The present disclosure relates to the field of quantum communication. More particularly, it relates to a method for information transfer over long distance using negatively charged sub-atomic particles.
BACKGROUND
[0002] Background description includes information that may be useful in understanding the present disclosure. It is not an admission that any of the information provided herein is prior art or relevant to the presently claimed disclosure, or that any publication specifically or implicitly referenced is prior art. [0003] Transferring huge volume of information over long distance typically requires huge amount of time and the received information is not real-time as the communication suffers from transmission delays. Therefore there is need in the art to develop a method for fast transfer of information by using inherent properties of sub-atomic particles.
[0004] Concept of quantum teleportation using shared entanglement state between electrically paired negatively charged particles has been discussed in prior art. Instantaneous induction of change of spin state of a Cooper pair of negatively charges sub-atomic particles have been investigated and reported in existing literature. Another disclosure discusses the applicability of quantum communication to interstellar distances. However none of the disclosures describe the step by step procedure of capturing negatively charged sub-atomic particles with shared electrical properties and transmission of information by controlling motion of any or a combination of both negatively charges sub-atomic particles. [0005] The proposed method describes the sequence of functional steps involved in capturing of electrically paired negatively charged sub-atomic particles, determining spin state and controlling of the spin states of the captured negatively charged sub-atomic particles for instantaneous transfer of information generated at a first location to a second location, the first and the second locations being separated by long distances.

OBJECTS OF THE PRESENT DISCLOSURE
[0006] Some of the objects of the present disclosure, which at least one embodiment herein satisfies are as listed herein below.
[0007] It is an object of the present disclosure to provide a method for information transfer over long distance using negatively charged sub-atomic particles.
[0008] It is an object of the present disclosure to provide a method for information transfer over long distance comprising a step that facilitates entrapping of a pair of electrically coupled negatively charged sub-atomic particles using single electron transistors, the pair of negatively charged sub¬atomic particles being separated by long distance.
[0009] It is an object of the present disclosure to provide a method for information transfer over long distance comprising a step that enables a user to determine spin states of any or a combination of the pair of entrapped negatively charged sub-atomic particles by magnetic deflection of the negatively charged sub-atomic particles using a first and a second Stern-Gerlach apparatus. [0010] It is an object of the present disclosure to provide a method for information transfer over long distance comprising a step that enables controlling the spin states of any or a combination of the pair of negatively charged sub¬atomic particles by applying beam of light and a second magnetic field to any or a combination of the pair of entrapped negatively charged sub-atomic particles. [0011] It is an object of the present disclosure to provide a method for information transfer over long distance comprising a step that enables encoding event pertaining to change of spin states of any or a combination of the pair of negatively charged sub-atomic particles into digital information comprising of binary digits.
[0012] It is an object of the present disclosure to provide a method for information transfer over long distance that induces changes in spin states of a first negatively charged sub-atomic particle to changes in spin states of a second negatively charged sub-atomic particle, the first and the second negatively

charged sub-atomic particles pertaining to the pair of electrically coupled negatively charged sub-atomic particles.
SUMMARY
[0013] The present disclosure relates to the field of quantum communication. More particularly, it relates to a method for information transfer over long distance using negatively charged sub-atomic particles.
[0014] An aspect of the present disclosure pertains to a method for information transfer over long distance that may use negatively charged sub¬atomic particles.
[0015] In an aspect, the method may facilitate entrapping of a Cooper pair of electrically coupled negatively charged sub-atomic particles using single electron transistors.
[0016] In an aspect, a first negatively charged sub-atomic particle may be captured by a first single electron transistor and a second negatively charged sub¬atomic particle may be captured by a second single electron transistor, the first and the second negatively charged sub-atomic particles pertaining to the Cooper pair of negatively charged sub-atomic particles.
[0017] In an aspect the first and the second single electron transistors may be placed at a first and a second location, the first and the second locations being separated by long distance.
[0018] In an aspect, the method may enable a user to determine spin states of any or a combination of the pair of entrapped negatively charged sub-atomic particles by magnetic deflection of the negatively charged sub-atomic particles using a first and a second Stern-Gerlach apparatus.
[0019] In an aspect, the first Stern-Gerlach apparatus may be placed at the first location and the second Stern-Gerlach apparatus may be placed at the second location.
[0020] In an aspect the method may enable controlling the spin states of any or a combination of the pair of negatively charged sub-atomic particles by applying beams of light and a second magnetic field to any or a combination of

