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Plant Physiol, January 2001, Vol. 125, pp. 33-37
Photosynthetic Reaction Centers
Warwick
Hillier and
Gerald T.
Babcock*
Department of Chemistry, Michigan State University, East Lansing,
Michigan 48824
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THE CONCEPT AND PHYSICAL REALITY OF REACTION CENTERS
(RCs) |
The capture of solar radiation and
the conversion of its free energy into chemical energy involves a
sequence of reactions that occur within a physical structure called the
photosynthetic RC. Following the initial capture of a photon by antenna
pigments, the photon is transferred to the RC pigments, where it gives
rise to a separation and stabilization of charge across the
photosynthetic membrane. Figure 1 depicts
this process and illustrates the time scales typically involved. One
feature of the photochemistry is that all photosynthetic RCs undergo
charge separation with a quantum yield approaching unity, which makes
them marvelous molecular machines.

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Figure 1.
Primary processes in the photosynthetic RC. Here,
P represents the charge-separating (bacterio) chlorophyll pigments (the
"primary electron donor") and A represents the first "stable"
acceptor. Energy transfer from the antenna pigments leads to
photoexcitation of P on the fs-ps time scale (left). Charge separation
produces oxidized P+ and
A- on the ps-ns scale (center). The
recombination of P+A- to
produce PA, heat, and potentially damaging chemical species is
efficiently prevented by further forward electron transfer that is now
proton coupled. These more complex chemical processes ultimately
produce stable photosynthetic products and occur, initially, on the ns
and µs time scales (right).
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The first notions of the operation of a photosynthetic RC originated
with the photosynthetic unit experiments of Emerson and Arnold (9),
which demonstrated that approximately 2,500 chlorophyll molecules were
involved in the release of just one molecule of O2. Thus, a photosynthetic unit contains numerous
pigments but the photochemically active chromophores are present in
much lower concentration. This pioneering concept led to the
distinction of two types of pigments: the light-harvesting, but
photochemically inactive, antenna chromophores; and the photochemically
active RC pigments. The antenna pigments physiologically increase the absorption cross section of the RC dramatically. Moreover, they ensure
that the potentially reactive intermediates containing unpaired
electron spins (e.g. semiquinones) generated by single photon
photochemistry are efficiently converted by a second photochemical event to products (e.g. hydroquinones) that contain only paired spins.
For efficient energy transfer between the antenna and the RC, the RC
absorbs at longer wavelengths, effectively forming a trap for
excitation energy. Despite these conceptual advances, more than 35 years passed before the first physical isolation of a pigment protein
RC complex was reported (17). Since that time, many other RCs have been
isolated and characterized biophysically and biochemically.
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STRUCTURAL AND OPERATIONAL INSIGHTS |
Insight into the molecular organization of the RC has been
derived, initially, from spectroscopic studies and, subsequently, from
the development and analysis of high-resolution crystal structures of
several photosynthetic organisms. The first RC structurally resolved (3 Å) was of the purple bacterial RC from Rhodopseudomonas viridis (7), for which the 1988 Nobel Prize was awarded. This was
soon followed by the elucidation of several other purple bacterial structures. We are now witnessing the appearance of detailed RC structures from oxygenic systems, most notably the 4Å structure of
photosystem I (PSI; 13). Good progress is also being made toward achieving two- and three-dimensional structures of photosystem II
(PSII) crystals. It is surprising that the structures of all of the
different RCs show a dimeric core with a
pseudo-C2 axis of symmetry. This feature is
illustrated in Figure 2 in the example of
a purple bacterial RC. The holoprotein is shown on the left. The
charge-separating RC pigments contained within the structure (Fig. 2,
right) are aligned along the C2 symmetry axis
with the two photochemically active (bacterio) chlorophyll pigments
positioned in close proximity. Exciton coupling between these two
pigments provides a red shift in the optical spectrum that contributes substantially to forming the low-energy trap discussed above. The
conversion of photons to chemical potential involves photoexcitation and initial charge separation to produce an oxidized (bacterio) chlorophyll and reduction of one of the other chlorin pigments in the
RC. From this chlorin, the electron migrates to reduce a quinone in
less than a nanosecond (Fig. 2). It is interesting that the strength of
the dimer exciton coupling has changed substantially during the course
of oxygenic RC evolution from photosynthetic bacteria. The bacteria
usually have strong couplings, approximately 2,000 cm 1, whereas the plant and algal RCs have a
much weaker coupling, typically approximately 300 cm 1 (8). The weaker coupling in the oxygenic
RCs increases the thermodynamic efficiency of photon capture so that a
significant improvement in useful free energy capture from the photon
is realized. Subsequent proton-coupled electron transfer steps (Fig. 1)
stabilize the charge separation effectively and ensure the near-unity
quantum efficiency of photosynthesis.

