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Peridinin-chlorophyll-protein reconstituted with chlorophyll mixtures: Preparation, bulk and single molecule spectroscopy

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Reconstitution of the 16 kDa N-terminal domain of the peridinin-chlorophyll-protein, N-PCP, with mixtures of chlorophyll a (Chl a) and Chl b, resulted in 32 kDa complexes containing two pigment clusters, each bound to one N-PCP. Besides homo-chlorophyllous complexes, hetero-chlorophyllous ones were obtained that contain Chl a in one pigment cluster, and Chl b in the other. Binding of Chl b is stronger than that of the native pigment, Chl a. Energy transfer from Chl b to Chl a is efficient, but there are only weak interactions between the two pigments. Individual homo- and hetero-chlorophyllous complexes were investigated by single molecule spectroscopy using excitation into the peridinin absorption band and scanning of the Chl fluorescence, the latter show frequently well resolved emissions of the two pigments.
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Peridinin–chlorophyll–protein reconstituted with chlorophyll
mixtures: Preparation, bulk and single molecule spectroscopy
T.H.P. Brotosudarmo
a,b
, E. Hofmann
c
, R.G. Hiller
d
,S.Wo
¨rmke
b
, S. Mackowski
b
,
A. Zumbusch
e
, C. Bra
¨uchle
b
, H. Scheer
a,*
a
Department Biologie I Bereich Botanik, Ludwig-Maximilians-Universita
¨tMu
¨nchen, Menzinger Str. 67, D-80638 Mu
¨nchen, Germany
b
Department Chemie und Biochemie Physikalische Chemie, and Center for Nanoscience, Ludwig-Maximilians Universita
¨t, Mu
¨nchen, Germany
c
Fakulta
¨tfu
¨r Biologie, Biophysik, Ruhr Universita
¨t Bochum, Germany
d
Macquarie University, Sydney, Australia
e
Fachbereich Chemie, Universita
¨t Konstanz, Germany
Received 23 July 2006; revised 21 August 2006; accepted 24 August 2006
Available online 5 September 2006
Edited by Miguel De la Rosa
Abstract Reconstitution of the 16 kDa N-terminal domain of
the peridinin–chlorophyll–protein, N-PCP, with mixtures of
chlorophyll a(Chl a) and Chl b, resulted in 32 kDa complexes
containing two pigment clusters, each bound to one N-PCP.
Besides homo-chlorophyllous complexes, hetero-chlorophyllous
ones were obtained that contain Chl ain one pigment cluster,
and Chl bin the other. Binding of Chl bis stronger than that
of the native pigment, Chl a. Energy transfer from Chl bto
Chl ais efficient, but there are only weak interactions between
the two pigments. Individual homo- and hetero-chlorophyllous
complexes were investigated by single molecule spectroscopy
using excitation into the peridinin absorption band and scanning
of the Chl fluorescence, the latter show frequently well resolved
emissions of the two pigments.
2006 Federation of European Biochemical Societies. Published
by Elsevier B.V. All rights reserved.
Keywords: Photosynthesis; Light-harvesting; Chlorophyll;
Carotenoid; Energy transfer; Single molecule spectroscopy
1. Introduction
Peridinin–chlorophyll–proteins (PCP) are water-soluble
light-harvesting complexes from dinoflagellates [1]. The native
complex from Amphidinium (A.) carterae is a homotrimer. The
boat-shaped, a-helical protomer is the 32 kDa large PCP
(l-PCP). It has an approximate C
2
-symmetry containing two
clusters of pigments, each consisting of one chlorophyll a
(Chl a) that is nested between two pairs of peridinins (Per)
[2]. The pigments in each cluster are in Van der Waals contact.
There is also contact between Per molecules from the two clus-
ters, while the center-to-center distance of the two Chl is
17.4 A
˚. Small PCP (s-PCP) of half the size (16 kDa) of the
A.carterae complex which contain a single Per
4
–Chl acluster,
has been found in several species including Heterocapsa pyg-
maea [3]. These s-PCP dimerize, resulting in a similar topology
as the monomeric protomers from A.carterae [4]. An analo-
gous aggregate is also formed by the 16 kDa N-terminal
domain of PCP from A.carterae (N-PCP) reconstituted with
Chl aand Per [5]
1
.
Tight clustering, an exceptionally high carotenoid-Chl ratio,
and the presence of a highly modified carotenoid, Per, with an
unusually long-lived S
1
-state [6] render the PCPs a challenge to
understand pigment interactions and excitation energy transfer
(EET). Pairing of Per and a close spacing of the pigments had
been inferred already in 1976 from circular dichroism (CD)
spectra of PCP [7]. Moderately strong excitonic coupling
among the pigments within a cluster was also supported by
simulations of the CD and absorption spectra, which were
based on the X-ray structure [8]. However, the details are still
controversial and may require contributions from inter-cluster
interactions. Rapid fluorescence depolarization (7 ps) has been
assigned to intra-monomer EET between the Chls, a much
slower component (350 ps) to Fo
¨rster type inter-monomer
EET transfer in PCP trimers from A.carterae [9]. EET from
Per to Chl has been studied using N-PCP that have been recon-
stituted with different Chls [10], the results support theoretical
predictions [11] of a major contribution of the relatively long-
lived S
1
-state of Per [6,12,13] as donor to the Chls. The contri-
butions of the different Per excited states have been reviewed
[14]; the S
1
-state is stabilized by symmetry breaking and by
intra-Per charge-transfer [6,13,15].
