Optical Spectroscopy

0.0(0)
Studied by 0 people
call kaiCall Kai
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/44

encourage image

There's no tags or description

Looks like no tags are added yet.

Last updated 10:02 AM on 5/29/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai

No analytics yet

Send a link to your students to track their progress

45 Terms

1
New cards

What does sign nu (ν) represent?

Frequency

2
New cards

What does sign nu tilde () represent?

Wavenumber

3
New cards

An ideal emitter

At all freq.s emits the same amount of or more radiation than any other body at the same temperature.

4
New cards

A diffuse emitter

Emits the same amount of radiation in all directions.

5
New cards

A blackbody emitter is

Ideal and diffuse

6
New cards

Stopping voltage is

a property of the metal

7
New cards

Planck-Einstein Relation

E=hv(nu)

8
New cards

de Broglie wavelength equation

λ = h/mv(nu)

9
New cards

de Broglie wavelength represents

the length scale at which its wave-like properties are important

10
New cards

Microwave radiation causes

rotational spectroscopy

11
New cards

Infra-red radiation causes

vibrational spectroscopy

12
New cards

Spectroscopy definition

the study of the interaction of EM radiation with matter

13
New cards

Peak intensity is determined by

Population, transition probability, state degeneracy, path length of sample

14
New cards

Heisenberg uncertainty equation

ΔEΔt >=h/2π, t is time spent in excited state

15
New cards

Natural linewidth is

the limit to how narrow spectral lines can be.

16
New cards

In order for an atom or molecule to absorb/emit a photon at a specific frequency,

it must possess a dipole oscillating at that frequency.

17
New cards

Beer-Lambert Law

A = εLc

18
New cards

A =

log(I0/I), I=intensity

19
New cards

ln(I0/I) =

σLc = αL, σ=absorption cross-section, α=absorption coefficient

20
New cards

T (transmittance)=

I/I0

21
New cards

z (collisional frequency) =

σv(rel)p/kT

22
New cards

v(rel) =

(8kT/πμ)^0.5

23
New cards

collisional/pressure broadening

z/2π

24
New cards

Lifetime of the excited state

τsp

25
New cards

A1←0 =

1/τsp

26
New cards

lifetime broadening

broadening (Δṽ) = A1←0/2πc

27
New cards

doppler broadening

Δṽ = 2ṽ/c * (2kbTln2/m)^0.5

28
New cards

For rotational spectroscopy to be possible,

energy level of electrons must change by 1

29
New cards

B (rotational constant (cm^-1)) =

ћ/4πcI

30
New cards

ћ =

h/2π

31
New cards

I (inertia)=

μr², r=bond length

32
New cards

FJ (energy of state J) =

BJ(J+1)

33
New cards

transition between energy levels (ṽ(J+1←J)) =

2B(J+1)

34
New cards

The bit we observe is

the transition between energy levels

35
New cards

J’’ is the

initial energy level

36
New cards

J’ is the

final energy level

37
New cards

How does population affect line intensity?

If there is no population in a state, no transitions from that state will be seen

38
New cards

Boltzmann expression:

NJ/N = gJe^(-EJ/kT)

39
New cards

gJ (degeneracy of level J) =

2J + 1

40
New cards

EJ (energy level in joules)=

hc * BJ(J+1) (hc to convert cm^-1 to J)

41
New cards

Jmax (J value with highest intensity peak) =

(kT/2hcB)^0.5 - 0.5

42
New cards

correctional factor for centrifugal distortion:

DJJ²(J+1)²

43
New cards

DJ =

4B³/ṽ² (this means higher bond strength = lower centrifugal distortion)

44
New cards

ΔFJ(J+1←J) =

2B(J+1) - 4DJ(J+1)³

45
New cards

difference between requirement for rotational and vibrational spectroscopy

Rotational requires permanent dipole moment, vibrational can have permanent or induced dipole moment.