The present disclosure relates to a quantum bit circuit, a quantum computer, and a method for manufacturing the quantum bit circuit.
A quantum computer using Majorana particles has been studied. As a structure for generating the Majorana particles, for example, the following two types of techniques have been proposed. One is a technique using a one-dimensional semiconductor nanowire, and another one is a technique using a two-dimensional topological insulator.
Examples of the related art include: [Patent Document 1] Japanese Laid-open Patent Publication No. 2013-247267; [Patent Document 2] Japanese National Publication of International Patent Application No. 2020-511780; [Non-Patent Document 1] Coulomb-assisted braiding of Majorana fermions in a Josephson junction array, New Journal of Physics 14, 035019 (2012); [Non-Patent Document 2] Minimal circuit for a flux-controlled Majorana qubit in a quantum spin-Hall insulator, Physica Scripta T164, 014007 (2015); and [Non-Patent Document 3] Direct visualization of a two-dimensional topological insulator in the single-layer 1T′-WTe2, Physical Review B 96, (2017).
According to an aspect of the embodiments, there is provided a quantum bit circuit including: a first Majorana carrier extended in a first direction; and a second Majorana carrier extended in a second direction that intersects with the first direction, wherein the First Majorana carrier includes a first region where a Majorana particle is able to exist, in a portion that overlaps the second Majorana carrier in plan view, the second Majorana carrier includes a second region where a Majorana particle is able to exist, in a portion that overlaps the first Majorana carrier in plan view, and the Majorana particle in the first region and the Majorana particle in the second region are exchangeable.
The object and advantages of the invention will be realized and attained by means of the elements and combinations particularly pointed out in the claims.
It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory and are not restrictive of the invention.
Although proposals based on theories have been made, it is extremely difficult to manufacture a quantum bit circuit that can be easily controlled, with a high yield.
An object of the present disclosure is to provide a quantum bit circuit that can manufacture a structure that can be easily controlled, with a high yield, a quantum computer, and a method for manufacturing the quantum bit circuit.
Hereinafter, embodiments of the present disclosure will be specifically described with reference to the attached drawings. Note that, in the present specification and drawings, components having substantially the same functional configuration are denoted with the same reference numeral, and redundant descriptions may be omitted.
First, a first embodiment will be described. The first embodiment relates to a quantum bit circuit including a two-dimensional topological insulator.
As illustrated in
The lower Majorana carrier 121 is, for example, a two-dimensional topological insulator layer, and includes a first edge 161 and a third edge 163 extending in the X-axis direction. The first edge 161 is positioned on a −Y side of the third edge 163. The lower Majorana carrier 121 may be formed of a single two-dimensional topological insulator or may be formed by laminating a plurality of two-dimensional topological insulators. A material of the lower Majorana carrier 121 is, for example, tungsten ditelluride (WTe2). In the present embodiment, the plurality of lower Majorana carriers 121 is arranged side by side in the Y-axis direction. The lower Majorana carrier 121 is an example of a first Majorana carrier.
The upper Majorana carrier 122 is, for example, a two-dimensional topological insulator layer and includes a second edge 162 and a fourth edge 164 extending in the Y-axis direction. The second edge 162 is positioned on a −X side of the fourth edge 164. The upper Majorana carrier 122 may be formed of a single two-dimensional topological insulator or may be formed by laminating a plurality of two-dimensional topological insulators. A material of the upper Majorana carrier 122 is, for example, tungsten ditelluride (WTe2). In the present embodiment, the plurality of upper Majorana carriers 122 is arranged side by side in the X-axis direction. The upper Majorana carrier 122 is an example of a second Majorana carrier.
A lower s-wave superconductor layer 131 in contact with a lower surface of the lower Majorana carrier 121 is provided. The lower s-wave superconductor layer 131 is provided along the first edge 161 and the third edge 163, for each region overlapping the upper Majorana carrier 122 in plan view. An end of each lower s-wave superconductor layer 131 in the X-axis direction is separated from the second edge 162 and the fourth edge 164 of the upper Majorana carrier 122 in plan view. The lower s-wave superconductor layer 131 is, for example, an Al layer.
