Help with the complex tensor notations

  • Thread starter Thread starter raj07
  • Start date Start date
  • Tags Tags
    Complex Tensor
raj07
Messages
4
Reaction score
0
i have attached two pages from a research paper.can someone interpret the mathematics in them or provide link that will help me in understanding the papers.i need help with the complex tensor notations involved.
the full paper can be downloaded from url given below:

http://www.google.co.in/url?sa=t&source=web&ct=res&cd=1&url=http%3A%2F%2Figitur-archive.library.uu.nl%2Fphys%2F2005-0622-155106%2FQuantum_theory_of_gravitation.pdf&ei=iBJbSvueEYyPkQXZwfzTBQ&usg=AFQjCNEqtBtRvoMKOJk4Gk2EDliH4CZBvQ&sig2=KBQZSSFO4az265cwjaLWtQ
 

Attachments

  • qm1.jpg
    qm1.jpg
    9.4 KB · Views: 439
  • Qm.jpg
    Qm.jpg
    18.2 KB · Views: 419
Last edited by a moderator:
Physics news on Phys.org


This is just usual tensor notation, nothing hard or complex here...

search this forum for "Tensors without tears" https://www.physicsforums.com/showthread.php?t=240285&highlight=tensors

search this forum for Quantum Field Theory: https://www.physicsforums.com/showthread.php?t=227115&highlight=quantum+field http://www.physics.ucsb.edu/~mark/qft.html (Try before you buy! Click here to download a pdf file of a prepublication draft of the text)

search this forum for General Relativity: https://www.physicsforums.com/showthread.php?t=101428&highlight=tensors Without a pretty strong background in General Relativity and Quantum field theory, it's going to be REALLY difficult for you to understand these class notes though =/

have fun good luck

BTW thanks for the link, looks like a good course given by one of the masters of QFT ^^
 
Last edited by a moderator:
Thread 'Why is there such a difference between the total cross-section data? (simulation vs. experiment)'
Well, I'm simulating a neutron-proton scattering phase shift. The equation that I solve numerically is the Phase function method and is $$ \frac{d}{dr}[\delta_{i+1}] = \frac{2\mu}{\hbar^2}\frac{V(r)}{k^2}\sin(kr + \delta_i)$$ ##\delta_i## is the phase shift for triplet and singlet state, ##\mu## is the reduced mass for neutron-proton, ##k=\sqrt{2\mu E_{cm}/\hbar^2}## is the wave number and ##V(r)## is the potential of interaction like Yukawa, Wood-Saxon, Square well potential, etc. I first...
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...

Similar threads

Replies
4
Views
2K
Replies
8
Views
2K
Replies
12
Views
4K
Replies
4
Views
3K
Replies
2
Views
2K
Replies
1
Views
3K
Back
Top