the pair of entrapped negatively charged sub-atomic particles in the first and the
second location.
[0021] In an aspect, the spin states of any or a combination of the pair of
entrapped negatively charged sub-atomic particles may be either preserved or
inverted in response to interaction with the beams of light.
[0022] In an aspect the method may comprise a step that enables encoding
change of spin states of any or a combination of the pair of negatively charged
sub-atomic particles into digital information comprising of binary digits.
[0023] In an aspect, the method facilitates changes in spin states of the first
negatively charged sub-atomic particle to induce changes in spin states of the
second negatively charged sub-atomic particle and vice versa instantaneously.
BRIEF DESCRIPTION OF THE ACCOMPANYING DRAWINGS
[0024] The accompanying drawings are included to provide a further
understanding of the present disclosure, and are incorporated in and constitute a
part of this specification. The drawings illustrate exemplary embodiments of the
present disclosure and, together with the description, serve to explain the
principles of the present disclosure.
[0025] The diagrams described herein are for illustration only, which thus are
not limitations of the present disclosure, and wherein:
[0026] FIG. 1 illustrates exemplary steps of the proposed method (100) for
information transfer over long distance using negatively charged sub-atomic
particles in accordance with an embodiment of the present disclosure.
[0027] FIG. 2 illustrates exemplary representation (200) of a single electron
transistor pertaining to the proposed method (100) for information transfer over
long distance using negatively charged sub-atomic particles in accordance with an
embodiment of the present disclosure.
[0028] FIG. 3 illustrates exemplary flow diagram (300) of the proposed
method (100) for information transfer over long distance using negatively charged
sub-atomic particles in accordance with an embodiment of the present disclosure.

DETAILED DESCRIPTION
[0029] In the following description, numerous specific details are set forth in order to provide a thorough understanding of embodiments of the present invention. It will be apparent to one skilled in the art that embodiments of the present invention may be practiced without some of these specific details. [0030] If the specification states a component or feature "may", "can", "could", or "might" be included or have a characteristic, that particular component or feature is not required to be included or have the characteristic. [0031] As used in the description herein and throughout the claims that follow, the meaning of "a," "an," and "the" includes plural reference unless the context clearly dictates otherwise. Also, as used in the description herein, the meaning of "in" includes "in" and "on" unless the context clearly dictates otherwise.
[0032] While embodiments of the present invention have been illustrated and described in the accompanying drawings, the embodiments are offered only in as much detail as to clearly communicate the disclosure and are not intended to limit the numerous equivalents, changes, variations, substitutions and modifications falling within the spirit and scope of the present disclosure as defined by the appended claims.
[0033] Groupings of alternative elements or embodiments of the invention disclosed herein are not to be construed as limitations. Each group member can be referred to and claimed individually or in any combination with other members of the group or other elements found herein. One or more members of a group can be included in, or deleted from, a group for reasons of convenience and/or patentability. When any such inclusion or deletion occurs, the specification is herein deemed to contain the group as modified thus fulfilling the written description of all groups used in the appended claims.
[0034] Each of the appended claims defines a separate invention, which for infringement purposes is recognized as including equivalents to the various elements or limitations specified in the claims. Depending on the context, all references below to the "invention" may in some cases refer to certain specific

