photochemistry reactions involving photons. (radiation-induced chemical processes: chemical...
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PhotochemistryReactions involving photons.
(Radiation-induced chemical processes: chemical transformations induced by high energy photons.
Radiochemistry (nuclear chemistry): processes in the nuclei of atoms.)
Tamás Vidóczy Institute of Structural Chemistry Chemical Research Center, HAS
http://oktatas.ch.bme.hu/oktatas/konyvek/fizkem/fizkem2/fotokemia
Electromagnetic spectrum important for photochemistry
IR
E
UV
~700 nm
~400 nm
E = hν = hc/λ
~200 nmVUV
Excited states and related bond strength
Multiplicity
Name redived from: 2S + 1
S = 0 singlet
S = ½ doublet
S = 1 triplet
The Jablonski diagram
E
S S1 S2 T1 T2
involving a photon
without photons
singlet – triplet splitting
The basic law of photochemistry: only absorbed radiation can cause
chemical change
spectroscopic transitions are quantized - line spectra (in gas phase at low pressure), band spectra (in condensed phases)
Absorption
E
S S1 S2 T1 T2
Lambert – Beer law
I = I0 10-εcl
ε: decadic absorption coefficient
unit: dm3mol-1cm-1
T = I/I0 T(%) = 100 I/I0
A = -lg T = lg (1/T) = lg I0/I = εcl
Typical absorptions
n → * carbonyls, tiocarbonyls, nitro-, azo- and imino- group containing compounds
→ * alkenes, alkynes, aromatics
n → * amines, alcohols, haloalkanes
→ * alkanes
Absorption
S S1 S2 T1 T2
Vibrational relaxation
E
S S1 S2 T1 T2
Deactivation channels of the singlet state
E
S S1 S2 T1 T2
?
Fluorescence: emissionwithout change of spin state
E
S S1 S2 T1 T2
IC: internal conversion
E
S S1 S2 T1 T2
ISC: intersystem crossing(spinváltó átmenet)
E
S S1 S2 T1 T2
Phosphorescence: emissionwith change of spin state
E
S S1 S2 T1 T2
Quenching
Deactivation of an excited state with the help of another species. We investigate the process from the point of view of the excited species, the state of the quencher is irrelevant.
Deactivation channels of the excited singlet state
1M
M + h` kfl
M kIC3M kISC
M (+ Q or Q*) kq+Q
Miso or M` + M`` kmr
MA or M+ + A- kbr
+A
MAQ]M[ 1
1
brmrqISCICfl kkkkkkdt
d
3M
M + h`` kph
M kISC`
M (+ Q or Q*) kq+Q
Miso or M` + M`` kmr
MA or M+ + A- kbr
+A
MAQ]M[ 3
`
3
brmrqISCph kkkkkdt
d
Deactivation channels of the triplet state
Quantum efficiency
= number (rate) of chosen process
number (rate) of photons absorbed Mk
Mk
channelsdeactii
flfl
1
.
1
channelsdeacti
i.
1
channelsdeacttripletjj
phISCph k
k
..
channelsdeactii
flfl k
k
.
Quantum efficiency
1M
M + h` kfl
M kIC3M kISC
M (+ Q or Q*) kq+Q
Miso or M` + M`` kmr
MA or M+ + A- kbr
+A
channelsdeactii
flfl k
k
.
Stern-Volmer plot
k
Qk
k
Qkk
k
k
I
I
Qkk
k
q
fl
qfl
fl
fl
q
flfl
1
I
0
fl
1
I0/I
[Q]
Energy transfer
• Through radiation (trivial)
• Without radiation– long-range, coulomb-interaction (Förster)– short-range, electron-exchange (Dexter)
Trivial energy transfer
Condition: the emission spectrum of the donor and absorption spectrum of the acceptor must overlap.
Long-range dielectric interaction
The rate is proportional to the -6th power of the distance between donor and acceptor
Short-range, electron exchange interaction
The rate is proportional to (e-r/l)2, r: the distance between donor and acceptor, l: van derWaals distance
Triplet-triplket energy transferPHOTOSENSITIZATION