Chapter III Dirac Field Lecture 1 Books Recommended:

Slides:



Advertisements
Similar presentations
From Quantum Mechanics to Lagrangian Densities
Advertisements

Quantum Chemistry Revisited Powerpoint Templates.
Fermions and the Dirac Equation In 1928 Dirac proposed the following form for the electron wave equation: The four  µ matrices form a Lorentz 4-vector,
X y z z′ R (  1,  2,  3 ) = 11 y′ 11 =x′ 22 22 22 x′′ z′′ =y′′ 33 y′′′ z′′′ = x′′′ 33 33.
Symmetries By Dong Xue Physics & Astronomy University of South Carolina.
Quantum Mechanics Classical – non relativistic Quantum Mechanical : Schrodinger eq.
(also xyzyzxzxy) both can be re-written with
} space where are positive and negative energy solutions to free KG equation time.
The Klein Gordon equation (1926) Scalar field (J=0) :
+ } Relativistic quantum mechanics. Special relativity Space time pointnot invariant under translations Space-time vector Invariant under translations.
Aug 29-31, 2005M. Jezabek1 Generation of Quark and Lepton Masses in the Standard Model International WE Heraeus Summer School on Flavour Physics and CP.
The World Particle content. Interactions Schrodinger Wave Equation He started with the energy-momentum relation for a particle he made the quantum.
Monday, Apr. 2, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #12, 13, 14 Monday, Apr. 2, 2007 Dr. Jae Yu 1.Local Gauge Invariance 2.U(1) Gauge.
The World Particle content All the particles are spin ½ fermions!
10 lectures. classical physics: a physical system is given by the functions of the coordinates and of the associated momenta – 2.
Fundamental principles of particle physics Our description of the fundamental interactions and particles rests on two fundamental structures :
Wednesday, Feb. 28, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #9 Wednesday, Feb. 28, 2007 Dr. Jae Yu 1.Quantum Electro-dynamics (QED) 2.Local.
7. Relativity Wave Equations and Field Theories 7.1. The Klein-Gordon Equation 7.2. Scalar Field Theory for Free Particles 7.3. The Dirac Equation and.
Wednesday, Mar. 5, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #13 Wednesday, Mar. 5, 2003 Dr. Jae Yu Local Gauge Invariance and Introduction.
Nojoon Myoung De Broglie’s matter wave (1924) Heisenberg’s matrix mechanics (1925) Schrodinger equation (1926) Klein-Gordon equation (1927)
Relativistic Quantum Mechanics
The inclusion of fermions – J=1/2 particles
Quantization of free scalar fields scalar field  equation of motin Lagrangian density  (i) Lorentzian invariance (ii) invariance under  →  require.
Announcements Reading quiz shifted to tomorrow 9/12 Lectures through Monday posted Homework solutions 1, 2a, 2b posted.
Lecture from Quantum Mechanics. Marek Zrałek Field Theory and Particle Physics Department. Silesian University Lecture 6.
Fundamental principles of particle physics Our description of the fundamental interactions and particles rests on two fundamental structures :
Relativistic Quantum Mechanics Lecture 1 Books Recommended:  Lectures on Quantum Field Theory by Ashok Das  Advanced Quantum Mechanics by Schwabl  Relativistic.
Relativistic Quantum Mechanics
Relativistic Quantum Mechanics
Quantum Field Theory (PH-537) M.Sc Physics 4th Semester
Canonical Quantization
Lagrange Formalism & Gauge Theories
Chapter V Interacting Fields Lecture 3 Books Recommended:
Handout 2 : The Dirac Equation
Chapter III Dirac Field Lecture 2 Books Recommended:
Relativistic Quantum Mechanics
Chapter V Interacting Fields Lecture 1 Books Recommended:
Representation Theory
Fundamental principles of particle physics
Physics 222 UCSD/225b UCSB Lecture 10 Chapter 14 in H&M.
Relativistic Quantum Mechanics
Countries that signed the nuclear arms treaty with Iran
Spin and Magnetic Moments
Fermion Condensate in Lower Dimensions
Announcements Exam Details: Today: Problems 6.6, 6.7
Canonical Quantization
Lecture 9 Weak Neutral Currents Chapter 13 in H&M.
Canonical Quantization
Spin and Magnetic Moments (skip sect. 10-3)
Chapter II Klein Gordan Field Lecture 2 Books Recommended:
The World Particle content.
Chapter IV Gauge Field Lecture 1 Books Recommended:
Chapter V Interacting Fields Lecture 7 Books Recommended:
Chapter IV Gauge Field Lecture 3 Books Recommended:
Chapter II Klein Gordan Field Lecture 5.
Chapter V Interacting Fields Lecture 5 Books Recommended:
Relativistic Quantum Mechanics
Relativistic Quantum Mechanics
前回まとめ 自由scalar場の量子化 Lagrangian 密度 運動方程式 Klein Gordon方程式 正準共役運動量 量子条件
Chapter II Klein Gordan Field Lecture 3 Books Recommended:
Theory of Scattering Lecture 4.
Chapter III Dirac Field Lecture 4 Books Recommended:
Relativistic Quantum Mechanics
Chapter V Interacting Fields Lecture 2 Books Recommended:
Relativistic Quantum Mechanics
Relativistic Quantum Mechanics
Chapter III Dirac Field Lecture 5 Books Recommended:
Chapter II Klein Gordan Field Lecture 1 Books Recommended:
Chapter IV Gauge Field Lecture 2 Books Recommended:
Linear Vector Space and Matrix Mechanics
Presentation transcript:

Chapter III Dirac Field Lecture 1 Books Recommended: Lectures on Quantum Field Theory by Ashok Das A First Book of QFT by A Lahiri and P B Pal

Dirac Equation (For details on Dirac Eq and its Sol see lectures of QM-II, III Semester ) Klein Gordon lead to negative energy solutions. Probability density can be negative. This is because it has first derivative of wave function w.r.t. t. We need to have first derivative of ϕ w.r.t time in wave equation. But then, spatial derivative should. Also be of first order because of Lorentz invariance. We can do this if energy and momentum are linearly dependent.

In terms of Gamma matrices, Dirac Eq is given by -----(1) Which is Covariant form of Dirac eq. Feynman slash notation -------(2) Where v is some arbitrary vector

In terms of Feynman slash notation, Dirac Eq will be ------(3) In terms of Dirac eq (1) can be written as (in natural units) -----(4) -----(5)

Properties of Gamma matrices: Gamma matrices are even dimensional Matrices (Pauli-Dirac representation) ---(6) Where sigma Pauli matrices are ---(7)

Gamma matrices satisfy the Clifford algebra ----(8) From above we have -----(9)

-----(10) --(11)

---(12) ---(13) We define six antisymmetric matrices ----(14)

--------(15) ----(16)

Matrices represent spin operator for Dirac particle. We can identify using -----(17) as spin operator.

We constructed following 16 matrices ----(18)

Pauli’s fundamental theorem: If satisfy Clifford algebra, then they must be related through the similarity transformations. i.e. if -----(20) ------(21) Then there exist non-singular matrix S such that ------(22)

Starting from We have Where,

Other representations for Dirac matrices Majorana Representation: In this are Purely imaginary. We have for Useful for study of Majorana fermions which Are charge neutral particle.

Dirac matrices in Dirac Pauli representation and Majorana representation are related through the unitary transformation

Weyl Representation: Used for study of massless fermions where Dirac Pauli representation and Weyl representation are related through