Chapter 28 Quantum Physics 2 Fig. 28-CO, p. 937.

Chapter 28

Quantum Physics

2Fig. 28-CO, p. 937

3

28.1 Simplification Models Particle Model

Allowed us to ignore unnecessary details of an object when studying its behavior

Systems and rigid objects Extension of particle model

Wave Model Two new models

Quantum particle Quantum particle under boundary conditions

4

Blackbody Radiation An object at any temperature is known

to emit thermal radiation Characteristics depend on the temperature

and surface properties The thermal radiation consists of a

continuous distribution of wavelengths from all portions of the em spectrum

5

Blackbody Radiation, cont At room temperature, the wavelengths of the

thermal radiation are mainly in the infrared region

As the surface temperature increases, the wavelength changes It will glow red and eventually white

The basic problem was in understanding the observed distribution in the radiation emitted by a black body Classical physics didn’t adequately describe the

observed distribution

6

Blackbody Radiation, final A black body is an ideal system that

absorbs all radiation incident on it The electromagnetic radiation emitted

by a black body is called blackbody radiation

7

Blackbody Approximation A good approximation of

a black body is a small hole leading to the inside of a hollow object

The nature of the radiation leaving the cavity through the hole depends only on the temperature of the cavity walls

Fig 28.1

8

Blackbody Experiment Results The total power of the emitted radiation

increases with temperature Stefan’s Law P = A e T4

For a blackbody, e = 1 The peak of the wavelength distribution shifts

to shorter wavelengths as the temperature increases Wien’s displacement law max T = 2.898 x 10-3 m.K

9

Stefan’s Law – Details P = Ae T4

P is the power is the Stefan-Boltzmann constant

= 5.670 x 10-8 W / m2 . K4

Was studied in Chapter 17

10

Wien’s Displacement Law

max T = 2.898 x 10-3 m.K max is the wavelength at which the curve

peaks T is the absolute temperature

The wavelength is inversely proportional to the absolute temperature As the temperature increases, the peak is

“displaced” to shorter wavelengths

11

Intensity of Blackbody Radiation, Summary The intensity increases

with increasing temperature

The amount of radiation emitted increases with increasing temperature The area under the curve

The peak wavelength decreases with increasing temperature

Fig 28.2

12

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Active Figure28.2

13

Ultraviolet Catastrophe At short wavelengths, there

was a major disagreement between classical theory and experimental results for black body radiation

This mismatch became known as the ultraviolet catastrophe You would have infinite

energy as the wavelength approaches zero

Fig 28.3

14

Max Planck 1858 – 1947 He introduced the

concept of “quantum of action”

In 1918 he was awarded the Nobel Prize for the discovery of the quantized nature of energy

15

Planck’s Theory of Blackbody Radiation In 1900, Planck developed a structural model

for blackbody radiation that leads to an equation in agreement with the experimental results

He assumed the cavity radiation came from atomic oscillations in the cavity walls

Planck made two assumptions about the nature of the oscillators in the cavity walls

16

Planck’s Assumption, 1 The energy of an oscillator can have only

certain discrete values En

En = n h ƒ n is a positive integer called the quantum number h is Planck’s constant ƒ is the frequency of oscillation

This says the energy is quantized Each discrete energy value corresponds to a

different quantum state

17

Planck’s Assumption, 2 The oscillators emit or absorb energy only in

discrete units They do this when making a transition from

one quantum state to another The entire energy difference between the initial

and final states in the transition is emitted or absorbed as a single quantum of radiation

An oscillator emits or absorbs energy only when it changes quantum states

18

Energy-Level Diagram An energy-level diagram

shows the quantized energy levels and allowed transitions

Energy is on the vertical axis

Horizontal lines represent the allowed energy levels

The double-headed arrows indicate allowed transitions

Fig 28.4

19

Correspondence Principle Quantum results must blend smoothly with

classical results when the quantum number becomes large Quantum effects are not seen on an everyday

basis since the energy change is too small a fraction of the total energy

Quantum effects are important and become measurable only on the submicroscopic level of atoms and molecules

20Fig. 28-5, p. 940

28

28.2 Photoelectric Effect The photoelectric effect occurs when

light incident on certain metallic surfaces causes electrons to be emitted from those surfaces The emitted electrons are called

photoelectrons The effect was first discovered by Hertz

29

Photoelectric Effect Apparatus When the tube is kept in the

dark, the ammeter reads zero When plate E is illuminated by

light having an appropriate wavelength, a current is detected by the ammeter

The current arises from photoelectrons emitted from the negative plate (E) and collected at the positive plate (C)

