Undergrad What basically is Klein tunneling ?

  • Thread starter Thread starter phywithAK
  • Start date Start date
  • Tags Tags
    Klein Tunneling
Click For Summary
Klein tunneling refers to the phenomenon where Dirac electrons can tunnel through energy barriers without being affected by their width or height, a concept first theorized by Oskar Klein in 1929. This behavior is particularly observed in graphene, where massless Dirac electrons exhibit transmission probabilities that differ from classical predictions. When the barrier potential is approximately equal to the rest mass energy (V ≅ mc²), the tunneling behavior changes significantly, allowing for enhanced transmission at various angles. The α−T3 model further illustrates this by showing perfect transmission across potential steps and barriers for incoming electrons. Klein tunneling highlights the transition from classical to relativistic mechanics in quantum physics.
phywithAK
Messages
8
Reaction score
1
Recently, in my quantum physics classes i was introduced to the concept of tunneling of particle through a barrier potential and about transmission probability.
Our instructor mentioned about something known as "Klein tunneling".
Can somebody explain to me what is Klein tunneling and why behavior of the particle which is tunneling changes when barrier potential is approximately equal to rest mass energy,
V≅MC2 .
 
Physics news on Phys.org
phywithAK said:
Recently, in my quantum physics classes i was introduced to the concept of tunneling of particle through a barrier potential and about transmission probability.

one has to look up the following

We investigate Klein tunneling for the α−T3 model, which interpolates between graphene and the dice lattice via parameter α. We study transmission across two types of electrostatic interfaces: sharp potential steps and sharp potential barriers. We find both interfaces to be perfectly transparent for normal incidence for the full range of the parameter α for both interfaces. For other angles of incidence, we find that transmission is enhanced with increasing α. For the dice lattice, we find perfect, all-angle transmission across a potential step for incoming electrons with energy equal to half of the height of the potential step. This is analogous to the “super”, all-angle transmission reported for the dice lattice for Klein tunneling across a potential barrier.

Klein tunneling in the α−T3 model
E. Illes and E. J. Nicol
Phys. Rev. B 95, 235432 – Published 26 June 2017

 
  • Like
Likes phywithAK
that 1929 paper may be interesting...

However, the Dirac electrons found in graphene can tunnel through energy barriers regardless of their width and energy height; a phenomenon called Klein tunneling, described theoretically for 3D massive Dirac electrons by the Swedish physicist Oskar Klein in 1929. Graphene was the first material in which Klein tunneling was observed experimentally, as massive Dirac electrons required energy barriers too large to be observed.

Read more at: https://phys.org/news/2011-11-secrets-tunneling-energy-barriers.html#jCp
 
  • Like
Likes phywithAK
drvrm said:
that 1929 paper may be interesting...

However, the Dirac electrons found in graphene can tunnel through energy barriers regardless of their width and energy height; a phenomenon called Klein tunneling, described theoretically for 3D massive Dirac electrons by the Swedish physicist Oskar Klein in 1929. Graphene was the first material in which Klein tunneling was observed experimentally, as massive Dirac electrons required energy barriers too large to be observed.

Read more at: https://phys.org/news/2011-11-secrets-tunneling-energy-barriers.html#jCp

Thanks drvrm for this interesting link, so because of the electrons behaving as massless particles they no longer follow the classical physics energy equation
E=P2/2M ,
and tend to follow relativistic mechanics. So that would mean they would not also follow Schrodinger's equation also.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

Similar threads

  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 14 ·
Replies
14
Views
2K
  • · Replies 13 ·
Replies
13
Views
3K
Replies
1
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 21 ·
Replies
21
Views
5K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K