The high carotenoid content and relatively small Chl–Chl
interactions also render PCP a candidate to study EET
between two Chls in a structurally well-known situation that
is relatively simple as compared to other photosynthetic sys-
tems. In this context, it is desirable to study PCP containing
two different, spectrally separated Chls [5]. Here, we report
on such complexes prepared by reconstitution of N-PCP from
Abbreviations: A.,Amphidinium; CD, circular dichroism; Chl, chloro-
phyll; EET, excitation energy transfer; l-PCP, large (32 kDa PCP);
N-PCP, N-terminal 16 kDa-domain of PCP; PCP, peridinin–chloro-
phyll–protein; Per, peridinin; s-PCP, small (16 kDa) PCP; SMS, single
molecule spectroscopy
*
Corresponding author. Fax: +49 89 17861 271.
E-mail address: hugo.scheer@lmu.de (H. Scheer).
1
The term ‘monomer’ is used here in a topological context, referring
to l-PCP from A.carterae from which the X-ray structure has been
solved. l-PCP is a 32 kDa protein, it originates from a gene duplication
and binds two Chl/Per clusters. For historical reasons, this species is
generally referred to as the PCP monomer. With respect to this l-PCP
monomer, the 16 kDa s-PCP discovered subsequently, as well as N-
PCP generated from the A.carterae protein, are topologically ‘‘half-
mers’’: they carry only a single Chl/Per
4
cluster, and dimerize to species
that are homologous to the l-PCP monomer.
0014-5793/$32.00 2006 Federation of European Biochemical Societies. Published by Elsevier B.V. All rights reserved.
doi:10.1016/j.febslet.2006.08.049
FEBS Letters 580 (2006) 5257–5262
A.carterae with Chl aand Chl b. The procedure yields dimeric
aggregates that correspond topologically to l-PCP monomers
1
,
and are mixtures with respect to their pigment composition:
besides homo-chlorophyllous Chl a/Chl aand Chl b/Chl b
complexes, the preparation yields hetero-chlorophyllous com-
plexes containing Chl ain one cluster and Chl bin the other.
While these complexes could not be separated by chromato-
graphy, identification of the hetero-chlorophyllous complexes
and their investigation was possible by difference spectroscopy,
and by single molecule spectroscopy (SMS).
2. Materials and methods
2.1. Materials
Trimeric PCP was isolated from A. carterae [2]. The N-terminal do-
main of the apoprotein (N-PCP) was obtained as published [5]. Per was
extracted from A. carterae as published [6]. Chl awas extracted from
spray-dried Spirulina geitleri, Chl bfrom the Chl a/bmixture extracted
from frozen spinach, and purified over DEAE cellulose [16].
2.2. Reconstitution
Reconstitution followed the protocol of [5]. 625 ll apo-N-PCP
(20 lM) in tricine buffer (50 mM, pH 8.0) were combined with
225 ll tricine buffer (50 mM, pH 7.6) containing KCl (10 mM). An
ethanolic solution (150 ll) of Per (80 lM) and Chl a(or b) (20 lM)
was added, the mixture incubated at 4 C for 48 h, and the crude
reconstitution product purified over a small DEAE Tris–acryl col-
umn (5 ·25 mm, tricine buffer (5 mM, pH 7.6, 2 mM KCl), NaCl
step gradient 100, 200 and 500 mM). Fractions containing the recon-
stituted complex (100 mM NaCl) were dialyzed against the starting
buffer.
2.3. Spectroscopy
Absorption spectra were recorded with a Lamda 2 spectrophotome-
ter (Perkin–Elmer), bulk fluorescence excitation and emission spectra
with a model LS55 spectrofluorimeter (Perkin–Elmer), and circular
dichroism spectra with a model J810 spectropolarimeter (Jasco). All
measurements were done at room temperature. Data were transferred
to Origin 6.0 (Microcal) for further analysis. Chl aand Chl bextinction
coefficients in the reconstitution system were determined relative to the
known ones in acetone [17]. The respective pigment was dissolved in
acetone, and an absorption spectrum recorded. The solvent was then
evaporated in a stream of Ar, the pigment re-dissolved in the same vol-
O
COCH3
o
OO
O
OH
R
Mg
O
N N
N N
H
H
COOCH3
H
COOC20H39
Fig. 1. Molecular structures of the cofactors of the PCP complex. Top: Per and Chl ain the two pigment clusters of a PCP monomer from A.
carterae ([2], pdb entry 1PPR) are shown as orange and green bold stick models, the two lipids as wire models, using DS ViewerPro V5 (Accelrys).
The center-to-center (Mg–Mg) distance of the Chls is 17.3 A
˚. Chemical structures of Per (center) and of Chl a(R = CH
3
) and Chl b(R = CHO)
(bottom).
5258 T.H.P. Brotosudarmo et al. / FEBS Letters 580 (2006) 5257–5262
ume of the buffer system by first adding the appropriate amount of eth-
anol and the aqueous components, and then the absorption was re-
corded again (see Fig. 1).
Single molecule spectra were obtained using a modified scanning
confocal microscope (ZEISS LSM 410). Fluorescence spectra of single
immobilized complexes were recorded after excitation into the Per
absorption (532 nm). Fluorescence emission in the spectral range from
575 to 725 nm was dispersed with a Amici-prism and projected onto a
CCD camera (Princeton Instruments). Typical integration times were
0.3 s with a spectral resolution of 1.5 nm. Further details will be de-
scribed in a paper dedicated to single molecule spectroscopy of PCP
[24].