Fig 28.7

30


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Active Figure28.7

31

Photoelectric Effect, Results At large values of V, the

current reaches a maximum value All the electrons emitted at E

are collected at C The maximum current

increases as the intensity of the incident light increases

When V is negative, the current drops

When V is equal to or more negative than Vs, the current is zero Fig 28.8

32

Photoelectric Effect Feature 1 Dependence of photoelectron kinetic energy

on light intensity Classical Prediction

Electrons should absorb energy continually from the electromagnetic waves

As the light intensity incident on the metal is increased, the electrons should be ejected with more kinetic energy

Experimental Result The maximum kinetic energy is independent of light

intensity The current goes to zero at the same negative voltage

for all intensity curves

33

Photoelectric Effect Feature 2 Time interval between incidence of light and

ejection of photoelectrons Classical Prediction

For very weak light, a measurable time interval should pass between the instant the light is turned on and the time an electron is ejected from the metal

This time interval is required for the electron to absorb the incident radiation before it acquires enough energy to escape from the metal

Experimental Result Electrons are emitted almost instantaneously, even at very

low light intensities Less than 10-9 s

34

Photoelectric Effect Feature 3 Dependence of ejection of electrons on light

frequency Classical Prediction

Electrons should be ejected at any frequency as long as the light intensity is high enough

Experimental Result No electrons are emitted if the incident light falls below

some cutoff frequency, ƒc

The cutoff frequency is characteristic of the material being illuminated

No electrons are ejected below the cutoff frequency regardless of intensity

35

Photoelectric Effect Feature 4 Dependence of photoelectron kinetic energy

on light frequency Classical Prediction

There should be no relationship between the frequency of the light and the electric kinetic energy

The kinetic energy should be related to the intensity of the light

Experimental Result The maximum kinetic energy of the photoelectrons

increases with increasing light frequency

36

Photoelectric Effect Features, Summary The experimental results contradict all four

classical predictions Einstein extended Planck’s concept of

quantization to electromagnetic waves All electromagnetic radiation can be

considered a stream of quanta, now called photons

A photon of incident light gives all its energy hƒ to a single electron in the metal

37

Photoelectric Effect, Work Function Electrons ejected from the surface of the

metal and not making collisions with other metal atoms before escaping possess the maximum kinetic energy Kmax

Kmax = hƒ – is called the work function The work function represents the minimum energy

with which an electron is bound in the metal

38

Some Work Function Values

39

Photon Model Explanation of the Photoelectric Effect Dependence of photoelectron kinetic energy on

light intensity Kmax is independent of light intensity K depends on the light frequency and the work function The intensity will change the number of photoelectrons

being emitted, but not the energy of an individual electron

Time interval between incidence of light and ejection of the photoelectron Each photon can have enough energy to eject an

electron immediately

40

Photon Model Explanation of the Photoelectric Effect, cont Dependence of ejection of electrons on

light frequency There is a failure to observe photoelectric

effect below a certain cutoff frequency, which indicates the photon must have more energy than the work function in order to eject an electron

Without enough energy, an electron cannot be ejected, regardless of the light intensity

41

Photon Model Explanation of the Photoelectric Effect, final Dependence of photoelectron kinetic

energy on light frequency Since Kmax = hƒ – As the frequency increases, the kinetic

energy will increase Once the energy of the work function is

exceeded There is a linear relationship between the

kinetic energy and the frequency

42

Cutoff Frequency The lines show the linear

relationship between K and ƒ

The slope of each line is h The absolute value of the

y-intercept is the work function

The x-intercept is the cutoff frequency This is the frequency below

which no photoelectrons are emitted

Fig 28.9

43

Cutoff Frequency and Wavelength The cutoff frequency is related to the work

function through ƒc = / h The cutoff frequency corresponds to a cutoff

wavelength

Wavelengths greater than c incident on a material having a work function do not result in the emission of photoelectrons

ƒcc

c hc

44

Applications of the Photoelectric Effect Detector in the light meter of a camera Phototube

