Two-dimensional electrostrictive field effect transistor (2D-EFET)
A device and method for manufacturing a two-dimensional electrostrictive field effect transistor having a substrate, a source, a drain, and a channel disposed between the source and the drain. The channel is a two-dimensional layered material and a gate proximate the channel. The gate has a column of an electrostrictive or piezoelectric or ferroelectric material, wherein an electrical input to the gate produces an elongation of the column that applies a force or mechanical stress on the channel and reduces a bandgap of two-dimensional material such that the two-dimensional electrostrictive field effect transistor operates with a subthreshold slope that is less than 60 mV/decade.
1. A two-dimensional electrostrictive field effect transistor comprising:
a substrate having a surface;
a source;
a drain;
a channel with a bandgap disposed between the source and the drain, the channel being a two-dimensional layered material, the bandgap of the channel being switchable between a first bandgap and a second bandgap, the first bandgap being larger than the second bandgap;
a gate having a column of an electrostrictive or piezoelectric or ferroelectric material, wherein an electrical input to the gate produces an elongation of the column from a length L 1 to a length L 2 , the length L 2 being greater than the length L 1 ;
the transistor switchable between an off state and an on state, the column having the length L 1 in the off state, the column having the length L 2 after the electrical input is applied to the gate, the channel having the first bandgap in the off state; and
a capping, the substrate, the source, the drain, and the channel being embedded inside the capping, the capping directly contacting the surface of the substrate, the gate disposed such that the elongation of the column of the gate from the length L 1 to the length L 2 due to the electrical input applies a force on the channel and dynamically reduces the first bandgap of the two-dimensional layered material to the second bandgap thereby switching the transistor to the on state,
wherein removal of the electrical input produces dimensional change in the column from the length L 2 to the length L 1 thereby removing the force on the channel, dynamically increasing the second bandgap to the first bandgap and switching the transistor to the off state.
2. The two-dimensional electrostrictive field effect transistor of claim 1 , wherein the two-dimensional layered material comprises a semiconductor of MX 2 , wherein M is a transition metal atom of Molybdenum (Mo), Tungsten (W) or Tin (Sn) and X is a chalcogen atom of Sulphur (S), Selenium (Se) or Tellurium (Te).
3. The two-dimensional electrostrictive field effect transistor of claim 1 , wherein the elongation of the column is such that the channel transitions from an insulator or large bandgap semiconductor to a metal or small bandgap semiconductor.
4. The two-dimensional electrostrictive field effect transistor of claim 1 , wherein the electrical input to the gate is a voltage.
5. The two-dimensional electrostrictive field effect transistor of claim 1 , wherein the elongation of the column is such that the bandgap of the two-dimensional layered material of the channel substantially decreases to zero.
6. The two-dimensional electrostrictive field effect transistor of claim 1 , wherein the channel has two or more layers of the two-dimensional layered material.
7. The two-dimensional electrostrictive field effect transistor of claim 1 , wherein the two-dimensional electrostrictive field effect transistor has a subthreshold swing of less than 60 mV/decade.
8. The two-dimensional electrostrictive field effect transistor of claim 1 , further comprising:
another gate having another column of an electrostrictive or piezoelectric or ferroelectric material, the electrical input to the another gate produces an elongation of the another column; and
the channel having a first surface and a second surface, wherein the column of the gate applies the force on the first surface of the channel and the another gate is disposed such that the elongation of the another column applies another force on the second surface of the channel and reduces the bandgap of the two-dimensional layered material.
9. A method of manufacturing a two-dimensional electrostrictive field effect transistor comprising:
forming a substrate having a surface;
forming a source;
forming a drain;
forming a channel of two-dimensional layered material and disposing the channel between the source and the drain, the channel having a bandgap that is switchable between a first bandgap and a second bandgap, the first bandgap being larger than the second bandgap;
forming a gate proximate the channel, the gate comprising a column of an electrostrictive or piezoelectric or ferroelectric material, the two-dimensional electrostrictive field effect transistor configured such that applying an electrical input to the gate produces an elongation of the column from a length L 1 to a length L 2 , the length L 2 being greater than the length L 1 , the transistor being switchable between an off state and an on state, the column having the length L 1 in the off state, the column having the length L 2 after the electrical input is applied to the gate, the channel having the first bandgap in the off state;
providing a capping; and
embedding the substrate, the gate, the source, the drain and the channel inside the capping, with the capping directly contacting the surface of the substrate, such that the elongation of the column of the gate from the length L 1 to the length L 2 due to the electrical input to the gate applies a force or mechanical stress on the channel and dynamically reduces the first bandgap of the two-dimensional layered material to the second bandgap thereby switching the transistor to the on state,
wherein removal of the electrical input produces dimensional change in the column from the length L 2 to the length L 1 thereby removing the force on the channel, dynamically increasing the second bandgap to the first bandgap and switching the transistor to the off state.
10. The method of claim 9 , wherein the two-dimensional layered material comprises semiconductor of MX 2 , wherein M is a transition metal atom of Molybdenum (Mo), Tungsten (W) or Tin (Sn) and X is a chalcogen atom of Sulphur (S), Selenium (Se) or Tellurium (Te).
11. The method of claim 9 , wherein the step of forming the gate comprises forming the column of an electrostrictive or piezoelectric or ferroelectric material whose elongation applies the force such that the channel transitions from an insulator or large bandgap semiconductor to a metal or small bandgap semiconductor.
12. The method of claim 9 , further applying a voltage as the electrical input to the gate to produce the elongation of the column.
13. The method of claim 9 , further configuring the two-dimensional electrostrictive field effect transistor such that the elongation of the column decreases the bandgap of the two-dimensional material of the channel to substantially zero.
14. The method of claim 9 , wherein the step of forming the channel comprises forming the channel from two or more layers of the two-dimensional layered material.
15. The method of claim 9 , wherein the two-dimensional electrostrictive field effect transistor has a subthreshold swing of less than 60 mV/decade.
16. The method of claim 9 , further comprising forming a second gate, wherein the channel being disposed between the gate and the second gate, the second gate having a second column of an electrostrictive or piezoelectric or ferroelectric material, the second gate producing an elongation of the second column that applies a force or mechanical stress on the channel and reduces the bandgap of the two-dimensional layered material.