3. Results and discussion
Reconstitution [10] of N-PCP from A.carterae with Chl a
(1.1 moles/mole protein) and Per (4.4 moles/mole protein) re-
sults in hetero-chlorophyllous complexes as evidenced by their
optical spectra (see below). Quantitatively, the pigment ratios
in the reconstituted and purified complexes were determined
spectroscopically [18], after dilution into acetone to a 20:80
water/acetone ratio. The Chl a/bratio is decreased from 1:1
in the reconstitution mixture to 43/57 in the purified complex,
indicating a slight preference for the non-natural pigment, viz.
Chl b. Chls with CO groups at C-3 and C-7 have been
bound before to N-PCP [5]. In the X-ray structure, the region
around C-7
1
carrying the carbonyl-oxygen in Chl b, has two
hydrophilic groups nearby that could assist binding: a ring-N
of His66 (3.8 A
˚) and a backbone C=O of Ala-63 (5.1 A
˚)[2].
Binding of Chl bis, however, even possible in relatively hydro-
phobic environments [19,20].
Absorption and circular dichroism. The homo-chlorophyllous
N-PCP complex containing only Chl ahas absorption and CD
spectra (Fig. 2B) that are similar to those of native l-PCP from
the same organism (Fig. 2A), the spectra of the latter are iden-
tical to the ones of PCP reported before [8]. However, the
negative CD-band of Per peaking around 530 nm is slightly
red-shifted and broadened in Chl a–N-PCP as compared to
native l-PCP. The CD-spectrum of both complexes is domi-
nated by an intense, s-shaped band system peaking at 530
() and 445 (+), with the zero-crossing near the absorption
maximum of peridinin. Superimposed on the positive lobe of
this signal is a much smaller and narrower, s-shaped band sys-
tem that is centered near the absorption maximum of Chl a. Its
negative lobe shows as a dip in the intense positive Per band,
0.00
0.02
0.04
0.06
0.08
0.10
0.12
0.00
0.05
0.10
0.15
0.20
0.25
0.00
0.05
0.10
0.15
0.20
0.25
400 500 600 700
0.00
0.05
0.10
0.15
0.20
0.25
-20
-15
-10
-5
0
5
10
15
20
669
474
437
437 474
670
460
648
460
668
427460
444
529
673
427458
443
531
672
443
485
467 525
649
Absorbance [a.u.]Absorbance [a.u.]Absorbance [a.u.] Absorbance [a.u.]
A: l-PCP
B: Chl
a
-N-PCP
C: Chl
b
-N-PCP
Wavelen
g
th [nm]
441
650
D: Chl
a/b
-N-PCP
AL-AR [Milidegrees]
-30
-20
-10
0
10
20
30
AL-AR [Milidegrees]
-30
-20
-10
0
10
20
30
AL-AR [Milidegrees]
400 500 600 700
-30
-20
-10
0
10
20
30
AL-AR [Milidegrees]
Wavelen
g
th [nm]
428
441
447
468
483
530
649
661
669
Fig. 2. Absorption (left) and circular dichroism spectra (right) of (A) native PCP, and of RPCP reconstituted with Chl a(B); Chl b(C) and a 1:1
mixture of Chl aand Chl b(D).
T.H.P. Brotosudarmo et al. / FEBS Letters 580 (2006) 5257–5262 5259
that is located 7 nm to the red of the Chl aabsorption max-
imum (437 nm). The positive lobe is discernible as a distinct
peak in the largely unstructured Per band, located 10 nm to
the blue of the Chl aabsorption maximum. There is no such
splitting for the Q
Y
-band of Chl aat 672 nm. The major
band of Chl ain the Soret-region is the B
x
-band [21,22]. Since
the orientation factors are similar for the x- and y-polarized
transitions, the lack of a split Q
Y
CD-signal indicates that
the split Soret CD-signal is not due to excitonic interactions
among the Chls of adjacent pigment clusters, but results
mainly from coupling with Per within a single cluster [4,8].
Reconstitution with Chl binstead of Chl ayields a complex
with a blue-shifted Q
y
band of the Chl and a red-shifted Soret
band (Fig. 2C), these shifts are similar to those of Chl avs. Chl
bin acetone. The red-shifted (460 nm) and more pronounced
Soret band reflects the larger extinction coefficient of Chl b
as compared to Chl a[23]. Accordingly, the absorption of
the Chl bcomplex is dominated by the latter (460 nm). The
s-shaped CD signal in the Soret region is also much more
prominent than in the Chl a-containing complex, as shown
already by Miller et al. [5]. The zero-crossing of the intense,
s-shaped feature is close to the Chl babsorption maximum.
The Q
y
-band shows, like in the Chl acomplex, no splitting;
this further supports [4,8] that excitonic interactions of the
Chls occur mainly with Per.
The spectrum of the hetero-chlorophyllous complex
(Fig. 2D) is superficially a mixture of the ones of the homo-
chlorophyllous complexes. However, a closer inspection re-
veals differences, that are likely due to Chl a/Chl binteractions.