Used in burglar alarms and soundtrack of motion picture films

Largely replaced by semiconductor devices Photomultiplier tubes

Used in nuclear detectors and astronomy

45Fig. 28-10, p. 946

48

28.3 Arthur Holly Compton 1892 - 1962 Director at the lab of

the University of Chicago

Discovered the Compton Effect

Shared the Nobel Prize in 1927

49

The Compton Effect, Introduction Compton and coworkers dealt with Einstein’s

idea of photon momentum Einstein proposed a photon with energy E carries

a momentum of E/c = hƒ / c Compton and others accumulated evidence

of the inadequacy of the classical wave theory

The classical wave theory of light failed to explain the scattering of x-rays from electrons

50

Compton Effect, Classical Predictions According to the classical theory,

electromagnetic waves of frequency ƒo incident on electrons should Accelerate in the direction of propagation of the x-

rays by radiation pressure Oscillate at the apparent frequency of the radiation

since the oscillating electric field should set the electrons in motion

Overall, the scattered wave frequency at a given angle should be a distribution of Doppler-shifted values

51

Compton Effect, Observations Compton’s

experiments showed that, at any given angle, only one frequency of radiation is observed

Fig 28.11

52Fig. 28-12, p. 948

53

Compton Effect, Explanation The results could be explained by treating the

photons as point-like particles having energy hƒ and momentum hƒ / c

Assume the energy and momentum of the isolated system of the colliding photon-electron are conserved Adopted a particle model for a well-known wave

This scattering phenomena is known as the Compton Effect

54

Compton Shift Equation The graphs show the

scattered x-ray for various angles

The shifted peak, ', is caused by the scattering of free electrons

This is called the Compton shift equation

' 1 cosoe

h

m c

Fig 28.13

55

Compton Wavelength The unshifted wavelength, o, is caused

by x-rays scattered from the electrons that are tightly bound to the target atoms

The shifted peak, ', is caused by x-rays scattered from free electrons in the target

The Compton wavelength is 0.00243

e

hnm

m c

58

28.4 Photons and Waves Revisited Some experiments are best explained by the

photon model Some are best explained by the wave model We must accept both models and admit that

the true nature of light is not describable in terms of any single classical model

Light has a dual nature in that it exhibits both wave and particle characteristics

The particle model and the wave model of light complement each other

59

28.5 Louis de Broglie 1892 – 1987 Originally studied

history Was awarded the

Nobel Prize in 1929 for his prediction of the wave nature of electrons

60

Wave Properties of Particles Louis de Broglie postulated that

because photons have both wave and particle characteristics, perhaps all forms of matter have both properties

The de Broglie wavelength of a particle is

h h

p mv

61

Frequency of a Particle In an analogy with photons, de Broglie

postulated that particles would also have a frequency associated with them

These equations present the dual nature of matter particle nature, m and v wave nature, and ƒ

ƒE

h

62

Davisson-Germer Experiment If particles have a wave nature, then

under the correct conditions, they should exhibit diffraction effects

Davission and Germer measured the wavelength of electrons

This provided experimental confirmation of the matter waves proposed by de Broglie

69

Electron Microscope The electron microscope

depends on the wave characteristics of electrons

The electron microscope has a high resolving power because it has a very short wavelength

Typically, the wavelengths of the electrons are about 100 times shorter than that of visible light

Fig 28.14

70Fig. 28-14b, p. 953

71

28.6 Quantum Particle The quantum particle is a new

simplification model that is a result of the recognition of the dual nature of light and of material particles

In this model, entities have both particle and wave characteristics

We much choose one appropriate behavior in order to understand a particular phenomenon

72Fig. 28-15, p. 954

73

Ideal Particle vs. Ideal Wave An ideal particle has zero size

Therefore, it is localized in space An ideal wave has a single frequency

and is infinitely long Therefore, it is unlocalized in space

A localized entity can be built from infinitely long waves

74Fig. 28-16, p. 955

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Active Figure28.16

76

Particle as a Wave Packet Multiple waves are superimposed so that one

of its crests is at x = 0 The result is that all the waves add

constructively at x = 0 There is destructive interference at every

point except x = 0 The small region of constructive interference

is called a wave packet The wave packet can be identified as a particle

77

Wave Envelope

The blue line represents the envelope function

This envelope can travel through space with a different speed than the individual waves

