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Lecture notes on the general methodology of spectroscopy, which is the study of matter through its interaction with different frequency components of the electromagnetic spectrum. the goals of spectroscopy and how it can be adapted to extract information about the energies of electronic, vibrational, and rotational states, as well as the structure and symmetry of molecules. The document also discusses the different types of spectrometers and how absorption spectra are measured.
Typology: Lecture notes
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What is spectroscopy?
Studying the properties of matter through its interaction with different frequency components of the electromagnetic spectrum.
Latin: “spectron”—ghost or spirit Greek: “ σκοπειν ”—to see
With light, you aren’t looking directly at the molecule—the matter—but its “ghost.” You observe the light’s interaction with different degrees of freedom of the molecule. Each type of spectroscopy—different light frequency—gives a different picture → the spectrum.
Spectroscopy is a general methodology that can be adapted in many ways to extract the information you need (energies of electronic, vibrational, rotational states, structure and symmetry of molecules, dynamic information).
Goals:
The immediate questions that we want to address are:
What does a spectrum measure?
Interaction of light with a sample can influence the sample and/or the light.
Method involves: (1) excitation and (2) detection.
The basic idea:
Light (E.M. wave)
In most spectroscopies, we characterize how a sample modifies light entering it.
We measure the absorption of light at different frequency or wavelength.
ω/λ/ν (characteristic frequency/wavelength of light entering sample)
Sample
Characterize light after sample.
Characterize change in sample. (photoacoustic spec.) Other excitation source This borders on photochemistry
2a
2b
I (^0)
sample
I
detector
Wavelength λ (nm, μm, Å),
Frequency ν (cycles/sec or s-1^ or Hz)
c 2
ω = = π λ
ω = 2πν (rad/sec) (angular frequency)
ν = ω/2πc = 1/λ expressed in units of cm-1^ (wavenumbers)
Energy E = hν (expressed as eV or as cm-1^ using E/hc = ν/c)
Conversions ν ( cm -1^ ) = 10^7 / λ( nm )
ν ( eV ) = 1240 / λ( nm )
0
I 0 = light intensity incident on the sample I = light intensity after the sample
c = concentration (M) L = sample length (cm)
This comes from assuming that the fraction of light absorbed as you propagate though the sample is proportional to the distance traversed: dI I = −αdx
How do your measure absorption spectra?
Measure the change of intensity of light at different frequencies as it passes through a sample.
This is a way of processing all wavelength/frequencies simultaneously → IR/NMR
red
blue sample detector
slit
prism
I (^0)
I
ω/λ ω/λ
A