A A question about T-matrix in two-body scattering

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The T-matrix in two-body scattering can be expressed as a power series in the coupling strength, with the leading order being the first non-trivial term in this expansion. The zeroth-order term indicates no scattering occurs. Feynman diagrams, such as those in figure 2.3, correspond to specific terms in the perturbation series, illustrating the relationship between visual representations and mathematical expressions. Understanding the connection between these diagrams and equations 2.24-2.26 is crucial for grasping the underlying physics. This framework helps clarify the concept of "leading order" in the context of scattering processes.
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How to understand T-matrix in two-body scattering? Especially how to understand "leading order" in the text.
How can we understand T-matrix in two-body scattering? Especially term "leading order" in the text. In addition, how to understand the connection between fig2.3 and equation 2.24-2.26?
Thanks.
 

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Bin Jiang said:
Summary:: How to understand T-matrix in two-body scattering? Especially how to understand "leading order" in the text.

How can we understand T-matrix in two-body scattering? Especially term "leading order" in the text. In addition, how to understand the connection between fig2.3 and equation 2.24-2.26?
Thanks.
The T-matrix, whose precise definition must be given somewhere else in the book, can be expanded into a power series in the coupling strength g. The zeroth- order term is trivial, as it corresponds to no scattering at all. The term containing the lowest non-vanishing power of g (g^1 in this example) is the leading order.
The diagrams in fig. 2.3 are so called Feynman-diagrams and there are rules how they are in a one to one correspondence with actual terms in the perturbation series.
 
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