Fig 28.17

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Active Figure28.17

79

Speeds Associated with Wave Packet The phase speed of a wave in a wave

packet is given by

This is the rate of advance of a crest on a single wave

The group speed is given by

This is the speed of the wave packet itself

phasev k

gdv dk

80

Speeds, cont The group speed can also be expressed

in terms of energy and momentum

This indicates that the group speed of the wave packet is identical to the speed of the particle that it is modeled to represent

2 1

22 2g

dE d pv p u

dp dp m m

81

28.18 Electron Diffraction, Set-Up

Fig 28.18

82

Electron Diffraction, Experiment Parallel beams of mono-energetic

electrons are incident on a double slit The slit widths are small compared to

the electron wavelength An electron detector is positioned far

from the slits at a distance much greater than the slit separation

83

Electron Diffraction, cont If the detector collects electrons

for a long enough time, a typical wave interference pattern is produced

This is distinct evidence that electrons are interfering, a wave-like behavior

The interference pattern becomes clearer as the number of electrons reaching the screen increases

Fig 28.19

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Active Figure28.19

85

Electron Diffraction, Equations A minimum occurs when

This shows the dual nature of the electron The electrons are detected as particles at a

localized spot at some instant of time The probability of arrival at that spot is determined

by finding the intensity of two interfering waves

sin sin2 2 x

hd or

p d

86

Electron Diffraction, Closed Slits

If one slit is closed, the maximum is centered around the opening

Closing the other slit produces another maximum centered around that opening

The total effect is the blue line

It is completely different from the interference pattern (brown curve)

Fig 28.20

87Fig. 28-20, p. 958

88

Electron Diffraction Explained An electron interacts with both slits

simultaneously If an attempt is made to determine

experimentally which slit the electron goes through, the act of measuring destroys the interference pattern It is impossible to determine which slit the electron

goes through In effect, the electron goes through both slits

The wave components of the electron are present at both slits at the same time

89

Werner Heisenberg 1901 – 1976 Developed matrix

mechanics Many contributions

include Uncertainty Principle

Rec’d Nobel Prize in 1932

Prediction of two forms of molecular hydrogen

Theoretical models of the nucleus

90

28.8 The Uncertainty Principle, Introduction In classical mechanics, it is possible, in

principle, to make measurements with arbitrarily small uncertainty

Quantum theory predicts that it is fundamentally impossible to make simultaneous measurements of a particle’s position and momentum with infinite accuracy

91

Heisenberg Uncertainty Principle, Statement The Heisenberg Uncertainty Principle

states if a measurement of the position of a particle is made with uncertainty x and a simultaneous measurement of its x component of momentum is made with uncertainty p, the product of the two uncertainties can never be smaller than

2px x

92

Heisenberg Uncertainty Principle, Explained It is physically impossible to measure

simultaneously the exact position and exact momentum of a particle

The inescapable uncertainties do not arise from imperfections in practical measuring instruments

The uncertainties arise from the quantum structure of matter

93

Heisenberg Uncertainty Principle, Another Form Another form of the Uncertainty

Principle can be expressed in terms of energy and time

This suggests that energy conservation can appear to be violated by an amount E as long as it is only for a short time interval t

2tE

96

28.9 Probability – A Particle Interpretation From the particle point of view, the

probability per unit volume of finding a photon in a given region of space at an instant of time is proportional to the number N of photons per unit volume at that time and to the intensity

Probability

V

NI

V

97

Probability – A Wave Interpretation From the point of view of a wave, the

intensity of electromagnetic radiation is proportional to the square of the electric field amplitude, E

Combining the points of view gives

2Probability

VE

2I E

98

Probability – Interpretation Summary For electromagnetic radiation, the probability

per unit volume of finding a particle associated with this radiation is proportional to the square of the amplitude of the associated em wave The particle is the photon

The amplitude of the wave associated with the particle is called the probability amplitude or the wave function The symbol is

99

Wave Function The complete wave function for a

system depends on the positions of all the particles in the system and on time The function can be written as (r1, r2, … rj…., t) = (rj)e-it

rj is the position of the jth particle in the system = 2 ƒ is the angular frequency 1i

100

Wave Function, cont The wave function is often complex-valued The absolute square ||2 = is always real

and positive * is the complete conjugate of It is proportional to the probability per unit volume

of finding a particle at a given point at some instant

The wave function contains within it all the information that can be known about the particle