A lower s-wave superconductor layer 132 in contact with an upper surface of the lower Majorana carrier 121 is provided. The lower s-wave superconductor layer 132 is provided along the first edge 161 and the third edge 163, for each region between the upper Majorana carriers 122 adjacent to each other in plan view. An end of each lower s-wave superconductor layer 132 in the X-axis direction is separated from the second edge 162 and the fourth edge 164 of the upper Majorana carrier 122 in plan view. The lower s-wave superconductor layer 132 is, for example, an Al layer. The lower s-wave superconductor layers 131 and 132 are examples of a first s-wave superconductor layer.
An upper s-wave superconductor layer 133 in contact with an upper surface of the upper Majorana carrier 122 is provided. The upper s-wave superconductor layer 133 is provided along the second edge 162 and the fourth edge 164, for each region overlapping the lower Majorana carrier 121 and each region between lower Majorana carriers 121 adjacent to each other, in plan view. An end of the upper s-wave superconductor layer 133 in the X-axis direction is separated from the first edge 161 and the third edge 163 of the lower Majorana carrier 121 in plan view. The upper s-wave superconductor layer 133 is, for example, an Al layer. The upper s-wave superconductor layer 133 is an example of a second s-wave superconductor layer.
An etching stopper 140 is provided between the lower Majorana carrier 121 and the upper Majorana carrier 122. A material of the etching stopper 140 is, for example, graphene or graphite. In a case where the material of the etching stopper 140 is graphite, the thickness thereof is preferable as thin as possible, and is preferable to be equal to or less than five nm, for example. As described later, this is because Majorana particles tunnel through the etching stopper 140 between the lower Majorana carrier 121 and the upper Majorana carrier 122.
Wiring is individually coupled to the lower s-wave superconductor layer 131, the lower s-wave superconductor layer 132, and the upper s-wave superconductor layer 133.
In the quantum bit circuit 1, the Majorana particles can exist in a portion between the lower s-wave superconductor layer 131 and the lower s-wave superconductor layer 132 adjacent to each other at the first edge 161 in plan view and a portion between the lower s-wave superconductor layer 131 and the lower s-wave superconductor layer 132 adjacent to each other at the third edge 163 in plan view. Then, for example, in these portions where the Majorana particles can exist, a portion of the first edge 161 overlapping the second edge 162 functions as a first region 171, and a portion of the third edge 163 overlapping the second edge 162 functions as a third region 173. Furthermore, for example, in these portions where the Majorana particles can exist, a portion of the first edge 161 overlapping the fourth edge 164 functions as a fifth region 175, and a portion of the third edge 163 overlapping the fourth edge 164 functions as a seventh region 177.
Similarly, the Majorana particles can exist in a portion between the two upper s-wave superconductor layers 133 adjacent to each other at the second edge 162 in plan view and a portion between the two upper s-wave superconductor layers 133 adjacent to each other at the fourth edge 164 in plan view. Then, for example, in these portions where the Majorana particles can exist, a portion of the second edge 162 overlapping the first edge 161 functions as a second region 172, and a portion of the fourth edge 164 overlapping the first edge 161 functions as a sixth region 176. Furthermore, in these portions where the Majorana particles can exist, a portion of the second edge 162 overlapping the third edge 163 functions as a fourth region 174, and a portion of the fourth edge 164 overlapping the third edge 163 functions as an eighth region 178.
The Majorana particles existing in the first region 171 and the Majorana particles existing in the second region 172 can pass through the etching stopper 140 by a tunnel effect and interact with each other. Therefore, both Majorana particles can be regarded as the same Majorana particle. The same applies to a pair of the third region 173 and the fourth region 174, a pair of the fifth region 175 and the sixth region 176, and a pair of the seventh region 177 and the eighth region 178.
