What Is the Central Charge in Conformal Field Theory?

  • Thread starter Thread starter Pacopag
  • Start date Start date
  • Tags Tags
    Charge
Click For Summary
SUMMARY

The central charge in Conformal Field Theory (CFT) is a crucial concept that represents an operator commuting with all other symmetry operators, known as a Casimir operator. It is denoted by the letter 'c', which can also refer to its eigenvalue, leading to potential confusion. CFT allows for fractional central charges, such as c=1/2 for free fermions, and imposes constraints on allowed values based on unitary representations of the Virasoro algebra, specifically requiring c≥1 and h≥0. The relationship between central charge in CFT and other Lie algebras, like Galilei or Poincare, is fundamentally similar, rooted in the principle of central extension.

PREREQUISITES
  • Understanding of Conformal Field Theory (CFT)
  • Familiarity with the Virasoro algebra
  • Knowledge of Casimir operators in quantum mechanics
  • Basic principles of Lie algebras and their representations
NEXT STEPS
  • Study the properties of the Virasoro algebra in detail
  • Explore the implications of central charge on unitary representations
  • Investigate fractional central charges in various CFTs
  • Read Ginsparg's lectures on CFT for comprehensive insights
USEFUL FOR

The discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, string theory, and mathematical physics, as well as students seeking to deepen their understanding of conformal field theories.

Pacopag
Messages
193
Reaction score
4
Hi. I'm trying to learn CFT on my own, and central charge seems to be a pretty important concept. It seems that I can only find mathematical definitions in terms of the stress-energy tensor, or the Virasoro algebra. I was wondering if someone could give me a physical interpretation of central charge, or at least a definition in plain English.

Thanks.
 
  • Like
Likes   Reactions: spaghetti3451
Physics news on Phys.org
they're the casimirs of the theory. A casimir of a theory is an operator that commutes with all other symmetry operators of a theory. For angular momentum this is the L_i L^i operator. The eigenvalues of the Casimir are used to determine the system, such as the j(j+1) for the angular momentum.

Hope that was of some use
 
  • Like
Likes   Reactions: spaghetti3451
Sure. That helps a bunch.

So when we say that a CFT has central charge of, say, c=2, do we really mean that the "eigenvalue" of c is 2?.
 
  • Like
Likes   Reactions: spaghetti3451
Yes, the letter c is used to denote both the operator and it's eigenvalue. This confusing state of affairs is the convention
 
  • Like
Likes   Reactions: spaghetti3451
So if c is an operator, then I'm guessing that it may carry several eigenvalues. But I've never heard of a CFT with more than one central charge. Maybe I just haven't read far enough yet. Is there such thing as fractional or irrational central charges? Like, say, c=pi?
 
  • Like
Likes   Reactions: spaghetti3451
I have to step down at this point since I'm not familiar with CFT I only know about central charges from string theory
 
  • Like
Likes   Reactions: spaghetti3451
No problem. Thanks for your help. I guess I just have to keep reading.
 
  • Like
Likes   Reactions: spaghetti3451
sgd37 said:
they're the casimirs of the theory. A casimir of a theory is an operator that commutes with all other symmetry operators of a theory. For angular momentum this is the L_i L^i operator. The eigenvalues of the Casimir are used to determine the system, such as the j(j+1) for the angular momentum.

Hope that was of some use

Does the notion of central charge in the context of the conformal field theory differ so radically from the notion of central charge for any other Lie algebra, like for example the Galilei or Poincare ones ? I'm just asking, because I don't see any reason, even if we complement the CFT algebra of n-dimensional space-time with SUSY generators. In other words the concept of central charge should be uniform (and essentially mathematic) for any physical Lie algebra or superalgebra.
 
  • Like
Likes   Reactions: spaghetti3451
bigubau said:
Does the notion of central charge in the context of the conformal field theory differ so radically from the notion of central charge for any other Lie algebra, like for example the Galilei or Poincare ones ? I'm just asking, because I don't see any reason, even if we complement the CFT algebra of n-dimensional space-time with SUSY generators. In other words the concept of central charge should be uniform (and essentially mathematic) for any physical Lie algebra or superalgebra.

The central charge in a CFT is based on the same principle of central extension as in any other Lie algebra. The Virasoro algebra projects onto the Witt algebra when you divide by the center. Both are subalgebras of the algebra of diffeomorphisms on S^1.

There was a question about allowed values of the central charge. If we're talking about representations of the Virasoro algebra, the constraint arises from demanding that the representations be unitary (no negative norm states). All values of c\geq 1, h\geq 0 are allowed (h is the conformal weight), while between 0<c<1 there is a discrete set of points

c= 1 -\frac{6}{m(m+1)}, ~ m=3,4,\ldots .

A blatant example of a fractional value of c is that of a free fermion, which has c=1/2. Ginsparg's lectures http://arxiv.org/abs/hep-th/9108028 are a great reference for many CFT topics.
 
  • Like
Likes   Reactions: Demystifier

Similar threads

Replies
3
Views
3K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 10 ·
Replies
10
Views
2K
Replies
98
Views
3K
  • · Replies 3 ·
Replies
3
Views
4K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 12 ·
Replies
12
Views
2K
Replies
27
Views
3K
  • · Replies 50 ·
2
Replies
50
Views
4K
  • · Replies 6 ·
Replies
6
Views
3K