Why is the axial current said to create particles?
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In Peskin and Schroeder p. 669 it is argued that the axial current can be parametrized between the vacuum and an on-shell pion state as:
<0|
j
μ5
(x)|
π
b
(p)>=−i
p
μ
f
π
δ
ab
e
−ipx
<0|jμ5(x)|πb(p)>=−ipμfπδabe−ipx
This is then described as a parametrization of the amplitude for the axial current to create a pion state from the vacuum. This interpretation puzzles me: isn't it the role of the creation operators of a given theory to do this? Does the above expression correspond to an actual physical process or is it just part of an amplitude in a Feynman diagram for an actual process?
<0|
j
μ5
(x)|
π
b
(p)>=−i
p
μ
f
π
δ
ab
e
−ipx
<0|jμ5(x)|πb(p)>=−ipμfπδabe−ipx
This is then described as a parametrization of the amplitude for the axial current to create a pion state from the vacuum. This interpretation puzzles me: isn't it the role of the creation operators of a given theory to do this? Does the above expression correspond to an actual physical process or is it just part of an amplitude in a Feynman diagram for an actual process?
Answered by
0
In Peskin and Schroeder p. 669 it is argued that the axial current can be parametrized between the vacuum and an on-shell pion state as: $$<0|j^{\mu 5}(x)|\pi^b(p)>=-ip^\mu f_\pi$$
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