JP2006032570A - Spin filter and spinning state separating method - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a spin filter capable of obtaining a spin deflection angle sufficient for separating the spinning state of different carriers propagating through a semiconductor, and to provide a spinning state separating method. <P>SOLUTION: When a gate insulation layer 12 of different thickness is inserted in the y-axis direction, an effective gate voltage being applied to a two-dimensional electron gas channel 14 has a gradient in the spin filter 10, and the g-factor of the two-dimensional electron gas channel 14 beneath a gate electrode 11 causes spatial gradient in the y-axis direction. When an electron spin propagates through that space in the x-axis direction, spin upward carrier and downward carrier receive a force in reverse direction and being separated spatially. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

  The present invention relates to a spin filter and a spin state separation method for separating spin states of carriers propagating in a semiconductor.

  In conventional semiconductor devices, only the charge of electrons has been used. Electrons have a spin degree of freedom as well as an electric charge, but until now no device has actively used the spin properties of electrons. Recently, semiconductor devices are reaching the limit of miniaturization, and the field of spintronics has been attracting attention as a new device with an unprecedented function by simultaneously using the "charge" and "spin" possessed by electrons. It has come to be. In order to realize a spin device in a semiconductor, an operation method has been established: (1) generation of spin-polarized carriers, (2) spin transport, storage, arithmetic operation, and (2) final spin state detection. There is a need to.

  Among these, as the most established technique for generating spin-polarized electrons in a semiconductor, there is a method of exciting spin-polarized electrons from a valence band to a conductor with circularly polarized light. However, in this method, it is impossible to obtain 100% spin-polarized electrons due to the restriction by the selection rule, and holes are generated in pairs with electrons. There has been a problem that the relaxation time of cannot be made sufficiently long.

  Further, it has been theoretically pointed out that spin injection from a ferromagnetic electrode to a semiconductor makes it difficult to obtain a large degree of spin polarization in the semiconductor due to the difference in conductance between the metal and the semiconductor. As a method for overcoming such a difference in conductance, a method of inserting a tunnel barrier between a ferromagnet and a semiconductor has been proposed, but at present, a large degree of spin polarization has not been obtained.

  Recently, it has become possible to synthesize III-V dilute magnetic semiconductors in which Group III is partially substituted with Mn, but also in this regard, carriers are p-type and spin relaxation is fast due to the influence of spin-orbit interaction. Also, there is a problem that the ferromagnetic dislocation temperature (Curie temperature Tc) is below room temperature (Tc = 110 K).

Under such circumstances, from the viewpoint of generation and transport of spin-polarized electrons, and detection of the spin state, a spin filter using a non-uniform magnetic field using the Stern-Gerach effect (hereinafter referred to as SG effect) has been proposed. (For example, see Non-Patent Document 1.)
FIG. 8 is a diagram conceptually showing the SG effect. Stern-Gerlach (1922) developed a spin-up and down-spin by conducting an experiment in which silver (Ag) atoms having a spin 1/2 are removed from the oven furnace through a slit and passed through this non-uniform magnetic field gradient. Succeeded in spatially separating atoms e ₁ and e ₂ each having

Non-Patent Document 1 proposes a spin filter that combines a one-dimensional or two-dimensional electron gas of GaAs (gallium arsenide) and a non-uniform magnetic field using the SG effect.
J. Wroebel, T. Dietl, K. Fronc, A. Lusakowski, M. Czeczott, G. Grabecki, R. Hey, and KH Ploog, Physica E 10, 91 (2001).

  However, since the spin filter using the SG effect described above has a high electron velocity in the semiconductor channel and the interaction time passing through the inhomogeneous magnetic field is short, a sufficient deflection angle of the upward and downward spins cannot be obtained. It was impossible to realize.

  In addition, inhomogeneous magnetic field using a magnetic material, it is difficult to make the component perpendicular to the two-dimensional electron gas zero, and the perpendicular component of this magnetic field acts as Lorentz force on electrons, so spin upwards and downwards. Regardless, there is a problem that it works as an effect of bending the trajectory in a certain direction and prevents the carrier spin space separation due to the SG effect.

