Electron wave combining/branching devices and quantum interference devices

Claim 2

A quantum interference device comprising: a semiconductor member having a source, a gate, and a drain, said source and drain comprising spaced regions of said semiconductor body, and said gate lying generally between the source and drain; an electron waveguide structure extending between said source and said drain, said electron waveguide structure having a gate controlled channel portion immediately adjacent said gate and source and drain channel portions lying between said gate controlled channel portion and said source and drain, said electron waveguide structure comprising a pair of quantum confinement structures of a first semiconductor material each having a first dimension in a direction normal to the direction between said source and drain and being separated in said direction normal to the direction between said source and drain by a barrier layer having a second dimension in said direction normal to the direction between said source and drain, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said electron waveguide structure are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; said electron waveguide structure having a Fermi level for electrons; said gate structure including an electrode; and means for applying a voltage to said electrode of said gate structure with respect to said source or said drain such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves in said electron waveguide structure are coupled between said pair of quantum confinement structures when said energy of said next lowest energy level is above the energy level of said Fermi level, and electron waves in said electron waveguide structure are decoupled between said pair of quantum confinement structures when said energy of said next lowest energy level is below the energy level of said Fermi level.

Claim 3

A quantum interference device according to claim 1, wherein, when the voltage applied to said gate electrode is varied, a phase difference is caused between the electron waves propagating through said first and second electron waveguides due to Aharonov-Bohm effect, so as to interfere with each other, whereby an electric current flowing between said source and said drain is modulated by the interference.

Claim 4

A quantum interference device according to claim 1, further comprising means for applying a magnetic field to said first and second electron waveguides, whereby an electric current flowing between said source and said drain is modulated as a result of a modulation of said magnetic field.

Claim 5

A quantum interference device according to claim 1, further comprising: means for applying a light to said gate, whereby an electron current flowing between said source and said drain is modulated as a result of modulation of said light.

Claim 6

A quantum interference device according to claim 4, wherein the photon energy of the light applied is detuned from the difference between said first quantum energy level and said second quantum energy level.

Claim 7

A quantum interference device according to claim 1, comprising two pairs of said first and second electron waveguides.

Claim 8

A quantum interference device according to claim 1, wherein the following condition is met: L.sub.G ≧π/(2κ) wherein L G represents the length of said gate as measured in the direction of propagation of said electron wave, and κ represents the coefficient of coupling between said first and second electron waveguides.

Claim 9

A quantum interference device according to claim 1, wherein each of said first and second electron waveguides includes a quantum line.

Claim 10

A quantum interference device according to claim 1 wherein said first and second quantum wells include first and second quantum well layers formed on a substrate, said quantum interference device further comprising a barrier layer provided between said first and second quantum well layers.

Claim 11

A quantum interference device according to claim 9, wherein said first and second quantum well layers have different thicknesses.

Claim 12

A quantum interference device according to claim 9, further comprising first and second clad layers which cooperate with each other in sandwiching therebetween said barrier layer and said first and second quantum well layers.

Claim 13

A quantum interference device according to claim 1, further comprising a back gate which cooperates with said gate electrode in sandwiching therebetween said first and second electron waveguides.

Claim 14

A quantum interference device according to claim 1, wherein said gate electrode includes a first gate electrode and a second gate electrode which are arranged side by side in the direction of propagation of the electron wave, said first and second gate electrodes being supplied with voltages independently of each other.

Claim 15

A quantum interference device according to claim 1, further comprising a sub-gate disposed between said source and said gate, said sub-gate transmitting to said gate only an electron wave of a predetermined energy level from among the electron waves from said source.

Claim 16

A quantum interference device according to claim 1, further comprising a sub-gate disposed between said drain and said gate, said sub-gate reflecting toward said gate only an electron wave of a predetermined energy level, from among the electron waves directed to said drain.

Claim 17

An optical detecting device, comprising: a semiconductor member having a source, a gate and a drain, said source and drain comprising spaced regions of said semiconductor body, and said gate lying generally between the source and drain; an electron waveguide structure extending between said source and said drain, said electron waveguide structure having a gate controlled channel portion immediately adjacent said gate and source and drain channel portions lying between said gate controlled channel portion and said source and drain, said electron waveguide structure comprising a pair of quantum confinement structures of a first semiconductor material each having a first dimension in a direction normal to the direction between said source and drain and being separated in said direction normal to the direction between said source and drain by a barrier layer having a second dimension in said direction normal to the direction between said source and drain, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said electron waveguide structure are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; said electron waveguide structure having a Fermi level for electrons; said gate structure including an electrode; and means for applying a voltage to said electrode of said gate structure with respect to said source or said drain such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves in said electron waveguide structure are coupled between said pair of quantum confinement structures when said energy of said next lowest energy level is above the energy level of said Fermi level, and electron waves in said electron waveguide structure are decoupled between said pair of quantum confinement structures when said energy of said next lowest energy level is below the energy level of said Fermi level.

