topic 3 Flashcards

(16 cards)

1
Q

ψ^2 (wavenumber squared)

A
  • at any given point in space gives the probability of finding the particle at that point (born interpretation)
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2
Q

wavefunction

A
  • represents the spatial distribution of a particle
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3
Q

probabilites must be

A

postive and real
- use modulus

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4
Q

modulus of wavefunction squares

A

gives the probability density

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5
Q

a wavefunction is said to be normalized if

A
  • sun of modulus wavenumber squared at all points in space = 1
  • mathematical equivalent of integration
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6
Q

quantiziation of wavefunction rules

A
  • must be contiuous
  • gradient must be constinuous
  • must have single value at any point in space
  • must be finite
  • cannot be zero everywhere
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7
Q

heisenberg uncertainity principle

A
  • uncertainity in position x uncertainity in momentum is greater than or equal to reduced planks constant over 2
  • i.e there is no concept of particle trajectory
  • can know both momentum and postion if in different axis
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8
Q

to localise a wavefunction in space must (specifiy posititon)

A
  • wave of different wavelenghts must be superimposed to form large change in momentum (p=h/wavelength)
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9
Q

zero point energy

A
  • vibration energy doesn’t eqaul zero even at T=0K
  • also consequence of uncertainity principle
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10
Q

equation relating energy and lifetime

A
  • change energy x change in lifetime greater than or equal to reduced planks constant
  • leads to lifetime broadening of spectral lines
  • short lived excited states possess large uncertainty in the energy of the state
  • leads to broad peaks in spectrum
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11
Q

eigenfunction equation

A

operator x wavefunction = observable propertity (eigenvalue) x wavefunction

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12
Q

operators

A
  • instructions to carry out an action on wavefunction
  • if it gives back the same function multiped by a constant it is referered to as eigenfunction
  • and constant in output is eigenvalue
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13
Q

operator for position in the X - direction

A
  • multipication by x
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14
Q

operator for linear momentum in the x -direction

A
  • check book
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15
Q

commutation

A
  • the operators do not communicate in quantum mechanics therefore order operations are done is important
  • operation1 x opertaion 2 - operation 2 x operation 1 do not equal 0
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16
Q

expectation values of operator

A
  • calculates mean value of a large number of measurement of an observable
  • if wavefucntion normilaised doniminator = 1
  • if wavefunction is an eigenfunction of operator A, the exception value is actually the same as the eigenvalue