EP 228: Quantum Mechanics P. Ramadevi, 2 nd floor Dept of Physics, - - PowerPoint PPT Presentation

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EP 228: Quantum Mechanics P. Ramadevi, 2 nd floor Dept of Physics, - - PowerPoint PPT Presentation

EP 228: Quantum Mechanics P. Ramadevi, 2 nd floor Dept of Physics, IIT Bombay rama0072006@gmail.com Extn: 7563 References Griffiths-Introduction to Quantum Mechanics Sakurai Modern Quantum Mechanics Shankar-Principles of


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SLIDE 1

EP 228: Quantum Mechanics

  • P. Ramadevi, 2nd floor Dept of

Physics, IIT Bombay rama0072006@gmail.com Extn: 7563

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SLIDE 2

References

  • Griffiths-Introduction to Quantum

Mechanics

  • Sakurai – Modern Quantum

Mechanics

  • Shankar-Principles of Quantum

Mechanics

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SLIDE 3

In-Sem, End-sem

  • Two 10 marks quiz (one in first week
  • f Feb and other in the last week of

March)

  • Mid-Sem 30 marks
  • End-Semester 40 marks
  • Assignment 10 marks
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SLIDE 4

Before Mid-Sem

  • Review quantum ideas

(Wavefunction formalism)

  • Linear vector spaces
  • Operator, state vecor formalism of

Harmonic oscillator

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SLIDE 5

After Mid-Sem

  • Hydrogen atom, Angular Momentum
  • Spin
  • Addition of angular momentum
  • Clebesh-Gordan coefficients
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SLIDE 6

Limitations of Classical ideas- need for Quantum theory

  • Experimental data in the Microscopic World (inside an

atom or nucleus) – classical laws are inadequate

1) Black-Body Spectrum 2) Photo-electric effect 3) Compton scattering

Needed introduction of a fundamental constant h (Planckconstant) leading to the `Quantum’ regime Photons obey E= hν and using relativistic energy for massless particles imply momentum of photon p=h/ λ

Daring proposal of de-Broglie: equation for the wavelength of matter waves must obey the same equation of photon momentum

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SLIDE 7

Matter waves

  • For an electron moving in a circular orbit of

radius r, constructive interference of the electron wave with itself in the orbit requires 2 πR = n λ

  • Substituting de-Broglie proposal gives Bohr

quantization mvr= n h/2π

  • Electron diffraction expts : Davisson-Germer

(confirms wave nature of electron)

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SLIDE 8

Interference expt

plot C for electron beam is observed (wave info)

The plot is actually probability curve for electron

Attempting which slit the electron came from gives plot B(particle info)

Either particle or wave nature can be observed

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SLIDE 9

Wave-particle duality

  • Classical Mechanics
  • both x, p can be

simultaneously found

  • Equation is

Newton’s law determines x,p

  • Quantum Mechanics
  • x,p cannot be simultaneously

determined precisely-

Heisenberg’s uncertainty principle

  • Equation is Schrodinger eqn

which determines probability amplitude Ψ(x,t) (complex) whose modulus squared gives probability

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SLIDE 10

Particle nature of light

Blackbody radiation Photo-electric Effect Compton effect Wave-nature

  • f particles

(de-Broglie wave) Diffraction experiment Uncertainty principle Wavepacket, probability Average Schrodinger Eqn Matter wave

Quantum Mechanics

We will see in detail

Flow chart

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SLIDE 11

Wave-function

< ∞ (for square

Integrable)

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SLIDE 12

Square-Integrable functions

  • Square integrable wavefunction Ψ(x,t) must

go to zero faster than 1/√|x| as |x| -> +∞

  • We can normalize such functions giving

normalised wavefunction obeying

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SLIDE 13

Normalisation constant

Where N is finite Normalised wavefunction The normalisable wavefunctions satisfy Using time-dependent Schrodinger equation, show that Exercise 1

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SLIDE 14

More Exercises

2) Starting from expectation value of x, show Exercise 3 Ehrenfest Theorem- expectation values obey classical laws

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SLIDE 15

Discontinuous potentials V(x)

Step function at x=0

For finite potentials, show that

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SLIDE 16

For infinite potential

Derivative of wavefunction is not continuous at x=0