embodiments only. In other cases it will be recognized that references to the "invention" will refer to subject matter recited in one or more, but not necessarily all, of the claims.
[0035] Various terms as used herein are shown below. To the extent a term used in a claim is not defined below, it should be given the broadest definition persons in the pertinent art have given that term as reflected in printed publications and issued patents at the time of filing.
[0036] The present disclosure relates to the field of quantum communication. More particularly, it relates to a method for information transfer over long distance using negatively charged sub-atomic particles.
[0037] FIG. 1 illustrates exemplary steps of the proposed method (100) for information transfer over long distance using negatively charged sub-atomic particles in accordance with an embodiment of the present disclosure. [0038] In an embodiment the method (100) may include a step (102) that may be facilitated to enable a user to select a Cooper pair of negatively charged sub¬atomic particles, the Cooper pair comprising a first negatively charged sub-atomic particle loosely electrically coupled to a second negatively charged sub-atomic particle. The first and the second negatively charged sub-atomic particles have opposite spin states, spin state pertaining to rotational motion of the negatively charged sub-atomic particle about a predetermined axis. The spin state of the first negatively charged sub-atomic particle may pertain to a first spin orientation and the second negatively charged sub-atomic particle may pertain to a second spin orientation. The first spin orientation may pertain to clockwise rotational motion about the predetermined axis and the second spin orientation may pertain to counter clockwise rotational motion about the predetermined axis or vice versa. In an embodiment, change in the first spin state may induce change in the second spin state and vice versa instantaneously. In an embodiment, the Cooper pair of negatively charged sub-atomic particles may be selected by the user from a superconductive material at a predetermined temperature.
[0039] In an embodiment, proposed method (100) for information transfer over long distance using negatively charged sub-atomic particles may include a

step (104) that may facilitate entrapping of the first negatively charged sub-atomic particle using a first single electron transistor and the second negatively charged sub-atomic particle using a second single electron transistor. In an exemplary embodiment, the first and the second single electron transistors may be coupled to a superconductive material comprising the Cooper pair of negatively charged sub-atomic particles. By way of example, the first and the second single electron transistors may be implemented using a first and a second field effect transistor, each field effect transistor being configured to have a first, second and a third electrode. The first and the second electrodes may be coupled to a power supply unit that may be configured to provide electric power of predetermined specifications to the first, second and the third electrode of the single electron transistor.
[0040] In an exemplary embodiment, the first electrode may be enabled to receive a first electrical signal of predetermined magnitude and the second electrode may be enabled to receive a second electrical signal of predetermined magnitude, the first and the second electrical signals being opposite in polarity. The negatively charged sub-atomic particles may pertain to the set of negatively charged sub-atomic particles comprising current flow from the first to the second electrode of any or a combination of the first and the second single electron transistors. Rate of current flow from the first to the second electrode may be controlled magnitude and polarity of a third electrical signal applied to the third electrode of the single electron transistor, the first, second and third electrical signals corresponding to either a voltage or a current signal. [0041] In an embodiment, any or a combination of the first and the second single electron transistors may be fabricated to facilitate formation of an isolated conducting channel between the first and the second electrode of any of the first and the second single electron transistor. A first junction may be generated between the first electrode and the isolated conducting channel and a second junction may be generated between the second electrode and the isolated conducting channel. By way of example, the negatively charged sub-atomic particles pertaining to current flow from the first to the second electrode of any of

the first and the second single electron transistor may be configured to tunnel through the first and the second junction depending on the potential applied to the third electrode. The selected first and the second negatively charged sub-atomic particles may be trapped in the isolated conducting channels of the first and the second field effect transistors.
[0042] In an embodiment, the method (100) may comprise a step (106) that may be configured to place the first negatively charged sub-atomic particle in the first single electron transistor to be placed in a first location and transfer the second negatively charged sub-atomic particle in the second single electron transistor to be placed in a second location. In an embodiment, the first location may include a first Stern-Gerlach apparatus configured to accommodate the first single electron transistor and the second location may include a second Stern-Gerlach apparatus configured to accommodate the second single electron transistor. The first and the second locations may be separated by long distance. By way of example, the first single electron transistor may be placed on earth and the second single electron transistor may be placed on Mars, Mars and Earth being 3.03 light minutes away from each other, that enables traditional communication delay of 6.06 minutes at least. Proposed method (100) may facilitate transfer of information instantaneously.
[0043] In an embodiment, the method (100) may include a step (108) that may enable determination of spin states of any or a combination of the trapped first and the second negatively charged sub-atomic particles located in the first and the second locations. In an exemplary embodiment, inside any or a combination of the first and the second Stern-Gerlach apparatus, a first magnetic field may be applied to the trapped first and the second negatively charged sub-atomic particles, the first inhomogeneous magnetic field pertaining to predetermined strength and duration. The negatively charged sub-atomic particles may be deflected in response to application of the first magnetic field. The direction and magnitude of deflection of the trapped negatively charged sub-atomic particles under the influence of the first magnetic field may be configured to determine spin state of the corresponding first and the second negatively charged sub-atomic particles.

