Symmetry conservation of Dirac fermion with double junction and gauge field of Weyl fermion with single junction

Majorana fermion and Weyl fermion have matters and antimatters. But Majorana fermion has zero resistance and Weyl fermion has a resistance. It was confirmed that CP symmetry is preserved in the case of Dirac fermion because it only has spin current as the antimatter. Dirac fermion is supercurrent because CP symmetry is preserved by double schottky contact, but the Majorana fermion with ohmic contact has decreased current due to symmetry violation. Parity symmetry conservation was confirmed from the electrical properties of transistors, and charge symmetry conservation was confirmed in diode properties.


Introduction
The study of superconductors operating on the basis of magnetic energy is mainly dealt with in the field of spintronics and is classified as a two-class superconductor. The study of superconductors began in 1911 when mercury was observed to be resistance zero by the Onnes of the Netherlands, and the principle of operation of superconductors was found to be BCS theory. In 1957, the BCS theory explained the superconductor theoretically with two pairs of electronic coopers consisting of reverse spin direction. In order to confirm superconductivity, the resistance must be demonstrated to be zero, to prevent the moving of electrons and to appear the moving of spins, Meissner effect (resistance R=0) occurs in a strong magnetic field and at very low temperatures 1 -2 . In superconductors, there are many materials that have emerged as semiconductor technology has developed. The theory of copper-based semi-conductors in 1987 and iron-based superconductors in 2006 is described as spindensity wave (SDW). A superconductor that has been studied recently is a phase insulator. Phase insulators are internal insulators, but surface currents flow from the surface. To become a topological insulator, a small, thin 2D structure and magnetic field and low temperature are required [3][4][5] .
By using semiconductor-specific process technology, it can be made from a large area of material. The same material also increases its energy electromagnetic as its surface area widens. Thus, the topological insulator has superconductivity without magnetic field due to its structural effect with a large area.
Therefore, topological insulators have high surface energy, so the electronic energy relationships and differences of common insulators appear. Typically, topological insulators exhibit superconductivity without a magnetic field. This is called the Anomalous Quantum Hall Effect (AQHE). The surface current of the phase insulator starts from the kinetic energy of the spin rotation by the kinetic momentum of the electron. The magnetic field is generated by the electro-momentum and spin motion, and magnetic energy forms a spin current [6][7][8] .
The electron and spin are related to the matter and the antimatter. The electron, which is the matter, makes the charge current, and the spin, which is the antimatter, makes the spin current [9][10][11][12] . Matters and antimatters have the same physical quantity physically and chemically, but have a relationship of chiral symmetry, with opposite polarity electrically. Therefore, the charge current and spin current are opposite in polarity. The charge current has a + resistance in the field, and the spin current shows a negative resistance in the magnetic field. The spin current of the topological insulator is negative resistance characteristic and there is no loss of thermal resistance, so the super current flows [13][14][15][16] . Thus the topological insulator is an insulator, but it is the principle of current flow.
Studies of insulators have led to studies of schottky contact and low-k materials [17][18][19] , and recently reported that low-k materials are phase insulators 3 .
There has been a lot of research in the past on the cause of the increase in current values due to schottky contact. Schottky contact is caused by a depletion layer that occurs in the interface of semiconductor PN junction, and it is a good environment for schottky contact to make spin current, so it is highly likely that super current will be created [20][21] . Schottky resistance by schottky contact is the opposite concept of ohmic resistance. Low-k material produces spin current from a material that implements a schottky contact, so low-k makes it 10 times faster than normal OTFT movement 22 . Electromagnetic energy is preserved by Lenz's law. Matters and antimatters are symmetrical, and the antimatter of electrons are spin. The causes of the spin current of Majorana fermion, 23 Dirac fermion and Weyl fermion start from the electromagnetic energy momentum and the gauge field will occur when the energy gap is separated. Understanding the relationship between electromagnetic energy momentum and gauge field helps to understand the state of spin, quantum-spin-hole effect and abnormal quantum hall effect.
Unusual phenomena and studies of phase insulators are being reported as they create spin currents. [24][25][26] The conservation of the symmetry of fermion from the electrical properties of transistors using phase insulator was studied. Matters and antimatters have electro-magnetic energy composed of electric field and magnetic field by electron matters and spin antimatters. In figure 1, matters are three-dimensional structures, and the antimatters are obtained from twodimensional structures. The study of matters and antimatters has developed into classical mechanics that study matter and quantum mechanics that study the state of matter. The energy conservation law is maintained because it has the same energy value although the three dimensional kinetic energy (E=mc 2 ) and two dimensional wave energy (E=hγ). As the dimension changes, the plane of symmetry changes. In accordance with the Lenz Act, which is the energy conservation law of the electric field and the magnetic field, the Lenz plane, which becomes the reference plane where the electric field and the magnetic energy are symmetrical, is the threshold voltage in three dimensions. It is Weyl fermion that the energy moves in one direction according to the threshold voltage. Dirac fermion and Majorana fermion are energy state that follow the Dirac function, which are treated in two-dimensional quantum mechanics. The two-dimensional Dirac function is symmetrical, and the criterion of symmetry is Fermi-level. Electrically, if the fermi-level and the Lenz plane are in the same position, the energy is in the Majorana fermion state. However, it is difficult to make in the case of Majorana fermion, and most of the energy is in the state of Dirac fermion or Weyl fermion. The depletion layer is caused by two PN junctions, and the depletion layer creates a schottky contact. As shown in figure 2, the schottky contact is caused by magnetic field energy generated by the potential barrier. The spin produced by magnetic energy moves in positive (+) direction current and negative (-) direction, resulting in spin current by rotation and divergence. Therefore, the spin current depends on the schottky contact. There is a Dirac fermion where the spin current in a double junction becomes stronger due to the occurrence of the gauge field, a Weyl fermion that weakens the spin current, and a Majorana fermion that does not have a schottky contact before the gauge field occurs. Since Majorana fermion, Dirac fermion, and Weyl fermion are spin currents, quantum spins hall effects and quantum tunneling phenomena by the antimatter are shown.  Therefore, the Majorana fermion has both matters and antimatters. Weyl fermion also has both particles and carriers, but has high resistance. But Majorana fermion has no resistance. Dirac fermion, which has only the antimatter, also has no resistance. There is a difference in the method and amplification of electron energy of Majorana fermion and Dirac fermion.

