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Wave packet etc
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Wave Packet Etc

Apr 13, 2018

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Abhilash GS
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Page 1: Wave Packet Etc

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Wave packet etc

Page 2: Wave Packet Etc

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Plane Waves

• a plane wave is an ideal wave withsingle wavenumber k. The wave fronts(surfaces of constant phase) of a plane

wave are innite parallel planes ofconstant peak-to-peak amplitude normalto the phase velocit vector.

• !f a wave is of innite e"tent onl then itwill propagate as a plane wave. !n mostpractical cases waves are appro"imatelplane waves in a locali#ed region of space.

Page 3: Wave Packet Etc

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Plane Wave

Page 4: Wave Packet Etc

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Plane Wave

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Phase $elocit of a PlaneWave

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Plane Wave

Equation of a Plane% plane in &d-space has the e'uation

ax + by + cz = d,where at least one of the numbers a b c must be

non#ero.

Page 7: Wave Packet Etc

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Wave packet in bothposition and momentum space

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$elocit of a Wave Packet

• !f the position of the wave packetchanges with time then the rate atwhich the ma"imum point moves is a

reasonabl good measure of thevelocit of the wave packet

∫ ∞

∞−

−=   dk ek at  x   wt kxi )()(),(ψ  

Page 9: Wave Packet Etc

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%ppro"imations•

!n order for the momentum of the particleto be reasonabl well dened

--- et us assume that the harmonic wavespresent in ψ ("t) have wave vectors lingwithin a small range centered around avalue *k+

k  p   =

)( 

)()( 

)()(

k k 

k k k d 

d k 

k k dk 

k k k 

==

+=

+= =

ω ω 

ω ω ω 

ω 

ω ω 

Page 10: Wave Packet Etc

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%t the ,a"imum of Wave packet at ",%

0=  

  

 

=   MAX  x xdx

d ψ  

∫ ∞

∞−

−=   dk ek at  x   wt kxi )()(),(ψ  

Page 11: Wave Packet Etc

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%t the ,a"imum of Wave packet at ",%

∫ ∞

∞−

−=   dk ek at  x   wt kxi )()(),(ψ  

∫    =−0dk eik k a

  t kxi MAX   )(

))((  ω  

0=  

  

 

=   MAX  x xdx

d ψ  

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urther di/erentiating wrt to time

∫    =−0dk eik k a

  t kxi MAX  

)())((

  ω  

( )[ ]∫    =−   −0dk e xk iik k a

  t kxi

 MAX  

 MAX   )())((

  ω  

ω  

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0sing the %ppro"imation

( )[ ]∫    =−   −0dk e xk iik k a

  t kxi

 MAX  

 MAX   )())((

  ω  

ω  

)()(   k k k d 

d k    −

+=  ω 

ω ω 

∫ ∫    =

−−

−   −−

022

dk keik ak k d 

d dk eik k a

k d 

wd  x

  t kxit kxi

 MAX  

 MAX   MAX   )()())(( ))((

  ω  ω    ω  

ω  

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0sing the %ppro"imation

∫ ∫    =

−−

−   −− 022 dk keik ak 

k d 

d dk eik k a

k d 

wd  x   t kxit kxi MAX  

 MAX   MAX   )()( ))(( ))((   ω  ω    ω  

ω  

∫    =−0dk eik k a

  t kxi MAX   )(

))((  ω  

∫    =

−   −

02

 ))(()(dk eik k a

k d 

wd  x

  t kxi

 MAX  

 MAX     ω  

0=  

  

 

=   MAX  x xdx

d ψ  

Page 15: Wave Packet Etc

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0sing the %ppro"imation

∫    =

−   −0

2 ))((

)(dk eik k a

k d 

wd  x

  t kxi

 MAX  

 MAX     ω  

02

2

≠   

 

 

 

=  MAX  x x

dx

d  ψ  

The term in the above integral ison!zero"

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$elocit of the Peak

PacketWavetheof VelocityGroupcalledisG

G

 MAX  

 MAX  

 MAX  

V  

k d 

wd V  

k d 

wd 

dt 

dx

k d 

wd 

dt 

dx

k d 

wd  x

=

=

=

=

0

0

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Phsical 1ignicance of $2

•  The $elocit of a free particle (bothnon-relativistic and relativistic) canbe written as

  dp

dE v =

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Phsical 1ignicance of $2

•  The $elocit of a particle (both non-relativistic and relativistic) can bewritten as

  dp

dE v particle =

k p & E    ==   ω with

G particle   V dk 

dp

dE v ~ 

ω ==

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 The Particle Picture

G particle   V dk 

dp

dE v ~ ω ==

% small wave packet consisting of small band of3e 4roglie waves moves somewhat like a

classical free particle.

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Wave-Particle 3ualit

G particle   V dk 

dp

dE v ~ ω ==

% small wave packet consisting of small band of3e 4roglie waves moves somewhat like a

classical free particle.

 The appro"imation is valid onl to the e"tent that onecan ignore the fundamental limitations placed b thewave packet picture on the accurac with which boththe position and momentum of a particle can be