Applied Physics A manuscript No.
(will be inserted by the editor)

Circularly Polarized Near-field Scanning Optical Microscopefor Investigations of Edge States of a Two-dimensional ElectronSystemShintaro Nomura · Syuhei Mamyouda · Hironori Ito · Yusuke Shibata ·Tomoya Ohira · Luno Yoshikawa · Youiti Ootuka · Satoshi Kashiwaya ·Masumi Yamaguchi · Hiroyuki Tamura · Tatsushi Akazaki

Received: date / Accepted: date

Abstract We report on investigations of the quantumHall chiral edge states using a near-field scanning optical microscope that enables us to irradiate circularly
polarized light from the probe tip with spatial resolution below the diffraction limit. We have found a clear
evidence for the formation of spin-split incompressible
strips near the edge of a two-dimensional electron system in high magnetic fields.
Keywords near-field scanning optical microscope ·quantum Hall effect · spin injection

1 Introduction
A near-field scanning optical microscope (NSOM) [1,2] has been intensively utilized to investigate opticalproperties of semiconductors at spatial resolution below the diffraction limit. NSOMs have been successfullyproviding a method to clarify phenomena closely related to charge distributions and the potential profiles
in semiconductors such as ground- and excited-statesin single self-assembled quantum dots [3], localization
This work was partly supported by Kakenhi Nos. 25103704,26610079, 15H03673.
S. Nomura · S. Mamyouda · H. Ito · Y. Shibata · T. Ohira ·L. Yoshikawa · Y. Ootuka
Division of Physics, Univ. of Tsukuba, 1-1-1 Tennoudai,Tsukuba 305-8571, Japan
Fax: +81-29-8536618
E-mail: nomura.shintaro.ge@u.tsukuba.ac.jp
S. Kashiwaya
National Institute of Advanced Industrial Science andTechnology, 1-1-1 Umezono, Tsukuba, 305-8568, JapanM. Yamaguchi · H. Tamura · T. Akazaki
NTT Basic Research Laboratories,Wakamiya, Atsugi, 243-0198, Japan

3-1

Morinosato-of the electrons in the random potential [4], imagingof excitons and biexcitons in naturally occurring quantum dots [5], and the edge of a two-dimensional electronsystem (2DES) in high magnetic field [6]. By contrast,
applications of NSOMs to investigate spin properties ofsemiconductors have been very limited, mainly becauseof the difficulty in emitting or detecting circularly polarized light using an NSOM probe tip since the polarization is disturbed by birefringence induced by small
tensions or torsions at the NSOM probe tip. Here we
report on our successful development of circularly polarized NSOM and investigations of the spin-dependent
properties of the edge states of a 2DES [7].

2 Methods
2.1 Experimental
We used a method to control the polarization of thelight emitted from an NSOM probe by controlling thepolarization of the incident light with a Berek compensator [7]. A double tapered NSOM probe was preparedby the method described in the literatures [8, 7]. We
have fabricated an NSOM probe tip with an aperture
with good axial symmetry by focused ion beam slicingof the apex of the probe tip. Furthermore, cares havebeen taken to avoid any stress or torsion by twisting or
bending to minimize possible extrinsic birefringence inhigh magnetic field region using a dilution refrigerator
specially designed for this purpose. This minimizes possible birefringence accompanied by the Faraday effectfor a diamagnetic material [9]. The compensation parameter of the Berek compensator is mostly explainedby the extrinsic birefringence added by a single turn
coil of the optical fiber with radius (r) of 0.25 m that

2Shintaro Nomura et al.

is located outside of the cryostat and is mechanicallysupported by an aluminum rail as shown in Fig. 1 inorder to fix the path of the optical fiber.
We used a Hall-bar structure of a GaAs/Al0.3 Ga0.7 As
single heterojunction with the mobility and the electron
density of 180 m2 /Vs and 4.6 × 1011 cm2 , respectively.
The optical excitation power was 1.1 nW at the excitation photon energy of 1.5140 eV, which is 5.7 meVabove the onset of the absorption of GaAs single heterojunction. Measurements were performed using a tube
piezoscanner and a piezoelectric inertial sliding stageat 250 mK in magnetic fields perpendicular to the sample surface in a dilution refrigerator. Photovoltage between the ohmic contacts 1 and 2 in Fig. 1 was detectedsynchronously with a lock-in amplifier at 159 Hz.
2.2 Theory
The electronic structure of spin-resolved states near thesample edge in perpendicular magnetic field B is calculated based on the local-spin-density approximation
formalism [7, 10, 11]. The Hamiltonian is given by
H = H0 + Vc (r) + VH (n, r) + Vxs (n↑ , n↓ , r) +Fig. 1 Schematics of measurement setup. The photo voltage
between the ohmic contacts 1 and 2 is measured by scanningthe position of the NSOM probe on the surface of a Hallbar structure. Magnetic field is applied perpendicular to thesurface of the sample.