(i) The Chl b-related Q
y
-CD band at 649 nm is stronger than
that of Chl aat 669 nm, while based on the homo-chlorophyl-
lous complexes (Fig. 2, see also [5]) and the Chl a/b-ratio of 43/
57 (see above), at most equal intensities are expected. (ii) The
red absorption and CD-bands of Chl aare blue-shifted by
2 nm in the Chl a/bcomplex as compared to the Chl a only
sample (Fig. 2A). (iii) Subtraction of the absorption spectra of
the homo-chlorophyllous Chl a–N-PCP or Chl b–N-PCP com-
plex from that of the hetero-chlorophyllous complex always
gave additional bands (Fig. 3). It should be noted that the sit-
uation could be further complicated by the possibility that
there are mono-chlorophyllous complexes, in which one bind-
ing site is empty, and by the presence of ‘‘half-mers’’
1
carrying
only a single Chl/Per
4
cluster. However, these are unlikely
based on the tight pigment binding and dimerization of indi-
vidual N-PCP, and were not considered here. Fluorescence
spectroscopy of bulk samples gave likewise inconclusive results
(data not shown).
The emission spectra of the hetero-chlorophyllous complex
show one major peak at 673 nm and a smaller one at
652 nm, corresponding to emissions from Chl aand Chl b,
respectively (Fig. 4). The excitation spectrum for the shorter-
wavelength emission shows, accordingly, mainly contributions
of Per and Chl b. The excitation spectrum for the long-wave-
length peak has contributions from Per (k
max
505 nm), Chl
b(k
max
= 463 nm) and Chl a(k
max
= 437 nm). This clearly indi-
cates inter-cluster energy transfer from Chl bto Chl ain the
hetero-chlorophyllous N-PCP complex. Assuming that the
pigment geometry is similar to that in the l-PCP monomer,
and the separation of the two emission bands corresponds to
the equilibrium energy difference between Chl aand Chl b; rel-
ative contributions of 6.1:1 can be estimated for the emissions
of Chls aand b, respectively. This value was estimated in the
following way: Boltzmann equilibrium (n
Chl a
/n
Chl b
=
exp(-DE/kT) between the two emittors (673 and 651 nm,
respectively) results, at a temperature of 298 K, in relative pop-
ulations of 10.1:1. Since the fluorescence results from a mixture
of species consisting of the homo-chlorophyllous complexes,
(Chl a)
2
–N-PCP and (Chl b)
2
–N-PCP, and the hetero-chloro-
phyllous complex, Chl a/b–N-PCP, contributions from the
three components have to be summed. Their relative popula-
tions were estimated assuming a random distribution of Chls
aand bin the experimentally determined pigment ratio of
43:57 (see above), resulting in relative populations of 18.5%,
32.5% and 49%. Finally, the emission of Chl bwas corrected
by the relative fluorescence yield of 0.45 [5] of Chl b–N-PCP
compared to Chl a–N-PCP. The experimentally obtained Chl
a/bemission ratio, determined from the data in Fig. 4 by
0.00
0.02
0.04
0.00
0.02
0.04
600 650 700 750
0.00
0.02
0.04
Absorbance [a.u.]
C
B
Absorbance [a.u.]
A
Wavelength [nm]
Absorbance [a.u.]
Fig. 3. Comparison of homo- and hetero-chlorophyllous N-PCP
complexes. Absorption spectra of Chl a/b–N-PCP (—) and absorption
differences (- - - -) with the spectra of Chl a–N-PCP (A), Chl b–N-PCP
(B) and the sum of Chl a–N-PCP and Chl b–N-PCP (C). The
subtracted homo-chlorophyllous spectra are shown as dotted lines,
they were scaled to give minimum deviation in the region of the
respective Chls.
400 500 600 700
0
3000
6000
9000
Intensity
Wavelength [nm]
λem = 650 nm
λem = 670 nm
λexc = 500 nm
Fig. 4. Fluorescence of reconstituted Chl a/b–N-PCP complex; emis-
sion (k
exc
= 500 nm, ) and excitation spectra (k
em
= 650 nm,
;k
em
= 670 nm, ). Excitation spectra were normalized
to the Per maximum near 505 nm.
5260 T.H.P. Brotosudarmo et al. / FEBS Letters 580 (2006) 5257–5262
Gaussian deconvolution, is 4.7. This is somewhat lower than
the estimated theoretical value of 6.1, but indicates nearly
complete equilibration between the two Chls in the Chl a/b-
complex. A more detailed analysis is difficult, however, consid-
ering the aforementioned interactions among the Chls, whose
contributions are difficult to estimate, and the assumptions
used in the analysis.
The Chl aemission of the hetero-chlorophyllous complex
(671 nm) is red-shifted by 2 nm compared to the Chl a only
complex. Minor but reproducible shifts are also seen in the
Soret-region. Likewise there were minor shifts in the Chl b-
bands when comparing the hetero-chlorophyllous complex
with that of the one containing only Chl b. All these shifts
point to small, but distinct Chl–Chl interactions between the
Chls in the two clusters.
Proof that hetero-chlorophyllous complexes are indeed
formed can be obtained by investigations of single complexes.