Originally, the SG effect experiment was performed using silver atoms with zero charge and spin 1/2 as described above, and therefore the SG effect of charged atoms or electrons is subject to Lorentz force. Therefore, it has been predicted that it is difficult to verify the SG effect. The reason is that uncertainty is generated in the spin deflection angle due to the Lorentz force. The reason is as follows. According to electromagnetism, the magnetic field B satisfies ▽ · B = 0 because there is no magnetic charge.

Here, for the sake of simplicity, assuming that ∂B _x / す_ると_x = 0 in the coordinate system of FIG. 8, if the magnetic field gradient ∂B _y / ∂y in the y-axis direction is not zero, it is perpendicular to the carrier propagation direction. There is also a non-zero magnetic field gradient ∂B _z / ∂z = − (∂B _y / ∂y) in the z-axis direction (in this case, the magnitude of the magnetic field component in the z direction | ∂B _z / ∂z | Maximum).

Due to the presence of the magnetic field gradient ∂B _z / ∂z in the z-axis direction, electrons distributed in the z-axis direction receive different forces, and an uncertainty Δφ _SG occurs in the spin deflection angle. That is, it is pointed out that carriers with electric charges are subjected to Lorentz force, and therefore the spin deflection angle is uncertain, and the widening of this deflection angle is an essential problem in the observation of the SG effect.

  The present invention has been made in order to solve the above-described problems. A spin deflection angle sufficient to separate different spin states of carriers propagating in a semiconductor can be obtained without using a non-uniform magnetic field. It is an object to provide a spin filter and a spin state separation method that can be obtained.

  In order to achieve the above object, the present invention according to claim 1 is a spin filter for separating carriers for each spin state of carriers propagating in a semiconductor, in a direction perpendicular to a direction in which the carriers propagate. A uniform magnetic field applying means for applying a uniform magnetic field; a semiconductor channel for confining the carrier and propagating the carrier; and a voltage applying means for applying a gate voltage to the semiconductor channel. The g-factor of the semiconductor channel is controlled to be non-uniform with a spatial gradient in the same direction as the applied magnetic field direction.

  According to a second aspect of the present invention, in the first aspect of the present invention, the spin filter inserts layers having different thicknesses on the semiconductor channel, so that the g-factor of the semiconductor channel has a spatial gradient. Features.

  According to a third aspect of the present invention, in the first aspect of the present invention, the gate voltage applying means includes a plurality of gate electrodes to be applied with different voltages, and the g-factor of the semiconductor channel has a spatial gradient. Features.

  The present invention according to claim 4 is the invention according to any one of claims 1 to 3, wherein an elastic scatterer is introduced into the semiconductor channel.

  According to a fifth aspect of the present invention, in the invention according to any one of the first to fourth aspects, an electrode for spin detection using a magnetic material is provided on the output side.

  The present invention according to claim 6 is the invention according to any one of claims 1 to 5, wherein an electrode for spin injection using a magnetic material is provided on the input side.

  The present invention according to claim 7 is a spin state separation method for separating carriers for each spin state of carriers propagating in a semiconductor, wherein the carriers are confined in a semiconductor channel for propagating the carriers. A uniform magnetic field is applied in a direction perpendicular to the propagation direction, a gate voltage is applied to the semiconductor channel, and the g-factor of the semiconductor channel is spaced in the same direction as the applied magnetic field direction by the gate voltage. It is characterized by controlling so as to be non-uniform with a gradient.

  According to an eighth aspect of the present invention, in the spin filter including the semiconductor channel according to the seventh aspect, a layer having a different thickness is inserted on the semiconductor channel, and a spatial gradient is applied to a g-factor of the semiconductor channel. It is characterized by having.

  According to a ninth aspect of the present invention, in the seventh aspect of the present invention, the gate voltage applying means for applying the gate voltage includes a plurality of gate electrodes with different voltages to be applied, and a space is provided in the g-factor of the semiconductor channel. It is characterized by having a gradient.

  According to a tenth aspect of the present invention, in the invention according to any one of the seventh to ninth aspects, an elastic scatterer is introduced into the semiconductor channel.

