Single-charge tunnelling device

Abstract
A single-electron transistor (1) has an elongate conductive channel (2) and a side gate (3) formed in a 5 nm-thick layer (4) of Ga0.98Mn0.02As. The single-electron transistor (1) is operable, in a first mode, as a transistor and, in a second mode, as non-volatile memory.
Description

BRIEF DESCRIPTION OF THE DRAWINGS

Embodiments of the present invention will now be described, by way of example, with reference to the accompanying drawings in which:



FIG. 1 is perspective schematic view of a single-electron transistor in accordance with certain embodiments of the present invention;



FIG. 2 shows electron-beam micrographs of the single-electron transistor shown in FIG. 1;



FIG. 3 is a schematic plan view of a Hall bar including the single-electron transistor 1 shown in FIG. 1 and a test structure;



FIG. 4 shows plots of resistance against magnetic field for the test structure shown in FIG. 3;



FIGS. 5
a and 5b show plots of resistance against magnetic field for the single-electron transistor shown in FIG. 1;



FIGS. 6
a and 6b show plots of resistance against magnetic field orientation for different gate voltages for the single-electron transistor shown in FIG. 1;



FIG. 7 shows a plot of resistance against magnetic field orientation for the single-electron transistor shown in FIG. 1;



FIG. 8 shows a circuit model for a single-electron transistor;



FIG. 9 illustrates current-voltage plots for the single-electron transistor shown in FIG. 1;


Referring to FIGS. 10a and 10b show contributions to Gibbs energy associated with the transfer of charge from a lead to an island of a single-electron transistor;



FIG. 11 shows plots of density-dependent chemical potentials with respect to uniaxial anisotropy modelled using a k.p kinetic-exchange model;



FIG. 12 shows a plot of Coulomb blockade conductance as a function of gate voltage for the single-electron transistor shown in FIG. 1;



FIG. 13 shows a plot of resistance as a function of gate bias and magnetic field strength for the single-electron transistor shown in FIG. 1;



FIG. 14 shows plots of resistance against magnetic field for the single-electron transistor shown in FIG. 1;



FIGS. 15
a to 15c illustrate steps in a process of fabricating of the single-electron transistor shown in FIG. 1;



FIG. 16 shows Coulomb blockade oscillation curves for the single-electron transistor shown in FIG. 1;



FIG. 17 show plots of resistance against magnetic field for the single-electron transistor shown in FIG. 1;



FIGS. 18
a to 18c show illustrative potential distributions and stable magnetization states for different magnetisations angles;



FIG. 19 illustrates electrical switching of states;



FIG. 20 is a greyscale plot of conductance as a function of magnetic field for the single-electron transistor shown in FIG. 1;



FIGS. 21
a and 21b are conductance plots as a function of magnetic field for the single-electron transistor shown in FIG. 1;



FIG. 22 show plots of conductance against gate bias for B=0 T, B=−0.1 T, B=−0.022 T and B=−0.035 T for the single-electron transistor shown in FIG. 1;



FIG. 23 illustrates a process for manipulating and storing information using the single-electron transistor shown in FIG. 1;



FIG. 24 is a state table;



FIG. 25 is a schematic diagram of a generic device in accordance with certain embodiments of the present invention;



FIG. 26 shows a lateral conduction device in accordance with certain embodiments of the present invention;



FIG. 27 is a cross-section of the device shown in FIG. 26 taken along the line A-A′;



FIG. 28 illustrates a vertical conduction device in accordance with certain embodiments of the present invention;



FIG. 29 shows self-assembled islands;



FIG. 30 illustrates shape anisotropy;



FIG. 31 illustrates stabilization of magnetization of a ferromagnetic region in an external field; and



FIG. 32 illustrates a head in accordance with certain embodiments of the present invention.