g c µBsz Bh̄(1)whereh̄2
H0 = − ∗2m"∂2∂2+−∂x2∂z 2eBx
1 ∂+i ∂yh̄

2 #(2)is the kinetic energy in the Landau gauge A = (0, Bx, 0)
and Vc , VH , and Vxs are the confinement potential, theHartree term, and the exchange-energy term, ns (r) is
the electron charge density for spin s =↑, ↓ at finitetemperature, and gc , µB , and m∗ are the effective electron g-factor, the Bohr magneton, and the electron effective mass. A plane-wave basis set is used for they-direction. The center of the cyclotron-motion X is2
given by X = −lB
ky , where lB and ky are the magnetic length and the wavevector in the y-direction. The
higher-order finite difference method [10, 12] is used in
two-dimensional grids of 690 × 7 and 690 × 33 per unit
cell for the calculations of the wave function and thepotential, respectively, for the x- and z directions. Theconfinement potential is given by Vc (r) = Vl (x)+Vz (z).
We consider a quantum wire structure with a widthof 3150 nm, assuming lateral confinement potentials ofVl (x) = V0 (x) + V4 (x), and Vl (x) = V0 (x) + V2 (x). Weassume V0 = 1000 eV for x < 0 and x > 3150 nm
and 0 eV for 0 ≤ x ≤ 3150 nm, and consider V4 (x) =22C4 (x − x0 )4 , and V2 (x) = m2 ω0 (x − x0 ) as shown inFig. 2, where we use x0 = 2500 nm, C4 = 8.37 × 10−15Fig. 2 Lateral confinement potentials assumed in the calculations, (i) fourth-order polynomial and (ii) parabolic confinement potentials.

eV/nm4 , and h̄ω0 = 0.3465 meV that give the depletion layer thickness of 134 nm and determine the sizeof the edge states. For the vertical confinement potential, we set Vz (z) = 0 eV for 90 ≤ z ≤ 115 nm and0.270 eV elsewhere. Material parameters for GaAs andAlAs can be found in the literatures [13]. Details of thecalculation can be found elsewhere [7]Circularly Polarized Near-field Scanning Optical Microscope

3Fig. 3 Calculated electron densities near the sample edge for (a) ν = 5.4 and (b) ν = 6.3, by using V4 (x). The black curve
denotes the total density and the red and blue curves denote the densities for up- and down-spin electrons, respectively, asfunctions of x. νL denotes the local electron filling factor. Calculated subband structures for (c) ν = 5.4 and (d) ν = 6.3
as functions of the center of the cyclotron motion X. The red and blue curves denote the subbands for up- and down-spin
electrons, respectively. wa and wb denote the widths of the innermost incompressible strips. N denotes the Landau level index.
The origin of the energy is taken at the Fermi level.

Fig. 4 Calculated occupations near the Fermi level as definedby Eq. (3) for (a) fourth-order polynomial and (b) parabolic
confinement potentials as functions of X. w+ and w− denote
the widths of the innermost incompressible strips at ν + andν − , respectively.

3 Results and Discussions
3.1 Compressible and incompressible strips
The alternating strips of the compressible and incompressible liquids are formed near the edge of the 2DESin a magnetic field due to the screening of the confinement potential [14–17, 10, 18] as shown in Fig. 3,
calculated by using V4 (x). There is a region of constant electron density with a finite energy gap at theFermi level. The spin-unpolarized incompressible strip(I) is formed in the case where the energy gap is opened
due to the cyclotron energy h̄ωc , and the spin-split incompressible strip (Is ) is formed due to the exchange
energy-enhanced spin gap [19] in high magnetic fields
as shown in Fig. 3. In-between the spin-unpolarized
and spin-split incompressible strips, there are regionsof smoothly varying electron density and of constantsubband energy of either up- or down-spin electrons,
called the spin-polarized compressible strips (C↑ , C↓ ).
Figure 4 shows calculated occupations near the Fermi
level for V4 (x) and V2 (x) as defined byPE F =′′1
f (Ej,ky ,↑ (B)) − f (Ej,ky ,↓ (B))
f ′ (EF ) j′X(3)

where f (E) is the first derivative of the Fermi distribution function at T = 0.25 K, and Ej,ky ,s (B) is the4Shintaro Nomura et al.