  The invention according to claim 11 is the invention according to any one of claims 7 to 10, characterized in that an electrode using a magnetic material is provided on the output side to detect the spin state of the carrier. To do.

  A twelfth aspect of the present invention is the method according to any one of the seventh to eleventh aspects, wherein an electrode using a magnetic material is provided on the input side, and spin-polarized carriers are injected. To do.

  According to the present invention, since the g-factor of the semiconductor channel can be controlled by the gate voltage, the Stern-Gerlach effect can be realized in the semiconductor using the spatial gradient of the g-factor.

  As a result, a spin deflection angle sufficient to separate different spin states of carriers propagating in a semiconductor can be obtained without using a non-uniform magnetic field.

  Hereinafter, embodiments of the present invention will be described with reference to the drawings.

<Basic matters>
First, basic matters that are preconditions for carrying out the present invention will be described. The basic matters described below are common to all embodiments of the present invention.

The g-factor depends on the semiconductor band structure and electron energy, and is given by the following equation (see AA Kiselev, EL Ivchenko, and U. Rossler, Phys. Rev. B58, 16353 (1998)).

Here, E is energy from the band edge of the conduction band and corresponds to Fermi energy. The Eg is the energy gap, g _o is the free electron g- factor, delta _so the separation energy due to spin-orbit interaction in the valence band, the 2p ² _cv / m _o interband matrix elements of the conduction band and the valence band It is. Therefore, the g-factor is a substance-specific parameter. However, recently, it has been experimentally shown that the g-factor value can be controlled by the gate voltage by changing the proportion of the existence probability between materials having different electron wave functions using the semiconductor heterostructure. (G. Salis, Y. Kato, K. Ensslin, DC Driscoll, AC Gossard, and DD Awschalom, Nature 414, 619 (2001), HW Jiang and E. Yablonovitch, Phys. Rev. B64, R041307 ( 2001), J. Nitta, Y. Lin, T. Akazaki, and T. Koga, Appl. Phys. Lett. 83,4565 (2003)).

FIG. 1 shows the gate voltage dependence of the g-factor obtained by the coincidence method in a semiconductor heterostructure in which InAs is inserted into an InGaAs channel. FIG. 1A shows each layer of the semiconductor, and FIG. 1B shows the potential energy and the existence establishment of electrons in the thickness direction of the semiconductor shown in FIG. 1A and 1B show that electrons are localized in the InAs channel. Further, according to FIG. 1C, it can be confirmed that the effective g-factor g ^* decreases as the gate voltage Vg increases, and changes from about 4 to about 3. This is because, by increasing the gate voltage, the existence probability <Φ _InAs > of the electron wave function originally present in the InAs channel having a large g-factor decreases, and the ratio existing in InGaAs having a small g-factor. By increasing <Φ _InGaAs >, the overall g-factor is changed by the gate voltage. That is,
g _total (E) = g _InAs (E) <Φ _InAs > + g _InGaAs (E) <Φ _InGaAs > (2)

It is. This result shows that the g-factor can be electrically controlled by controlling the leakage effect of the wave function by the gate voltage by designing the heterostructure of the semiconductor well. Also, as a result, in a system to which a uniform magnetic field is applied, if the g-factor is given a spatial gradient by the gate voltage, the spin separation energy gμ _B B due to the Zeeman effect changes spatially. Here, g is a g-factor, μ _B is a Bohr magneton, and B is a magnetic field. In the present invention, a spin filter is configured by the SG effect using the spatial gradient of the spin separation energy. The magnetic field may be a uniform magnetic field that is parallel to the semiconductor two-dimensional electron gas. Therefore, the present invention is characterized in that the magnetic field component in the z-axis direction shown in FIG. 8 can always be zero, and the effect of bending the carrier trajectory by the Lorentz force can be eliminated.

  Here, the SG effect shown in FIG. 8 will be described. The Hamiltonian due to the Zeeman effect is given by the following equation in the magnetic field B.