Claim 18

An optical detecting device, comprising: a semiconductor member having a source, a gate and a drain, said source and drain comprising spaced regions of said semiconductor body, and said gate lying generally between the source and drain; an electron waveguide structure extending between said source and said drain, said electron waveguide structure having a gate controlled channel portion immediately adjacent said gate and source and drain channel portions lying between said gate controlled channel portion and said source and drain, said electron waveguide structure comprising a pair of quantum confinement structures of a first semiconductor material each having a first dimension in a direction normal to the direction between said source and drain and being separated in said direction normal to the direction between said source and drain by a barrier layer having a second dimension in said direction normal to the direction between said source and drain, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said electron waveguide structure are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; said electron waveguide structure having a Fermi level for electrons; said gate structure including an electrode; and means for applying a voltage to said electrode of said gate structure with respect to said source or said drain such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves in said electron waveguide structure are coupled between said pair of quantum confinement structures when said energy of said next lowest energy level is above the energy level of said Fermi level, and electron waves in said electron waveguide structure are decoupled between said pair of quantum confinement structures when said energy of said next lowest energy level is below the energy level of said Fermi level.

Claim 19

An optical communication system, comprising: an optical signal transmitter which emits a light modulated in accordance with a communication signal; and an optical signal receiver having a photodetector for detecting said light from said optical transmitter; wherein said optical detector comprises: a semiconductor member having a source, a gate and a drain, said source and drain comprising spaced regions of said semiconductor body, and said gate lying generally between the source and drain; an electron waveguide structure extending between said source and said drain, said electron waveguide structure having a gate controlled channel portion immediately adjacent said gate and source and drain channel portions lying between said gate controlled channel portion and said source and drain, said electron waveguide structure comprising a pair of quantum confinement structures of a first semiconductor material each having a first dimension in a direction normal to the direction between said source and drain and being separated in said direction normal to the direction between said source and drain by a barrier layer having a second dimension in said direction normal to the direction between said source and drain, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said electron waveguide structure are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; said electron waveguide structure having a Fermi level for electrons; said gate structure including an electrode; and means for applying a voltage to said electrode of said gate structure with respect to said source or said drain such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves in said electron waveguide structure are coupled between said pair of quantum confinement structures when said energy of said next lowest energy level is above the energy level of said Fermi level, and electron waves in said electron waveguide structure are decoupled between said pair of quantum confinement structures when said energy of said next lowest energy level is below the energy level of said Fermi level.

Claim 20

An optical communication system, comprising: an optical signal transmitter which emits a light modulated in accordance with a communication signal; and an optical signal receiver having a photodetector for detecting said light from said optical transmitter; wherein said optical detector comprises: a semiconductor member having a source, a gate and a drain, said source and drain comprising spaced regions of said semiconductor body, and said gate lying generally between the source and drain; an electron waveguide structure extending between said source and said drain, said electron waveguide structure having a gate controlled channel portion immediately adjacent said gate and source and drain channel portions lying between said gate controlled channel portion and said source and drain, said electron waveguide structure comprising a pair of quantum confinement structures of a first semiconductor material each having a first dimension in a direction normal to the direction between said source and drain and being separated in said direction normal to the direction between said source and drain by a barrier layer having a second dimension in said direction normal to the direction between said source and drain, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said electron waveguide structure are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; said electron waveguide structure having a Fermi level for electrons; said gate structure including an electrode; and means for applying a voltage to said electrode of said gate structure with respect to said source or said drain such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves in said electron waveguide structure are coupled between said pair of quantum confinement structures when said energy of said next lowest energy level is above the energy level of said Fermi level, and electron waves in said electron waveguide structure are decoupled between said pair of quantum confinement structures when said energy of said next lowest energy level is below the energy level of said Fermi level.

Claim 21

An electron wave branching device comprising: a pair of quantum confinement structures for propogating an electron wave of a first semiconductor material; a source region for emitting the electron wave to said quantum confinement structures; a drain region for draining the electron wave from said quantum confinement structures, said source and drain regions comprising spaced regions of said first semiconductor material; and a gate region, lying generally between the source and drain, having a gate electrode provided in the vicinity of said quantum confinement structures; wherein each of said quantum confinement structures has a first dimension in a direction normal to the direction between said source region and said drain region and being separated in said direction normal to the direction between said source region and said drain region by a barrier layer having a second dimension in said direction normal to the direction between said source region and said drain region, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said pair of quantum confinement structures are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; and wherein said pair of quantum confinement structures having a Fermi level for electrons; and wherein when a positive voltage is applied to said gate region, such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves are decoupled between said pair of quantum confinement structures when said energy of said next lowest energy level is below the energy level of said Fermi level.