By way of example, the first negatively charged sub-atomic particle may be deflected in a first direction and the second negatively charged sub-atomic particle may be deflected in a second direction, the first and the second directions being opposite in sense and the directions pertaining to vertical or horizontal displacements of the negatively charged sub-atomic particles. [0044] In an embodiment, the first negatively charged sub-atomic particles may have a first spin state and the second negatively charged sub-atomic particles may have a second spin state, the first and the second spin states pertaining to either positive or negative spin orientations. The first and a second spin state may correspond to a clockwise rotation and a counter clockwise rotation or vice versa, the rotations being configured about any of a set of orthogonal axes. The exemplary set of axes may pertain to the x, y and the z axis. Strength and duration of the applied first magnetic fields in the first and the second Stern-Gerlach apparatus may be predetermined. By way of non-limiting example a positive half spin may pertain to deflection in vertically up direction and a negative half spin may pertain to deflection in vertical down direction.
[0045] In an embodiment, the method (100) may comprise a step (110) that may be configured to control the spin states of any or a combination of the entrapped negatively charged sub-atomic particles by applying beam of light and a second magnetic field to the first and the second entrapped negatively charged sub-atomic particles in the first and the secondlocations. By way of example, the beam of light may pertain to predetermined wavelength and may be applied to the entrapped negatively charged sub-atomic particles for predetermined durations. The second magnetic field may pertain to predetermined strength. The application of the beam of light and second magnetic field in the first and the second Stern-Gerlach apparatus may be configured to perform any of operations including but not limited to preservation of original spin state of the corresponding entrapped negatively charged sub-atomic particle and change of spin state of the entrapped negatively charged sub-atomic particle, the negatively charged sub-atomic particle pertaining to any or a combination of the first and the second negatively charged sub-atomic particle. The operations may be caused by interaction of the entrapped

negatively charged sub-atomic particles with the photon particles of the beams of light.
[0046] In an embodiment, the method (100) may include a step (112) that may be configured to encode in a predetermined fashion, occurrence of an event of change of spin state of any or a combination of the entrapped negatively charged sub-atomic particles into digital information. By way of example, the digital information encoding the change of spin state events may pertain to any of binary digits 0 and 1, the first change of spin state being encoded as 0 and subsequently second change of spin state being encoded as 1 or vice versa, based on the original spin state determined in step (108).
[0047] FIG. 2 illustrates exemplary representation (200) of a single electron transistor pertaining to the proposed method (100) for information transfer over long distance using negatively charged sub-atomic particles in accordance with an embodiment of the present disclosure.
[0048] In an illustrative embodiment, any or a combination of the first and the second single electron transistors may be implemented using field effect transistor. The first and the second electrodes of the first and the second field effect transistor may be coupled to the power supply unit that may be configured to provide electric power of predetermined specifications. By way of example, the single electron transistor may pertain to any of a metallic and a semiconducting tunneling device for a negatively charged sub-atomic particle. The first electrode may be enabled to receive the first electrical signal of predetermined magnitude and the second electrode may be enabled to receive the second electrical signal of predetermined magnitude, the first and the second electrical signals being opposite in polarity. By way of example, the first electrode may be coupled to a +5 volt supply and the second electrode may be coupled to a 0 volt supply. In another embodiment, the first electrode may be coupled to a +2.5 volt supply and the second electrode may be coupled to a -2.5 volt supply. Rate current flow from the first to the second electrode may be controlled by magnitude and polarity of the third electrical signal applied to the third electrode. A third junction formed between the third electrode and the isolated conducting channel between the fist

