Fundamentals of Quantum Mechanics Flashcards
(18 cards)
Young’s double slit experiment
Shows that light acts as a wave
Radial waves emitted by diffraction –> overlap & interfere
“a wave can be at the same point in space and time” –> CONSTRUCTIVE or DESTRUCTIVE interference -|- waves
e- diffracted through 2 slits
same results as Young’s double slit experiment –> e- are waves too
quantum mechanically, the e- goes through both slits simultaneously BUT if you measure it, you’ll only find it going through one
e- diffraction (e.g. x-rays)
light acts as a particle
e- diffracted at variety of FIXED angles –> particle behaviour
Equation for photon’s E
E = hν
E = energy, J
ν (nu) = freq., Hz (s^-1)
h = Planck’s (proportionality) constant, Js (how many J per unit freq = per s^-1 –> cancels to s)
Photoelectric effect
If photon E > work function of metal, photoelectric effect will occur = e- will be ejected from material
RED (low freq) = no e-
GREEN = e-
BLUE (high freq) = high KE e-
linear trend –> E is directly proportional to freq of light
de Broglie wavelength
wavelength of light
𝛌 = h/p = h/mv
p = momentum, kg m s^-1
m = mass, kg
v = velocity, m s^-1
bigger mass = smaller 𝛌 (negligent) –> QM doesn’t matter for large objects (classical limit)
Bigger objects follow Newtonian mechanics
QM when 𝛌 of particles becomes similar to size of system
ψ
wavefunction - holds all info about a system & is the solution to the Schrödinger equation
“the wavefunction is the function ψ(x) for which the s-eqn is satisfied)
Schrodinger equation
KE + PE = total E x
(2nd derivative ψ)∝(V-E)ψ
- ignore constant
- all wrt x
THUS curvature of ψ∝(KE*ψ)
definition: “an observable”, Ω
any measurable property of a physical system
definition: “an operator”, Ω(hat)
any symbol that indicates an operation to be performed
e.g. √, d/dx, a hat over a letter
In QM, observables are defined by “mathematical” operations on ψ
Hamiltonian operator
Ĥ = operator for the total E
allows s-eqn to be written in shorthand:
Ĥψ(x) = Eψ(x)
where Ĥ = - (ħ/2m)*(2drv) + V(x)
ħ = ?
ħ = h/2π
QM
A study of how matter exists when we think of matter as waves
KE operator
Ê(kin) = -(ħ/2m)*(2drvψ)
Ω(hat)ψ(x) = Ωψ(x)
In general, there exists an operator, Ω(hat), which acts on ψ(x) to yield an observable, Ω, multiplied by ψ(x)
Operator for position in QM
x̂ = x
–> can write: x̂ψ(x) = xψ(x)
S-eqn: curvature & magnitude
curv. ψ(x) of depends on whether V(x) > or < E
magnitude of curv. is defined by KE (V(x)-E)
Normal regime (world)
V(x) < E
curvature∝(V-E)ψ
curvature = 2nd deriv (ψ)
so curv. ∝ -ψ
ψ(x) > 0 -ve curvature
ψ(x) < 0 +ve curvature
–> ψ(x) ALWAYS curves TOWARDS the x-axis
kinds of functions that naturally do this: sine & cosines
show: ψ(x) = sin(kx)
apply to free particle ψ: V(x)=0 AKA particle is moving under no external force
-(ħ/2m)(2drv_sin(kx)) = Esin(kx)
-(ħ/2m)(2drv_sin(kx)) = Esin(kx)
[INCOMPLETE]
d/dx (sin x) = cos x
d/dx (cos x) = -sin x