101

Wave Function, General Comments, Final The probabilistic interpretation of the

wave function was first suggested by Max Born

Erwin Schrödinger proposed a wave equation that describes the manner in which the wave function changes in space and time This Schrödinger Wave Equation represents a

key element in quantum mechanics

102

Wave Function of a Free Particle The wave function of a free particle moving

along the x-axis can be written as (x) = Aeikx

k = 2 is the angular wave number of the wave representing the particle

A is the constant amplitude If represents a single particle, ||2 is the

relative probability per unit volume that the particle will be found at any given point in the volume ||2 is called the probability density

103

Wave Function of a Free Particle, Cont In general, the probability

of finding the particle in a volume dV is ||2 dV

With one-dimensional analysis, this becomes ||2 dx

The probability of finding the particle in the arbitrary interval axb is

and is the area under the curve

b

a

2

ab dxP

Fig 28.21

104

Wave Function of a Free Particle, Final Because the particle must be

somewhere along the x axis, the sum of all the probabilities over all values of x must be 1

Any wave function satisfying this equation is said to be normalized

Normalization is simply a statement that the particle exists at some point in space

1dxP 2

ab

105

Expectation Values is not a measurable quantity Measurable quantities of a particle can

be derived from The average position is called the

expectation value of x and is defined as

dxx*x

106

Expectation Values, cont The expectation value of any function of

x can also be found

The expectation values are analogous to averages

dxxf*xf

107

28.10 Particle in a Box A particle is confined to a

one-dimensional region of space The “box” is one-

dimensional The particle is bouncing

elastically back and forth between two impenetrable walls separated by L

Classically, the particle’s momentum and kinetic energy remain constant

Fig 28.22

108

Wave Function for the Particle in a Box Since the walls are impenetrable, there

is zero probability of finding the particle outside the box (x) = 0 for x < 0 and x > L

The wave function must also be 0 at the walls The function must be continuous (0) = 0 and (L) = 0

109

Potential Energy for a Particle in a Box

As long as the particle is inside the box, the potential energy does not depend on its location We can choose this energy

value to be zero The energy is infinitely large

if the particle is outside the box This ensures that the wave

function is zero outside the box

Fig 28.22

110

Wave Function of a Particle in a Box – Mathematical The wave function can be expressed as

a real, sinusoidal function

Applying the boundary conditions and using the de Broglie wavelength

2( ) sin

xx A

( ) sinn x

x AL

111

Graphical Representations for a Particle in a Box

Fig 28.23

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Active Figure28.23

113

Wave Function of the Particle in a Box, cont Only certain wavelengths for the particle

are allowed ||2 is zero at the boundaries ||2 is zero at other locations as well,

depending on the values of n The number of zero points increases by

one each time the quantum number increases by one

114

Momentum of the Particle in a Box Remember the wavelengths are

restricted to specific values Therefore, the momentum values are

also restricted

2

h nhp

L

115

Energy of a Particle in a Box We chose the potential energy of the

particle to be zero inside the box Therefore, the energy of the particle is

just its kinetic energy

The energy of the particle is quantized

22

21, 2, 3

8n

hE n n

mL

116

Energy Level Diagram – Particle in a Box

The lowest allowed energy corresponds to the ground state

En = n2E1 are called excited states

E = 0 is not an allowed state The particle can never be at

rest The lowest energy the particle

can have, E = 1, is called the zero-point energy

Fig 28.24

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Active Figure28.24

123

28.11 Boundary Conditions Boundary conditions are applied to determine

the allowed states of the system In the model of a particle under boundary

conditions, an interaction of a particle with its environment represents one or more boundary conditions and, if the interaction restricts the particle to a finite region of space, results in quantization of the energy of the system

In general, boundary conditions are related to the coordinates describing the problem

124

28.12 Erwin Schrödinger 1887 – 1961 Best known as one of

the creators of quantum mechanics

His approach was shown to be equivalent to Heisenberg’s

Also worked with statistical mechanics color vision general relativity

125

Schrödinger Equation The Schrödinger equation as it applies

to a particle of mass m confined to moving along the x axis and interacting with its environment through a potential energy function U(x) is

This is called the time-independent Schrödinger equation

2 2

22

h dU E

m dx

126

Schrödinger Equation, cont Both for a free particle and a particle in

a box, the first term in the Schrödinger equation reduces to the kinetic energy of the particle multiplied by the wave function

Solutions to the Schrödinger equation in different regions must join smoothly at the boundaries