H _z = sgμ _B B (3)
Here, spin s = ± 1/2, g is a g-factor, μ _B is a Bohr magneton, and B is a magnetic field. This spatial change of Zeeman energy corresponds to the spatial change of potential and exerts a force on electron spin. For example, when a spatial gradient is given to the y-axis component of the magnetic field B shown in FIG.

However, spins that are upward and downward with respect to the y-axis direction receive forces in opposite directions, and separation occurs when the spin propagates through this spatial magnetic field gradient. The spin deflection angle φ _SG due to the SG effect is given as follows.

Here, Delta] t corresponds to the time the electron spin propagates in nonuniform magnetic field, which corresponds to result in a change in momentum Delta] p _y in the y-axis direction. p _x is the momentum component of the electron spin in the x-axis direction, and F _y · Δt is the impulse that the electron spin receives in the y-axis direction.

The main point of the present invention is that the g-factor that can be controlled by the gate voltage has a spatial gradient, and the spin upward carrier has a spatial gradient in the upward energy difference Δ = ± (1/2) gμ _B B. In other words, the spin filter is configured to apply a reverse force to the downward carrier and perform spatial separation. This corresponds to the realization of a spin filter function in which the spin separation energy is given a spatial gradient by the spatial gradient of the g-factor instead of the spatial gradient of the magnetic field B, in comparison with the SG effect described above. . In this case, since there is no spatial gradient of the magnetic field B, the magnetic field in the z-axis direction perpendicular to the two-dimensional digitized gas can be made zero, and the Lorentz effect that hinders the SG effect can be eliminated.

  As described above, in a conventional spin filter using a magnetic field gradient created by a ferromagnetic material, electrons have a charge together with spin, and therefore, the Lorentz force is generated by a magnetic field component perpendicular to the two-dimensional electron gas plane (xy plane). The effect of bending the electron spin trajectory cannot be ignored, and it is difficult to construct a spin filter.

On the other hand, in the present invention, since the gradient of the potential felt by the spin formed by the spatial gradient of the g-factor that can be controlled by the gate voltage is used, no inhomogeneous magnetic field is required at all. Therefore, the effect of bending the electron trajectory due to the Lorentz force is completely negligible. By analogy with the SG effect, when a spatial gradient g (y) is given to the g-factor, upward and downward spins receive forces in opposite directions, and can be expressed as follows.

Similar to the SG effect, spin separation can be achieved. The spin deflection angle φ _SG due to the SG effect is

Given in. Here, Δt = L / v _F and p _x = m ^* v _F. Note that L is the length of the semiconductor channel, v _F is the Fermi velocity, and m ^* is the effective mass of the electrons. By forming a channel in which the g-factor at the conduction band edge of InAs is −15 and the g-factor of In _0.53 Ga _0.47 As is −4, but the composition ratio of In and Ga is continuously changed. It can be expected that | Δg | = 10 as a change in g-factor due to the gate voltage.

Recently, it has become possible to form a two-dimensional electron gas having a very low carrier concentration, and a low concentration of 1 × 10 ¹⁰ cm ⁻² or less has been realized (Y. Hirayama, K. Muraki). , and T. Saku, Appl. Phys. Lett. 72, 1745 (1998)).

The Fermi velocity v _F can be reduced by such a low concentration carrier. For example, the channel width W is 1 μm, the region where the spin orbit interaction is spatially changed in the y-axis direction is L = 3 μm, the carrier concentration is n _s = 1 × 10 ¹⁰ cm ⁻² , the effective mass m ^* = 0. Assuming 03, the Fermi velocity is v _F = 96700 m / sec. If a uniform external magnetic field By = 1T is applied, a sufficient deflection angle φ _SG = 28.5 [deg] can be obtained by substituting into the above equation. In addition, it is possible to further increase the spin deflection angle by making the g-factor spatially changing region L longer. For example, when L = 10 μm, φ _SG = 61.2 deg and a sufficient spin deflection angle can be obtained.

<Device configuration of spin filter>
FIG. 2 is a block diagram showing an outline of a functional configuration of the spin filter 1 configured based on the basic items described above. The spin filter 1 shown in FIG. 2 confins carriers and propagates a semiconductor channel 2, a uniform magnetic field application unit 3 that applies a uniform magnetic field to the semiconductor channel, and a gate voltage application unit that applies a gate voltage to the semiconductor channel 2. 4. A g factor spatial gradient generation unit 5 is provided that generates a g factor spatial gradient of the semiconductor channel 2 by the applied gate voltage.