Fig. 5 Color mappings of photovoltage as functions of lateral position and magnetic field for (a) right and (b) left circularly
polarized light at B > 0, and (c) left and (d) right circularly polarized light at B < 0 at the excitation energy of 1.5140 eV.
Solid circles in (a) and (b) denote the positions where the photovoltage is larger in LCP than in RCP.

energy of the jth electron state with wavevector ky andspin s. The red (blue) in Fig. 4 indicates the regions
where up- (down-) spin electrons occupy the subband
at the Fermi level. The positions of the incompressible
strips I and Is as indicated by the white regions inFig. 4 move inwards of the sample with increase in themagnetic field. Note here that the positions of I and Is
depend on the curvature of the lateral confinement potential. The positions of I and Is are closer to the edgeof the sample for harder lateral confinement potential
V4 (x) as compared to V2 (x).
3.2 Circular polarization dependence of photovoltage
mapping
Our circularly polarized NSOM enables us to injectspin polarized electrons locally to the 2DES layer. Figure 5(a) and 5(b) show mappings of photovoltage forright and left circularly polarized light excitation, respectively, as functions of lateral position and magnetic
field. Upon illumination of the heterojunction sample,
electron-hole pairs are created in the thick GaAs layer.
The photoinduced holes move to the rear side whereas
the electrons move to the front side of the sample dueto the strong vertical electric field in the heterojunction
sample. The electrons optically created near the edge ofthe sample either diffuse to the compressible strips at

the same side of the sample of the laser spot or to thecompressible strips at the opposite side of the sample
across the bulk region. The diffusion current is balancedby the Hall current, leading to the change of the chemical potential of the edge states [20]. This change of thechemical potential is detected as the Hall photovoltage
between the contacts 1 and 2 in Fig. 1.
Periodic photovoltage signals are observed correlated with the bulk electron filling factor ν. The photovoltage is vanishingly small at the integer ν as shown inFig. 5 at the condition for the quantum Hall effect. The
positive photovoltage is observed in Figs. 5(a) and 5(b)at the bulk electron filling factor slightly larger than theinteger (ν + ) where the diffusion current across the bulk
region is small. This is a consequence of the large widthof the innermost I or Is at ν + (w+ ) as shown in Fig.
4. By contrast, the negative photovoltage is observedat the bulk electron filling factor slightly smaller than
the integer (ν − ), where the diffusion current across thebulk region is large because of the small width of theinnermost I or Is at ν − (w− ). Inverting the directionof the magnetic field as shown in Figs. 5(c) and 5(d)reverses the sign of the photovoltage.
Clear circular polarization dependence of the photovoltage is observed as shown in Fig. 5. Figures 5(a) and5(b) show that the photovoltage at 3.5 T (ν = 5.4) islarger in left circular polarization (LCP) where down-Circularly Polarized Near-field Scanning Optical Microscopespin electron is optically created than in right circularpolarization (RCP) where up-spin electron is created.
Similarly, the photovoltage at ν = 7.3 and 9.3 is larger
in LCP than in RCP. This circular polarization dependence of the photovoltage is reversed at B < 0.
The observed circular polarization dependence ofthe photovoltage is understood by the type of the innermost incompressible strip, whether it is Is or I, that
separates the bulk and the edge regions [7] as schematically shown in Fig. 6. A spin-split incompressible strip
Is with a width wa separates the bulk and the edge
regions for 2m − 1 < ν < 2m, for m integer as shownin Fig. 3(c). Consider here the case where up- or downspin electrons are optically created in the edge region inFig. 3(c). The subband energy of the up-spin electronis flat on C↑ adjoining to the innermost incompressible
strip Is at νL = 5, whereas the subband energy of thedown-spin electron increases with increase in X. Consequently, the diffusion current of the optically created
up-spin electrons from the edge across the bulk region islarger than that of the down-spin electrons as schematically shown in Fig. 6(a), resulting in larger photovoltage
in LCP (V+LCP ) for creating down-spin electrons thanphotovoltage in RCP (V+RCP ) as shown in Figs. 5(a)and 5(b). At 2m < ν < 2m + 1, a spin-unpolarized incompressible strip I with a width wb separates the bulk
and the edge regions as shown in Fig. 3(d). Because I
is formed due to the cyclotron energy h̄ωc , this strip ismore robust to disorders than Is which is formed dueto the exchange energy-enhanced spin gap as schematically shown in Fig. 6(b). As a consequence the diffusion
current of both the up- and down-spin electrons fromthe edge across the bulk region is small. This explains
the small circular polarization dependence of the observed photovoltage in this case.
4 Conclusions
We have demonstrated successful optical spin injection
using a circularly polarized near-field optical microscope.
Our method should be widely applied to investigate
spin dependent phenomena in nanostructured materials.
Acknowledgements We acknowledge the stimulated discussion in the meeting of the Cooperative Research Projectof the Research Institute of Electrical Communication, Tohoku University.

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