Quantum mechanical framework for interaction of OAM with matter and applications in solid states, biosciences and quantum computing
A system for applying orbital angular momentum (OAM) to electrons of a semiconductor material comprises a light source generator for generating a plane wave light beam. Orbital angular momentum (OAM) processing circuitry applies at least one orbital angular momentum to the plan wave light beam to generate an OAM light beam. The OAM processing circuitry controls transitions of electrons between quantized states within the semiconductor material to perform quantum entanglement within the semiconductor material responsive to the at least one orbital angular momentum applied to the plane wave light beam. A transmitter transmits the OAM light beam at the semiconductor material to induce the transitions of the electrons between the quantize states and perform the quantum entanglement within the semiconductor material.
1. A method for applying orbital angular momentum (OAM) to electrons of a semiconductor material, comprising:
generating a plane wave light beam;
applying at least one orbital angular momentum to the plane wave light beam to generate an OAM light beam;
controlling transitions of electrons between quantized states within the semiconductor material to perform quantum entanglement within the semiconductor material responsive to the at least one orbital angular momentum applied to the plane wave light beam; and
transmitting the OAM light beam at the semiconductor material to induce the transitions of the electrons between the quantize states and perform the quantum entanglement within the semiconductor material.
2. The method of claim 1 , wherein the step of controlling further comprises the step of controlling at least one of spectrum, pulse shape, time of arrival, transverse wave vector and position of quantized states of photons within the OAM light beam to control the transition of electrons between the quantized states.
3. The method of claim 1 , wherein the step of controlling further comprises the steps of measuring a state of at least one photon within the OAM light beam to cause states of remaining photons to collapse, wherein the collapse of the states of the remaining photons enable the remaining photons to interact and entangle.
4. The method of claim 1 , wherein step of controlling further comprises further comprises creating qudits responsive to the at least one orbital angular momentum applied to the plane wave light beam.
5. The method of claim 4 , wherein the step of controlling further comprises creating a higher order radix system to create the qudits responsive to the at least one orbital angular momentum applied to the plane wave light beam.
6. The method of claim 1 , wherein the induced transitions of the electrons create a net electric current and magnetic field.
7. The method of claim 1 , wherein the step of controlling further controls the transitions of electrons between the quantized states using OAM-generalized semiconductor Bloch equations and coherences of the electrons.
8. The method of claim 1 , wherein the step of controlling further uses cylindrical coordinates to decouple Heisenberg equations.
9. The method of claim 1 , wherein the OAM light beam is within frequencies from an infrared spectrum to a UV spectrum.
10. The method of claim 1 , wherein the step of controlling further comprises spatially buffering information in time by controlling a size and shape of the OAM light beam to obtain different apparent sub-liminal velocities for different values of OAM.
11. The method of claim 1 , wherein the step of controlling further comprises encoding information in a twist of a state function.
12. The method of claim 11 , wherein the step of encoding further comprises the step of exchanging positions of Majorana quasiparticles in a non-Abelian unitary transformation depending only on a topology of trajectories of the Majorana quasiparticles.
13. The method of claim 1 , wherein the step of controlling further comprises the step of braiding Majorana fermion with Majorana photons that are carrying the orbital angular momentum within the OAM light beam.
14. The method of claim 1 , wherein the step of controlling further comprises using temperature control to go from one symmetry space to another to braid wave functions within the OAM light beam.
15. A system for applying orbital angular momentum (OAM) to electrons of a semiconductor material, comprising:
a light source generator for generating a plane wave light beam;
orbital angular momentum (OAM) processing circuitry for applying at least one orbital angular momentum to the plan wave light beam to generate an OAM light beam, wherein the OAM processing circuitry controls transitions of electrons between quantized states within the semiconductor material to perform quantum entanglement within the semiconductor material responsive to the at least one orbital angular momentum applied to the plane wave light beam; and
a transmitter for transmitting the OAM light beam at the semiconductor material to induce the transitions of the electrons between the quantize states and perform the quantum entanglement within the semiconductor material.
16. The system of claim 15 , wherein the OAM processing circuitry controls at least one of spectrum, pulse shape, time of arrival, transverse wave vector and position of quantized states of photons within the OAM light beam to control the transition of electrons between the quantized states.
17. The system of claim 15 , wherein the OAM processing circuitry measures a state of at least one photon within the OAM light beam to cause states of remaining photons to collapse, wherein the collapse of the states of remaining photons enable the remaining photons to interact and entangle.
18. The system of claim 15 , wherein OAM processing circuitry creates qudits responsive to the at least one orbital angular momentum applied to the plane wave light beam.
19. The system of claim 18 , wherein the OAM processing circuitry creates a higher order radix system to create the qudits responsive to the at least one orbital angular momentum applied to the plane wave light beam.
20. The system of claim 15 , wherein the induced transitions of the electrons create a net electric current and magnetic field.
21. The system of claim 15 , wherein the OAM processing circuitry controls the transitions of electrons between quantized states using OAM-generalized semiconductor Bloch equations and coherences of the electrons.
22. The system of claim 15 , wherein the OAM processing circuitry uses cylindrical coordinates to decouple Heisenberg equations.
23. The system of claim 15 , wherein the OAM light beam is within frequencies from an infrared spectrum to a UV spectrum.
24. The system of claim 15 , wherein the OAM processing circuitry spatially buffers information in time by controlling a size and shape of the OAM light beam to obtain different apparent sub-liminal velocities for different values of OAM.
25. The system of claim 15 , wherein the OAM processing circuitry further encodes information in a twist of a state function.
26. The system of claim 25 , wherein the OAM processing circuitry further encodes by exchanging positions of Majorana quasiparticles in a non-Abelian unitary transformation depending only on a topology of trajectories of the Majorana quasiparticles.
27. The system of claim 15 , wherein the OAM processing circuitry braids Majorana fermion with Majorana photons that are carrying the orbital angular momentum within the OAM light beam.
28. The system of claim 15 , wherein the OAM processing circuitry uses temperature control to go from one symmetry space to another to braid wave functions within the OAM light beam.