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Figure 2.
Structure of the purple bacterial RC
(Rhodobacter sphaeroides from MH. Stowell et al; Protein
Data Band file no. 1AIJ). The heterodimeric RC (left) is
comprised of a C2-symmetrical heterodimer of the
L and M polypeptides shown in orange and blue respectively. A third
subunit, H, is also shown in green. The pseudo-C2
symmetric cofactor arrangement and the active pathway of electron
transfer are indicated on the right. Charge separation from the RC Chl
dimer (P) to the BChl monomer to B-Phe occurs in approximately 3 ps
down the active L branch. This is followed by charge stabilization with
electron transfer to the quinones. The phytyl and isoprenoid chain have
been removed for visualization.
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A remarkable aspect of the RC structures is the occurrence of two
almost identical electron acceptor pathways arranged along the
C2 axis relative to the primary charge-separating
dimer (bacterio) chlorophyll (Fig. 2). This finding posed a key
question: Does electron transfer involve both branches? In the purple
bacterial RC, only one branch is active although the inactive branch
can be forced into operation with modification of amino acid side chains on the active branch (1). The strong asymmetry imposed on
primary charge separation photo-chemistry in the purple bacterial RC
results from two homologous polypeptides that function as a heterodimer. A heterodimer is also involved in the core of the RCs of
PSI and PSII. However, some RCs, such as heliobacteria (2) and green
sulfur bacteria (6, 18), contain two identical homodimeric polypeptides, and electron transfer is potentially bifurcated.
Genetic sequence information has greatly improved the understanding of
the origin of the RC proteins. From the sequence analysis, it became
clear that the purple bacteria RC is remarkably similar to that of
PSII, and PSI was also discovered to have similarity with that of the
green sulfur bacteria (6, 10). Further elaboration with 16S-rRNA
phylogenic trees (5) and broader homology comparison (14) revealed a
close interrelationship among many RCs. Recent structural comparisons
between PSI and PSII, for example, show a distinct structural homology,
which suggests that even these two RCs likely share a common ancestor (13).
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TYPES OF RCs |
The general details of RC structure and function described above
persist among photosynthetic organisms, but differences in detail have
become apparent. Today, we recognize six different classes
of photosynthetic RCs. The principal variations lie in the RC pigments
(chlorophyll versus bacteriochloropyll), the size and nature of the
antenna pigment array, the associated longest wavelength maximum and
strength of the pigment exciton coupling, and the thermodynamic
coupling of the primary donor chlorophyll dimer (P) to its acceptor
system (i.e. its midpoint reduction potential). Figure
3 presents a summary of the various RCs,
cofactors, and electron transport chains. The six classes of RC divide
into two forms: the type I and type II RCs (10, 15). The type I RCs comprise PSI, the gram-positive heliobacteria, and the green sulfur bacteria, all of which share iron-sulfur clusters as electron acceptors. The type II RCs from PSII, purple bacteria and the green
filamentous bacteria, share quinone acceptors that serve as
two-electron reductants. Two of these RCs, from heliobacteria and the
green filamentous bacteria, have only been recognized quite recently
and there may be others that await discovery the field continues to
progress rapidly.

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Figure 3.
Electron-transfer pathways for the two different
types and six classes of RCs shown according to the midpoint potentials
of key redox components. In Type I RCs (left), iron-sulfur clusters are
used as the electron acceptors. Type I is subdivided into three
classes: PSI, green sulfur bacteria, and heliobacteria (see text). In
Type II RCs, quinones are used as the first "stable" electron
acceptors (left). Type II is also subdivided into three classes: PSII,
purple bacteria, and green filamentous bacteria. Intermediates in the
scheme have the following designations: the RC primary donor, P;
transient initial (bacterio) pheophytin acceptor, (B) Ph; "stable"
quinone acceptors, QA and
QB; transient initial chlorophyll
(A0) and quinone (A1)
acceptors; "stable" iron-sulfur cluster acceptors,
FX, FA, and
FB; and final NADP acceptor (NADP). The electron
donors are a Tyr residue, TyrZ, and a cluster of
4 manganese ions for PSII, a plastocyanin molecule (PC) for PSI, and
cytochrome c for the bacterial RCs. The intermediate
electron transfer complexes, cytochrome
bc1 and b6f,
are boxed.