Experimental method
The SiOC film was prepared by RF magnetron sputtering with a 2-in. diameter ceramic target

Results and discussions (1) Quantum tunneling phenomenon with zero resistance
The IDS-VGS transfer characteristics of transistors were studied to identify the spin current characteristics of phase insulator. The SiOC (19 sccm) ~SiOC (27 sccm) transistor has shown bidirectional transfer characteristics as shown in figure 6. It is observed that the negative IDS increases in SiOC (25 sccm). The logarithmic transformation was made as shown in figure 7 to identify quantum tunneling phenomena that occur when the resistance reaches zero. Tunneling is occurring at VDS =0 V. As VDS increases, tunneling is disappearing. When the internal magnetic field of phase insulator is large, tunneling phenomenon is caused by spin current. The reason why it operates in both directions is because spin current flows.      IDS current was compared from IDS-VDS input/output characteristics at VDS=0V. Comparing the IDS-VDS transmission characteristics of transistors in figure 12(a), large currents are dimmed at 19 sccm in areas where the voltage is low, but in figure 12(b), more current flows at 25 sccm as the voltage increases. Figure 11 to 19sccm shows the ohmic contact and 25sccm shows the double junction characteristics. It can be seen that the current has increased at 25 sccm, where the spin current is strongly made. The spin current was not made because the schottky contact was not made at 19sccm. Therefore, 19sccm is Majorana fermion, and 25sccm is Dirac fermion. Figure 13 shows the IDS-VGS transmission characteristics of quantum tunneling transistors at VDS=0.001 V.  Symmetry was shown at 25sccm, and as shown in Figure 14 (d), the Dirac fermion shows an increase in negative IDS current. The 19 sccm without symmetry can be seen as a Majorana fermion by the symmetry breaking as shown in Figure 14

(4) Charge symmetry conservation for super currents
Dirac fermion has only spin current. Therefore, the spin current is caused by the super current because the symmetry conservation. The spin current that occurs when the resistance is zero is most magnetic energy, so it becomes a super current as energy is converted into charge current by C symmetry conservation. Fig. 16. Generation of super currents from spin currents to charge currents by C symmetry. 3.0x10 -7 3.5x10 -7

(d)
As shown in figure 16, the Dirac fermion is amplified by CP symmetry preservation. Currentvoltage was measured with diode characteristics to examine the amplification effect of energy.
Comparing the current voltage diode characteristics in figure 17, there is a lot of charge current flowing at 25 sccm. In figure 18, the current voltage diode characteristics show that the current is rapidly changing at 17 sccm and 29 sccm. The thin film of 19 sccm to 25 sccm shows the properties of phase insulator as negative current is increasing. Fermion is made by phase isolator, and it can be seen that it is a negative current.    The phase isolator of 25 sccm has a large capacitance and a large loss at the same time. This is because the phase insulator has magnetic energy and negative resistance. Thus, the phase insulator of 25 sccm has a large loss, but the magnetic energy is so great that the capacitance is high that the current is greatly increased as shown in figure 17. Figure 7 shows that the IDS current of 25 sccm is small, but as explained in figure 5, the current of 25 sccm is greatly increased due to the amplification effect of the antimatter, as shown in figure 17.

Conclusion
The double-schottky junction was made for the conservation of parity symmetry, and supercurrents were created by magnetic energy with strong Dirac fermion in narrow doublejunctions. But the single schottky contacted Weyl fermion was not made of super current.
Mjyorana fermion had the lowest capacitance and no loss, and no schottky junctions were made and ohmic contacts were made. Thus, symmetry violation was identified in Majorana fermion, and the current was relatively very low as the voltage increased. Parity symmetry conservation was confirmed from the electrical properties of transistors, and charge symmetry conservation was confirmed in diode properties.