circular polarization degree in reciprocal space (Fig. 4a-b) similar to that of Figs. 3a-b. The presence of the defect results in a strengthening of both the total intensity and the polarization degree (by a factor 2.7) of the Rayleigh signal. The real space images (Fig. 4c-d) clearly show spin currents of polaritons scattered from the defect in the negative diagonal direction. These spin currents could not be observed in the absence of a defect because in this case scattering takes place homogeneously all over the excitation spot. If we turn by 90 the plane of the polarization of excitation, spin currents follow the same direction with opposite sign (not shown). Note that the concentric ring-like structure of Fig. 2d is still observable in the polarization degree, both in the experimental and simulation images.

Conclusion.- The OSHE relies on the combined effects of Rayleigh scattering of polaritons and pseudospin precession, well described by the introduction of effective magnetic fields physically representing the polarization splitting caused by TE-TM splitting and/or sample anisotropy. The Rayleigh scattering can be engineered to occur at specific points in the microcavity sample, where directional spin currents are efficiently generated and enhanced due to the presence of the intrinsic anisotropic fields. These features can be exploited for the implementation of integrated light-polarization based logic gates Liew2008 .

Acknowledgements.- We are very grateful to R. Houdré for providing us with the microcavity sample. This work was supported by the IFRAF. A.A. was funded by the Agence Nationale pour la Recherche, A.B. is a member of the Institut Universitaire de France.

References

  • (1) P M Tedrow and R Merservey, Phys. Rev. Lett., 26, 192 (1971).
  • (2) M Julliere, Phys. Lett. A, 54, 225 (1975).
  • (3) M Johnson and R H Silsbee, Phys. Rev. Lett., 55, 1790 (1985).
  • (4) Th Gerrits,et al., Nature, 418, 509 (2002).
  • (5) D D Awschalom and M E Flatté, Nature Phys., 3, 153 (2007).
  • (6) A T Hanbicki, et al., Appl. Phys. Lett., 82, 4092 (2003).
  • (7) M I Dyakonov, V I Perel, Phys. Lett. A, 35, 459 (1971).
  • (8) Y K Kato, et al., Science 306, 1910 (2004).
  • (9) J Wunderlich, et al., Phys. Rev. Lett., 94, 047204 (2005).
  • (10) C Leyder, et al., Nature Phys., 3, 628 (2007).
  • (11) T C H Liew, et al., Phys. Rev. Lett., 101, 016402 (2008).
  • (12) A V Kavokin, et al., Microcavities, Oxford University Pres (2007).
  • (13) A V Kavokin, et al., Phys. Rev. Lett., 95, 136601 (2005).
  • (14) See e.g. W Jantsch, Z Wiliamowski, in Spin Physics in Semiconductors ed by M I Dyakonov, Springer, Berlin, 2007, p. 179.
  • (15) Ł. Kłopotowski, et al., Solid State Commun. 139, 511 (2006).
  • (16) D N Krizhanovskii, et al., Phys. Rev. B, 73, 073303 (2006).
  • (17) J Kasprzak, et al., Nature, 443, 409 (2006).
  • (18) M M Glazov, et al., Phys. stat. sol. (c), 4, 638 (2007).
  • (19) W Langbein, et al., Phys. Rev. B 75, 075323 (2007).
  • (20) T C H Liew, et al., Phys. Rev. B, 79, 125314 (2009).
  • (21) V Savona and W Langbein, Phys. Rev. B, 74, 075311 (2006).
  • (22) H Haug, S W Koch, Quantum theory of the optical and electronic properties of semiconductors, Singapore: World Scientific (1994).
  • (23) F P Laussy, et al., J. Phys.: Condens. Matter, 16, S3665 (2004).
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