The semiconductor channel 2 has a two-dimensional region in which the movable region in one spatial dimension direction of the carrier is so small that it can be ignored as compared with the movable regions in the other two spatial dimension directions. It behaves as a two-dimensional electron gas (hereinafter, this two-dimensional region is referred to as a “two-dimensional electron gas channel”). The two-dimensional electron gas channel confines carriers in a two-dimensional region by forming a semiconductor quantum well structure, for example. As is well known, for example, a semiconductor quantum well structure having a narrow width in the one-dimensional direction of space, for example, can be formed by laminating both surfaces of a GaAs thin film with Al _0.3 Ga _0.7 As, or _{A 0.53} Ga _0.47 As thin film can be formed by sandwiching and laminating both surfaces of InP.

  The uniform magnetic field application unit 3 is configured using, for example, one or a plurality of ferromagnetic materials.

  The gate voltage application unit 4 applies an effective gate voltage to the semiconductor channel 2 below the gate electrode. The gate electrode may be either a top gate or a back gate, and may include two gate electrodes, a top gate and a back gate.

  The g-factor space gradient generation unit 5 is a characteristic part of the present invention, and specifically, various modes can be considered as described later. Hereinafter, a specific configuration of the spin filter will be described.

  3A is a schematic view of the spin filter 10 according to one embodiment of the present invention as viewed from the z-axis direction (top view), and FIG. 3B is a cross-sectional view taken along line AB of FIG. It is sectional drawing.

  As shown in FIG. 3B, the spin filter 10 has an effective gate voltage gradient applied to the two-dimensional electron gas channel 14 by inserting the gate insulating layers 12 having different thicknesses in the y-axis direction. Therefore, the g-factor of the two-dimensional electron gas channel 14 below the gate electrode 11 is spatially inclined in the y-axis direction. Accordingly, while electron spin propagates in this space in the x-axis direction, spin-up carriers and spin-down carriers receive forces in opposite directions, and the spins are spatially separated. For example, if a Y-shaped branch is provided behind the gate electrode 11, an upward spin flows into the terminal T1 and a downward spin flows into the terminal T2. In FIG. 3, the magnetic field B is applied uniformly in the y-axis direction.

Here, as shown in FIG. 3, if the length of the two-dimensional electron gas channel 14 is L and the width is W, the conditions for separating the 100% spin-polarized electrons in the Y-type branch are as follows:
tanφ _SG > W / L
It is. For example, when L = 2 μm, it is possible to sufficiently reduce W to 1 μm or less. For example, if φ _SG = 22 deg, W = 0.8 μm and the above condition is satisfied.

  The configuration of the spin detection means is not limited to the Y-type branch described above, and any configuration is possible as long as the separated spin state can be measured along the y-axis direction in FIG. May be. The gate insulating layer 12 is not necessarily an insulator, and may be a semiconductor.

  FIG. 4 is a schematic view of the spin filter 20 according to one embodiment of the present invention viewed from the z-axis direction. In the spin filter 10, the gate insulating layer 12 having a different thickness in the y-axis direction is inserted to give a spatial gradient to the g-factor. Is provided with a plurality of gate electrodes 21i (i = a, b,..., N; three in FIG. 4) having a different gate voltage so that the g-factor has a spatial gradient. is there. Other configurations are the same as those of the spin filter 10. In the following embodiments, only configurations and functions different from those in the first embodiment will be described, and with regard to other configurations and functions, the same portions are denoted by the same reference numerals, and description thereof will be omitted.

  FIG. 5 is a schematic view of the spin filter 30 according to one embodiment of the present invention viewed from the z-axis direction. The spin filter 30 introduces anti-dots or artificial impurities into the two-dimensional electron gas channel 14 of the spin filter 10 or 20, slows the propagation of electron spin, which is a carrier, to a drift velocity, and increases the relaxation length of the spin. It is something to keep.