Claims
  • 1. A single-charge tunnelling device comprising: first and second leads; anda conductive island arranged such that charge is transferable from the first lead to the second lead via the conductive island;a gate for changing an electrostatic energy of the conductive island;wherein at least one of said first lead, second lead, island and gate comprises a ferromagnetic material which exhibits a change in chemical potential in response to a change in direction of magnetisation.
  • 2. A device according to claim 1, wherein the first lead, the second lead and the island each comprise the same ferromagnetic material.
  • 3. A device according to claim 2, wherein the gate comprises the same ferromagnetic material.
  • 4. A device according to claim 1, wherein the first lead, the second lead and the island are formed in a layer of the ferromagnetic material.
  • 5. A device according to claim 4, wherein the first lead, the second lead, the island and lead are formed in a layer of the ferromagnetic material
  • 6. A device according to claim 4, wherein the layer has a constriction and the conductive island is formed within the constriction.
  • 7. A device according to claim 2, wherein shapes of the first lead, the second lead and the island are arranged such that magnetisation of at least one of the first lead, second lead and island is forced along a direction transverse to magnetisation of remaining ones of the first lead, second lead and island or is forced along a different direction from the other direction for which the chemical potentials are different.
  • 8. A device according to claim 2, comprising at least two islands arranged such that charge is transferable from the first lead to the second lead via at least one of the at least two conductive islands.
  • 9. A device according to claim 1, wherein the conductive island (10) has a charging energy and the change in direction of magnetisation causes a change in chemical potential of at least of the order of the charging energy.
  • 10. A device according to claim 1, wherein at least two of the first lead, second lead and island comprises a ferromagnetic material and there is a net change in chemical potential in response to a change in direction of magnetisation of at least one of the at least two of the first lead, second lead and island.
  • 11. A device according to claim 1, wherein the change in chemical potential is at least 1 meV.
  • 12. A device according claim 1, wherein the change in chemical potential is at least 6 meV or at least 9 meV.
  • 13. A device according to claim 1, wherein said ferromagnetic material is GaMnAs.
  • 14. A device according to claim 1, wherein said ferromagnetic material is Ga0.98Mn0.02As.
  • 15. A device according to claim 1, wherein said ferromagnetic material comprises an alloy which includes a rare earth metal.
  • 16. A device according to claim 15, wherein said rare earth metal is Dy, Er or Ho.
  • 17. A device according to claim 1, wherein said ferromagnetic material comprises an alloy which includes a transition or noble metal
  • 18. A device according to claim 1, wherein said ferromagnetic material comprises FePt, CoPt or CoPd.
  • 19. A non-volatile memory comprising a device according to claim 1.
  • 20. A magnetic field sensor comprising a device according to claim 1.
  • 21. A single-charge tunnelling device comprising: first and second leads; anda conductive island arranged such that charge is transferable from the first lead to the second lead via the conductive island;wherein at least one of the first lead, second lead and island comprises a ferromagnetic material which exhibits a change in chemical potential in response to a change in direction of magnetisation.
  • 22. A device comprising: first and second leads;first and second tunnel barriers; anda conductive island arranged such that charge is transferable from the first lead to the second lead via the first tunnel barrier, the conductive island and the second tunnel barrier;wherein at least one of the first lead, second lead and island comprises a ferromagnetic material which exhibits a change in chemical potential in response to a change in direction of magnetisation.
  • 23. A method of operating a single-charge tunnelling device comprising first and second leads, a conductive island arranged such that charge is transferable from the first lead to the second lead via the conductive island and a gate for changing an electrostatic energy of the conductive island, at least one of said first lead, second lead, island and gate comprises a ferromagnetic material which exhibits a change in chemical potential in response to a change in direction of magnetisation, the method comprising: applying a first bias to the gate;removing said first bias from the gate;measuring a first resistance between the leads;applying a second, different bias to the gate;removing said second bias from the gate;measuring a second resistance between the leads;
  • 24. A method of operating a single-charge tunnelling device comprising first and second leads, a conductive island arranged such that charge is transferable from the first lead to the second lead via the conductive island, at least one of said first lead, second lead and island comprises a ferromagnetic material which exhibits a change in chemical potential in response to a change in direction of magnetisation, the method comprising: applying a first magnetic field;removing the first magnetic field;measuring a first resistance between the leads;applying a second, different magnetic field;removing the second magnetic field;measuring a second resistance between the leads;
Priority Claims (1)
Number Date Country Kind
06110428.7 Feb 2006 EP regional