Grassmann Numbers & Commutation Relations

Click For Summary
SUMMARY

The discussion centers on the properties of Grassmann numbers and their interaction with creation and annihilation operators in quantum mechanics. It establishes that the expression <0|\eta|0> is well-defined and equals zero, due to the anticommutation relations of Grassmann numbers with these operators. The participants clarify that while Grassmann numbers are referred to as "numbers," they function as operators, leading to the conclusion that <1|a^{\dagger} \eta a|1> results in -<1|\eta|1>, reinforcing the zero outcome of <0|\eta|0>.

PREREQUISITES
  • Understanding of Grassmann numbers and their properties
  • Familiarity with creation and annihilation operators in quantum mechanics
  • Knowledge of quantum state notation, such as bra-ket notation
  • Basic grasp of anticommutation relations in operator algebra
NEXT STEPS
  • Study the mathematical framework of Grassmann algebra
  • Explore the implications of anticommutation relations in quantum field theory
  • Learn about the role of Grassmann numbers in supersymmetry
  • Investigate the applications of Grassmann variables in path integral formulation
USEFUL FOR

Physicists, particularly those specializing in quantum mechanics and quantum field theory, as well as mathematicians interested in algebraic structures related to physics.

RedX
Messages
963
Reaction score
3
If you have a Grassman number \eta that anticommutes with the creation and annihilation operators, then is the expression:

&lt;0|\eta|0&gt;

well defined? Because you can write this as:

&lt;1|a^{\dagger} \eta a|1&gt;=-&lt;1| \eta a^{\dagger} a|1&gt;<br /> =-&lt;1|\eta|1&gt;

But if \eta is a constant, then shouldn't:


&lt;0|\eta|0&gt;=&lt;1|\eta|1&gt;=\eta ?
 
Physics news on Phys.org
RedX said:
If you have a Grassman number \eta that anticommutes with the creation and annihilation operators, then is the expression:

&lt;0|\eta|0&gt;

well defined? Because you can write this as:

&lt;1|a^{\dagger} \eta a|1&gt;=-&lt;1| \eta a^{\dagger} a|1&gt;<br /> =-&lt;1|\eta|1&gt;

But if \eta is a constant, then shouldn't:


&lt;0|\eta|0&gt;=&lt;1|\eta|1&gt;=\eta ?

Grassmann numbers are operators (though they are called numbers).
&lt;0|\eta|0&gt;=0 is well-defined and vanishes.
 

Similar threads

  • · Replies 11 ·
Replies
11
Views
4K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 0 ·
Replies
0
Views
1K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 27 ·
Replies
27
Views
3K
  • · Replies 2 ·
Replies
2
Views
4K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 2 ·
Replies
2
Views
1K