Therefore we recorded room temperature spectra of individual
complexes obtained from the N-PCP reconstitution with Chls
aand b[24]. After excitation at (532 nm) where absorption is
dominated (>90%) by Per, the detected fluorescence of the
Chls (k> 600 nm) originates predominantly from energy trans-
fer. Several hundred molecules of all three reconstituted
complexes have been investigated in this fashion. Most of them
can be grouped by their emission spectra into three types of
complexes. In the case of homo-chlorophyllous complexes, a
single line was observed, as displayed in the first and second
row in Fig. 5. The complexes containing only Chl ashow nar-
row emission lines centered around 670 nm, while the fluores-
cence emission measured for those containing only Chl bis
600 650 700 750
Intensity
600 650 700 750
Chl
b
-N-PCP
Intensity
600 650 700 750
Intensity
600 650 700 750
Intensity
Wavelength [nm]
600 650 700 750
Chl
a/b
-N-PCP
Intensity
Wavelength [nm]
600 650 700 750
Intensity
Wavelen
g
th [nm]
600 650 700 750
Intensity
600 650 700 750
Chl
a
-N-PCP
Intensity
Intensity
600 650 700 750
Fig. 5. Ambient temperature single molecule fluorescence spectra. Three different complexes each (k
exc
= 532 nm) of N-PCP reconstituted with Chl a
(top); Chl b(center) and a 1:1 mixture of Chl aand Chl b(bottom). The lines at 675 nm are drawn to guide the eye. The baselines were recorded at the
same position, after bleaching of the sample.
T.H.P. Brotosudarmo et al. / FEBS Letters 580 (2006) 5257–5262 5261
characterized by somewhat broader lines centered around
650 nm. The most interesting spectra are the ones measured
for the hetero-chlorophyllous complexes, shown in the bottom
row. These systems show a broadened and often split emission
composed of two lines attributed to Chl a(670 nm) and Chl b
(650 nm). The contribution from the short-wavelength com-
ponent, associated with Chl bemission, is in many cases con-
siderably larger than expected for an equilibrated emission (see
above), it is even dominant in one of the samples shown. While
details of the energy transfer in individual complexes are cur-
rently analyzed, the observed emission of both Chl aand
Chl bfrom single complexes unambiguously demonstrates
the successful production of hetero-chlorophyllous complexes.
Acknowledgements: Work was supported by the Deutsche Forschungs-
gemeinschaft, Bonn (SFB 533, projects A6 and B7). T.H.P.B. is
indebted for a stipend from the Evangelischer Entwicklungsdienst,
Bonn. S.M. acknowledges financial support from the Alexander-von-
Humboldt Foundation, Bonn.
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... The PCP monomer folds into two symmetrical domains, the Nand C-terminal domains. Each domain forms a hydrophobic cavity occupied by one Chl a molecule nested between four peridinin molecules (Hofmann et al. 1996) with a centreto-centre distance of the two Chl equal to 17.4 Å (Brotosudarmo et al. 2006). ...
... It is worth noting that the energy transfer could go from peridinin to all Chl species, and from Chl a to Importantly, our results show that Chl f is incorporated into N-PCP complexes and that these complexes are stable independently of whether other Chl species are added into the reaction or after the Chl f complexes have been formed. It is known that the kinetics of the complex formation varies between Chl species being faster for Chl b than that for Chl a (Brotosudarmo et al. 2006;Miller et al. 2005). This might explain the different results observed in the combining Chl species experiments. ...
Article
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Chlorophyll f is a new type of chlorophyll isolated from cyanobacteria. The absorption and fluorescence characteristics of chlorophyll f permit these oxygenic-photosynthetic organisms to thrive in environments where white light is scarce but far-red light is abundant. To explore the ligand properties of chlorophyll f and its energy transfer profiles we established two different in vitro reconstitution systems. The reconstituted peridinin-chlorophyll f protein complex (chlorophyll f-PCP) showed a stoichiometry ratio of 4:1 between peridinin and chlorophyll f, consistent with the peridinin:chlorophyll a ratio from native PCP complexes. Using emission wavelength at 712 nm, the excitation fluorescence featured a broad peak at 453 nm and a shoulder at 511 nm confirming energy transfer from peridinin to chlorophyll f. In addition, by using a synthetic peptide mimicking the first transmembrane helix of light-harvesting chlorophyll proteins of plants, we report that chlorophyll f, similarly to chlorophyll b, did not interact with the peptide contrarily to chlorophyll a, confirming the accessory role of chlorophyll f in photosystems. The binding of chlorophyll f, even in the presence of chlorophylls a and b, by PCP complexes shows the flexibility of chlorophyll-protein complexes and provides an opportunity for the introduction of new chlorophyll species to extend the photosynthetic spectral range.
... Total chlorophyll/carotenoids were proposed to be a good indicator of plant stress (Hendry and Price, 1993;Ahmed et al., 2021). Although carotenoids are important pigments to absorb light energy for use in photosynthesis and to protect chlorophyll from photo-damage (Armstrong, 1996), chlorophyll, especially chlorophyll a, is the main component of light reaction center which receive the light energy from carotenoids and chlorophyll b (Brotosudarmo et al., 2006;Akimoto and Mimuro, 2007). Therefore, the stable chlorophyll level and decreased carotenoids from our study implied that maize seedlings intend to trade off the secondary pigment to ensure the main pigment level and thereafter to protect the core function of photosynthesis against ZnO NPs treatment, finally to cope with the negative stress induced by ZnO NPs. ...
... The proteins used in this work were obtained by reconstituting apoproteins with pigments, using a protocol developed previously. 15 The optical properties of the PCP complexes have been studied and discussed previously. 16,17 While the absorption of PCP extends from 350 nm to 660 nm, enabling easy excitation of electronic transitions, the emission at 673 nm is associated with the uorescence of chlorophylls. ...
