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Femtosecond energy transfer in LHCII of green plants

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Title: Femtosecond energy transfer in LHCII of green plants


1
In vivo regulation of photocurrents
Herbert van Amerongen
Herbert van Amerongen Laboratory of
Biophysics Wageningen
2
Photosynthesis occurs in the chloroplasts of
green plants
3
The complexes of the thylakoid membrane
4
Absorption properties of the photosynthetic
pigments
S2
Qy
5
Absorption
Vibronic excited states
Electronic excited state
Absorption 6 fs
Electronic ground state
6
Decay of the excited state
Vibronic excited states
Electronic excited state
Internal conversion to the lowest excited
state ( 100 fs) Energy lost as heat
Electronic ground state
7
Decay of the excited state
Vibronic excited states
Electronic excited state
Internal conversion to the electronic ground
state (IC) Energy lost as heat
Electronic ground state
kIC 0.02 ns-1 tIC 50 ns
8
Decay of the excited state
Vibronic excited states
Electronic excited state
Decay by emission of a photon Energy lost as
fluorescence
Electronic ground state
kF 0.06 ns-1 tF 17 ns
9
Decay of the excited state
Electronic excited state
Decay to the triplet state (T) (Intersystem
crossing)
1 ms
Electronic ground state
kT 0.125 ns-1 tIT 8 ns
10
Lifetime of the excited state
t (k)-1 (kF kIC kT)-1
11
Decay of the excited state 2e
Vibronic excited states
Electronic excited state
Electron transfer to nearby molecule
Electronic ground state
Molecule 1
Molecule 2
12
carotenoids in plant photosynthesis
13
Carotenoid Absorption Spectra
S2 ? S0
14
(No Transcript)
15
Femtoseconde pump-probe
16
Femtoseconde pump-probe
17
Femtoseconde pump-probe
18
Femtoseconde pump-probe
19
LHCII energy transfer from carotenoids to Chl
20
(No Transcript)
21
  • Energy transfer from Chl b and Car to Chl a is
    ultrafast
  • Car and Chl need physical contact for energy
    transfer
  • Almost all the excitations are localized on Chl a
  • Energy transfer to the reaction center occurs via
    Chls a

22
Photosystems I and II are separated in the
thylakoid membrane
PSII and LHCII.
PSI.
23
Photosystems I and II can be studied separately
PSII and LHCII.
PSI.
We used BBY particles, no PSI present
24
Photosystem 2 (PSII)
PS2-LHC2 supercomplex
25
Picosecond fluorescence reveals excited-state
dynamics in PSII membranes
Excitation at 420 nm and 483 nm lead to different
extent of excitation of the outer antenna 68
and 86
Dt
26
Charge separation in PSII in the membrane
35 ps
5.3 ps
e-
5.5 ps
-
Antenna
DG 826 cm-1
e-
137 ps
e-
27
  • Excited-state lifetime of PSII in thylakoid
    membrane is around 300 ps

28
The destiny of the excited states
lt1
4
2
29
Triplet quenching in the antenna complexes LHCII
30
Triplet quenching in the antenna
10ms
1ns
31
Measure triplets with slow absorption
difference spectroscopy
  • Fast detector
  • Relatively more probe light than in a fs-ps
    experiment,

Ns laserpulse
?OD
Monochromator
Lamp
sample
Photomultiplieror photodiode
32
Triplets in LHCII
Peterman et al. 1995 Croce et al. 2007
33
525
507
510
490
L2
L1
Neoxanthin quenches singlet oxygen Violaxanthin
is available for xanthophyll cycle
34
3Chla
3Car
35
The other antenna complexes are protected in a
similar way
  • CP24, CP26 and CP29 act in the same way as LHCII
    (lutein and neoxanthin)
  • CP47 and CP43 use b-carotene

36
Two stages of photosynthesis
H2O
Chloroplast
ATP and NADPH
Water oxydation
The light is absorbed by chlorophylls
O2
Light reactions
Transformation of light energy into chemical
energy (ATP and NADPH)
37
If the photosynthetic apparatus gets saturated
somewhere (high light), this leads to blocking of
electron transfer in the RC ? Chl triplet
formation in the RC
38
There is no carotenoid in contact with Chl in
the RC
39
How to avoid photodamage in the RC?
  • The expression of light-harvesting complexes can
    be up- and down-regulated (hours)

40
State transitions
  • Only 15 of the LHC can migrate to PSI. Cyclic
    electron transfer around PSI contributes to
    proton gradient ATP formation can continue while
    PSII receives less photons.
  • State transitions are much more important in
    green algae (Chlamydomonas reinhardtii) gt80 of
    the LHC can migrate to PSI.
  • Phycobilisomes in cyanobacteria also participate
    in state transitions,

