Jörg Pieper

Excitonic Energy Level Structure and Pigment−Protein Interactions in the Recombinant Water-Soluble Chlorophyll Protein. I. Difference Fluorescence Line-Narrowing

Difference fluorescence line-narrowing spectroscopy at 4.5 K was employed to investigate electron-phonon and electron-vibrational coupling strengths of the lower exciton level of water-soluble chlorophyll-binding protein (WSCP) from cauliflower reconstituted with chlorophyll a or chlorophyll b, respectively. The electron-phonon coupling is found to be moderate with integral Huang-Rhys factors S in the order of 0.81-0.85. A weak dependence of S on excitation wavelength within the inhomogeneously broadened fluorescence origin band is attributed to a sizable contribution of nonresonant excitation that varies with excitation wavelength. The strongly asymmetric and highly structured one-phonon profile is characterized by a peak phonon frequency (ω(m)) of ~24 cm(-1) and further discernible peaks at 48 and 88 cm(-1), respectively. A structural assignment of this unusual one-phonon profile is proposed. As will be shown in the accompanying paper (part II) (DOI 10.1021/jp111457t), the parameters of electron-phonon coupling readily account for shape and position of the fluorescence origin bands at 666.1 and 683.8 nm for chlorophyll b- and chlorophyll a-WSCP, respectively. A rich structure of S(1)→S(0) vibrational frequencies was resolved in the wavenumber range between 180 and 1665 cm(-1) for both chlorophyll a- and chlorophyll b-WSCP. The corresponding individual Huang-Rhys factors fall in the range between 0.0011 and 0.0500. To the best of our knowledge, this is the first report of S-factors for vibrational modes of chlorophyll b. Most remarkable is the presence of two additional modes at 228 and 327 cm(-1) compared with the vibrational spectrum of chlorophyll in solution. The additional modes can most likely be attributed to H-bond formation in the vicinity of the chlorophyll molecule bound by WSCP.

Chromophore-chromophore and chromophore-protein interactions in monomeric light-harvesting complex II of green plants studied by spectral hole burning and fluorescence line narrowing.

Persistent nonphotochemical hole burning and delta-FLN spectra obtained at 4.5 K are reported for monomeric chlorophyll (Chl) a/b light-harvesting complexes of photosystem II (LHC II) of green plants. The hole burned spectra of monomeric LHC II appear to be similar to those obtained before for trimeric LHC II (Pieper et al. J. Phys. Chem. B 1999, 103, 2412). They are composed of three main features: (i) a homogeneously broadened zero-phonon hole coincident with the burn wavelength, (ii) an intense, broad hole in the vicinity of approximately 680 nm as a result of efficient excitation energy transfer to a low-energy trap state, and (iii) a satellite hole at approximately 649 nm which is correlated with the low-energy 680 nm hole. Zero-phonon hole action spectroscopy reveals that the low-energy absorption band is located at 679.6 nm and possesses a width of approximately 110 cm(-1) which is predominantly due to inhomogeneous broadening at 4.5 K. The electron-phonon coupling of the above-mentioned low-energy state(s) is weak with a Huang-Rhys factor S in the order of 0.6 and a peak phonon frequency (omega(m)) of approximately 22 cm(-1) within a broad and strongly asymmetric one-phonon profile. The resulting Stokes shift 2S omega(m) of approximately 26.4 cm(-1) readily explains the position of the fluorescence origin band at 680.8 nm. Thus, we conclude that the 679.6 nm state(s) is (are) the fluorescent state(s) of monomeric LHC II at 4.5 K. The absorption intensity of the lowest Q(y) state is shown to roughly correspond to that of one out of the eight Chl a molecules bound in the monomeric subunit. In addition, the satellite hole structure produced by hole burning within the 679.6 nm state is weak with only one shallow satellite hole observed in the Chl b spectral range at 648.8 nm. These results suggest that the 679.6 nm state is widely localized on a Chl a molecule, which may belong to a Chl a/b heterodimer. These characteristics are different from those expected for Chl a612, which has been associated with the fluorescent state at room temperature. Alternatively, the 679.6 nm state may be assigned to Chl a604, which is located in a cluster with several Chl b molecules resulting in a relatively weak excitonic coupling.

Excitonic energy level structure and pigment-protein interactions in the recombinant water-soluble chlorophyll protein. II. Spectral hole-burning experiments.