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High-resolution fluorescence imaging together with spectrally- and time-resolved analysis indicates a strong dependence of the energy transfer efficiency to graphene on the number of graphene layers. By correlating intensity and decays of emission, we found that energy transfer is the most efficient for single layer graphene, and reaches 89%. In contrast, for structures with more graphene layers (from 2 to 7), a substantial drop in energy transfer efficiency is observed. The results clearly show that the number of graphene layers, in addition to the distance between emitters and graphene as well as the excitation energy, is key parameter which can be used to control the acceptor properties of graphene in hybrid nanostructures.
... Peridinin-chlorophyll-protein (PCP) photosynthetic complexes were obtained according to protocol developed by Miller et al. [13,14]. Briefly, PCP apoprotein in 50 mM Tris-HCl pH 8.0 solution was added to 25 mM Tricine and 10 mM KCl (pH 7.6), mixed with a stoichiometric amount of PCP pigments dissolved in ethanol. ...
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We demonstrate that SiO2 nanoparticles coated with a gold island film (GIF) provide an efficient plasmonic platform for enhancing fluorescence intensity of chlorophyll-containing photosynthetic complexes. Fluorescence images obtained for single SiO2-Au coreshell nanoparticles mixed with photosynthetic complexes reveal very uniform emission patterns of a circular shape, similarly as observed for bare SiO2 nanoparticles. The fluorescence enhancement of chlorophyll emission for SiO2-Au nanostructures is up to four-fold compared to bare SiO2 nanoparticles and shortening of fluorescence decay indicates its plasmonic origin. For doublets or triplets of core-shell SiO2-Au nanoparticles, the intensity of emission is further increased as a result of hot-spot formation at the interfaces of such assemblies.
... This feature leads to more detailed exploration of interdomain Chl-Chl energy transfer. The existence of RFPCP dimers with mixed Chl sites was also confirmed by single molecule spectroscopy (Brotosudarmo et al. 2006; al. 2007, 2008). Absorption spectra of two such complexes, containing either Chl b/Chl d pairs or Chl a/Bchl-a pairs within a single RFPCP homodimer, are shown in Fig. 3.9b. ...
Chapter
An important component of the photosynthetic apparatus is a light-harvesting system that captures light energy and transfers it efficiently to the reaction center. Depending on environmental conditions, photosynthetic antennas have adopted various strategies for this function. The water soluble antenna complex of dinoflagellates, peridinin–chlorophyll a protein (PCP), represents a unique light-harvesting strategy because, unlike other antenna systems which have a preponderance of chlorophyll, the carotenoid peridinin serves in PCP as the major light-harvesting pigment. The key structural feature of peridinin is a conjugated carbonyl group which makes the spectroscopic properties of peridinin very sensitive to its local environment. This property is a crucial factor for maintaining the high efficiency of energy transfer between peridinin and Chl a in PCP. PCP is also amenable to site-directed mutagenesis and reconstitution with different pigments, allowing to study effects of both pigment and amino acid exchange on energy transfer pathways within the complex. Since high resolution structures of native, reconstituted and mutated PCP complexes are now available, this knowledge provides an ideal platform to relate structural motifs to energy transfer pathways and efficiencies in PCP. This Chapter summarizes results of structural and spectroscopic investigations of PCP and related proteins, emphasizing the specific light-harvesting strategy developed by dinoflagellates.
Article
The nature of intramolecular charge transfer (ICT) and the mechanism of intramolecular singlet fission (SF) in peridinin remain open research questions. Obtaining an understanding of the population evolution from the bright state to dark states following a photoinduced electronic transition is critical. Unambiguously describing this evolution in peridinin, and light-harvesting carotenoids in general, has proven elusive experimentally and computationally. To offer a balanced description of bright- and dark-state electronic structure, we here apply ab initio multireference perturbation theory quantum chemistry—the density matrix renormalization group self-consistent-field (DMRG-SCF) and complete-active space self-consistent field (CASSCF) with second-order N-electron valence perturbation theory (NEVPT2). At traditional bright- (S2) and dark-state (S1) optimized geometries, we find that an additional correlated triplet pair (CTP) state and ICT state are derived from the canonical polyene Bu (S3) and 3Ag (S4) dark singlet excited states, respectively. While the S3 state’s physical properties are insensitive to peridinin’s allene-tail donor and lactone-ring acceptor functionalization, the S4 state exhibits a markedly enhanced oscillator strength and HOMO-LUMO transition density. These changes suggest that ICT character stems from mixing between the bright S2 and putatively dark S4.
Article
We investigate the influence of plasmonic excitations in silver nanowires upon the photostability of a photosynthetic complex placed at their vicinity. Strong interaction between the two nanostructures is evident through an increase in the fluorescence intensity of the photosynthetic complexes close to the nanowires as compared to uncoupled ones and shortening of the fluorescence lifetime. The analysis of collected films, examined through a wide-field fluorescence microscope, with respect to temporal intensity variations for photosynthetic complexes located along and at the ends of the nanowires, indicates that the photostability is unaffected by the interaction with plasmonic excitations in metallic nanoparticles. Therefore, we conclude that in the case of studied hybrid nanostructures coupling with metallic nanoparticles results in a higher number of photons emitted from chlorophyll molecules.