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Further differentiation in photosynthetic organisms is found in the
structure and arrangement of the antenna pigments associated with each
RC. The RC from heliobacteria features a very simple organization with
a core containing approximately 40 chlorophyll g and
no additional auxiliary peripheral antenna proteins (2). Building on
this organizational theme are RCs from PSI and green sulfur bacteria,
which contain large numbers (~100) of pigments attached directly to
the polypeptides that bind the RC components (13), as well as an
extensive external antenna array with which the RCs communicate in a
controlled way. At the other extreme are the RCs from purple bacteria
and PSII, which contain only six to eight pigments arranged
along the C2 symmetry axis and are fundamental to
the charge separation process. These RCs rely on a substantial
antenna system as conduits of excitation energy. This antenna system is
bound to polypeptides distinct from the RC polypeptides.
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OXYGENIC PHOTOSYNTHESIS |
The incorporation of two RCs in series during the evolution of
plant and algal photosynthesis represents a brilliant strategy for
using an inexhaustible supply of water in the unlikely role of
reductant without sacrificing the ability to use photons in the red
( > 600 nm) region of the spectrum. For a single RC oxidizing water and reducing NADP, photons of about 500 nm or shorter would be
required to span the entire redox-potential range between the two
products (O2 and NADPH) with sufficient
irreversibility to ensure a high quantum yield. Using two
photoreactions in series, this energetic requirement is relaxed, and
photons in the longer wavelength region (680 nm [PSII] and 700 nm
[PSI]) become useful. The overall quantum requirement for water
oxidation increases from four photons to eight:
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but lower-energy photons, up to 700 nm, are able to drive the
process. Coordination of two photosystems, however, requires significantly greater sophistication to balance the incoming excitation energy to the RCs associated with the two photosystems. To meet this
requirement, PSI and PSII demonstrate significant differences in
pigment composition and placement of the antenna proteins as a function
of the light quality. In plants, this situation is highlighted by
the lateral heterogeneity between the two RCs, which results in the
physical separation of the PSII RC to the grana-appressed region and
the PSI RC to the nonappressed region of the thylakoid (3). This
division of RCs forms the basis of the biochemical isolation procedure
that has been the cornerstone of much of the biochemical and
biophysical work with PSII (4).
The charge-stabilizing reactions that occur following primary
charge separation in the RC are coming into sharper focus. A key
realization has been that these reactions are often proton coupled;
that is, the motion of the electron must be coupled in some fashion to
the motion of a proton (Fig. 1). This marks the conversion from pure
photon and electron chemistry to chemistry that involves nuclei as
well. Okamura and his coworkers have produced seminal results on
electron/proton coupling on the reducing side in the bacterial RC (16).
Results that incorporate these and other thoughts concerning
proton/electron coupling in PSII are emerging as the underlying
mechanism that drives water oxidation to produce O2.
To oxidize water, potentials upwards of 1 V must be generated in PSII;
moreover, the observations by Joliot and Kok (12) that O2 evolution follows a four-flash oscillatory
pattern necessitates that the oxidizing equivalents produced by
P680+ must be stored. To accomplish this,
P680+ (midpoint reduction potential at pH 7, approximately 1.2 V) is intimately coupled to a redox-active Tyr
(TyrZ) and an inorganic Mn4Ca1ClX
cluster where the water oxidation reaction is catalyzed. Current
insights into the cluster structure have been largely driven by x-ray
absorption spectroscopy, which predicts that the catalytic
manganese complex is organized as pair of manganese-oxo dimers
(20). The water oxidation reaction is more difficult to access. Recent
H216O/H218O
exchange measurements (11) show rapid exchange of substrate water (ms
time regime), supporting the notion that substrate water is bound
terminally to manganese. A number of other measurements concerning the
water oxidation reaction have led to a metalloradical model for PSII
water oxidation. In this proposal, TryZ is
directly involved in hydrogen atom abstraction from the substrate water terminally bound at the manganese cluster (19). This proposal, as with
most hypotheses, has attracted both supporters and detractors!
It is certain that in the next few years the structure of PSII and the
oxygen-evolving complex will be resolved at high resolution, as will be
the structures of many other photosynthetic RCs. Already the last 25 years have seen tremendous advances in the understanding of
photosynthetic RCs. Long-held concepts have been challenged, reinvestigated, and changed as the results of new structural, dynamic,
biochemical, and molecular biological insights. These have been
stimulating and exciting developments; undoubtedly they will continue.
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FOOTNOTES |
*
Corresponding author; e-mail Babcock{at}cem.msu.edu; fax
517-353-1793.
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© 2001 American Society of Plant Physiologists
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