  Here, the significance of introducing anti-dots or artificial impurities into the semiconductor channel 2 will be described.

  In general, in a system with a large g-factor, spin-orbit interaction is also strong, and it is predicted that spin information is not retained over a long distance due to spin relaxation. However, according to the calculation of spin relaxation time in a two-dimensional electron gas system with spin-orbit interaction using the recent Monte Carlo simulation technique, by introducing artificial elastic scatterers such as anti-dots It has been shown that the spin relaxation time becomes longer to 1000 times or more of the momentum relaxation time of electrons. This result is attributed to the fact that when the spin relaxation mechanism is caused by the D'yakonov-Perel 'mechanism, the spin precession is suppressed by scattering and the relaxation time becomes longer. In InGaAs-based two-dimensional electron gas, the D'yakonov-Perel 'mechanism has been confirmed to play an important role in spin relaxation, and artificial anti-dots and impurity scatterers should be introduced into the channel. This makes it possible to lengthen the spin relaxation (see T. Koga, J. Nitta, T. Akazaki, and H. Takayanagi, Phys. Rev. Lett. 89, 46801 (2002)).

In this case, the electron spin propagates through the non-uniform g-factor region at the drift velocity v _d by the scatterer. Then, the stay time Δt in the non-uniform g-factor region is increased, and a large deflection angle φ _SG can be obtained. The effective momentum in the x-axis direction is also <p _x > = m ^* v, and the deflection angle obtained by replacing v _F with v _d is given by the following equation.

This is because the Fermi velocity v _F in equation (7) is replaced by the drift velocity v _d , and the residence time in the non-uniform spin-orbit interaction region is obtained by making the semiconductor channel 2 a diffusive system. It shows that Δt is long and it is convenient to obtain a large deflection angle φ _SG . Incidentally, if the electron mobility μ is due to impurity scattering and μ = 10,000 cm ² / Vs, and an electric field E = 1 V / cm for accelerating electrons in the x direction is applied, the drift velocity v _d = 100 m / sec. _{| Δg | = 1, B y} = 1mT, large deflection angle as L = 1μm φ _SG = 86.6deg is obtained. In the case where carrier propagation due to drift velocity becomes dominant, it is shown that the applied uniform magnetic field is sufficient even if it is 1 mT or less.

  FIG. 6 is a schematic view of the spin filter 40 according to one embodiment of the present invention viewed from the z-axis direction. The spin filter 40 uses magnetic electrodes for the output side terminals T1 and T2 of the spin filter 10, 20, or 30. By rotating the spin of each magnetic electrode in the reverse direction, the carrier is applied to only one terminal. Is to flow. For example, in FIG. 6, a current flows only through the terminal T1, but no current flows through the terminal T2. However, when a magnetic field is applied to each magnetic electrode to reverse the direction of each spin, current flows through the terminal T2 and no current flows through the terminal T1.

  Thus, in the spin filter 40, the current between the terminals can be controlled by controlling the magnetic electrode on the output side.

  FIG. 7 is a schematic view of the spin filter 50 according to one embodiment of the present invention as viewed from the z-axis direction. The spin filter 50 uses a magnetic electrode for the input-side terminal T0 of the spin filter 10, 20, or 30. Either of the output-side terminals T1 and T2 depending on the spin direction of the carriers injected from the terminal T0. The carrier flows through only one terminal. For example, in FIG. 7, a current flows only through the terminal T1, but no current flows through the terminal T2. However, when a magnetic field is applied to the magnetic electrode to reverse the direction of the spin, a current flows through the terminal T2 and no current flows through the terminal T1.

  Although the embodiments of the present invention have been described, various modifications and changes can be made to the embodiments of the present invention without departing from the spirit of the present invention. For example, in the above embodiment, by inserting the gate insulating layers 12 having different thicknesses in the y-axis direction, or by providing the gate electrodes 21i having a plurality of different gate voltages in the y-axis direction, Although the g-factor of the two-dimensional electron gas channel 14 below 11 has a spatial gradient in the y-axis direction, the method for generating the spatial gradient of the g-factor is not limited to this. There may be. For example, the thickness of the two-dimensional electron gas channel 14 in the y-axis direction may be made nonuniform to generate a g-factor spatial gradient.