Chapter
Plasmon excitations in metallic nanoparticles provide elegant and effective means for manipulating the optical properties of emitters at the nanoscale. We describe several experimental results obtained for peridinin-chlorophyll-protein (PCP), an algal light-harvesting complex, coupled to metallic nanoparticles with varied morphology and thus plasmonic properties. These include spherical gold nanoparticles and silver nanowires. By combining fluorescence microscopy with spectrally and time-resolved fluorescence techniques, we demonstrate strong influence of plasmon excitations on the fluorescence of the light-harvesting complex. Depending on the actual geometry of a hybrid nanostructure, we can observe increase in fluorescence rate or increase in absorption or the combination of both processes. Fluorescence transients measured for the PCP complexes coupled to metallic nanoparticles indicate in most cases shortening of the fluorescence lifetime pointing toward modifications of radiative rate due to plasmonic interactions. The results can be applied for developing ways to plasmonically control the light-harvesting capability of photosynthetic complexes.
Conference Paper
Hybrid nanostructures consisting of silver nanowires and photosynthetic complexes were assembled and investigated by means of fluorescence microscopy and spectroscopy, both in continuous-wave and time-resolved modes. Coupling emitters with varied spectral characteristics to plasmonic excitations in silver nanowires resulted in strong increase of fluorescence intensity and shortening of the decay times. In most cases, the emission observed at the ends of the nanowires is higher than for emitters placed along them. Overall, the results of these experiments indicate that silver nanowires are quite unique metallic nanostructures that can be used for enhancing optical properties, guiding plasmons over relatively large distances, as well as affecting the energy transfer between organic molecules.
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Publisher Summary This chapter presents detailed information on chlorophylls and carotenoids to give practical directions toward their quantitative isolation and determination in extracts from leaves, chloroplasts, thylakoid particles, and pigment proteins. The chapter focuses on the spectral characteristics and absorption coefficients of chlorophylls, pheophytins, and carotenoids, which are the basis for establishing equations to quantitatively determine them. Therefore, the specific absorption coefficients of the pigments are re-evaluated. This is achieved by using a two-beam spectrophotometer of the new generation, which allows programmed automatic recording and printing out of the proper wavelengths and absorbancy values. Several procedures have been developed for the separation of the photosynthetic pigments, including column (CC), paper (PC), and thin-layer chromatography (TLC) and high-pressure liquid chromatography (HPLC). All chloroplast carotenoids exhibit a typical absorption spectrum that is characterized by three absorption maxima (violaxanthin, neoxanthin) or two maxima with one shoulder (lutein and β-carotene) in the blue spectral region.
Article
Full-text available
Abstract— Highly purified Chi a and b were prepared from spinach leaves in a short time by a combined use of the column chromatography with DEAE-Sepharose CL-6B and Sepharose CL-6B. The former chromatography eliminated carotenoids, phaeophytin and chlorophyllide, and the latter chromatography efficiently separated Chi a and b.
Chapter
Our knowledge of the diverse peripheral light-harvesting complexes (LHCs) found in species of algae which contain chlorophyll (Chi) c as an accessory pigment is reviewed. Sequencing of genes encoding intrinsic LHCs with three putative transmembrane helices is proceeding rapidly in all groups, but basic biochemistry, particularly of the LHC components attached to PS I-enriched complexes, is currently neglected. All LHCs appear to have two different environments for Chi c, and the longer wavelength forms (> 640 nm) have their Qy transition in the plane of the membrane, or the long axis of the particle. A limited amount of time-resolved spectroscopic data has been interpreted as excluding Chi c as an intermediate in energy transfer between either phycobilins or carotenoids and Chi a, but this may be premature. All the light-harvesting proteins seem to be encoded by multigene families, and for diatoms and brown algae, many genes have been sequenced. This will allow the role of individual gene products in determining the adaptive responses to environmental variation to be appraised.
Article
The molecular structure of the light-harvesting complex peridinin-chlorophyll-protein from the dinoflagellate Amphidinium carterae (A-PCP) provides the positions and orientations of the eight peridinin (Per) and two chlorophyll a (Chl) molecules in the complex whose apoprotein is 32 kD. We made structure-based calculations of the distinctive optical properties (absorption and CD spectra) of A-PCP and of the complex containing a ratio of four peridinin and one chlorophyll per complex (apoprotein ∼ 15 kD) obtained from the related species Heterocapsa pygmaea (H-PCP). The latter structure has not been determined but can be inferred from that of A-PCP. A point-monopole approximation was used to represent the low-energy transition of peridinin in the blue region of the spectrum and that of chlorophyll in the Soret region. Vibronic interactions are taken into account for peridinin because of the strong vibrational progression exhibited by the spectrum of the latter. From the calculations, we are able to simulate the absorption and CD spectra for H-PCP and A-PCP by using, in addition to the atomic coordinates taken from the A-PCP structure, one and only one set of parameters, adjusted for the small unit of four Per and one ChI common to both systems. In particular, the four peridinin site energies were assigned values in the range 18 500-19 500 cm-1, and those for the Bx and By transitions of chlorophyll a were given the common value 23 100 cm-1. The transition moments for peridinin were in the range 10.6-12.4 D, and those of the chlorophyll Bx and By transitions were 9.0 and 1.0 D, respectively. Each resolved vibronic transition was given the same Gaussian line width of 550 cm-1. Excitonic coupling among the different chromophores of the small cluster unit of the complex is not sufficient to describe the A-PCP optical properties. Intercluster interactions are necessary in order to reproduce the CD spectrum. The H-PCP spectrum, being practically identical to the former, is reproduced only if such interactions are maintained, meaning that the solution unit is a dimer of the monomeric polypeptide as previously inferred from the biochemical properties.
