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Derive the equations of motion for the complex scalar field with the folowing action S= Z d4x ∂µφ ∂µφ∗−λ 2(φ φ∗−v2)2

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Quantum field theory Exercises 6.

2005-12-05

•Exercise 6.1.

Derive the equations of motion for the complex scalar field with the folowing action S=

Z d4x

µφ ∂µφ−λ

2(φ φ−v2)2

.

•Exercise 6.2.

Check explicitly in the model of one scalar field with potentialV(φ) S=

Z d4x

1

2∂µφ ∂µφ−V(φ)

that the energy

E= Z

d3x

1

2φ˙2+1

2∂iφ ∂iφ+V(φ)

is conserved (dE/dt =0) on the equations of motion.

•Exercise 6.3.

Find the dimensions of scalar, spinor, and gauge fields in space-time of dimension d=4.

A useful starting point is the fact that dimension of action S is the dimension of the Plank’s constant, i.e. it is dimensionless in ¯h= 1 units. Repeat the anaysis in arbitrary number of dimensionsd, using actionS=RddxL with usual expressions for LagrangianL.

6

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