This can arise because of different ionization states of protein side chains close to their pKa, different orientations of side chains, slight distortions of the overall protein structure, and a host of similar small influences. The overall effect is to smear out the transition to produce inhomogeneous broadening. (3) Chlorophylls and other pigments are generally bound in a variety of non-equivalent sites in an individual protein complex. For example, the Fenna–Matthews–Olson (FMO) complex of green sulfur bacteria binds seven bacteriochlorophyll molecules each in a unique site. This type of inhomogeneous broadening may produce a set of more discrete Selleck Belnacasan transition energies than the

broadening arising by mechanism (2). Both (2) and (3) give transition energies that vary slowly or not at all on the time scale of the optical functions of photosynthetic complexes. (4) In many photosynthetic AZD6738 supplier complexes, the chromophores are held very close to one or more neighbors leading to electronic mixing and associated spectral shifts from the individual molecule’s unperturbed transition. This can lead to a set of chemically identical chromophores having a significantly broader spectrum than a similar,

but non-interacting, set of molecules. (5) Finally, several processes can, and often do, happen very fast in photosynthetic complexes, leading to lifetime broadening. An excellent summary of the spectroscopy of photosynthetic complexes can be found in Van Amerongen et al. (2000). Photon echo spectroscopy (Mukamel 1995; Parson 2007) can often see more remove or greatly diminish the type of broadening described in (2). Indeed, the inhomogeneous broadening can be used to observe the energy flow both within and between photosynthetic complexes. A newly developed form

of photon echo spectroscopy, two-dimensional Fourier transform photon echo spectroscopy, can be used to unravel the interactions described in (4) as well as remove type (2) broadening, and reveal, on their characteristic timescale, the relaxation pathways within individual complexes and reveal striking details about their design and the origins of their great efficiency. Below, we outline the origins of photon echo (and related) signals and describe a number of photon echo-based experimental techniques applied to problems in photosynthesis. The basis of photon Tyrosine-protein kinase BLK echo spectroscopy, as with other “ultrafast” techniques, is the interrogation of a system with laser pulses short enough to track dynamical processes of interest. In this work, ultrafast means tens of femtoseconds (where a femtosecond is 10−15 s), a timescale on which the fastest energy transfer processes occur between neighboring pigments in light-harvesting complexes. The method requires a sequence of laser pulses to interrogate the sample and, as with pump-probe and related experiments, allows observation of excited state dynamics.