Article
The molecular structure of the light-harvesting complex peridinin−chlorophyll−protein from the dinoflagellate Amphidinium carterae (A−PCP) provides the positions and orientations of the eight peridinin (Per) and two chlorophyll a (Chl) molecules in the complex whose apoprotein is 32 kD. We made structure-based calculations of the distinctive optical properties (absorption and CD spectra) of A−PCP and of the complex containing a ratio of four peridinin and one chlorophyll per complex (apoprotein 15 kD) obtained from the related species Heterocapsa pygmaea (H−PCP). The latter structure has not been determined but can be inferred from that of A−PCP. A point−monopole approximation was used to represent the low-energy transition of peridinin in the blue region of the spectrum and that of chlorophyll in the Soret region. Vibronic interactions are taken into account for peridinin because of the strong vibrational progression exhibited by the spectrum of the latter. From the calculations, we are able to simulate the absorption and CD spectra for H−PCP and A−PCP by using, in addition to the atomic coordinates taken from the A−PCP structure, one and only one set of parameters, adjusted for the small unit of four Per and one Chl common to both systems. In particular, the four peridinin site energies were assigned values in the range 18 500−19 500 cm-1, and those for the Bx and By transitions of chlorophyll a were given the common value 23 100 cm-1. The transition moments for peridinin were in the range 10.6−12.4 D, and those of the chlorophyll Bx and By transitions were 9.0 and 1.0 D, respectively. Each resolved vibronic transition was given the same Gaussian line width of 550 cm-1. Excitonic coupling among the different chromophores of the small cluster unit of the complex is not sufficient to describe the A−PCP optical properties. Intercluster interactions are necessary in order to reproduce the CD spectrum. The H−PCP spectrum, being practically identical to the former, is reproduced only if such interactions are maintained, meaning that the solution unit is a dimer of the monomeric polypeptide as previously inferred from the biochemical properties.
Article
We present theoretical confirmation of an intramolecular charge-transfer (CT) state in peridinin in agreement with experimental results of Frank and co-workers (J. Phys. Chem. B 1999, 103, 8751 and J. Phys. Chem. B 2000, 104, 4569). Quantum chemical calculations using time-dependent density functional theory under the Tamm−Dancoff approximation were made on two structures:  fully optimized peridinin and a molecule from the crystal structure of peridinin−chlorophyll−protein. The CT state appears as the third and second excited singlet state, respectively, for the two structures. A dipole-in-a-sphere model is used to estimate the solvation stabilization energies of each state in a variety of solvents. The energy of the CT state is shown to decrease dramatically in solvents of increasing polarity while the energy of the dark S1 (Ag--like) state remains comparatively constant.
Article
The spectroscopic properties and dynamics of the lowest excited singlet states of peridinin, fucoxanthin, neoxanthin, uriolide acetate, spheroidene, and spheroidenone in several different solvents have been studied by steady-state absorption and fast-transient optical spectroscopic techniques. Peridinin, fucoxanthin, uriolide acetate, and spheroidenone, which contain carbonyl functional groups in conjugation with the carbon-carbon pi-electron system, display broader absorption spectral features and are affected more by the solvent environment than neoxanthin and spheroidene, which do not contain carbonyl functional groups. The possible sources of the spectral broadening are explored by examining the absorption spectra at 77 K in glassy solvents. Also, carotenoids which contain carbonyls have complex transient absorption spectra and show a pronounced dependence of the excited singlet state lifetime on the solvent environment. It is postulated that these effects are related to the presence of an intramolecular charge transfer state strongly coupled to the S-1 (2(1)A(g)) excited singlet state. Structural variations in the series of carotenoids studied here make it possible to focus on the general molecular features that control the spectroscopic and dynamic properties of carotenoids.
Article
The spectroscopic properties and dynamic behavior of peridinin in several different solvents were studied by steady-state absorption, fluorescence, and transient optical spectroscopy. The lifetime of the lowest excited singlet state of peridinin is found to be strongly dependent on solvent polarity and ranges from 7 ps in the strongly polar solvent trifluoroethanol to 172 ps in the nonpolar solvents cyclohexane and benzene. The lifetimes show no obvious correlation with solvent polarizability, and hydrogen bonding of the solvent molecules to peridinin is not an important factor in determining the dynamic behavior of the lowest excited singlet state. The wavelengths of emission maxima, the quantum yields of fluorescence, and the transient absorption spectra are also affected by the solvent environment. A model consistent with the data and supported by preliminary semiempirical calculations invokes the presence of a charge transfer state in the excited state manifold of peridinin to account for the observations. The charge transfer state most probably results from the presence of the lactone ring in the pi-electron conjugation of peridinin analogous to previous findings on aminocoumarins and related compounds. The behavior of peridinin reported here is highly unusual for carotenoids, which generally show little dependence of the spectral properties and lifetimes of the lowest excited singlet state on the solvent environment.
Chapter
Analysis by a combination of absorption-, fluorescence-, circular dichroism-, mass- and nuclear magnetic resonance- spectrometry is often used to investigate the structure of chlorophylls. Here, we show several examples of spectroscopic determination of molecular structure of the recently-discovered chlorophylls and compare them with the well-known chlorophylls, chlorophyll a and bacteriochlorophyll a.