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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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