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NANOPHYSICS Dr. MC Ozturk, [email protected] E 304 3.1

NANOPHYSICS Dr. MC Ozturk, [email protected] 304 3.1

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Page 1: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

NANOPHYSICS

Dr. MC Ozturk, [email protected] 304

3.1

Page 2: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Early 1900s

Electrons are nice particles They obey laws of classical mechanics

Light behaves just like a wave should It reflects, refracts and diffracts

Then, things began to happen…

Page 3: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Electromagnetic Waves

EM waves include two oscillating components: electric field magnetic field

EM waves can travel in vacuum Mechanical waves (e.g. sound) need a medium (e.g. air)

EM Waves travel at the speed of light, c c = 299,792,458 m/s

frequency

wavelength

Page 4: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Electromagnetic Spectrum

Page 5: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Thermal Radiation

For human skin, T = 95oF, wavelength is 9.4 micrometer (infrared)

All hot bodies emit thermal radiation

Page 6: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Ultraviolet Catastrophe

Rayleigh-Jeans law described thermal radiation emitted by a black-body as

This implies that as the wavelength of an EM wave approaches zero (infinite frequency), its energy will become infinitely large! i.e. will get brighter and brighter

Experimentally, this was not observed… and this was referred to as the ultraviolet catastrophe

Page 7: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Rutherford Atom - Challenge

Belief: Attractive force between the positively charged nucleus and an electron orbiting around is equal to the centrifugal exerted on the electron. This balance determines the electron’s radius.

Challenge: A force is exerted on the electron, then, the electron should accelerate continuously according to F = ma. If this is the case, the electron should continuously lose its energy. According to classical physics, all accelerating bodies must lose energy. Then, the electrons must collapse with the nucleus.

Page 8: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Photoelectric Effect - Challenge

Light shining on a piece of metal results in

electron emission from the metal

There is always a threshold frequency of light below which no electron emission occurs from the metal.

Maximum kinetic energy of the electrons has nothing to do with the intensity of light. It is determined by the frequency of light.

Page 9: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Photoelectric EffectThe Experiment - 1

Light Sourceanode

cathode

Electrons emitted by the cathode are attracted to the positively charged anode.

A photocurrent begins to flow in the loop.

Page 10: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Photoelectric EffectThe Experiment - 2

Light Sourceanode

cathode

Electrons emitted by the cathode are repelled by the negatively charged anode.

The photocurrent decreases.

Page 11: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Photoelectric EffectThe Experiment - 3

Voltage

Current

IncreasingLight

Intensity

Regardless of the light intensity, the photocurrent becomes zero at V = - Vo

At this voltage, every emitted electron is repelledTherefore, qVo must be the maximum kinetic energy of the electron

This energy is independent of the light intensity

Vo

Page 12: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Photoelectric EffectThe Experiment - 4

fo

The maximum kinetic energy of electrons is determined by the frequency of light

The slope of this line is Planck’s constantIncreasing the light intensity only increases the number of photons

hitting the cathode

Frequency

Page 14: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Video:Max Planck & Quantum Physics https://www.youtube.com/watch?

v=2UkO_3NC3F4

Page 15: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

NANOPHYSICS

Dr. MC Ozturk, [email protected] 304

3.2

Page 16: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Hydrogen Atom

Page 17: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Hydrogen Atom

Orbitalthree dimensional space around the nucleus of all the places we are likely to find an electron.

Page 18: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Orbitals & Quantum Numbers Atoms have infinitely many orbitals Each orbital can have at most two

electrons Each orbital represents a specific

Energy level Angular momentum Magnetic moment

Sub-levels

Page 19: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Quantum Numbers

Principal Quantum Number, n = 1, 2, 3, … Determines the electron energy

Azimuthal Quantum Number, l = 0, 1, 2, … Determines the electron’s angular

momentum Magnetic Quantum Number, m = 0, ± 1, ± 2,

… Determines the electron’s magnetic moment

Spin Quantum Number, s= ± 1/2 Determines the electron spin (up or down)

The energy, angular momentum and magnetic moment of an orbital are quantized

i.e. only discrete levels are allowed

Page 20: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Principal Quantum Number

Always a positive integer, n = 1, 2, 3, … Determines the energy of the electron in

each orbital. Sub-levels with the the same principal

quantum number have the same energy

Only certain (discrete) energy levels are allowed!