41
Light stress
chloroplast
chloroplast
NPQ
Heat production
Photosynthesis
Heat production
Photosynthesis
42
Nonphotochemical quenching (NPQ) acts on a
second-minute time scale throw away excess
energy as heat
43
NPQ
  • Required DpH across thylakoid membrane (result
    of extensive charge separation)
  • PsbS can sense the low pH in the lumen via
    protonation (direct quencher or allosteric
    regulator)
  • Low pH in the lumen creates zeaxanthin (Zea) via
    the xanthophyll cycle (direct quencher or
    allosteric regulator)

44
PsbS belongs to lhc family, binds no Chls,
becomes protonated when lumen has low pH
45
Xanthophyll cycle leads to Zea formation at low
pH in the lumen
46
Is zeaxanthin a direct quencher of excitations?
  • Carotenoids with 11 conjugated bonds can quench
    Chl excitation via excitation energy transfer,
    whereas carotenoids with 9 conjugated bonds
    cannot.
  • R. Berera et al. (2006) Proc. Natl. Acad. Sci
    USA 103 5343

47
THE SYSTEM
A zinc Phthalocyanine covalently attached to a
series of carotenoids with conjugation length of
9,10 and 11.
Absorption in THF
48
THE EXPERIMENT
dyad 1, dyad 2 and dyad 3
Solvents
THF(e07.58), Acetone(e020.6), DMSO(e040.5)
We probe the visible (450-730 nm) and n-IR
regions (850-1000 nm) at different time delays (0
4.8 ns)
We pump the system at 680 nm (Qy
state of Pc)
excitation frequency 1 Khz width 100
fs energy 100 nJ/pulse
Objectives
Can a carotenoid directly quench the singlet
exited state of a Pc-based tetrapyrrole?
How does the process depend on the conjugation
length?
What is the underlying quenching mechanism?
49
KINETIC TRACES AT 680 nm IN THF
50
QUENCHING MODEL
Qy
slow
S1
ICT
fast
S0
S0
phtalocyanine
carotenoid
51
But zeaxanthin can also quench via electron
transfer
  • N.E. Holt et al. (2005) Science 307 433.

52
NPQ consists of rapid (seconds) qE (no Zea
required) and slower (minutes) qI (Zea required)
Picture from Peter Horton
53
LHCII can switch between 2 states
light-harvesting
Heat producing
54
Fluorescence quenching by pressure (4 kbar)
?Vqn 510-6 m3/mol 0.006 ? small
conformational change ?G0qn 7 kJ/mol 3
kT/LHCII
55
LHCII aggregation as a model system
56
FLIM of LHCII
Raman shows that crystal is similar to quenched
aggregates
LHCII in crystal is quenched as compared to LHCII
in detergent
Pascal et al. 2005, Nature 436, 134-137
57
Switching behavior in vivo
Nature (next week) A.V. Ruban et al. (2007)
Nature 450 575.
58
Upon aggregation, excitations decay via a Car S1
state (femtosecond pump-probe spectroscopy)
A.V. Ruban et al. (2007) Nature 450 575
59
Target analysis reveals the spectrum of the
quencher
60
proposed molecular model (LHCII)
61
Interactions Chl612/Lut620 are also present in
CP24, CP26, CP29 (Croce et al.)
62
conclusions
  • Luteins 1 and 2 quench triplets in
    light-harvesting complexes in PSII
  • Neoxanthin quenches singlet oxygen
  • Violaxanthin is source for zeaxanthin formation
  • DpH leads to zeaxanthin formation (NPQ, qI)
  • PsbS senses DpH and is needed for NPQ (qE and qI)
  • Zeaxanthin can in principle also quench in other
    ways
  • LHCII is responsible for qE via lutein 1 and Chl
    612
  • CP24, CP26 and CP29 have an identical quenching
    cluster and probably also participate in qE

63
Other systems
  • Diatoms have NPQ like higher plants but stronger
  • Cyanobacteria less NPQ (OCP and state
    transitions)
  • Green algae less NPQ, more state-transitions
  • Green bacteria Chlorosomes triplet excitons

64
Coworkers and collaborators
Wageningen Bart van Oort Koen Broess
Sashka Krumova Arie van Hoek Cor Dijkema
Jan Willem Borst Vilnius Gediminas
Trinkunas Leonas Valkunas Amsterdam Jan
Dekker Rienk van Grondelle Rudi
Berera Groningen Roberta Croce Szeged
Gyozo Garab
Sheffield Peter Horton Marseille Stefano
Caffarri London Jim Barber Alexander
Ruban Tel Aviv Nathan Nelson Verona
Roberto Bassi Saclay/Paris Bruno Robert
Andy Pascal Frankfurt Werner Kuhlbrandt
.A Ground state, B Excited state, C, D E
States reached after charge separation and
charge stabilization
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