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The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

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Page 1: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

The Particlelike Properties of Electromagnetics Radiation

Wei-Li Chen

10/27/2014

Page 3: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

The Photoelectric Effect• The maximum current is proportional to the incident light

intensity.• There is no minimum intensity below which the current is

absent.

• V0 is independent of the incident light intensity.

• Higher frequency will cause higher Vs.

• Current occurs when the light frequency is above certain value. This threshold frequency varies for different target materials.

• There is no time lag between the turning on of the light and and the appearance of the electron.

seVmv

max

2

2

1 Stopping potential

Page 4: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

tf f theifcurrent No

frequency with increase

energy) kinetic (maximum voltagestop The

different) (intensity

lights frequency different with Performed

The Photoelectric Effect

Page 5: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Einstein’s Photoelectric Effect Equation

tt

s

hchf

hfmveV

constant. s Planck' theis slope The

metal target theof function work theis

)2

1(

light. of sticcharacteri universala wasradiationblackbody thein

by Planck used onquantizatienergy that assumed Einstein

max2

photon. thecalled isenergy neticelectromag thecarries which bundleenergy The

frequency. its toalproportion is bundle

theof Econtent energy The speed.light at travelingspace limited ain localized

energy of bundle a as thought be should waveEM that suggestedEinstein 1905In

hvE

Page 6: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

atom.each fromelectron photo a generate energy toenough accumulate to

hours 5.5 requiresit ,101 isintensity light theIf

.101.84 2.28eV is Na offunction work The

.m 101.12 isdensity atomic theplane, lattice Na(110)On

24-

19-

2-19

Example

mW

J

Page 8: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

X-ray Spectra

Bremsstrahlung (braking radiation)

Characteristic spectra

o

A12400

Vm

Page 9: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

X-ray• X-rays were discovered in 1895 by W. Roentgen. They are

electromagnetic radiation whose wavelength is near the range from 1nm to 0.001nm. An X-ray photon carries energy 1keV or more.

• When high energy electrons hit metal target, the deceleration of electrons will generate electromagnetic radiation that is called bremsstrahlung.

• The most of the radiation are emitted near 90 degree to the direction of the electrons’ path.

• Strong characteristic X-rays produced by electron transitions between different energy levels superimpose on the bremsstrahlung spectrum.

• The characteristic peaks vary with different metal targets.• The X-ray spectrum drops to zero at a maximum feruency fmax which

follows Duane-Hunt law:0max eVKhf

Page 11: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Bragg Law• The size of the atoms in a crystal (~0.1nm) is

compatible to the wavelength of X-ray. In 1912 Laue suggested that a crystal can be used as 3D grating for X-ray.

• Bragg diffraction law:• Historically Bragg diffraction is an important tool to

study X-rays. Today Bragg diffraction is used to characterize the crystal structure and lattice constant.

nd sin2

Page 12: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Bragg Law

integer an is sin2 nnd

Crystalline planes

Page 13: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

X-ray Diffraction

Taylor fig.4.10

Page 14: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

cba

bac

cba

acb

cba

cba

h, k, lwhere

clbkahG

kkr

rdrkkirh

emsf

i

V

ie

2 ,2 ,2

and integers are

k-kkon constructi sEdward'

space. reciprocal the

in nt displaceme discrete with matches k wheredirection at the happens

ceinterferen veConstructi space. crystal real theof ansformfourier tr a is This

vectors.aveincident w and diffracted are and ector,position v theis where

])(exp[)(2

)(

scattering of amplitude The

i

20

Supplement for X-ray Diffraction

Page 15: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

The Compoton Effect

• Electromagnetic radiation interact with an electron will cause it to oscillate at the same frequency. Therefore, according to classical physics, the wavelength of the electromagnetic radiation after interact should remain constant. However, the scattered radiation wavelength becomes longer after collision.

• Compton derived the wavelength change of a photon after its collision with an electron based on energy and momentum conservation laws.

• The Compton effect proves that photons possess momentum, which is an essential characteristic of particles.

Page 16: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

θ

θ

Serves as the detector

integer an is sin2 nnd

Page 17: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

)cos1(

)cos1()(

)cos1()11

(

)cos1(2)(2

(**) and (*) Compare

(**) )(2

2

)(2)(

givesenergy of onConservati

ly.respective and are collisionafter and before electron theofenergy The

(*) cos2

gives momentum of onConservati

ly.respective and are photons scattered andincident theof momentum The

12

120

12

0

21210

21021

22

21

2

2220210

221

220

2220201

2220

20

2122

21

2

21

22

11

θmc

h

θhc

E

θppc

E

θppc

ppE

c

ppEppppp

cpEppcEppcE

cpEcpEcp

cpEcmE

θppppp

ppp

λ

hp

λ

hp

e

e

e

e

e

e

e

Compton wavelength

Page 18: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

cos'

sin'

cos'

sin'

cos

sintan

EE

E

pp

p

p

p

e

e

Experiment setup

Page 19: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Optical Spectrum Analyzer

Dispersion n(λ)

n1sinθ1=n2sinθ2

red

blue

Page 20: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Electromagnetic Wave Spectrum

Page 21: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Blackbody Radiation

• The technology that utilize the dispersion of light into different colors (wavelength) is called spectroscopy.

• When an object reaches thermal equilibrium with the environment, its temperature will be constant. It continuously absorb and emit radiation with equal amount. The electromagnetic radiation emitted by such an object is called thermal radiation.

