Superconductivity and Pauli exclusion principle

In summary, Cooper pairs are composed of fermions and behave like bosons due to their large size, allowing them to share the same quantum state. However, due to the Pauli exclusion principle, they do not completely behave like bosons. In superfluids, the momentum of the Cooper pairs is approximately zero, but the individual electrons still obey the Pauli principle and do not occupy the same state. This means that the electrons in different Cooper pairs can have different momenta, but they still share the same quantum state.
  • #1
haael
539
35
I have the following problem understanding Pauli exclusion principle.

Two identical fermions can't share the same quantum state. Two bosons can.
Now Cooper pairs are bosons made up from fermions. Everything clear up to this point.
Now several Cooper pairs can share the same quantum state, since they are bosons.

And now: how do electrons inside particular Cooper pairs consider them different?

I mean: if every Cooper pair is identical to any other and all of them are in the same quantum state, then every such Cooper pair is the same quantum state.

How do electrons know they belong to different Cooper pairs when all of them are the same?

I bet the interactions inside a pair have something to do with it. But how it is mathematically described? How come electrons can tell apart different pairs from inside and still each of them looks the same from outside?

My questions also extend to superfluids and all bosons composed of fermions that share the same quantum state.
 
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  • #2
Cooper pairs are very large, on the order of hundreds of atoms in diameter. This is what allows two Cooper pairs to effectively share states. In reality, two overlapping Cooper pairs cannot share exactly the same state, because the pairs are composed of fermions that obey Pauli exclusion. However, since the Cooper pairs are so large, very minute differences in quantum state can be effectively ignored, and so they behave more or less like bosons. Cooper pairs do not exactly follow a Bose-Einstein distribution, but they come quite close (and can be made arbitrarily close under appropriate conditions).
 
  • #3
Cooper pairs do not exactly follow a Bose-Einstein distribution, but they come quite close
Wait, does that mean that there are no true composite bosons and only elementary particles can have Bose-Einstein statistics?
 
  • #4
haael said:
I have the following problem understanding Pauli exclusion principle.

Two identical fermions can't share the same quantum state. Two bosons can.
Now Cooper pairs are bosons made up from fermions. Everything clear up to this point.
Now several Cooper pairs can share the same quantum state, since they are bosons.

And now: how do electrons inside particular Cooper pairs consider them different?

I mean: if every Cooper pair is identical to any other and all of them are in the same quantum state, then every such Cooper pair is the same quantum state.

How do electrons know they belong to different Cooper pairs when all of them are the same?

I bet the interactions inside a pair have something to do with it. But how it is mathematically described? How come electrons can tell apart different pairs from inside and still each of them looks the same from outside?

My questions also extend to superfluids and all bosons composed of fermions that share the same quantum state.

The problem here is two-fold.

1. Remember that via the indistinguishably concept, you can't really track which electron does what.

2. There is a continuous scattering in and out of the [itex](k_1,-k_1), (k_2, -k_2), ...[itex] states that make up all of these Cooper Pairs. In other words, one can imagine that electrons keep on scattering in and out of the states. When one goes out, another comes into fill that place (since there's a lot of electrons). But since we can't distinguish one with the other, it is the same as having the same two fixed electrons sticking together to form such a pair.

So no, they don't really know, or even care, which composite boson it goes to. All an electron knows is that such a state is open and in it goes.

Zz.
 
  • #5
1. Remember that via the indistinguishably concept, you can't really track which electron does what.

2. There is a continuous scattering in and out of the [itex](k_1,-k_1), (k_2, -k_2), ...[itex] states that make up all of these Cooper Pairs. In other words, one can imagine that electrons keep on scattering in and out of the states. When one goes out, another comes into fill that place (since there's a lot of electrons). But since we can't distinguish one with the other, it is the same as having the same two fixed electrons sticking together to form such a pair.

So no, they don't really know, or even care, which composite boson it goes to. All an electron knows is that such a state is open and in it goes.
You are cheating me somewhere here :).

Suppose we have a superconducting loop with current flowing round. We can measure the count of Cooper pairs by checking the current or charge. All Cooper pairs sit on the same ground state (am I right?).
Now: what are the momenta of the electrons? When we think of it, they are halves of Cooper pair's momenta. And all pairs have the same momentum, so all electrons have the same momentum.
Something isn't right.

Putting superconductivity aside, what happens with protons of helium when it reaches superfluidity state?
 
  • #6
The momentum is a vector, so it is not the same for all electrons. In 3D the electrons near or at the surface of the Fermi sphere form Cooper pairs which condense into the lowest-energy state. The momentum of the Cooper pairs is -- in some approximation -- zero, as it pairs electrons with opposite momentum. However, that does not imply the momenta of the electrons participating in the Cooper-pair condensate are all the same.

The electrons still obey the Pauli principle and do not occupy the same quantum state.
 
  • #7
The momentum of the Cooper pairs is -- in some approximation -- zero, as it pairs electrons with opposite momentum. However, that does not imply the momenta of the electrons participating in the Cooper-pair condensate are all the same.
Do I understand you right:
Electron pairs of different momenta can couple into Cooper pairs of the same quantum state?
In other words, Cooper pairs "forget" some information about their electrons and have the same state outside, despite electrons inside them have different states?
 
  • #8
haael said:
You are cheating me somewhere here :).

Suppose we have a superconducting loop with current flowing round. We can measure the count of Cooper pairs by checking the current or charge. All Cooper pairs sit on the same ground state (am I right?).
Now: what are the momenta of the electrons? When we think of it, they are halves of Cooper pair's momenta. And all pairs have the same momentum, so all electrons have the same momentum.
Something isn't right.

Putting superconductivity aside, what happens with protons of helium when it reaches superfluidity state?

Er.. no. All the electrons cannot have the same momentum, etc.. The Fermi-Dirac distribution still applies to them, even when they form the Cooper Pairs.

Note that I labeled the momentum with different subscripts. If you construct the BCS ground state wave function, you'll notice that it is a series of plane-waves, each one over different k values. So for an isotropic s-wave pairing, you have [itex]k_n, -k_n[/itex] pairs, summed over all n's.

Zz.
 

Related to Superconductivity and Pauli exclusion principle

1. What is superconductivity?

Superconductivity is a phenomenon in which certain materials exhibit zero electrical resistance and expel magnetic fields when cooled below a certain critical temperature. This allows for the flow of electricity with no energy loss, making it a highly sought-after property in various applications.

2. What is the Pauli exclusion principle?

The Pauli exclusion principle is a fundamental principle in quantum mechanics that states that no two identical fermions (particles with half-integer spin, such as electrons) can occupy the same quantum state simultaneously. This principle plays a crucial role in understanding the behavior of electrons in superconducting materials.

3. How does the Pauli exclusion principle relate to superconductivity?

The Pauli exclusion principle plays a key role in superconductivity by limiting the number of electrons that can occupy a given energy state in a superconducting material. This results in the formation of electron pairs, known as Cooper pairs, which are responsible for the zero resistance and other unique properties of superconductors.

4. What is the critical temperature in superconductors?

The critical temperature is the temperature below which a material exhibits superconductivity. This temperature varies depending on the material, but all superconductors have a critical temperature below which they behave as superconductors and above which they behave like normal conductors.

5. What are some potential applications of superconductivity?

Superconductivity has the potential to revolutionize various fields, including transportation, energy, and healthcare. Some potential applications include more efficient power transmission, faster and more powerful computers, and advanced medical imaging techniques. However, there are still challenges to overcome, such as finding materials that exhibit superconductivity at higher temperatures and developing cost-effective manufacturing methods.

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