and the second electrodes may be configured to exhibit capacitive electrical properties. By way of example, negative voltage signal may be coupled to the third electrode, the negative voltage signal being enabled to electrostatically influence the isolated conducting channel between the first and the second junctions. Negative charge depleted region formed due to application of the third electrical signal may be enabled to trap the negatively charged sub-atomic particle in the isolated conducting channel or quantum dot.
[0049] FIG. 3 illustrates exemplary flow diagram (300) of the proposed method (100) for information transfer over long distance using negatively charged sub-atomic particles in accordance with an embodiment of the present disclosure. [0050] In an illustrative embodiment, the first negatively charged sub-atomic particle may be trapped by the first single electron transistor and the second negatively charged sub-atomic particle may be trapped by the second single electron transistor. The first single electron transistor may be placed in the first Stern-Gerlach apparatus in the first location. By way of non-limiting example, the second single electron transistor may be placed in the second Stern-Gerlach apparatus in the second location. The first location may be on Earth and the second location may be on Mars. Inside any or a combination of the first and the second Stern-Gerlach apparatus, the first inhomogeneous magnetic field may be applied to the first and the second trapped negatively charged sub-atomic particles. The direction and magnitude of deflection of the trapped negatively charged sub-atomic particles under the influence of the first magnetic field may be configured to determine spin states of the first and the second negatively charged sub-atomic particles.
[0051] In an embodiment, the first and the second trapped negatively charged sub-atomic particles in the first and the second Stern-Gerlach apparatus may be subjected to the beam of light of predetermined wavelength in presence of the second magnetic field of predetermined strength. Under the impact of the beam of light, the spin states of the trapped negatively charged sub-atomic particles may either be preserved or changed, the spin-states being configured to pertain to any of the clockwise and counterclockwise orientations. By way of example, the spin

state change of the first negatively charged sub-atomic particle may be induced in the spin state of the second negatively charged sub-atomic particle or vice versa because of the electrical pairing between the first and the second negatively charged sub-atomic particles. Occurrence of spin-change event of the trapped negatively charged sub-atomic particles may be encoded as binary stream of information. The binary stream of information may be transmitted to any or a combination of a first computing device coupled to the first Stern-Gerlach apparatus and a second computing device coupled to the second Stern-Gerlach apparatus, the first and the second computing devices being configured to store the received information from the first and the second Stern-Gerlach apparatus. [0052] As used herein, and unless the context dictates otherwise, the term "coupled to" is intended to include both direct coupling (in which two elements that are coupled to each other contact each other) and indirect coupling (in which at least one additional element is located between the two elements). Therefore, the terms "coupled to" and "coupled with" are used synonymously. Within the context of this document terms "coupled to" and "coupled with" are also used euphemistically to mean "communicatively coupled with" over a network, where two or more devices are able to exchange data with each other over the network, possibly via one or more intermediary device.
[0053] The terms, descriptions and figures used herein are set forth by way of illustration only. Many variations are possible within the spirit and scope of the subject matter, which is intended to be defined by the following claims and their equivalents in which all terms are meant in their broadest reasonable sense unless otherwise indicated.
[0054] While the foregoing describes various embodiments of the invention, other and further embodiments of the invention may be devised without departing from the basic scope thereof. The scope of the invention is determined by the claims that follow. The invention is not limited to the described embodiments, versions or examples, which are included to enable a person having ordinary skill in the art to make and use the invention when combined with information and knowledge available to the person having ordinary skill in the art.

ADVANTAGES OF THE INVENTION
[0055] The present disclosure provides for a method for information transfer over long distance using negatively charged sub-atomic particles. [0056] The present disclosure provides for a method for information transfer over long distance comprising a step that facilitates entrapping of a pair of electrically coupled negatively charged sub-atomic particles using single electron transistors, the pair of negatively charged sub-atomic particles being separated by long distance.
[0057] The present disclosure provides for a method for information transfer over long distance comprising a step that enables a user to determine spin states of any or a combination of the pair of entrapped negatively charged sub-atomic particles by magnetic deflection of the negatively charged sub-atomic particles using a first and a second Stern-Gerlach apparatus.
[0058] The present disclosure provides for a method for information transfer over long distance comprising a step that enables controlling the spin states of any or a combination of the pair of negatively charged sub-atomic particles by applying beam of light and a second magnetic field to any or a combination of the pair of entrapped negatively charged sub-atomic particles.
[0059] The present disclosure provides for a method for information transfer over long distance comprising a step that enables encoding event pertaining to change of spin states of any or a combination of the pair of negatively charged sub-atomic particles into digital information comprising of binary digits. [0060] The present disclosure provides for a method for information transfer over long distance that induces changes in spin states of a first negatively charged sub-atomic particle to changes in spin states of a second negatively charged sub¬atomic particle, the first and the second negatively charged sub-atomic particles pertaining to the pair of electrically coupled negatively charged sub-atomic particles.