Claim 22

An electron wave branching device comprising: a pair of quantum confinement structures for propogating an electron wave of a first semiconductor material; a source region for emitting the electron wave to said quantum confinement structures; a drain region for draining the electron wave from said quantum confinement structures, said source and drain regions comprising spaced regions of said first semiconductor material; and a gate region, lying generally between the source and drain, having a gate electrode provided in the vicinity of said quantum confinement structures; wherein each of said quantum confinement structures has a first dimension in a direction normal to the direction between said source region and said drain region and being separated in said direction normal to the direction between said source region and said drain region by a barrier layer having a second dimension in said direction normal to the direction between said source region and said drain region, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said pair of quantum confinement structures are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; and wherein said pair of quantum confinement structures having a Fermi level for electrons; and wherein when a positive voltage is applied to said gate region, such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves are decoupled between said pair of quantum confinement structures when said energy of said next lowest energy level is below the energy level of said Fermi level.

Claim 23

An electron wave branching device according to claim 18, wherein said quantum confinement structures comprise a semiconductor substrate, a first clad layer provided on said substrate, a first quantum well layer provided on said first clad layer, a barrier layer provided on said first quantum well layer, a second quantum well layer provided on said barrier layer, and a second clad layer provided on said second quantum well layer, wherein bottom energy levels of the first clad layer, the second clad layer and the barrier layer are higher than bottom energy levels of the first and second quantum well layers in a conduction band.

Claim 24

An electron wave branching device according to claim 18, wherein each thickness of said first and second quantum well layers are different from each other.

Claim 25

An electron wave combining device comprising: a pair of quantum confinement structures for propagating an electron wave of a first semiconductor material; a source region for emitting the electron wave to said quantum confinement structures; a drain region for draining the electron wave from said quantum confinement structures, said source and drain regions comprising spaced regions of said first semiconductor material; and a gate region, lying generally between the source and the drain having a gate electrode provided in the vicinity of said quantum confinement structures; wherein each of said quantum confinement structures has a first dimension in a direction normal to the direction between said source region and said drain region and being separated in said direction normal to the direction between said source region and said drain region by a barrier layer having a second dimension in said direction normal to the direction between said source region and said drain region, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said pair of quantum confinement structures are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; and wherein said pair of quantum confinement structures having a Fermi level for electrons; and wherein, when a negative voltage is applied to said gate region, such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves in said electron waveguide structure are coupled between said pair of quantum confinement structures when said energy of said next lowest energy level is above the energy level of said Fermi level electron waveguide.

Claim 26

An electron wave combining device comprising: a pair of quantum confinement structures for propagating an electron wave of a first semiconductor material; a source region for emitting the electron wave to said quantum confinement structures; a drain region for draining the electron wave from said quantum confinement structures, said source and drain regions comprising spaced regions of said first semiconductor material; and a gate region, lying generally between the source and the drain having a gate electrode provided in the vicinity of said quantum confinement structures; wherein each of said quantum confinement structures has a first dimension in a direction normal to the direction between said source region and said drain region and being separated in said direction normal to the direction between said source region and said drain region by a barrier layer having a second dimension in said direction normal to the direction between said source region and said drain region, said barrier layer being made of a second semiconductor material having a lower affinity for electrons than said first semiconductor material, the difference in electron affinities between said first semiconductor material and said second semiconductor material and said first and second dimensions being such that, in said direction normal to the direction between said source and drain, energy levels for electrons in said pair of quantum confinement structures are quantized into discrete energy levels, the lowest of said discrete energy levels having a quantum mechanical electron wave function which is generally symmetrical about said barrier layer in said direction normal to the direction between said source and drain, the next lowest of said discrete energy levels being generally antisymmetrical about said barrier layer in said direction normal to the direction between said source and said drain, so that said lowest energy level has a wavefunction which is coupled between said pair of quantum confinement structures, and so that said next lowest energy level has a wavefunction which, by reason of its generally antisymmetrical nature, has a value of zero within said barrier layer and antisymmetrical nodes in said pair of quantum confinement structures so that the wavefunction of said next lowest energy level is decoupled between said pair of quantum confinement structures; and wherein said pair of quantum confinement structures having a Fermi level for electrons; and wherein, when a negative voltage is applied to said gate region, such that the energy of said next lowest energy level is shifted from an energy lying above the energy of said Fermi level to an energy lying below the energy of said Fermi level at the interface between said gate controlled channel portion and said source and drain channel portions, whereby electron waves in said electron waveguide structure are coupled between said pair of quantum confinement structures when said energy of said next lowest energy level is above the energy level of said Fermi level electron waveguide.

Claim 27

An electron wave combining device according to claim 21, wherein said quantum confinement structures comprises a semiconductor substrate, a first clad layer provided on said substrate, a first quantum well layer provided on said first clad layer, a barrier layer provided on said first quantum well layer, a second quantum well layer provided on said barrier layer and a second clad layer provided on said second quantum well layer, wherein bottom energy levels of the first clad layer, the second clad layer and the barrier layer are higher than bottom energy levels of the first and second quantum well layers in a conduction band.

Claim 28

An electron wave combining device according to claim 22, wherein each thickness of said first and second quantum well layers are different from each other.