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Atomic Spectroscopy
Atomic Spectra
• Electron excitation energy n = 1
– The excitation can occur at ∆E n = 2
different degrees n = 3,
• low E tends to excite the outmost etc.
e-’s first
• when excited with a high E (photon
of high v) an e- can jump more
than one levels
• even higher E can tear inner e-’s 4f
away from nuclei n=4 4d
4p
– An e- at its excited state is not stable and tends to 3d
return its ground state gy 4s
r n=3 3p
- jumped more than one energy levels because
– If an e ne 3s
of absorption of a high E, the process of the e- E n=2 2p
returning to its ground state may take several steps, - 2s
i.e. to the nearest low energy level first then down to n=1 1s
next …
Atomic Spectra
• Atomic spectra
– The level and quantities of energy energy n = 1
- ∆E
supplied to excite e ’s can be measured n = 2
& studied in terms of the frequency and n = 3,
the intensity of an e.m.r. - the etc.
absorption spectroscopy
– The level and quantities of energy
-
emitted by excited e ’s, as they return to
their ground state, can be measured &
studied by means of the emission
spectroscopy 4f
– The level & quantities of energy n=4 4d
absorbed or emitted (v & intensity of 4p
e.m.r.) are specific for a substance 3d
gy 4s
r n=3 3p
– Atomic spectra are mostly in UV ne 3s
(sometime in visible) regions E n=2 2p
n=1 2s
1s
Atomic spectroscopy
• Atomic emission
– Zero background (noise)
• Atomic absorption
– Bright background (noise)
– Measure intensity change
– More signal than emission
– Trace detection
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