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Lecture 14: Schrödinger and Matter Waves

Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

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Page 1: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Lecture 14: Schrödinger and Matter Waves

Page 2: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Particle-like Behaviour of Light

Planck’s explanation of blackbody radiation

Einstein’s explanation of photoelectric effect

Page 3: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

de Broglie: Suggested the converse

All matter, usually thought of as particles, should exhibit wave-like behaviour

Implies that electrons, neutrons, etc., are waves!

Prince Louis de Broglie (1892-1987)

Page 4: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

de Broglie Wavelength

Relates a particle-like property (p) to a wave-like property ()

Page 5: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

particle wave function

Wave-Particle Duality

Page 6: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Example: de Broglie wavelength of an electron

Mass = 9.11 x 10-31 kgSpeed = 106 m / sec

m10287m/sec) kg)(10 10(9.11secJoules10636 10

631

34

.

.

This wavelength is in the region of X-rays

Page 7: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Example: de Broglie wavelength of a ball

Mass = 1 kgSpeed = 1 m / sec

m10636m/sec) kg)(1 (1

secJoules10636 3434

..

This is extremely small! Thus, it is very difficult to observe the wave-like behaviour of ordinary objects

Page 8: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Wave Function

Completely describes all the properties of agiven particle

Called (x,t); is a complex function of position x and time t

What is the meaning of this wave function?

Page 9: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Copenhagen Interpretation:probability waves

The quantity 2 is interpreted as the probability that the particle can be found at a particular point x and a particular time t

The act of measurement ‘collapses’ the wave function and turns it into a particle

appletNeils Bohr (1885-1962)

Page 10: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Imagine a Roller Coaster ...

By conservation of energy, the car will climb up to exactly the same height it started

Page 11: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Conservation of Energy

E = K + Vtotal energy = kinetic energy + potential energy

In classical mechanics, K = 1/2 mv2 = p2/2m

V depends on the system – e.g., gravitational potential energy,

electric potential energy

Page 12: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Electron ‘Roller Coaster’

An incoming electron will oscillate betweenthe two outer negatively charged tubes

Page 13: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Solve this equation to obtain

Tells us how evolves or behaves in a given potential

Analogue of Newton’s equation in classical mechanics

Schrödinger’s Equation

appletErwin Schrödinger (1887-1961)

Page 14: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Wave-like Behaviour of Matter

Evidence: – electron diffraction– electron interference (double-slit experiment)

Also possible with more massive particles, such as neutrons and -particles

Applications:– Bragg scattering– Electron microscopes– Electron- and proton-beam lithography

Page 15: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Electron Diffraction

X-rays electrons

The diffraction patterns are similar because electrons have similar wavelengths to X-rays

Page 16: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Bragg Scattering

Bragg scattering is used to determine the structure of the atoms in a crystal from the spacing between the spots on a diffraction pattern (above)

Page 17: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Resolving Power of Microscopes

To see or resolve an object, we need to use light of wavelength no larger than the object itself

Since the wavelength of light is about 0.4 to 0.7 m,

an ordinary microscopecan only resolve objectsas small as this, such asbacteria but not viruses

Page 18: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Scanning Electron Microscope (SEM)

To resolve even smaller objects, have to use electronswith wavelengths equivalent to X-rays

Page 19: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

SEM Images

Guess the images ...

Page 20: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Particle Accelerator

Extreme case of an electron microscope, where electrons are accelerated to very near c

Used to resolve extremely small distances: e.g., inner structure of protons and neutrons

Stanford Linear Accelerator (SLAC)

Page 21: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Conventional Lithography

Page 22: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Limits of Conventional Lithography

The conventional method of photolithography hits its limit around 200 nm (UV region)

It is possible to use X-rays but is difficult to focus

Use electron or proton beams instead…

Page 23: Lecture 14: Schrödinger and Matter Waves. Particle-like Behaviour of Light n Planck’s explanation of blackbody radiation n Einstein’s explanation of photoelectric

Proton Beam Micromachining (NUS)

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