We Claim:

1. A method (100) for long distance information transfer using electrically paired negatively charged sub-atomic particles, the method (100) comprising the steps of :
selecting a first and a second negatively charged sub-atomic particles in a superconductive material, wherein the first and the second negatively charged sub-atomic particles pertain to a Cooper pair and wherein, the cooper pair is selected at predetermined temperature;
entrapping the pair of negatively charged sub-atomic particles, wherein the first negatively charged sub-atomic particle is captured by a first single electron transistor and wherein the second negatively charged sub-atomic particle is captured by a second single electron transistor;
placing the first negatively charged sub-atomic particle at a predetermined first location and transferring the second negatively charged sub-atomic particle at a predetermined second location, wherein the first and the second locations are separated by a long distance;
determining using a first and a second Stern-Gerlach apparatus, spin states of the corresponding first and the second negatively charged sub-atomic particles, wherein the spin states of the first and the second negatively charged sub-atomic particles pertain to a first and a second spin state, wherein the first and the second spin states are opposite in orientation;
controlling spin states of the entrapped negatively charged sub-atomic particles by applying a beam of light and a second magnetic field, wherein the beam of light pertains to predetermined wavelength;

encoding the change of spin events of the first and the second negatively charged sub-atomic particles into digital information based on the determined spin states of the corresponding first and the second negatively charged sub-atomic particles.
The method (100) as claimed in claim 1, wherein the first and the second single electron transistors correspond to a field effect transistors, wherein the field effect transistor is configured to enable flow of negatively charges sub-atomic particles from a first electrode of the field effect transistor to a second electrode of the field effect transistor, wherein the movement of negatively charges sub-atomic particles is controlled by a third electrode of the field effect transistor.
The method (100) as claimed in claim 2, wherein the field effect transistor is configured to have an isolated conducting channel, wherein the field effect transistor includes a first tunnel junction between the first electrode and the conducting channel and a second tunnel junction between the second electrode and the conducting channel, wherein the first and the second electrically paired negatively charged sub-atomic particles are facilitated to move across any or a combination of the first and the second tunnel junctions.
The method (100) as claimed in claim 2, wherein the negatively charged sub-atomic particles are captured in the isolated conducting channels of the first and the second single electron transistors in response to application of predetermined magnitude of voltages to the third electrode of the field effect transistors.
The method (100) as claimed in claim 1, wherein the first negatively charged sub-atomic particle of the Cooper pair pertains to a first spin state

and wherein the second negatively charged sub-atomic particle of the Cooper pair pertains to a second spin state.
The method (100) as claimed in claim 5, wherein the first and the second spin states of the negatively charged sub-atomic particles are determined along a predetermined axis, wherein the predetermined axis pertains to any of a three dimensional orthogonal set of axes, wherein the first spin state corresponds to clockwise rotation along the predetermined axis and wherein the second spin state corresponds to counterclockwise rotation along the predetermined axis.
The method (100) as claimed in claim 5, wherein spin states of the entrapped negatively charged sub-atomic particles pertain to predefined quantized angular momentum, the spin states being determined by application of a first magnetic field of predetermined strength, wherein the first magnetic field is inhomogeneous in nature and wherein the first magnetic field is configured to perform deflection of the negatively charged sub-atomic particles, the amount of deflection being predetermined and based on the corresponding spin states.
The method (100) as claimed in claim 1, wherein the applied second magnetic field pertains to predetermined strength, wherein the photon particles correspond to either the first or the second spin state, wherein, interaction between a photon particle and the negatively charged sub-atomic particle results in a first or a second outcome.
The method (100) as claimed in claim 8, wherein the first outcome corresponds to preservation of spin state of the negatively charged sub-atomic particle and wherein the second outcome corresponds to inversion of spin state of the negatively charged sub-atomic particle, wherein preservation and inversion of spin states result from positive alignment

and negative alignment of the negatively charged sub-atomic particles with the photon particles.
10. The method (100) as claimed in claim 1, wherein inversion of spin sate is encoded and stored as a bit of information based on the original spin state of the negatively charged sub-atomic particle, wherein the bit represents any of the digital states of 0 and 1.