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1.
J Phys Chem A ; 117(1): 34-41, 2013 Jan 10.
Article in English | MEDLINE | ID: mdl-23210463

ABSTRACT

We report simulations of the two-dimensional electronic spectroscopy of the Q(y) band of the D1-D2-Cyt b559 photosystem II reaction center at 77 K. We base the simulations on an existing Hamiltonian that was derived by simultaneous fitting to a wide range of linear spectroscopic measurements and described within modified Redfield theory. The model obtains reasonable agreement with most aspects of the two-dimensional spectra, including the overall peak shapes and excited state absorption features. It does not reproduce the rapid equilibration from high energy to low energy excitonic states evident by a strong cross-peak below the diagonal. We explore modifications to the model to incorporate new structural data and improve agreement with the two-dimensional spectra. We find that strengthening the system-bath coupling and lowering the degree of disorder significantly improves agreement with the cross-peak feature, while lessening agreement with the relative diagonal/antidiagonal width of the 2D spectra. We conclude that two-dimensional electronic spectroscopy provides a sensitive test of excitonic models of the photosystem II reaction center and discuss avenues for further refinement of such models.


Subject(s)
Computer Simulation , Models, Molecular , Photosystem II Protein Complex/chemistry , Spectrum Analysis/methods , Energy Transfer , Protein Conformation
2.
Phys Rev Lett ; 93(1): 018102, 2004 Jul 02.
Article in English | MEDLINE | ID: mdl-15324023

ABSTRACT

We report femtosecond visible pump, midinfrared probe, spectrally integrated experiments resolving the dynamics of CO in myoglobin upon photodissociation. Our results show a progressive change in absorption strength of the CO vibrational transition during its transfer from the heme to the docking site, whereas the vibrational frequency change is faster than our time resolution. A phenomenological model gives good qualitative agreement with our data for a time constant of 400 fs for the change in oscillator strength. Density-functional calculations demonstrate that indeed vibrational frequency and absorption strength are not linearly coupled and that the absorption strength varies in a slower manner due to charge transfer from the heme iron to CO.


Subject(s)
Carbon Monoxide/chemistry , Carbon Monoxide/metabolism , Models, Chemical , Myoglobin/chemistry , Myoglobin/metabolism , Biophysical Phenomena , Biophysics , Heme/chemistry , Heme/metabolism , Ligands , Photochemistry , Vibration
3.
Proc Natl Acad Sci U S A ; 100(9): 4990-4, 2003 Apr 29.
Article in English | MEDLINE | ID: mdl-12697894

ABSTRACT

Model studies of the ligand photodissociation process of carboxymyoglobin have been conducted by using amplified few-cycle laser pulses short enough in duration (<10 fs) to capture the phase of the induced nuclear motions. The reaction-driven modes are observed directly in real time and depict the pathway by which energy liberated in the localized reaction site is efficiently channeled to functionally relevant mesoscale motions of the protein.


Subject(s)
Cytochrome c Group/chemistry , Myoglobin/chemistry , Animals , Carbon Monoxide , Lasers
4.
Proc Natl Acad Sci U S A ; 98(11): 6110-5, 2001 May 22.
Article in English | MEDLINE | ID: mdl-11344263

ABSTRACT

Ligand transport through myoglobin (Mb) has been observed by using optically heterodyne-detected transient grating spectroscopy. Experimental implementation using diffractive optics has provided unprecedented sensitivity for the study of protein motions by enabling the passive phase locking of the four beams that constitute the experiment, and an unambiguous separation of the Real and Imaginary parts of the signal. Ligand photodissociation of carboxymyoglobin (MbCO) induces a sequence of events involving the relaxation of the protein structure to accommodate ligand escape. These motions show up in the Real part of the signal. The ligand (CO) transport process involves an initial, small amplitude, change in volume, reflecting the transit time of the ligand through the protein, followed by a significantly larger volume change with ligand escape to the surrounding water. The latter process is well described by a single exponential process of 725 +/- 15 ns. at room temperature. The overall dynamics provide a distinctive signature that can be understood in the context of segmental protein fluctuations that aid ligand escape via a few specific cavities, and they suggest the existence of discrete escape pathways.


Subject(s)
Myoglobin/chemistry , Animals , Energy Transfer , Horses , Ligands , Motion , Optics and Photonics
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