In this way, in the quantum bit circuit 1, the Majorana particles generated in the lower Majorana carrier 121 and the Majorana particles generated in the upper Majorana carrier 122 can easily interact with each other. Furthermore, as described later, such a structure can be manufactured with a high yield, with alignment accuracy of a typical semiconductor process.
Furthermore, by controlling states of the lower s-wave superconductor layers 131 and 132, the Majorana particles can be exchanged between the first region 171 and the fifth region 175 and between the third region 173 and the seventh region 177 adjacent to each other, with the lower s-wave superconductor layers 131 and 132 interposed therebetween. Similarly, by controlling a state of the upper s-wave superconductor layer 133, the Majorana particles can be exchanged between the second region 172 and the fourth region 174 and between the sixth region 176 and the eighth region 178 adjacent to each other, with the upper s-wave superconductor layer 133 interposed therebetween.
Moreover, in the quantum bit circuit 1, eight Majorana particles can be generated in a region where the lower Majorana carrier 121 and the upper Majorana carrier 122 overlap in plan view. Therefore, Majorana quantum bits can be accumulated at high density. Furthermore, the Majorana quantum bits can be regularly accumulated in a grid-like pattern, and wiring or the like can be easily designed.
Here, an example of an operation of the quantum bit circuit 1 will be described.
In this example, the Majorana particles are exchanged between the two fifth regions 175 adjacent to each other with the first region 171 interposed therebetween in the X-axis direction. In other words, a Majorana particle γ1 generated in one fifth region 175 and a Majorana particle γ4 generated in another fifth region 175 are exchanged via a Majorana particle γ2 generated in the first region 171 between these fifth regions 175 through charging.
Next, a method for manufacturing the quantum bit circuit 1 according to the first embodiment will be described.
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Thereafter, wiring (not illustrated) or the like that is individually coupled to the lower s-wave superconductor layer 131, the lower s-wave superconductor layer 132, and the upper s-wave superconductor layer 133 is formed.
In this way, the quantum bit circuit 1 according to the first embodiment can be manufactured.
With such a method, with alignment accuracy of a typical semiconductor process, it is possible to manufacture the quantum bit circuit 1 with a high yield.
Note that both of the lower s-wave superconductor layer 131 and the lower s-wave superconductor layer 132 may have contact with the lower surface of the lower Majorana carrier 121, and both of the lower s-wave superconductor layer 131 and the lower s-wave superconductor layer 132 may have contact with the upper surface of the lower Majorana carrier 121.
Next, a second embodiment will be described. The second embodiment is different from the first embodiment mainly in a configuration of a laminated structure including the lower Majorana carrier 121 and the upper Majorana carrier 122.
As in the first embodiment, a quantum bit circuit 2 according to the second embodiment includes a substrate 110, a lower Majorana carrier 121, an upper Majorana carrier 122, a lower s-wave superconductor layer 131, a lower s-wave superconductor layer 132, and an upper s-wave superconductor layer 133. On the other hand, instead of the etching stopper 140, an etching stopper 241, an etching stopper 242, and a semiconductor layer 250 are provided between the lower Majorana carrier 121 and the upper Majorana carrier 122. The etching stopper 241 is provided between the lower Majorana carrier 121 and the semiconductor layer 250, and the etching stopper 242 is provided between the semiconductor layer 250 and the upper Majorana carrier 122.
A material of the etching stoppers 241 and 242 is, for example, graphene or graphite. In a case where the material of the etching stoppers 241 and 242 is graphite, the thickness thereof is preferable as thin as possible, and is preferable to be equal to or less than five nm, for example. This is because Majorana particles tunnel through the etching stoppers 241 and 242 between the lower Majorana carrier 121 and the upper Majorana carrier 122.