Page 21: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Azimuthal Quantum Number

Each n yields n – 1 sub levels

l = 0 l = 1 l = 2 l = 3

n = 1 a

n = 2 a a

n = 3 a a a

n = 4 a a a a

Page 22: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Magnetic Quantum Number

l = 0 l = 1 l = 2 l = 3

n = 1 m=0

n = 2 0 -1, 0,+1

n = 3 0 -1, 0,+1 -2, -1, 0,+1,+2

n = 4 0 -1, 0,+1 -2, -1, 0,+1,+2 -3,-2, -1, 0,+1,+2,+3

s p d f

1 orbital 3 orbitals 5 orbitals 7 orbitals

Page 23: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Spin Quantum Number

l = 0 l = 1 l = 2 l = 3

n = 1 m=0

n = 2 0 -1, 0,+1

n = 3 0 -1, 0,+1 -2, -1, 0,+1,+2

n = 4 0 -1, 0,+1 -2, -1, 0,+1,+2 -3,-2, -1, 0,+1,+2,+3

s p d f

1 orbital2 states

3 orbitals6 states

5 orbitals10 states

7 orbitals14 states

(only two possibilities)

Page 24: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Levels, Sublevels of Atomic Orbitals http://en.wikipedia.org/wiki/

Atomic_orbital

Electrons fill the lowest energy states first

Page 25: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Atomic Number

Page 26: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Example 1: Silicon Atom

1 s

2 s

2 p

3 s

3 p

4 s

3 d

Silicon has 14 electrons

1s22s22p63s23p2

Empty States

Occupied States

Page 27: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Example 2: Titanium Atom

1 s

2 s

2 p

3 s

3 p

4 s

3 d

Titanium has 22 electrons

1s22s22p63s23p63d24s2

Empty States

Occupied States

Page 28: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Atomic Orbitals

Hydrogen

Larger Atoms

Page 29: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

s (l=0) p (l = 1) d (l = 2) f (l = 3)

Page 31: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

NANOPHYSICS

Dr. MC Ozturk, [email protected] 304

3.3

Page 32: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Electromagnetic Waves

EM waves can travel in vacuum Mechanical waves (e.g. sound) need a

medium (e.g. air) EM Waves travel at the speed of light, c

c = 299,792,458 m/s

frequency

wavelength

Page 33: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Electromagnetic Spectrum

Page 34: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

How EM Waves are made?

1. Electric field around the electron accelerates

2. The field nearest to the electron reacts first

3. Outer field lags behind4. Electric field is distorted – bend in

the field5. The bend moves away from the

electron6. The bend carries energy

Charges often accelerate and decelerate in an oscillatory manner – sinusoidal waves

Page 35: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Energy is Quantized

Always a positive integer, n = 1, 2, 3, …

E = nhfOrbital’s energy level Principa

l Quantu

m Numbe

r

Planck’s Constant6.626 X 10-34 m2/ kg-s

Frequency at which the atom vibrates

Only certain (discrete) energy levels are allowed!

Page 36: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Photons & Electrons

Atoms gain and lose energy as electrons make transitions between different quantum states

A photon is either absorbed or emitted during these transitions

n=1

n=2

n=3

A photon is absorbed for this

transition

Bohr’s radius correspond to distance from the nucleus where the probability of finding the electron is highest in a given orbital.

Page 37: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Hydrogen Atom

n = 1, 2, 3, …

As n approaches infinity, energy approaches zero.