127

Schrödinger Equation, final (x) must be continuous (x) must approach zero as x

approaches ± This is needed so that (x) obeys the

normalization condition d / dx must also be continuous for

finite values of the potential energy

128

Solutions of the Schrödinger Equation Solutions of the Schrödinger equation may be

very difficult The Schrödinger equation has been

extremely successful in explaining the behavior of atomic and nuclear systems Classical physics failed to explain this behavior

When quantum mechanics is applied to macroscopic objects, the results agree with classical physics

129

Potential Wells A potential well is a graphical

representation of energy The well is the upward-facing region of

the curve in a potential energy diagram The particle in a box is sometimes said

to be in a square well Due to the shape of the potential energy

diagram

130

Schrödinger Equation Applied to a Particle in a Box In the region 0 < x < L, where U = 0, the

Schrödinger equation can be expressed in the form

The most general solution to the equation is (x) = A sin kx + B cos kx A and B are constants determined by the

boundary and normalization conditions

22

2 2

2d mEk

dx

131

Schrödinger Equation Applied to a Particle in a Box, cont. Solving for the allowed energies gives

The allowed wave functions are given by

The second expression is the normalized wave function These match the original results for the particle in a box

22

28n

hE n

mL

2( ) sin sin

n x n xx A

L L L

132

Application – Nanotechnology Nanotechnology refers to the design and

application of devices having dimensions ranging from 1 to 100 nm

Nanotechnology uses the idea of trapping particles in potential wells

One area of nanotechnology of interest to researchers is the quantum dot A quantum dot is a small region that is grown in a

silicon crystal that acts as a potential well Storage of binary information using quantum dots is

being researched

133

Quantum Corral Corrals and other

structures are used to confine surface electron waves

This corral is a ring of 48 iron atoms on a copper surface

The ring has a diameter of 143 nm

Fig 28.25

136

28.13 Tunneling The potential energy

has a constant value U in the region of width L and zero in all other regions

This a called a square barrier

U is the called the barrier height Fig 28.26

137

Tunneling, cont Classically, the particle is reflected by the

barrier Regions II and III would be forbidden

According to quantum mechanics, all regions are accessible to the particle The probability of the particle being in a classically

forbidden region is low, but not zero According to the Uncertainty Principle, the particle

can be inside the barrier as long as the time interval is short and consistent with the Principle

138

Tunneling, final The curve in the diagram represents a full

solution to the Schrödinger equation Movement of the particle to the far side of the

barrier is called tunneling or barrier penetration

The probability of tunneling can be described with a transmission coefficient, T, and a reflection coefficient, R

139

Tunneling Coefficients The transmission coefficient represents the

probability that the particle penetrates to the other side of the barrier

The reflection coefficient represents the probability that the particle is reflected by the barrier

T + R = 1 The particle must be either transmitted or reflected T e-2CL and can be non zero

Tunneling is observed and provides evidence of the principles of quantum mechanics

140

Applications of Tunneling Alpha decay

In order for the alpha particle to escape from the nucleus, it must penetrate a barrier whose energy is several times greater than the energy of the nucleus-alpha particle system

Nuclear fusion Protons can tunnel through the barrier

caused by their mutual electrostatic repulsion

141

More Applications of Tunneling – Scanning Tunneling Microscope An electrically conducting probe with a very

sharp edge is brought near the surface to be studied

The empty space between the tip and the surface represents the “barrier”

The tip and the surface are two walls of the “potential well”

The vertical motion of the probe follows the contour of the specimen’s surface and therefore an image of the surface is obtained

145

28.14 Cosmic Temperature In the 1940’s, a structural model of the

universe was developed which predicted the existence of thermal radiation from the Big Bang The radiation would now have a

wavelength distribution consistent with a black body

The temperature would be a few kelvins

146

Cosmic Temperature, cont In 1965 two workers at Bell Labs found

a consistent “noise” in the radiation they were measuring They were detecting the background

radiation from the Big Bang It was detected by their system regardless

of direction It was consistent with a back body at about

3 K

147

Cosmic Temperature, Final Measurements at

many wavelengths were needed

The brown curve is the theoretical curve

The blue dots represent measurements from COBE and Bell Labs

Fig 28.27

Chapter 28 Quantum Physics 2 Fig. 28-CO, p. 937.

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Transcript of Chapter 28 Quantum Physics 2 Fig. 28-CO, p. 937.