Feynman’rules’for’Scalar’Electrodynamics’ · 2017-01-20 ·...
Transcript of Feynman’rules’for’Scalar’Electrodynamics’ · 2017-01-20 ·...
Feynman rules for Scalar Electrodynamics
LSZ for scalars:
LSZ for vectors:
(c.f.6.1 Schwartz) Time ordered
Feynman rules for Scalar Electrodynamics
LSZ formula c.f. scalar case ch 10 Srednicki
δ j ≡
1i
δδ J (x j )
Feynman rule example: vertex rule
0 T φ x1( )φ x2( )φ x2( )( ) 0 = δ1δ 2δ3Z(J ) |J=0 ,
δ j ≡
1i
δδ J x j( )
0 T φ x1( )φ x2( )φ x2( )( ) 0 = δ1δ 2δ3Z(J ) |J=0
= δ1δ 2δ3
ig3!
1i
⎛⎝⎜
⎞⎠⎟
3i2
⎛⎝⎜
⎞⎠⎟
3
23 d 4 y1,2,3,a∫ Π i=1,2,3J ( yi )Δ yi − ya( ) at O(g)
= ig
3!1i
⎛⎝⎜
⎞⎠⎟
3i2
⎛⎝⎜
⎞⎠⎟
3
23 1i
⎛⎝⎜
⎞⎠⎟
3
3! d 4 yaΠ iΔ(xi − ya )∫
Insert in LSZ formula:
f i = −g i( )3
d 4x1,2,3d4 yae
i(k1x1+k2x2−k3x3 )∫ Π i −∂i2+ m2( )Δ(xi − ya )
= ig 2π( )4δ 4(k1 + k2 − k3) ≡ 2π( )4
δ 4(k1 + k2 − k3)iT
iT = ig Feynman rule for vertex
−( )
−∂i
2+ m2( )Δ(xi − ya ) = δ 4(xi − ya )
Feynman rules
× No scaIering
δ1δ2δ3δ4
δ1 removes a source and labelsthe propagator end-point x1
(photon :−∂i2Δµν xi − y( ) = gµνδ 4 xi − y( ) in Lorentz gauge)−∂i
2 +m2( )Δ xi − y( ) = δ 4 xi − y( )
Feynman rules
iT is given by the sum of all diagrams
ie k + k '( )µ −2ie2gµν −iλ
NB Combinatoric factors
Feynman rules for Scalar Electrodynamics
Feynman rules for Scalar Electrodynamics
ie k + k '( )µ −2ie2gµν −iλ
ie k + k '( )µ −2ie2gµν −iλ
Feynman rules for Scalar Electrodynamics
−igµν / k2 − iε( ) −i / k2 +m2 − iε( )
ελiµ*(k), ελi
µ (k) for incoming and outgoing photons respectively
ApplicaNon of the Feynman rules: I. Tree level
e−e− → e−e−
ξ dependence vanishes (gauge invariance)...here just through k µJµ = 0
(Moller scaIering)
⇒
α = e2
4π, fine structure constant
⇒
α = e2
4π, fine structure constant
3 32 42 4 2
4 6
1 (2 ) ( )2 2 (2 ) 2 2
C DC D A B
A B C D
d p d pVd p p p p VE E V E E
πσ δπ
= + − −Av
M
Exercise
+
Ward idenNty and gauge invariance
Gauge invariance:
c.f. Ward idenNty if matrix element for on-‐shell photon is εµ Mµ
Ward IdenNty more general, applies even if photon non-‐physical
e.g. Consider
Assuming only electron on-‐shell
−
+
Ward idenNty ε3µ
* → p3µ ?
≠ 0
−
Ward idenNty ε3µ
* → p3µ ?
≠ 0
−
≠ 0
−