Wavefunctions Flashcards

1
Q

Born interpetation

A

The intensity of a quantum wave at a given point in space is proportional to the probability of finding the particle at that point by measurement.

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2
Q

The intensity of a quantum wave at a given point in space is proportional to the probability of finding the particle at that point by measurement.

A

Born interpetation

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3
Q

finding the probability that a particle will be in a certain area

A

integrate the squared wave equation over the are in questin

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4
Q

integrate the squared wave equation over the are in questin

A

finding the probability that a particle will be in a certain area

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5
Q

normalizing a wave function

A

a wave function, when the probability form infinity to negative infinity is found, can’t have a result higher than 1. If the result isn’t one then solve for a N^2 that will make it equal to 1

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6
Q

a wave function, when the probability form infinity to negative infinity is found, can’t have a result higher than 1. If the result isn’t one then solve for a N^2 that will make it equal to 1

A

normalizing a wave function

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7
Q

requirments for born interpetaion

A

no jumping to infinity, no more than one value per space, and both the equation and it’s derivative must be continuous.

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8
Q

no jumping to infinity, no more than one value per space, and both the equation and it’s derivative must be continuous.

A

requirments for born interpetaion

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9
Q

wave packet

A

a representation of the area where a quantum partical could be. Marking one spot makes it look like a clasical particle.

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10
Q

a representation of the area where a quantum partical could be. Marking one spot makes it look like a clasical particle.

A

wave packet

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11
Q

equation for a particle in a box

A

𝟁(x)=sqrt(2/a)sin((nπx)/a)

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12
Q

𝟁(x)=sqrt(2/a)sin((nπx)/a)

A

equation for particle in a box

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13
Q

Purpose of n in the box’ed particle equation.

A

The edges of the box must equal zero, so only certain energy states can be used

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14
Q

The edges of the box must equal zero, so only certain energy states can be used

A

Purpose of n in the box’ed particle equation.

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15
Q

zero point energy

A

the lowest energy state (n) a particle in a box can occupy, can’t actualy be 0

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16
Q

the lowest energy state (n) a particle in a box can occupy, can’t actualy be 0

A

Zero point energy

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17
Q

to find the probability in a particle being in a certain part of the box

A

integrate psi squared from 0 to target

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18
Q

integrate psi squared from 0 to target

A

to find the probability in a particle being in a certain part of the box

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19
Q

Everything is in a box

A

in the real universe, everything is under some sort of constraint

20
Q

in the real universe, everything is under some sort of constraint

A

Everything is in a box

21
Q

Energy of a quantum step in a box

A

h^2n^2/8ma^2

22
Q

h^2n^2/8ma^2

A

Energy of a quantum step in a box

23
Q

scaling particle in a box to clasical

A

as the partigle grows it’s mass grows and the minimum size of the box also grows, since m and a^2 are on the bottom the gap between n’s shrinks to indistinguishable.

24
Q

as the partigle grows it’s mass grows and the minimum size of the box also grows, since m and a^2 are on the bottom the gap between n’s shrinks to indistinguishable.

A

scaling particle in a box to clasical

25
When a particle hits an infinite barrier that it has enough energy to pass through
Transmittance is high, but the chance of reflection is never zero
26
Transmittance is high, but the chance of reflection is never zero
When a particle hits an infinite barrier that it has enough energy to pass through
27
transmittance for a high energy particle against an infinite barriar
T=(4k_2^2)/(k_1+k_2)^2 (where k is the wave vector magnitude)
28
T=(4k_2^2)/(k_1+k_2)^2 (where k is the wave vector magnitude)
transmittance for a high energy particle against an infinite barriar
29
Reflectance for a high energy particle against an infinite barriar
R=(k_1-k_2)^2/(k_1+k_2)^2 (where k is the wave vector magnitude)
30
R=(k_1-k_2)^2/(k_1+k_2)^2 (where k is the wave vector magnitude)
Reflectance for a high energy particle against an infinite barriar
31
When a particle hits an infinite barrier and doesn't have enough energy to pass through
it will always be reflected, but it has a chance of penitrating into the barrier before turning around.
32
it will always be reflected, but it has a chance of penitrating into the barrier before turning around.
When a particle hits an infinite barrier and doesn't have enough energy to pass through
33
when a particle with greter anergy than a barrier hit a non-infinite barriar
the particle still has a small chance of reflection, but it will most likely be transmitted to the other side, with the same waveleingth but different amplitude
34
the particle still has a small chance of reflection, but it will most likely be transmitted to the other side, with the same waveleingth but different amplitude
when a particle with greter anergy than a barrier hit a non-infinite barriar
35
Transmittance for a high energy particle and a non-infinite barriar
T=[1+(((sin^2(𝜒*√(ε -1))/(4ε (ε -1)))]^-1
36
T=[1+(((sin^2(𝜒*√(ε -1))/(4ε (ε -1)))]^-1
Transmittance for a high energy particle and a non-infinite barriar
37
Reflectance for a high energy particle and a non-infinite barriar
R=[1+(4ε (ε -1))/(sin^2(𝜒*√(ε -1))]^-1
38
R=[1+(4ε (ε -1))/(sin^2(𝜒*√(ε -1))]^-1
Reflectance for a high energy particle and a non-infinite barriar
39
value of epsilon
ε=E/V_o
40
ε=E/V_o
value of epsilon
41
value of Chi
𝜒=(a√2mV_o)/h
42
𝜒=(a√2mV_o)/h
value of Chi
43
Transmission resonance
when the energy of the particle is equal to specific values, transmitance is extremely high (1) becaue of resonance while inside the barriar
44
when the energy of the particle is equal to specific values, transmitance is extremely high (1) becaue of resonance while inside the barriar
Transmission resonance
45
Equation for Transmission resonance
E=V_o+(h^2n^2)/(8ma^2
46
E=V_o+(h^2n^2)/(8ma^2
Equation for Transmission resonance