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The Standard Model of Electroweak Physics Christopher T. Hill Head of Theoretical Physics Fermilab.

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Presentation on theme: "The Standard Model of Electroweak Physics Christopher T. Hill Head of Theoretical Physics Fermilab."— Presentation transcript:

1 The Standard Model of Electroweak Physics Christopher T. Hill Head of Theoretical Physics Fermilab

2 Lecture I: Incarnations of Symmetry

3 Emmy Noether 1882-1935 Noether’s Theorem is as important to us now as the Pythagorean Theorem

4 Electricity and Magnetism Electric charge: Electric charge is conserved:

5 What is the Symmetry that leads, by Noether’s Theorem to electric charge conservation?

6 In Five Easy Pieces

7 electron = electron + gauge field Local Gauge Symmetry of Electrodynamics I.

8

9 Electromagnetic force

10 Electromagnetic force Quark color force

11 Weak Force: u d e nu W What gives rise to masses of W and Z boson? Higgs Field? SU(2)xU(1) is “Spontaneously broken Symmetry” SU(2) x U(1)

12 U(1) Local Gauge Invariance on a Wallet Card covariant derivative

13 U(1) Local Gauge Invariance on a Wallet Card field strength invariants

14 Yang-Mills Local Gauge Invariance on a Wallet Card

15 Homework: Verify all of the transformations laws stated on the previous pages for U(1) and Yang-Mills gauge theories.

16 Can a gauge field have a mass? II.

17 Can a gauge field have a mass? Yes!

18

19 Superconductivity === Massive Gauge Field

20 Cartoon Feature: Gauge Boson Mass +z axis time light cone

21 Massless Photon +z axis time light cone

22 A massive photon +z axis time light cone

23 A massive photon oscillates through spacetime, colliding with the condensate and mixing with phase degree of freedom: spin is conserved Charge condensate

24 Superconductivity === Massive photon Field

25 Our vacuum is an electroweak superconductor Massive W and Z bosons Superconductivity === Massive photon Field

26 Homework: Consider a charged scalar field coupled to the photon and described the Lagrangian: Show that this is gauge invariant under: Show that if : then the photon acquires a gauge invariant mass:

27 III. Massless Fermions and Chiral Symmetry

28 Massless Fermions have Chiral Symmetry

29 Both currents are conserved when fermions are massless and chiral symmetry is exact (modulo anomalies)

30 Each chiral current corresponds to a different “chiral charge” e.g., L couples to W-bosons while R does not Standard Model is “flavor chiral”

31 Cartoon Feature: Fermion Mass and Chirality +z axis time light cone

32 A massless right-handed fermion s z = +1/2 +z axis time spin momentum

33 +z axis time spin momentum A massless left-handed fermion s z = +1/2

34 Can couple fermions to gauge bosons and preserve chiral symmetry: +z axis time right-handed Chirality is conserved

35 e.g., couple electron to the photon in a L-R symmetric way +z axis time left-handed Chirality is conserved

36 The left-handed and right-handed electrons have the same electric charge QED is “vectorlike”

37 Only left-handed fermions have electroweak charge and form doublets under SU(2) Right handed’s are “sterile” under SU(2) Standard Model is not “vectorlike” !!!

38 only L fermions couple to the W-boson +z axis time left-handed

39 Reflection Symmetry (parity) doubletssinglets

40 Helicity of decay products in pion decay: ? ? Mirror Images

41 Parity is violated in pion decay: (Lederman)

42 Chiral symmetry is broken by mass

43

44 Cartoon: a massive electron +z axis time light cone

45 A massive fermion oscillates in chirality through spacetime: right-handed left-handed Chirality nonconservation by the mass term electric charge is conserved spin is conserved

46

47 Homework: Verify that: Hint: use the Dirac equation

48 How do we make a massive fermion but conserve weak charge? right-handed left-handed Mass Violates Electroweak Gauge Symmetry!!! mass violates weak charge!!!

49 Spontaneous Symmetry Breaking IV.

50

51

52 Nambu-Goldstone Boson “Higgs” Boson

53

54 Engineer a Coupling to a Complex Scalar Boson that conserves chirality

55 Couple to a Complex Scalar +z axis time left-handed right-handed Chiral charge is conserved complex boson

56 Can we have a massive fermion but conserve chirality? right-handed left-handed

57 Boson Condenses in vacuum! +z axis time Chiral charge is hidden in vacuum !! Complex boson vacuum expectation value = f

58 Fermion Masses generated spontaneously right-handed left-handed

59 Ungauged Spontaneously Broken Chiral Symmetry

60 Gauged Spontaneously Broken Chiral Symmetry

61

62 Putting it all together: Gauged Spontaneously Broken Chiral Symmetry V.

63 We’re ready for the Standard Model !!! Weak Force: u d e nu W What gives rise to masses of W and Z boson? Higgs Field? SU(2)xU(1) is “Spontaneously broken Symmetry” SU(2) x U(1)


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