A material of the semiconductor layer 250 is, for example, a two-dimensional semiconductor such as tin diselenide (SnSe2). A conductivity type of the semiconductor layer 250 is not limited, and for example, may be an intrinsic semiconductor or an n-type semiconductor. The semiconductor layer 250 may be configured from a single two-dimensional semiconductor or may be configured by laminating a plurality of two-dimensional semiconductors. The semiconductor layer 250 is an example of a tunnel barrier layer.
A lower electrode 251 is provided between the lower s-wave superconductor layers 131 that are adjacent to each other in an X-axis direction. Similarly to the lower s-wave superconductor layer 131, the lower electrode 251 is covered with the lower Majorana carrier 121. For example, the lower electrode 251 is provided in a region that does not overlap the upper Majorana carrier 122 in plan view. The lower electrode 251 is provided, for example, in each of the vicinity of a first region 171, the vicinity of a third region 173, the vicinity of a fifth region 175, and the vicinity of a seventh region 177.
Furthermore, an upper electrode 252 is provided on the upper Majorana carrier 122. The upper electrode 252 is provided, for example, in each of the vicinity of a second region 172, the vicinity of a fourth region 174, the vicinity of a sixth region 176, and the vicinity of an eighth region 178.
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Other components are similar to those of the first embodiment.
In the quantum bit circuit 2, a laminated film of the etching stopper 241, the semiconductor layer 250, and the etching stopper 242 exists between the lower Majorana carrier 121 and the upper Majorana carrier 122. Here, an example of a band diagram of a valence band and a conduction band of a laminate of the lower Majorana carrier 121, the etching stopper 241, the semiconductor layer 250, the etching stopper 242, and the upper Majorana carrier 122 is illustrated in
Because the semiconductor layer 250 is provided, a tunnel barrier exists between the Majorana particle generated in the lower Majorana carrier 121 and the Majorana particle generated in the upper Majorana carrier 122. A height of this tunnel barrier can be adjusted according to a magnitude of a gate voltage to be applied from the power supply 253. For example, by applying the gate voltage, it is possible to change a band of the semiconductor layer 250 and lower the tunnel barrier so as to induce a tunnel effect.
Here, an example of an operation of the quantum bit circuit 2 will be described.
In the quantum bit circuit 1 according to the first embodiment, the Majorana particle can be exchanged through charging. Whereas, in the quantum bit circuit 2 according to the second embodiment, the Majorana particles can be exchanged with the tunnel effect through control of the gate voltage, in addition to the exchange of the Majorana particles through charging.
In the exchange with the tunnel effect, as described above, by applying the gate voltage VG, the Majorana particles are exchanged between the first region 171 and the second region 172, for example. In other words, the Majorana particle γ2 generated in the first region 171 and the Majorana particle generated in the second region 172 are exchanged through a tunnel of the semiconductor layer 250.
Furthermore, in the exchange through charging, for example, the Majorana particles are exchanged between the two fifth regions 175 adjacent to each other with the first region 171 interposed therebetween in the X-axis direction. In other words, a Majorana particle γ1 generated in one fifth region 175 and a Majorana particle γ4 generated in another fifth region 175 are exchanged via a Majorana particle γ2 generated in the first region 171 between these fifth regions 175 through charging.
Next, a method for manufacturing the quantum bit circuit 2 according to the second embodiment will be described.
First, as in the first embodiment, the lower s-wave superconductor layer 131 is formed on the substrate 110. The lower s-wave superconductor layer 131 can be formed by a deposition method, for example. Furthermore, the lower electrode 251 is formed on the substrate 110. The lower electrode 251 can be formed by the deposition method, for example. Next, as illustrated in
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In this way, the quantum bit circuit 2 according to the second embodiment can be manufactured.
Next, a third embodiment will be described. The third embodiment relates to a quantum bit circuit including a semiconductor nanowire.
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The lower Majorana carrier 321 is a semiconductor nanowire, for example, including InAs. In the present embodiment, the plurality of lower Majorana carriers 321 is arranged side by side in the Y-axis direction. The lower Majorana carrier 321 is an example of a first Majorana carrier.
