Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Absorption spectroscopy
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
===Theory=== Absorption lines are typically classified by the nature of the quantum mechanical change induced in the molecule or atom. [[Rotational spectroscopy|Rotational lines]], for instance, occur when the rotational state of a molecule is changed. Rotational lines are typically found in the microwave spectral region. [[Vibrational spectroscopy|Vibrational lines]] correspond to changes in the vibrational state of the molecule and are typically found in the infrared region. Electronic lines correspond to a change in the electronic state of an atom or molecule and are typically found in the visible and ultraviolet region. X-ray absorptions are associated with the excitation of [[electronic structure#Shells and subshells|inner shell]] electrons in atoms. These changes can also be combined (e.g. [[rotational–vibrational coupling|rotation–vibration transitions]]), leading to new absorption lines at the combined energy of the two changes. The energy associated with the quantum mechanical change primarily determines the frequency of the absorption line but the frequency can be shifted by several types of interactions. Electric and magnetic fields can cause a shift. Interactions with neighboring molecules can cause shifts. For instance, absorption lines of the gas phase molecule can shift significantly when that molecule is in a liquid or solid phase and interacting more strongly with neighboring molecules. The width and shape of absorption lines are determined by the instrument used for the observation, the material absorbing the radiation and the physical environment of that material. It is common for lines to have the shape of a [[Gaussian distribution|Gaussian]] or [[Lorentzian distribution|Lorentzian]] distribution. It is also common for a line to be described solely by its intensity and [[spectral linewidth|width]] instead of the entire shape being characterized. The integrated intensity—obtained by [[integral|integrating]] the area under the absorption line—is proportional to the amount of the absorbing substance present. The intensity is also related to the temperature of the substance and the quantum mechanical interaction between the radiation and the absorber. This interaction is quantified by the [[transition moment]] and depends on the particular lower state the transition starts from, and the upper state it is connected to. The width of absorption lines may be determined by the [[spectrometer]] used to record it. A spectrometer has an inherent limit on how narrow a line it can [[spectral resolution|resolve]] and so the observed width may be at this limit. If the width is larger than the resolution limit, then it is primarily determined by the environment of the absorber. A liquid or solid absorber, in which neighboring molecules strongly interact with one another, tends to have broader absorption lines than a gas. Increasing the temperature or pressure of the absorbing material will also tend to increase the line width. It is also common for several neighboring transitions to be close enough to one another that their lines overlap and the resulting overall line is therefore broader yet.
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)