5 postulates Flashcards

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1
Q

Postulate 1

A

A sum of all the particle’s behaviors can be represented by a wavefunction

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2
Q

A sum of all the particle’s behaviors can be represented by a wavefunction

A

Postulate 1

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3
Q

orthorombic wave functions

A

two wave functions are orthorombic if they equal zero when multipleid (and one of them is the imaginary coeficient)

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4
Q

two wave functions are orthorombic if they equal zero when multipleid (and one of them is the imaginary coeficient)

A

orthorombic wave functions

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5
Q

Orthonormal

A

the function(s) are both normalized and ortorombic

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6
Q

the function(s) are both normalized and ortorombic

A

Orthonormal

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7
Q

how to determine probabilities when the function is Orthonormal.

A

if the function s c*y than the probability of the partical being found in that range of locations is |c|^2

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8
Q

if the function s c*y than the probability of the partical being found in that range of locations is |c|^2

A

how to determine probabilities when the function is Orthonormal.

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9
Q

Postulate 2

A

by applying hermitian Operants to the wavefunction we can extract certain values

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10
Q

by applying hermitian Operants to the wavefunction we can extract certain values

A

Postulate 2

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11
Q

hermitian operant

A

an eigenfunction that alwasy gives a real eigenvalue

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12
Q

an eigenfunction that alwasy gives a real eigenvalue

A

hermitian operant

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13
Q

after completing the function, you get your input wavefunction as part of the output.

A

Eigenfunction

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14
Q

Eigenfunction

A

after completing the function, you get your input wavefunction as part of the output.

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15
Q

Eigenvalue

A

the valiue multiplying the wavefunction after competing an eigenfunction

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16
Q

the valiue multiplying the wavefunction after competing an eigenfunction

A

Eigenvalue

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17
Q

OPerator for position

A

x*wavefunction

18
Q

x*wavefunction

A

Operator for position

19
Q

Operator for 1d momentum

A

-iħ(d/dx)* wavefunction

20
Q

-iħ(d/dx)* wavefunction

A

Operator for 1d momentum

21
Q

Operator for kinetic energy

A

-ħ^2/2m d^2/dx^2

22
Q

-ħ^2/2m d^2/dx^2

A

Operator for kinetic energy

23
Q

Postulate 3

A

when you take a measuremnt you can only mesure something that is an eigenvalue of the appropriate opportator.

24
Q

when you take a measuremnt you can only mesure something that is an eigenvalue of the appropriate opportator.

A

Postulate 3

25
Q

if a wavefunction is an eigenvalue of the operator

A

we will always measure the same value if

26
Q

we will always measure the same value if

A

if a wavefunction is an eigenvalue of the operator

27
Q

If a wavefunction is not an eigenvalue of the operator

A

we will measure one of several different values if

28
Q

we will measure one of several different values if

A

If a wavefunction is not an eigenvalue of the operator

29
Q

Postulate 4

A

The probability of getting result A from a measurment of a wavefunction (where we apply operator Ahat) is given by |c|^2 (where c is added to the function for the purpose of weighting the probabilities)

30
Q

The probability of getting result A from a measurment of a wavefunction (where we apply operator Ahat) is given by |c|^2 (where c is added to the function for the purpose of weighting the probabilities)

A

Postulate 4

31
Q

The average of all measurements of A

A

<a>=sum(|c|^2a) where A is one of the possible eigenvalue measurments, and c is the coeficient for the probability of that measurement.</a>

32
Q

<a>=sum(|c|^2a) where A is one of the possible eigenvalue measurments, and c is the coeficient for the probability of that measurement.</a>

A

The average of all measurements of A

33
Q

commutive operators

A

measuring the wavefunction with one operator will not signifcantly change the wavefunction to measure the other operators

34
Q

measuring the wavefunction with one operator will not signifcantly change the wavefunction to measure the other operators

A

commutive operators

35
Q

physical commutive propery

A

we can determine both properties of the particle at the same time

36
Q

non-comutive functions

A

measuring one value changes the function, so we cannot determine both at once, this is what causes the uncertainty principle.

37
Q

measuring one value changes the function, so we cannot determine both at once, this is what causes the uncertainty principle.

A

non-comutive functions

38
Q

Determining if two functions are commutive

A

if P[T𝟁(x)]-T[P𝟁(x)]=0 than the two opperators are commutive.

39
Q

Postulate 5

A

schrodinger’s equation governs the change in an equation over time

40
Q

schrodinger’s equation governs the change in an equation over time

A

Postulate 5