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I have encountered an equation in page 33 in the book of D.MacMahon titled QFT demystefied.

It is the third equation from the top....how did the sum appear as a middle step of the equation?

best regards.

Abolaban

- Thread starter Abolaban
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- #1

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I have encountered an equation in page 33 in the book of D.MacMahon titled QFT demystefied.

It is the third equation from the top....how did the sum appear as a middle step of the equation?

best regards.

Abolaban

- #2

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What should have been done is to pick a different summation index for the Lagrangian (or why not differentiate with respect to ##\partial_\rho\varphi##???). You can then apply the rules for a derivative of a product and note that ##\partial(\partial_\mu \varphi)/\partial(\partial_\rho \varphi) = \delta_\mu^\rho##.

Edit: To be clear, the end result is correct, the middle step is not.

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where can one correctly learn about the usuage of such notations?

- #4

ChrisVer

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I don't know any book that would go into showing calculations as Demystified... In most of cases you have to be very careful yourself of the writer's steps and what he is actually doing... eg if you did the same calculation yourself, you wouldn't use same-indices with the derivatives.where can one correctly learn about the usuage of such notations?

- #5

ChrisVer

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:D Correct by luck...Edit: To be clear, the end result is correct, the middle step is not.

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The best (i.e., worst) way of being correct. Although I think it is rather a case of "IknowwhatIshouldgetsoIwillbesloppyinthemiddlesteps"-syndrome.:D Correct by luck...

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I have the following books, however, it is hard to recognize which could match the QFT tensor analysis...what do you recommend among them?

-Daniel Fleisch: A Student's Guide to Vectors and Tensors

-Derek F.Lawden: An Introduction to Tensor Calcul

-J.A.Schouten:Tensor Analysis for Physicists

-Mikhail Itskov: Tensor Algebra and Tensor Analysi

-Nadir Jeevanjee: An Introduction to Tensors

-Nazrul Islam: Tensors and their applications

Abolaban

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$$

\frac{\partial \mathcal L}{\partial(\partial_\rho\varphi)} = \frac{\partial}{\partial(\partial_\rho\varphi)} g^{\mu\nu}(\partial_\mu\varphi)(\partial_\nu\varphi)

= g^{\mu\nu}[ \delta_\mu^\rho \partial_\nu\varphi + \delta_\nu^\rho\partial_\mu\varphi] = 2\partial^\rho\varphi

$$

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I went through "Tensor analysis" in Math Meth for Physicists by Arfken and Weber pages 133 and beyond but I could not recognize how did you split that term into summation!?

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Do you understand the following result for ordinary derivatives of functions of one variable?

I went through "Tensor analysis" in Math Meth for Physicists by Arfken and Weber pages 133 and beyond but I could not recognize how did you split that term into summation!?

$$

\frac{d}{dx}f(x) g(x) = f'(x) g(x) + f(x) g'(x)

$$

- #12

ChrisVer

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there will be more that look similar to this, but this is straightforward to see... equation 2.130b he uses the same "summation" thing, generally called the product rule...I went through "Tensor analysis" in Math Meth for Physicists by Arfken and Weber pages 133 and beyond but I could not recognize how did you split that term into summation!?

- #13

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yeah...you use this from vector analysis...dealing with tensors carry special flavours...so the tast might sometimes mix in one's tongue.

--equation 2.130b seems to carry different flavour...namely by Christoffel

- #14

ChrisVer

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flavour?--equation 2.130b seems to carry different flavour...namely by Christoffel

Well what he did was write [itex]\textbf{V} = V^i e_i [/itex]

and take the derivative [itex] \frac{d}{dq^j} \textbf{V} =\frac{d}{dq^j} (V^i e_i) =\frac{dV^i}{dq^j} e_i + V^i \frac{de_i}{dq^j} [/itex]

Especially at this point, it is just vector-analysis...

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- #16

ChrisVer

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The kinetic term can as well be written by using the metric:

[itex] (\partial_{\mu} \phi) g^{\mu \nu} (\partial_\nu \phi) = (\partial_\mu \phi) (\partial^\mu \phi ) =(\partial^\mu \phi ) (\partial_\mu \phi) [/itex]

But using just the metric he can easily use the:

[itex] \frac{\partial (\partial_{\nu} \phi) }{\partial (\partial_\mu \phi)} = \delta_{\nu}^\mu [/itex].

instead of having:

[itex] \frac{\partial (\partial^{\nu} \phi) }{\partial (\partial_\mu \phi)} = g^{\nu \rho} \delta_{\rho}^\mu[/itex].

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ok...now it is clear....thank you "ChrisVer"

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