World sheet EM tensor in complex coordinates

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Discussion Overview

The discussion centers on the expression for the holomorphic component of the energy-momentum tensor in complex coordinates as presented in Becker, Becker, Schwarz. Participants explore the reasoning behind using complex coordinates and the implications for the energy-momentum tensor in the context of conformal invariance.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions why the expression for the holomorphic component of the energy-momentum tensor is formulated in complex coordinates.
  • Another participant expresses confusion about the validity of using complex coordinates, suggesting that there is nothing inherently wrong with them.
  • A third participant references E. Kiritsis to explain that complex coordinates simplify the transformation of tensor components and facilitate achieving 2-dimensional conformal invariance.
  • One participant attempts to derive the expression for the energy-momentum tensor in complex coordinates but arrives at a result that suggests it should vanish, leading to uncertainty about how the original expression was obtained.
  • A later reply affirms the result of the energy-momentum tensor vanishing but does not clarify the derivation of the original expression.

Areas of Agreement / Disagreement

Participants express differing levels of understanding regarding the use of complex coordinates and the derivation of the energy-momentum tensor expression. There is no consensus on the clarity of the original formulation or the reasoning behind it.

Contextual Notes

Some participants note that the book's treatment of the topic may assume prior knowledge or intuitive understanding of the relationship between complex coordinates and the energy-momentum tensor, which could lead to confusion.

da_willem
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In my Book (Becker, Becker, Schwarz) it is stated (eq 3.23) that the holomorphic component of the EM tensor is given by

[tex]T_X(z)=T_{zz}=-2 : \partial _z X \cdot \partial _z X :[/tex]

Now why is the expression for the (holonorphic, zz, component of the) energy momentum tensor in complex coordinates?
 
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da_willem said:
In my Book (Becker, Becker, Schwarz) it is stated (eq 3.23) that the holomorphic component of the EM tensor is given by

[tex]T_X(z)=T_{zz}=-2 : \partial _z X \cdot \partial _z X :[/tex]

Now why is the expression for the (holomorphic, zz, component of the) energy momentum tensor in complex coordinates?

I do not really understand the question, what is wrong with using complex coordinates?

nonplus
 
See e.g. E. Kiritsis, hep-th/9709062, page 44.
Essentially, you introduce new coordinates z=x+iy and \bar{z}=x-iy and then transform the components of the energy-momentum to new coordinates by the usual rules of tensor transformation.
If your question is why complex coordinates are introduced at the first place, the answer is because the requirement of 2-dimensional conformal invariance is particularly easy to achieve with complex coordinates. See e.g. (6.1.6) and (6.1.7) in the reference above.
 
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Hmm, they were so short about it in the book that I think they presumed the relation should be intuitively clear or common knowledge or something. Well, I tried the transformation to complex coordinates:

[tex]T(z)= T_{zz} = (\frac{\partial x^0}{\partial z})^2T_{00} + (\frac{\partial x^1}{\partial z})^2T_{11}[/tex]

As the off-diagonal elements are zero. Now using [itex]x^0=\frac{1}{2}(z+/bar{z})[/tex] and [itex]x^1=\frac{i}{2}(z-/bar{z})[/tex] we get that <br /> <br /> [tex]T(z)=\frac{1}{4}(T_{00} -T_{11}[/tex]<br /> <br /> which is zero, as the terms are equal. This is the correct result, the ws em tensor should vanish, but leaves me blank as to how they got that expression...[/itex][/itex]
 
da_willem said:
This is the correct result, the ws em tensor should vanish, but leaves me blank as to how they got that expression...
The same way you did. :smile:
 

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