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Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

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Page 1: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Semiconductor nanotechnology: quantum dots

Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Page 2: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Semiconductors – Micheal

Page 3: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Insulators

Insulators have tightly bound electrons in their outer shellThese electrons require a very large amount of energy to free them for conduction

Let’s apply a potential difference across the insulator above…

The force on each electron is not enough to free it from its orbit and the insulator does not conduct

Insulators are said to have a high resistivity / resistance

Insulators - explained

Page 4: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Insulator – conductor transition

However, if we apply a little heat to the silicon….

An electron may gain enough energy to break free of its bond…

It is then available for conduction and is free to travel throughout the material

Page 5: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

We have positive charges too!

Let’s take a closer look at what the electron has left behind

There is a gap in the bond – what we call a hole

Let’s give it a little more character…

Page 6: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Optoelectronics – Micheal “moo”

Page 7: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Lights – Einstein and Planck

1905 Einstein –related wave and particle properties of light

Planck - WAVE-PARTICLES DUALITY

E = h Total E of the Photon (particle side)

Frequency (wave side)

Light is emitted in multiples of a certain minimum energy unit. The size of the unit – photon.

Explain the photoelectric effect - electron can be emitted if light is shone on a piece of metal

Energy of the light beam is not spread but propagate like particles

e

Page 8: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

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Page 9: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Quantum mechanics – Will

Page 10: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Bohr’s model

The electron is a wave, it must traverse an integer number of waves in a single orbit of the proton.

Page 11: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

To the board we go!!

Page 12: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Quantum dots - Josh

Page 13: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Quantum dots

A quantum dot is a ‘blob’ of one semiconductor embedded in another. The blob is so small that its length scale is close to the electron’s wavelength – so electrons behave as waves.

Page 14: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

14Quantum dots from Lancaster

20nm

Electrons are used to image individual atoms…

Page 15: Semiconductor nanotechnology: quantum dots Micheal Robinson, Micheal McGlen, Will Parr and Josh Conneely

Quantum networks

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Entangled photon source Quantum memory

To build a secure quantum network we’ll need to be able to store single photons without ‘reading’ them, a quantum repeater. We intend to develop a cheap, scalable repeater using quantum dots.