Section 2 Flashcards

1
Q

mod-squared gives

A

a probability density

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2
Q

probability of density in [x,x+dx] at t =

A

|Ψ(x,t)|^2

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3
Q

the normalisation of probability density

A

∫ |Ψ(x,t)|^2 dx = 1

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4
Q

dispersion relation

A

E = hv = ℏω ; p = ℏk

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5
Q

same intensity everywhere, fully delocalised

A

|Ψ(x,t)| = Ψ(x,t) * Ψ(x,t) = |A|^2

well-defined k, undefined x

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6
Q

plane-wave space and time derivatives:

A

-iℏ ∂/∂x Ψ = pΨ

-iℏ ∂/∂t Ψ = EΨ

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7
Q

localise the wave-function using a Fourier transform

A

f(x) = 1/√2π (-∞ ∫ ∞) dk g(k) exp[i(kx-ω(k)t)]

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8
Q

wave-packet

A

localised sum of waves

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9
Q

stationary phase approximation: dominant amplitude for

A

∂/∂k kx-ω(k)t = 0

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10
Q

group velocity

A

x/t = (dω/dk)|k=k0 = vg

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11
Q

wave-packet does not disperse when

A

ω(k) = vk, dω/dk = const

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12
Q

Parsaval’s theorem

A

(-∞ ∫ ∞) |f(x)|^2dx = (-∞ ∫ ∞) |g(k)|^2 dk

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13
Q

time-evolution of each definite-k / definite-ω is just

A

a phase exp[iω(k)t]

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14
Q

Domains related by FT are

A

conjugate

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15
Q

Gaussian function is special under FT

A

maps to another Gaussian

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16
Q

Heisenberg’s uncertainty principle

A

ΔpΔx > ℏ/2

17
Q

the smallness of ℏ is why

A

neither wavelike phenomena nor quantum uncertainty are seen in macroscopic systems

18
Q

Uncertainty is central to QM

A

Natural spectral line-widths
Estimation of the pion mass

19
Q

Position and momentum are

A

conjugate : when one is wide, the other is narrow