Grassmann numbers and Fermions

Click For Summary
SUMMARY

This discussion clarifies the relationship between fermions and Grassmann numbers in Quantum Field Theory (QFT). While Grassmann numbers, such as ##\theta_1## and ##\theta_2##, yield zero when multiplied in certain combinations, the term ##\bar{\psi}(x)\psi(x)\bar{\psi}(x)\psi(x)## in the Quantum Electrodynamics (QED) Lagrangian does not automatically equate to zero. This is due to the fact that fermions are quantum particles governed by Fermi-Dirac statistics, and their creation and annihilation operators belong to a Clifford Algebra rather than solely a Grassmann algebra. The discussion emphasizes the importance of explicitly writing out terms in spinor components to understand their behavior.

PREREQUISITES
  • Understanding of Quantum Field Theory (QFT)
  • Familiarity with Grassmann algebra
  • Knowledge of Fermi-Dirac statistics
  • Basic concepts of Clifford Algebra
NEXT STEPS
  • Study the properties of Grassmann numbers in Quantum Field Theory
  • Learn how to derive terms in the QED Lagrangian explicitly using spinor components
  • Explore the structure and applications of Clifford Algebra in quantum mechanics
  • Investigate the implications of Fermi-Dirac statistics on particle behavior
USEFUL FOR

Physicists, particularly those specializing in Quantum Field Theory, theoretical physicists, and students seeking to deepen their understanding of fermions and their mathematical representations.

kelly0303
Messages
573
Reaction score
33
Hello! I am a bit confused about fermions in QFT when they are considered grassmann numbers. If you have 2 grassmann numbers ##\theta_1## and ##\theta_2##, something of the form ##\theta_1\theta_2\theta_1\theta_2## gives zero. However, a term in a QED lagrangian of the form ##\bar{\psi(x)}\psi(x)\bar{\psi(x)}\psi(x)## is not automatically zero. If fermions are Grassmann numbers, why isn't that term also zero?
 
  • Like
Likes   Reactions: arivero
Physics news on Phys.org
Fermions are not Grassmann numbers. Fermions are quantum particles with Fermi-Dirac statistics.
That statistics can be expressed by the fact that their creation operators are elements of a Grassmann algebra, and dually their annihilation operators are also elements of a (dual) Grassmann algebra. But the full algebra of Fermi-Dirac creation and annihilation operators forms a neutral signature Clifford Algebra.

Specifically:
\bar{\psi}_a(x)\psi_b(y) +\psi_b(y)\bar{\psi}_a(x) = \delta_{ab} \delta(y-x)\boldsymbol{1}
(That's the Kronecker and Dirac delta functions on the r.h.s.)
 
  • Like
Likes   Reactions: arivero
kelly0303 said:
Hello! I am a bit confused about fermions in QFT when they are considered grassmann numbers. If you have 2 grassmann numbers ##\theta_1## and ##\theta_2##, something of the form ##\theta_1\theta_2\theta_1\theta_2## gives zero. However, a term in a QED lagrangian of the form ##\bar{\psi(x)}\psi(x)\bar{\psi(x)}\psi(x)## is not automatically zero. If fermions are Grassmann numbers, why isn't that term also zero?
Well, how do you do derive that ##\theta_1\theta_2\theta_1\theta_2## gives zero? I guess you write ##\theta_1\theta_2\theta_1\theta_2 = - \theta_1\theta_1\theta_2\theta_2 = -0 \times 0 = 0##.

So the question is: if you write out the term ##\bar{\psi}(x)\psi(x)\bar{\psi}(x)\psi(x)## explicitly in spinorcomponents of ##\psi##, what do you get? I leave that explicit writing out to you; that's the essential part of your question, I think ;) So pick a basis and write it out.

edit: your tex-code should read \bar{\psi}(x) instead of \bar{\psi(x)} for readability if you ever want to use that in your own texts.
 

Similar threads

  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 49 ·
2
Replies
49
Views
7K
  • · Replies 13 ·
Replies
13
Views
3K
  • · Replies 20 ·
Replies
20
Views
1K
  • · Replies 38 ·
2
Replies
38
Views
5K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K