Persistent spectral hole burning at 4.5 K has been used to investigate the excitonic energy level structure and the excited state dynamics of the recombinant class-IIa water-soluble chlorophyll-binding protein (WSCP) from cauliflower. The hole-burned spectra are composed of four main features: (i) a narrow zero-phonon hole (ZPH) at the burn wavelength, (ii) a number of vibrational ZPHs, (iii) a broad low-energy hole at ~665 and ~683 nm for chlorophyll b- and chlorophyll a-WSCP, respectively, and (iv) a second satellite hole at ~658 and ~673 nm for chlorophyll b- and chlorophyll a-WSCP, respectively. The doublet of broad satellite holes is assigned to an excitonically coupled chlorophyll dimer. The lower-energy holes at ~665 and ~683 nm for chlorophyll b- and chlorophyll a-WSCP, respectively, represent the lower exciton states. Taking into account the parameters of electron-phonon coupling, the lower exciton state can be assigned as the fluorescence origin. The lower exciton state is populated by two processes: (i) exciton relaxation from the higher exciton state and (ii) vibrational relaxation within the lower exciton state. Assuming identical site energies for the two excitonically coupled chlorophyll molecules, the dipole-dipole interaction energy J is directly determined to be 85 and 100 cm(-1) for chlorophyll b- and chlorophyll a-WSCP, respectively, based on the positions of the satellite holes. The Gaussian low-energy absorption band identified by constant fluence hole burning at 4.5 K has a width of ~150 cm(-1) and peaks at 664.9 and 682.7 nm for chlorophyll b- and chlorophyll a-WSCP, respectively. The action spectrum is broader and blue-shifted compared to the fluorescent lower exciton state. This finding can be explained by a slow protein relaxation between energetically inequivalent conformational substates within the lowest exciton state in agreement with the results of Schmitt et al. (J. Phys. Chem. B2008, 112, 13951).

Reaction pattern of photosystem II: oxidative water cleavage and protein flexibility.

This short communication addresses three topics of photosynthetic water cleavage in Photosystem II (PS II): (a) effect of protonation in the acidic range on the extent of the ‘fast’ ns kinetics of P680+· reduction by YZ, (b) mechanism of O–O bond formation and (c) role of protein flexibility in the functional integrity of PS II. Based on measurements of light-induced absorption changes and quasielastic neutron scattering in combination with mechanistic considerations, evidence is presented for the protein acting as a functionally active constituent of the water cleavage machinery, in particular, for directed local proton transfer. A specific flexibility emerging above a threshold of about 230 K is an indispensable prerequisite for oxygen evolution and plastoquinol formation.

Protein Dynamics Tunes Excited State Positions in Light-Harvesting Complex II

Light harvesting and excitation energy transfer in photosynthesis are relatively well understood at cryogenic temperatures up to ∼100 K, where crystal structures of several photosynthetic complexes including the major antenna complex of green plants (LHC II) are available at nearly atomic resolution. The situation is much more complex at higher or even physiological temperatures, because the spectroscopic properties of antenna complexes typically undergo drastic changes above ∼100 K. We have addressed this problem using a combination of quasielastic neutron scattering (QENS) and optical spectroscopy on native LHC II and mutant samples lacking the Chl 2/Chl a 612 pigment molecule. Absorption difference spectra of the Chl 2/Chl a 612 mutant of LHC II reveal pronounced changes of spectral position and their widths above temperatures as low as ∼80 K. The complementary QENS data indicate an onset of conformational protein motions at about the same temperature. This finding suggests that excited state positions in LHC II are affected by protein dynamics on the picosecond time scale. In more detail, this means that at cryogenic temperatures the antenna complex is trapped in certain protein conformations. At higher temperature, however, a variety of conformational substates with different spectral position may be thermally accessible. At the same time, an analysis of the widths of the absorption difference spectra of Chl 2/Chl a 612 reveals three different reorganization energies or Huang-Rhys factors in different temperature ranges, respectively. These findings imply that (dynamic) pigment-protein interactions fine-tune electronic energy levels and electron-phonon coupling of LHC II for efficient excitation energy transfer at physiological temperatures.