E1 = 13.6 eV - Ground energy of the electron in the hydrogen atom

If you provide this much energy to the electron, it can leave the hydrogen atom

Page 38: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Photon & Electrons

The momentum of a photon (or an electron) is given by

This relationship is true for all particles Even large particles…

This equation was postulated for electrons by de Broglie in 1924

Page 39: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Video - Double Slit Experiment This is the experiment that confirmed

the wave nature of electrons http://www.youtube.com/watchv=Q1Yqg

PAtzho&list=PLREtcqhPesTcTAI6di_ysff0ckrjKe83I&index=1

Page 40: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Bullets Thru Double-Slit

P12 = P1 + P2

Page 41: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Waves Thru Double-Slit

P12 ≠ P1 + P2

I12 ≠ I1 + I2 + 2sqrt(I1I2) cos(Phi)

Page 42: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Electrons Thru Double-Slit

P12 ≠ P1 + P2

Page 43: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Electrons Thru Double-Slit

Page 44: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Electrons Observed Thru Double-Slit

No device can determine which slit the e- passes thru, w/o changing the interference.

Photon has momentum – after the collision between the photon and the electron, the electron’s momentum is no longer the same and we do not know what it is althought we know electron’s location rather precisely.

Page 45: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Heisenberg Uncertainty Principle

“Accepting quantum mechanics means feeling certain that you are uncertain”…a great statement from your textbook

Page 47: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

NANOPHYSICS

Dr. MC Ozturk, [email protected] 304

3.4

Page 48: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Erwin Schrodinger

1887-1961 Austrian Physicist Formulated the wave

equation in quantum physics

1933 Nobel Prize 1937 Max Planck

Medal

Page 49: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Schrodinger’s Equation

Schrodinger’s Equation is one of the most important equations in modern physics.

E = Energy

Page 50: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Wave Function – Physical Meaning A wave function is a complex quantity of

the form

The probability of finding an electron at a given location is given by

This is the ONLY physical meaning attached to the wave function

where

Page 51: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Complex Numbers – A Brief Review

a

ib

Page 52: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Free Particle

A free particle is not bound to anything It can freely move and go anywhere… Its energy must be purely kinetic energy

Schrodinger’s Equation

The solution of this equation is…

Page 53: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Free Particle – Continued

Page 54: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

What does this mean?

A free particle has kinetic energy only…

But we found…

This mean, the electron momentum is given by

Page 55: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Infinite Potential Well

A single electron is placed in an infinite potential well The walls are

infinitely high The electron is

trapped The probability of

finding the electron outside is…

Which implies…

∞∞

- L/2 + L/20

Page 56: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Infinite Potential Well – Continued The solutions are of the form

Verify:

Inside the well, the electron’s energy is purely kinetic (the potential is zero)

Page 57: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Infinite Potential Well – Solutions The solution was

Applying the boundary conditions

Adding and subtracting the equations:

Page 58: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Infinite Potential Well – Solutions We must satisfy

We have two options

Page 59: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Allowed Momenta

Only discrete momentum values are allowed!

Momentum is quantized…

Page 60: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Allowed Wavelengths

Only certain wavelengths are allowed!

Page 61: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Allowed Energy Levels

Only discrete energy levels are allowed!

Energy is quantized…

Page 62: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Particle in a Well

The result is strikingly similar to atomic orbitals in atoms

Recall:For a hydrogen atom,

En = - 13.6 / n2 eV

Page 63: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Finite Potential Well

A particle has a finite number of allowed energy levels in the potential well

A particle with E > Vo is not bound to the potential well

A particle with E < Vo has a finite probability of escaping the well

- L/2 + L/20

Vo Vo

Page 64: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Infinite vs. Finite Potential WellWave Functions

Vo

The wavefunctions are decaying exponentially outside the potential well

There is a finite probability of finding the electron outside the potential well

Page 65: NANOPHYSICS Dr. MC Ozturk, mco@ncsu.eduE 304 3.1

Particle (e.g. electron) Tunneling

An electron can tunnel through a potential barrier even though its initial kinetic energy is smaller than the potential barrier.

Electron tunneling is an important topic in nanoelectronics

The frequency of the wave is related to the momentum and the kinetic energy of the particle.