Majorana fermion confirmed after 77 years

Post Reply
User avatar
Pigeon
Posts: 18058
Joined: Thu Mar 31, 2011 3:00 pm

Majorana fermion confirmed after 77 years

Post by Pigeon » Sun Oct 05, 2014 3:11 pm

A team of physicists at Princeton University and the University of Texas at Austin announced on October 2 that they have observed a new particle that has eluded detection for nearly 80 years.

This new particle was first predicted by Italian physicist Ettore Majorana in 1937, and is unique because it is the only particle in existence that can adopt both matter and antimatter characteristics simultaneously without annihilating itself in the process.

The conflicting qualities in Majorana fermions work in such a way that the particle rarely interacts with its environment. While this makes it difficult to detect it also means that this new particle could be the next major advance in the pursuit of quantum computing.

Quantum computers will transmit data through quantum bits, called qbits. But qbits will take on a quantum state that allows them to be both a one and zero simultaneously. The problem is that it's difficult for scientists to find a particle that can act as a qbit without readily interacting with nearby material, which would destroy the quantum system. But the Majorana fermion could be the solution.

The material that the team used was an ultra pure crystal of lead. The crystal contained ridges that the scientists filled with iron atoms forming an iron wire within the lead. Under freezing conditions, -457 degrees Fahrenheit, the Majorana fermions begin to form at both ends of the wires, and Yazdani and the team were able to snap a picture of this in action, which is shown above.

Yazdani and the team new exactly where to look for Majorana fermions because many years of theoretical calculations had indicated that if these particles existed, then they would show up at opposite ends of a material.

Link


User avatar
Pigeon
Posts: 18058
Joined: Thu Mar 31, 2011 3:00 pm

Re: Majorana fermion confirmed after 77 years

Post by Pigeon » Sun Oct 05, 2014 3:15 pm

In particle physics, a fermion (a name coined by Paul Dirac from the surname of Enrico Fermi) is any particle characterized by Fermi–Dirac statistics and obeying the Pauli exclusion principle. Fermions include all quarks and leptons, as well as any composite particle made of an odd number of these, such as all baryons and many atoms and nuclei. Fermions differ from bosons, which obey Bose–Einstein statistics.

A fermion can be an elementary particle, such as the electron, or it can be a composite particle, such as the proton. According to the spin-statistics theorem in any reasonable relativistic quantum field theory, particles with integer spin are bosons, while particles with half-integer spin are fermions.

Besides this spin characteristic, fermions have another specific property: they possess conserved baryon or lepton quantum numbers. Therefore what is usually referred as the spin statistics relation is in fact a spin statistics-quantum number relation.

As a consequence of the Pauli exclusion principle, only one fermion can occupy a particular quantum state at any given time. If multiple fermions have the same spatial probability distribution, then at least one property of each fermion, such as its spin, must be different.

Fermions are usually associated with matter, whereas bosons are generally force carrier particles, although in the current state of particle physics the distinction between the two concepts is unclear


Post Reply