Modeling of Optical Spectra of the Light-Harvesting CP29 Antenna Complex of Photosystem II—Part II

Until recently, it was believed that the CP29 protein from higher plant photosystem II (PSII) contains 8 chlorophylls (Chls) per complex (Ahn et al. Science 2008, 320, 794-797; Bassi et al. Proc. Natl. Acad. Sci. U.S.A. 1999, 96, 10056-10061) in contrast to the 13 Chls revealed by the recent X-ray structure (Pan et al. Nat. Struct. Mol. Biol. 2011, 18, 309-315). This disagreement presents a constraint on the interpretation of the underlying electronic structure of this complex. To shed more light on the interpretation of various experimental optical spectra discussed in the accompanying paper (part I, DOI 10.1021/jp4004328 ), we report here calculated low-temperature (5 K) absorption, fluorescence, hole-burned (HB), and 300 K circular dichroism (CD) spectra for CP29 complexes with a different number of pigments. We focus on excitonic structure and the nature of the low-energy state using modeling based on the X-ray structure of CP29 and Redfield theory. We show that the lowest energy state is mostly contributed to by a612, a611, and a615 Chls. We suggest that in the previously studied CP29 complexes from spinach (Pieper et al. Photochem. Photobiol.2000, 71, 574-589) two Chls could have been lost during the preparation/purification procedure, but it is unlikely that the spinach CP29 protein contains only eight Chls, as suggested by the sequence homology-based study (Bassi et al. Proc. Natl. Acad. Sci. U.S.A.1999, 96, 10056-10061). The likely Chls missing in wild-type (WT) CP29 complexes studied previously (Pieper et al. Photochem. Photobiol. 2000, 71, 574-589) include a615 and b607. This is why the nonresonant HB spectra shown in that reference were ~1 nm blue-shifted with the low-energy state mostly localized on about one Chl a (i.e., a612) molecule. Pigment composition of CP29 is discussed in the context of light-harvesting and excitation energy transfer.

Spectroscopic study of the light-harvesting CP29 antenna complex of photosystem II--part I.

Recent structural data revealed that the CP29 protein of higher plant photosystem II (PSII) contains 13 chlorophylls (Chls) per complex (Pan et al. Nat. Struct. Mol. Biol. 2011, 18, 309), i.e., five Chls more than in the predicted CP29 homology-based structure model (Bassi et al. Proc. Natl. Acad. Sci. U.S.A. 1999, 96, 10056). This lack of consensus presents a constraint on the interpretation of CP29 optical spectra and their underlying electronic structure. To address this problem, we present new low-temperature (5 K) absorption, fluorescence, and hole-burned (HB) spectra for CP29 proteins from spinach, which are compared with the previously reported data. We focus on excitation energy transfer (EET) and the nature of the lowest-energy state(s). We argue that CP29 proteins previously studied by HB spectroscopy lacked at least one Chl a molecule (i.e., a615 or a611), which along with Chl a612 contribute to the lowest energy state in more intact CP29, and one Chl b (most likely b607). This is why the low-energy state and fluorescence maxima reported by Pieper et al. (Photochem. Photobiol.2000, 71, 574) were blue-shifted by ~1 nm, the low-energy state appeared to be highly localized on a single Chl a molecule, and the position of the low-energy state was independent of burning fluence. In contrast, the position of the nonresonant HB spectrum shifts blue with increasing fluence in intact CP29, as this state is strongly contributed to by several pigments (i.e., a611, a612, a615, and a610). Zero-phonon hole widths obtained for the Chl b band at 638.5 nm (5 K) revealed two independent Chl b → Chl a EET times, i.e., 4 ± 0.5 and 0.4 ± 0.1 ps. The latter value is a factor of 2 faster than previously observed by HB spectroscopy and very similar to the one observed by Gradinaru et al. (J. Phys. Chem. B 2000, 104, 9330) in pump-probe experiments. EET time from 650 nm Chl b → Chl a and downward EET from Chl(s) a state(s) at 665 nm occurs in 4.9 ± 0.7 ps. These findings provide important constraints for excitonic calculations that are discussed in the accompanying paper (part II, DOI 10.1021/jp4004278 ).

Excitation energy transfer and electron-vibrational coupling in phycobiliproteins of the cyanobacterium Acaryochloris marina investigated by site-selective spectroscopy.

