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Tiêu đề Lecture Physics A2 Introduction to Quantum Physics Matter Waves and the Schrödinger Equation
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“‘Quantum mechanics’ is the description of the behavior of matter and light in all its details and, in particular, of the happenings on an atomic scale Things on a very small scale behave like nothing[.]

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“‘Quantum mechanics’ is the description

of the behavior of matter and light in all its details and, in particular, of the

happenings on an atomic scale Things on

a very small scale behave like nothing

that you have any direct experience

about They do not behave like waves,

they do not behave like particles, they do not behave like clouds, or billiard balls, or weights on springs, or like anything that you have ever seen.”

Richard P Feynman

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Lecture 6: Introduction to

Quantum Physics:

Matter Waves and the Schrödinger Equation

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Electron Diffraction particles as waves

Matter-wave Interference

Composite particles

Electron microscopy

Heisenberg Uncertainty Principle

Schrödinger Equation (SEQ)

Time-independent SEQ gives static solutions for wavefunctions

Physical interpretation of the wavefunction

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electron gun

Ni Crystal

detector

q

 In 1927-8, it was shown

(Davisson-Germer) that, like x-rays, ELECTRONS

can also diffract off crystals !

q

Interference peak !

Electrons can act like waves!!

What does this mean?

In discussion section:

q

Matter Waves

 DeBroglie (1924) proposed that, like

photons, particles have a wavelength:

l = h/p Inversely proportional to

momentum.

• We will see later that the discrete

atomic emission lines also arise from

the wavelike properties of the

electrons in the field of the nucleus:

Atomic

hydrogen

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“Double-slit” Experiment for Electrons

Electrons are accelerated to

50 keV  l = 0.0055 nm

Central wire is positively

charged  bends electron

paths so they overlap

A position-sensitive detector

records where they appear.

<< 1 electron in system at

any time

[A TONOMURA (Hitachi) pioneered electron holography]

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Exercise 1: Matter wavelengths

What size wavelengths are we talking about? Consider a photon with energy 3 eV, and therefore momentum p = 3 eV/c Its wavelength is:

a) le = lp b) le < lp c) le > lp

What is the wavelength of an electron with the same momentum?

c eV

s eV

p

h

414 10

3 10

4

1 3

10 14

l

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What size wavelengths are we talking about? Consider a photon with energy 3 eV, and therefore momentum p = 3 eV/c Its wavelength is:

a) le = lp b) le < lp c) le > lp

What is the wavelength of an electron with the same momentum?

le = h/pe Same relation for

particles and photons.

Compared to the energy of the photon (given above): Epc  3 eV

Note that the kinetic energy of the electron is different from the energy of the photon with the same momentum (and wavelength):

eV

eV / J

J

)

m )(

kg

(

s J

m

h m

p KE

6 19

24 2

9 31

2 34

2

2 2

10 8

8 10

602 1

10 41

1 10

414 10

11 9 2

10 625 6

2 2

l

s   m / snm

c eV

s eV

p

h

414 10

3 10

4

1 3

10 14

l

Exrcise 1: Matter wavelengths

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 The DeBroglie wavelength of an electron is inversely related

to the electron momentum:

Wavelength of an Electron

l = h/p

 Frequently we need to know the relation between the

electron’s wavelength l and its kinetic energy E

p and E are related through the classical formula:

2

-31 e

2

-15 2

p

2m h

2m

l

nm eV

E

2

2

505 1

l

l in nanometers

l

nm eV

E photon 1240 

p = h/l

For m = me:

(electrons)

always true!

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Interference of larger particles

Matter-wave interference has now been demonstrated with electrons, neutrons, atoms, small molecules, BIG molecules, & biological molecules

Recent Example: Interference of C 60 , a.k.a “fullerenes”, “buckyballs”

[A Zeilinger (U Vienna), 1999]

Mass = (60 C)(12 g/mole) = 1.2 x 10-24 kg 2

22

3

p

K E kT p kTm kg m s m

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