Zwiebach Page 197: Checking Translations & Commutators

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SUMMARY

The discussion focuses on Zwiebach's equation 11.60, where he examines whether the expression \( p^{\mu}(\tau) \) generates translations. The participants express confusion regarding the use of \( i \epsilon_{\rho} p^{\rho}(\tau) \) and the justification for taking the commutator with \( x^{\mu}(\tau) \) to demonstrate that translations are generated. It is concluded that a clearer presentation of the equations would enhance understanding, particularly by justifying each step in the derivation.

PREREQUISITES
  • Understanding of quantum mechanics, specifically the role of commutators in generating transformations.
  • Familiarity with the notation and concepts of field theory, including translations and symmetries.
  • Knowledge of Zwiebach's "String Theory" text, particularly equations related to translations.
  • Basic proficiency in mathematical physics, including manipulation of equations and understanding of tensors.
NEXT STEPS
  • Review the derivation of commutators in quantum mechanics, focusing on their role in generating symmetry transformations.
  • Study the implications of translations in quantum field theory, particularly in relation to Noether's theorem.
  • Examine other physics texts for alternative explanations of similar concepts to compare clarity and presentation.
  • Explore the mathematical foundations of tensor calculus as it applies to physics, enhancing comprehension of the notation used by Zwiebach.
USEFUL FOR

Students of theoretical physics, particularly those studying quantum mechanics and field theory, as well as educators seeking to improve their teaching methods in conveying complex mathematical concepts.

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Homework Statement


In equation 11.60, Zwiebach is supposed to be checking whether p^mu(tau) generates translations.

Firstly, I am not sure why he checks i epsilon_rho p^rho(tau) instead.

Second, I am not sure why taking the commutator with x^mu(tau) shows that this generates translations. He claims that taking commutators is the way to generate symmetry transformations above, but I do not see where he justifies that statement?



Homework Equations





The Attempt at a Solution

 
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This is an example of one of Zwiebach's habits that drives me up a wall. He is not the only author of physics books to do it. In school, I studied mathematics, not physics and in all of the textbooks I read, I never saw this practice. Here I go up on my soapbox.

Zwiebach writes:
[tex]\delta x^{\mu}(\tau) = [i\epsilon_{\rho}{p^{\rho}(\tau),x^{\mu}(\tau)] = i\epsilon_{\rho}(-i\eta^{\rho\mu}) = \epsilon^{\mu}.[/tex]

If this were changed to
[tex][i\epsilon_{\rho}{p^{\rho}(\tau),x^{\mu}(\tau)] = i\epsilon_{\rho}(-i\eta^{\rho\mu}) = \epsilon^{\mu} = \delta x^{\mu}(\tau).[/tex]

Then there would be 2 major improvements. First, each of the = signs in the equation could be justified by the previous text. The way Zwiebach wrote it, there is no justification for the first equal sign. Second, you could read the meat of the equation by removing the interior of the equation. In other words, if the author is trying to show that A = B, then A = B = C = D has B buried in the interior of the line where the reader has to dig it out. while A = C = D = B has the intended equation on the ends of the line where they are readable.

In the present case, Zwiebach is trying to show that

[tex][i\epsilon_{\rho}{p^{\rho}(\tau),x^{\mu}(\tau)] = \delta x^{\mu}(\tau).[/tex]
This is what he means by the expression [itex]i\epsilon_{\rho}p^{\rho}(\tau)[/itex] generates the translation (11.57)
 
Last edited:
I see. Thanks.
 

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