The upper Majorana carrier 322 is a semiconductor nanowire, for example, including InAs. In the present embodiment, the plurality of upper Majorana carriers 122 is arranged side by side in the X-axis direction. The upper Majorana carrier 322 is an example of a second Majorana carrier.
A buffer layer 381 and an underlying semiconductor layer 382 are provided on the substrate 310. For example, the buffer layer 381 is an In1-xAlxAs layer of which the thickness is about one μm, and an Al composition x may change so as to be lattice-matched with the substrate 310 and the underlying semiconductor layer 382, from an interface with the substrate 310 to an interface with the underlying semiconductor layer 382. For example, the underlying semiconductor layer 382 is an In0.81Ga0.19As layer of which the thickness is about four nm.
The lower Majorana carrier 321 is formed on the underlying semiconductor layer 382. The thickness of the lower Majorana carrier 321 is, for example, about five nm. A barrier layer 383 is formed on the underlying semiconductor layer 382 so as to cover the lower Majorana carrier 321. For example, the barrier layer 383 is an In0.9Al0.1As layer of which the thickness is about five nm, on the lower Majorana carrier 321. The lower Majorana carrier 321 is covered with the barrier layer 383 and functions as a quantum well.
The upper Majorana carrier 322 is formed on the barrier layer 383. The thickness of the upper Majorana carrier 322 is, for example, about five nm. A barrier layer 384 is formed on the barrier layer 383 so as to cover the upper Majorana carrier 322. For example, the barrier layer 384 is an In0.9Al0.1As layer of which the thickness is about five nm on the upper Majorana carrier 322. The upper Majorana carrier 322 is covered with the barrier layer 384 and functions as a quantum well.
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In the quantum bit circuit 3, the Majorana particles can exist in a portion of the lower Majorana carrier 321 overlapping the upper Majorana carrier 322 in plan view and a portion of the upper Majorana carrier 322 overlapping the lower Majorana carrier 321 in plan view. Then, for example, in these portions where the Majorana particles can exist, the portion of the lower Majorana carrier 321 overlapping the upper Majorana carrier 322 in plan view functions as a first region 371, and the portion of the upper Majorana carrier 322 overlapping the lower Majorana carrier 321 in plan view functions as a second region 372.
Furthermore, by controlling a state of the lower s-wave superconductor layer 331, the Majorana particles can be exchanged between the two first regions 371 adjacent to each other in the X-axis direction. Similarly, by controlling a state of the upper s-wave superconductor layer 332, the Majorana particles can be exchanged between the two second regions 372 adjacent to each other in the Y-axis direction. Moreover, by adjusting the gate voltage to be applied from the power supply 353, the Majorana particles can be exchanged between the first region 371 and the second region 372 adjacent to each other in the Z-axis direction.
Note that a graphene nanoribbon can be used as a Majorana carrier.
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Although the preferred embodiments and the like have been described in detail above, the present disclosure is not limited to the embodiments and the like described above, and various modifications and substitutions may be made to the embodiments and the like described above without departing from the scope described in claims.
All examples and conditional language provided herein are intended for the pedagogical purposes of aiding the reader in understanding the invention and the concepts contributed by the inventor to further the art, and are not to be construed as limitations to such specifically recited examples and conditions, nor does the organization of such examples in the specification relate to a showing of the superiority and inferiority of the invention. Although one or more embodiments of the present invention have been described in detail, it should be understood that the various changes, substitutions, and alterations could be made hereto without departing from the spirit and scope of the invention.
This application is a continuation application of International Application PCT/JP2020/048426 filed on Dec. 24, 2020 and designated the U.S., the entire contents of which are incorporated herein by reference.
Number | Date | Country | |
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Parent | PCT/JP2020/048426 | Dec 2020 | US |
Child | 18311261 | US |