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)
2
Q
wavefunction
A
- represents the spatial distribution of a particle
3
Q
probabilites must be
A
postive and real
- use modulus
4
Q
modulus of wavefunction squares
A
gives the probability density
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
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
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
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)
9
Q
zero point energy
A
- vibration energy doesn’t eqaul zero even at T=0K
- also consequence of uncertainity principle
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
11
Q
eigenfunction equation
A
operator x wavefunction = observable propertity (eigenvalue) x wavefunction
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
13
Q
operator for position in the X - direction
A
- multipication by x
14
Q
operator for linear momentum in the x -direction
A
- check book
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
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