• A body that absorbs all radiation incident on it is called an ideal blackbody.

- Stefan-Boltzmann law: The power per unit area radiated by an blackbody. - Wien displacement law: λm is wavelength of maximum emission.• Any body that emits radiation at each wavelength in a constant ratio less

than unity to that emitted by a black body at the same temperature.• An opaque object under equilibrium will emit less radiation than a

blackbody. The ratio is called emissivity ε.

4284 /1067037.5 KmWTI

mKTm3108978.2constant

Page 23: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

u(λ) Comments

Plank’s Law 8πhcλ-5 / [exp(hc/kλT) – 1]

match with experimental data

Raleigh-Jeans Law

8πkTλ-4

good approximation at long wavelength onlyultraviolet catastrophe

Wien Law c1λ-5exp(-c2 /λT) good approximation at short

wavelength only

Blackbody Radiation Formula

mm

joulu

3intervalength unit waveleunit volum

energy represents )(

Page 24: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

ultraviolet catastrophe

0

)( du

works only for long wavelengths

Wien law works only for short wavelengths

(Raleigh-Jeans law)

Page 25: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

constant. sPlanck' calledconstant a is

1 and ,...3,2,1,0

where

, of multipleinterger is soscillator theofenergy The variable.discrete a is

radiation) theofenergy thehence (and soscillator theofenergy theassuming

by explained becan data empiricalradiation blackbody that thefoundPlanck

equation. Jeans-Raleighin used iswhich

)(

is oscillatoran ofenergy average The

.energy with soscillator theoffraction theis )( andt coefficien a isA where

)(

:ondistributiBoltzmann -Maxwell

follows soscillator ofon distributienergy The s.oscillator harmonic like areThey

electrons. ngacceleratiby produced arecavity a inside wavesEM they,Classicall

00

h

e

hvEnnhvE

hvε

ε

kTdEEAedEEEfE

EEf

AeEf

kThvn

kT

E-

kT

E-

The difference betweenboth theories

Page 26: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

1

1)1(

)1(

,

(**)

)1()1(

1

respect toit with ateDifferenti .

1

1...1

(*) back toit Put 1

(*) 1

1

...)1(

)(

becomes nowon distributiBoltzmann -Maxwell The

20000

2020

32

0

32

00

kThv

kTkT

kTkT

n

kT

n

n

kT

n

n

kT

E

nn

nn

kT

kT

n

kT

n

kT

kT

n

kT

n

kT

kT

hv

kT

hv

kT

hv

n

kT

n

kT

hv

kT

hvkT

hv

kT

hv

kT

hv

n

kT

nhv

nn

kT

nhv

kT

n

n

e

hvE

ee

eeneAAenAeEfEE

Therefore

e

ene

e

e

kTe

kT

n

e

eeee

eA

e

AeeeAeAf

AeAeEf

n

page in this explained is 1

kThve

hvE

Page 28: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Density of Oscillation Modes

4

4

3

22

2

2

22

zyx

zyx

8)(

is space-in e)unit volumper modes ofnumber (the modes ofdensity The

824 is space-in modes ofnumber The

22

48

12 is to from modes ofnumber The

e.unit volum cubic 1 occupies modeEach .coordinate-nin indices integral point with a

as expressed becan that mode goscillatinan toingcorrespond is )n ,n ,(n ofset A

wave)(standing 2

L and integers positive are n ,n ,n

sinsinsinsinsinsin),,(

as expressed becan which wavestanding a bemust

function waveits box, theinsidestably exist can waveEMan if box, cubic metal aIn

g

dL

dLL

dL

dnL

n

dnπndnπndnnn

nwhere

zL

ny

L

nx

L

nAzkykxkAzyxE

i

zyxzyx

Page 30: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

08)(

lengthshort wavefor While

formula Jeans-Raleigh )8

)((or 8)(

h) wavelengt(long 1 1

1 ...1

)1(

8

1

8)()(

1

8

1

8)()(

functionon distributienergy The

8)(

888)(

5

3

24

2

3

3

3

2

5

4

3

2

3

2

24

4

4

kThcλ

kTλhc

x

kThvkThvvv

kTλhckTλhcλλ

v

ehcλu

c

πkTvλukTλuand

kT

hcfor

kT

hce

for xxxeBecause

ec

πhv

e

hv

c

πvEvgvu

e

πhcλ

e

λhc

λ

πEλgλu

c

vvg

dvc

vdv

v

c

c

vddg

awPlanck's l

Page 31: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Other Photon Processes

KEEEKEEE

K

KEEEEKEE

iffi

fifi

:anatomby absorbed is photon A

energy kinetic recoil is

)(

:photona emits atom An

Page 32: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

Pair Production Annihilation

2122

2

22

)()(

photonspositron electron

photons. by two replaced anddisappear

positrona and electron an process theIn :onannihilati positron-electron

02.12energy photon

)()(

positron electron photon

charge. electric positivea hasbut electron the tomas in identical is

that thatparticlea is positron A created. are positron)a and electron (an

particles twoand atom an energy to its losses photon A :productionPair

EEKcmKcm

MeVcmhf

KcmKcmEEhf

ee

e

ee

Page 33: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

What is a photon

• Like EM wave, velocity is c.• No mass and rest energy• Carrying energy and momentum• Can be created and destroyed.• Can collide with other particles.

Page 34: The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014

When a photon detected by the detector, it shows particle-like property.When it passes through the switch, it shows wave-like property.

Which Slit Does the Electron Go Through?