In adaption to its specific environmental conditions, the cyanobacterium Acaryochloris marina developed two different types of light-harvesting complexes: chlorophyll-d-containing membrane-intrinsic complexes and phycocyanobilin (PCB) - containing phycobiliprotein (PBP) complexes. The latter complexes are believed to form a rod-shaped structure comprising three homo-hexamers of phycocyanin (PC), one hetero-hexamer of phycocyanin and allophycocyanin (APC) and probably a linker protein connecting the PBPs to the reaction centre. Excitation energy transfer and electron-vibrational coupling in PBPs have been investigated by selectively excited fluorescence spectra. The data reveal a rich spectral substructure with a total of five low-energy electronic states with fluorescence bands at 635nm, 645nm, 654nm, 659nm and a terminal emitter at about 673 nm. The electronic states at ~635 and 645 nm are tentatively attributed to PC and APC, respectively, while an apparent heterogeneity among PC subunits may also play a role. The other fluorescence bands may be associated with three different isoforms of the linker protein. Furthermore, a large number of vibrational features can be identified for each electronic state with intense phonon sidebands peaking at about 31 to 37cm⁻¹, which are among the highest phonon frequencies observed for photosynthetic antenna complexes. The corresponding Huang-Rhys factors S fall in the range between 0.98 (terminal emitter), 1.15 (APC), and 1.42 (PC). Two characteristic vibronic lines at about 1580 and 1634cm⁻¹ appear to reflect CNH⁺ and CC stretching modes of the PCB chromophore, respectively. The exact phonon and vibrational frequencies vary with electronic state implying that the respective PCB chromophores are bound to different protein environments. This article is part of a special issue entitled: photosynthesis research for sustainability: keys to produce clean energy.

Perspectives in biological physics: the nDDB project for a neutron Dynamics Data Bank for biological macromolecules.

Neutron spectroscopy provides experimental data on time-dependent trajectories, which can be directly compared to molecular dynamics simulations. Its importance in helping us to understand biological macromolecules at a molecular level is demonstrated by the results of a literature survey over the last two to three decades. Around 300 articles in refereed journals relate to neutron scattering studies of biological macromolecular dynamics, and the results of the survey are presented here. The scope of the publications ranges from the general physics of protein and solvent dynamics, to the biologically relevant dynamics-function relationships in live cells. As a result of the survey we are currently setting up a neutron Dynamics Data Bank (n DDB) with the aim to make the neutron data on biological systems widely available. This will benefit, in particular, the MD simulation community to validate and improve their force fields. The aim of the database is to expose and give easy access to a body of experimental data to the scientific community. The database will be populated with as much of the existing data as possible. In the future it will give value, as part of a bigger whole, to high throughput data, as well as more detailed studies. A range and volume of experimental data will be of interest in determining how quantitatively MD simulations can reproduce trends across a range of systems and to what extent such trends may depend on sample preparation and data reduction and analysis methods. In this context, we strongly encourage researchers in the field to deposit their data in the n DDB.Graphical abstract

Electron–Phonon and Exciton–Phonon Coupling in Light Harvesting, Insights from Line-Narrowing Spectroscopies

In photosynthetic antenna complexes, apart from defining the positions and orientations of the pigment molecules, the protein matrix plays an important role in excitation energy transfer dynamics. The low-frequency protein vibrations—often referred to as phonons—serve as acceptor modes in nonadiabatic excitation energy transfer between energetically inequivalent electronic or excitonic energy states, assuring a spatially and energetically directed flow of excitation energy within an antenna complex. Due to electron–phonon and electron–vibrational coupling, the purely electronic or excitonic transitions of pigment molecules are usually accompanied by a broad and asymmetric low-frequency sideband spreading a few hundred wavenumbers and, in addition, by a number of distinct lines covering the frequency range between ~200 and 1,700 cm−1. The low-frequency sideband peaking at 20–30 cm−1 is typically identified with a continuous distribution of widely delocalized protein vibrations. The narrow lines at higher frequencies can mostly be attributed to localized pigment vibrations of (bacterio-) chlorophyll molecules, which are only slightly modified by the surrounding protein matrix. In conventional absorption or fluorescence spectra measured at cryogenic temperatures this substructure is usually hidden by significant inhomogeneous broadening due to the heterogeneity of the amorphous protein matrix. Line-narrowing spectroscopies like spectral hole burning and (difference) fluorescence line-narrowing have been proved to be powerful experimental tools for unraveling the hidden homogeneous spectral features from the inhomogeneously broadened spectra. This contribution focuses on electron–phonon and exciton–phonon coupling in photosynthetic pigment–protein complexes. It also discusses the underlying concepts of electron–phonon and electron–vibrational coupling starting from the Franck–Condon principle and the general composition of homogeneously and inhomogeneously broadened spectra of pigment–protein complexes. The advantages and limitations of different spectroscopic techniques in revealing the electron–phonon and electron–vibrational coupling parameters are discussed based on model calculations. The chapter concludes with a discussion of recent results on electron–phonon and electron–vibrational coupling for isolated (bacterio-) chlorophyll molecules as well as for selected photosynthetic pigment–protein complexes.