  As described above, according to the embodiment of the present invention, since the g-factor of the semiconductor channel can be controlled by the gate voltage, the SG effect can be realized in the semiconductor using the spatial gradient of the g-factor. it can.

  As a result, a spin deflection angle sufficient to separate different spin states of carriers propagating in a semiconductor can be obtained without using a non-uniform magnetic field.

  In addition, by introducing an elastic scatterer into the semiconductor channel, spin relaxation can be made sufficiently long, so that it can be operated even at room temperature.

It is a figure which shows the relationship between the g factor of a semiconductor channel, and gate voltage. It is a block diagram which shows the function structure of the spin filter which concerns on one Embodiment of this invention. FIG. 3 is a diagram illustrating a specific example 1 of the spin filter of FIG. 1. FIG. 6 is a diagram illustrating a specific example 2 of the spin filter of FIG. 1. FIG. 6 is a diagram illustrating a specific example 3 of the spin filter of FIG. 1. FIG. 6 is a diagram illustrating a specific example 4 of the spin filter of FIG. 1. FIG. 9 is a diagram illustrating a specific example 5 of the spin filter of FIG. 1. It is explanatory drawing which shows the experiment of Stern-Gerlach notionally.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1, 10, 20, 30, 40, 50 ... Spin filter 2 ... Semiconductor channel 3 ... Uniform magnetic field application part 4 ... Gate voltage application part 5 ... G factor space gradient generation part 11, 21i ... Gate electrode 12 ... Gate insulating layer 14 ... Two-dimensional electron gas channel

Claims (12)

A spin filter for separating carriers for each spin state of carriers propagating in a semiconductor,
Uniform magnetic field application means for applying a uniform magnetic field in a direction perpendicular to the direction in which the carriers propagate;
A semiconductor channel confining the carrier and propagating the carrier;
Voltage applying means for applying a gate voltage to the semiconductor channel;
And a g-factor of the semiconductor channel is controlled by the gate voltage so as to be non-uniform with a spatial gradient in the same direction as the applied magnetic field direction.   2. The spin filter according to claim 1, wherein layers having different thicknesses are inserted on the semiconductor channel so that a g-factor of the semiconductor channel has a spatial gradient.   2. The spin filter according to claim 1, wherein the gate voltage applying means includes a plurality of gate electrodes to which applied voltages are different, and gives a g-factor of the semiconductor channel to a spatial gradient.   4. The spin filter according to claim 1, wherein an elastic scatterer is introduced into the semiconductor channel.   The spin filter according to any one of claims 1 to 4, further comprising an electrode for spin detection using a magnetic material on an output side.   The spin filter according to any one of claims 1 to 5, further comprising an electrode for spin injection using a magnetic material on an input side. A spin state separation method for separating carriers for each spin state of carriers propagating in a semiconductor,
Applying a uniform magnetic field in a direction perpendicular to the direction of propagation of the carrier to the semiconductor channel for confining the carrier and propagating the carrier,
Applying a gate voltage to the semiconductor channel;
A spin state separation method, wherein the g-factor of the semiconductor channel is controlled by the gate voltage to be non-uniform with a spatial gradient in the same direction as the applied magnetic field direction.   The spin state separation method according to claim 7, wherein the spin filter including the semiconductor channel inserts layers having different thicknesses on the semiconductor channel to give a spatial gradient to the g-factor of the semiconductor channel.   8. The spin state separation method according to claim 7, wherein the gate voltage applying means for applying the gate voltage includes a plurality of gate electrodes with different voltages to be applied, and has a spatial gradient in the g-factor of the semiconductor channel. .   10. The spin state separation method according to claim 7, wherein an elastic scatterer is introduced into the semiconductor channel.   The spin state separation method according to any one of claims 7 to 10, wherein an electrode using a magnetic material is provided on an output side to detect the spin state of the carrier. 12. The spin state separation method according to claim 7, wherein an electrode using a magnetic material is provided on an input side, and spin-polarized carriers are injected.

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