Homework 2 Problems - Particle Physics | PHYSICS 735, Assignments of Physics

Material Type: Assignment; Class: Particle Physics; Subject: PHYSICS; University: University of Wisconsin - Madison; Term: Fall 2008;

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Physics 735: Homework 2
Due Thursday, October 2, 2008 (Give to Hiren Patel)
1. Using the explicit forms of the 2x2 Pauli matrices, compute their commutation
and anti-commutation relationships.
2. Using the Klein-Gordon equation together with the replacement
µ
µ
+iqA
µ
,
find the form of the potential,
ˆ
VKG
, in the corresponding equation,
+m2
( )
φ
=ˆ
VKG
φ
in terms of A.
3. In Majorana representation γ matrices are:
γ
0=0i
σ
1
i
σ
10
,
γ
1=
iI 0
0iI
,
γ
2=0
σ
2
σ
20
,
γ
3=0iI
iI 0
,
γ
5=0i
σ
3
i
σ
30
a. Show that this is a valid representation, i.e.,
γµ
,
γν
{ }
=2g
µν
I,
γµ
=
γ
0
γµγ
0,
γ
5,
γν
{ }
=0,
γ
5
( )
2=I
b. Show that
γµ
*=
γµ
c. Show that if ψ satisfies Dirac equation, then its complex conjugate also
does. What can you conclude about the particle represented by ψ?
4. Problem 5.4 from Aitchison & Hey
5. Problem 5.6 from Aitchison & Hey
6. Problem 5.7 from Aitchison & Hey
7. Problem 5.8 from Aitchison & Hey
8. Problem 6.6 from Aitchison & Hey
9. Problem 6.7 from Aitchison & Hey
10. Problem 6.9 from Aitchison & Hey
Aitchison & Hey is available on reserve in the physics library.
A scanned copy of chapter 5-7 are also available online.
http://www.hep.wisc.edu/~dasu/classes/physics735

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Physics 735: Homework 2

Due Thursday, October 2, 2008 (Give to Hiren Patel)

  1. Using the explicit forms of the 2x2 Pauli matrices, compute their commutation

and anti-commutation relationships.

  1. Using the Klein-Gordon equation together with the replacement (^) ∂

μ

→ ∂

μ

  • iqA

μ

,

find the form of the potential,

V

KG

, in the corresponding equation,

+ m

2

( )^ φ^ =^ −^

V

KG

φ

in terms of A.

  1. In Majorana representation γ matrices are:

γ

0

=

0 i σ 1

i σ 1

, γ

1

=

iI 0

0 − iI

, γ

2

=

0 σ 2

− σ 2

γ

3

=

0 iI

iI 0

, γ

5

=

0 i σ 3

i σ 3

a. Show that this is a valid representation, i.e.,

γ

μ

, γ

ν

= 2 g

μν

I , γ

μ †

= γ

0

γ

μ

γ

0

, γ

5

, γ

ν

= 0 , γ

5

2

= I

b. Show that γ

μ*

= − γ

μ

c. Show that if ψ satisfies Dirac equation, then its complex conjugate also

does. What can you conclude about the particle represented by ψ?

  1. Problem 5.4 from Aitchison & Hey
  2. Problem 5.6 from Aitchison & Hey
  3. Problem 5.7 from Aitchison & Hey
  4. Problem 5.8 from Aitchison & Hey
  5. Problem 6.6 from Aitchison & Hey
  6. Problem 6.7 from Aitchison & Hey
  7. Problem 6.9 from Aitchison & Hey

Aitchison & Hey is available on reserve in the physics library.

A scanned copy of chapter 5- 7 are also available online.

http://www.hep.wisc.edu/~dasu/classes/physics