Making Fermionic Condensates: Overcoming the Exclusion Principle

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SUMMARY

Fermionic condensates are achieved through the pairing of fermions, allowing them to behave collectively as bosons, which then undergo Bose-Einstein condensation. This process relies on the formation of Cooper pairs, where fermions with opposite quantum numbers can occupy the same state without violating the exclusion principle. Recent reports confirm the occurrence of pairing in fermionic gases, building on earlier findings by Deborah Jin's group that indicated condensation without observable pairing. These advancements deepen the understanding of quantum statistics and the behavior of fermions in condensed matter physics.

PREREQUISITES
  • Understanding of quantum mechanics, specifically the exclusion principle
  • Familiarity with Cooper pairs and their role in superconductivity
  • Knowledge of Bose-Einstein condensation principles
  • Basic grasp of quantum numbers and their significance in particle physics
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  • Research the formation and properties of Cooper pairs in superconductors
  • Explore the principles of Bose-Einstein condensation in detail
  • Investigate the latest findings in fermionic gases and their implications
  • Study the differences between single-particle and two-particle statistics in quantum systems
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Physicists, researchers in condensed matter physics, and students interested in quantum mechanics and superconductivity will benefit from this discussion.

p_branes
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My question is that how did people actually make a fermionic condensate? I would think this would be extremely difficult as the exclusion principle states that fermions cannot be in the same quantum state so how ebactly did people achieve this?
 
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p_branes said:
My question is that how did people actually make a fermionic condensate? I would think this would be extremely difficult as the exclusion principle states that fermions cannot be in the same quantum state so how ebactly did people achieve this?

They can't be in the same quantum state. Remember that if you describe a free particle as plane waves, there are two quantum numbers, n and k, that describe such a system. You can have two fermions having the same n, but having k1 and -k1 quantum numbers, k2 and -k2, etc...

For Cooper pairs in conventional superconductors, this is exactly the case. Equal but opposite electrons k's for two electrons pair up forming a singlet state. So for example, you have one pair with k1 and -k1, another pair having k2 and -k2, etc... So essentially, each fermions are STILL uniquely different as far as their quantum numbers are concerned. If n1,k1 is already taken, another electron cannot scatter into that state.

The difficulty in understanding all this is that the "single-particle" statistics for fermions is still obeyed. However, when you consider a bound pair, you now have to consider the two-particle statistics, which can be very different if these particle are bosons (or composite bosons in this case).

Zz.
 
A fermionic condensate is actually composed of particles which can form pairs. The paired up fermions act as if they were collectively a boson, and then the bosons Bose-Einstein condense.

http://physicsweb.org/article/news/8/1/14

- Warren
 
Thanks now i get it.
 
i think they made fermionic condensate cos i saw it in "Focus" the other day
 
Sometime things on here don't get followed up, or forgotten and another new string starts up asking the same thing all over again.

As a follow up to this, don't miss the new report on the further development of the saga of the Fermionic condensate. This time a pair of reports (still not out officially yet) have confirmed the occurrence of pairing in a fermionic gas upon condensation. This will be an analogous process occurring in superconductors with the formation of Cooper pairs.

http://physicsweb.org/article/news/8/7/12

The earlier report by the Deborah Jin's group only reported a condensation in a fermionic gas. They could not observe any pairing but hinted that it could happen. This new report seals the deal.

Zz.
 

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