QM - Postulates of quantum Flashcards

1
Q

Describe Ψ

A

The state of a system is fully described by a mathematical function Ψ called a wavefunction

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2
Q

Give an example of bra ket notation

A
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3
Q

Define a normalisation constant

A

A normalisation constant N is a constant such that the integral of Ψ(x)Ψ*(x) dx over all space = 1

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4
Q

Define an observable

A

An observable is a measurable property such as bond length or kinetic energy

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5
Q

State the postulate regarding observables and operators

A

Every observable B is represented by an operator B̂ and all operators can be built from the operators for position and momentum

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6
Q

Give and describe the operator for momentum

A

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7
Q

Give and describe the operator for position

A

x^ = multiply by x

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8
Q

State the hamiltonian

A

H^ is the total energy operator, T^ is the kinetic energy operator and V^ is the potential energy operator

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9
Q

Show how to derive the expression for kinetic energy

A
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10
Q

State the general form of an eigenvalue equation

A

B̂f = bf

Where the operator B̂ acts on the eigenfunction to regenerate f multiplied by the eigenvalue b (a constant)

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11
Q

Define an exact wavefunction of the Schrodinger equation

A

If Ψ(x) is an eigenfunction of H^, it is termed an exact wavefunction

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12
Q

Describe orthogonal and orthonormal wavefunctions

A
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13
Q

Give the expectation value for an operator B̂ for a wavefunction Ψ

A

The expectation value is denoted by and is given below.

Note: dτ symbolises integration over all space

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14
Q

Give if the wavefunction in question is an exact wavefunction, ie an eigenfunction of H^ and also an eigenfucntion of B^ such that B^Ψ = bΨ

A
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15
Q

Give if the wavefunction in question is normalised

A
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16
Q

State the Schrodinger equation

A
17
Q

State the postulate regarding

A

When a system is described by a wavefunction Ψ, the average value of the observable B is equal to the expectation value of the corresponding operator B^

18
Q

Describe the variation principle

A

For any trial wavefunction Ψ, the expectation energy can never be less than the energy of the ground state E0

19
Q
A