The Semiquinone-Iron Complex of Photosystem II: Structural Insights from ESR and Theoretical Simulation; Evidence that the Native Ligand to the Non-Heme Iron Is Carbonate
| dc.contributor.author | Cox, Nicholas | |
| dc.contributor.author | Jin, Lu | |
| dc.contributor.author | Jaszewski, Adrian | |
| dc.contributor.author | Smith, Paul J. | |
| dc.contributor.author | Krausz, Elmars | |
| dc.contributor.author | Rutherford, A. William | |
| dc.contributor.author | Pace, Ronald | |
| dc.date.accessioned | 2016-03-24T00:03:19Z | |
| dc.date.available | 2016-03-24T00:03:19Z | |
| dc.date.issued | 2009 | |
| dc.date.updated | 2016-06-14T08:59:43Z | |
| dc.description.abstract | The semiquinone-iron complex of photosystem II was studied using electron spin resonance (ESR) spectroscopy and density functional theory calculations. Two forms of the signal were investigated: 1), the native g approximately 1.9 form; and 2), the g approximately 1.84 form, which is well known in purple bacterial reaction centers and occurs in photosystem II when treated with formate. The g approximately 1.9 form shows low- and high-field edges at g approximately 3.5 and g < 0.8, respectively, and resembles the g approximately 1.84 form in terms of shape and width. Both types of ESR signal were simulated using the theoretical approach used previously for the BRC complex, a spin Hamiltonian formalism in which the semiquinone radical magnetically interacts (J approximately 1 cm(-1)) with the nearby high-spin Fe(2+). The two forms of ESR signal differ mainly by an axis rotation of the exchange coupling tensor (J) relative to the zero-field tensor (D) and a small increase in the zero-field parameter D ( approximately 6 cm(-1)). Density functional theory calculations were conducted on model semiquinone-iron systems to identify the physical nature of these changes. The replacement of formate (or glutamate in the bacterial reaction centers) by bicarbonate did not result in changes in the coupling environment. However, when carbonate (CO(3)(2-)) was used instead of bicarbonate, the exchange and zero-field tensors did show changes that matched those obtained from the spectral simulations. This indicates that 1), the doubly charged carbonate ion is responsible for the g approximately 1.9 form of the semiquinone-iron signal; and 2), carbonate, rather than bicarbonate, is the ligand to the iron. | |
| dc.description.sponsorship | The authors acknowledge the support of the Australian Research Council. A.R.J. thanks the University of Wroclaw for a two-year sabbatical for allowing a postdoctoral fellowship at Australian National University. The computations were performed using the Wroclaw Center of Networking and Supercomputing (grant No. 48) facility. A.W.R. was supported by the Research School of Chemistry as the Craig Professor, as a visiting research fellow, and by the France Australia Science and Technology Program (FAST). | en_AU |
| dc.identifier.issn | 0006-3495 | en_AU |
| dc.identifier.uri | http://hdl.handle.net/1885/100874 | |
| dc.publisher | Biophysical Society | |
| dc.rights | © 2009 by the Biophysical Society | |
| dc.source | Biophysical Journal | |
| dc.subject | absorption | |
| dc.subject | benzoquinones | |
| dc.subject | carbonates | |
| dc.subject | computer simulation | |
| dc.subject | electron spin resonance spectroscopy | |
| dc.subject | iron | |
| dc.subject | ligands | |
| dc.subject | photosystem ii protein complex | |
| dc.subject | quantum theory | |
| dc.subject | spinacia oleracea | |
| dc.subject | temperature | |
| dc.title | The Semiquinone-Iron Complex of Photosystem II: Structural Insights from ESR and Theoretical Simulation; Evidence that the Native Ligand to the Non-Heme Iron Is Carbonate | |
| dc.type | Journal article | |
| local.bibliographicCitation.issue | 7 | en_AU |
| local.bibliographicCitation.lastpage | 2033 | en_AU |
| local.bibliographicCitation.startpage | 2024 | en_AU |
| local.contributor.affiliation | Cox, Nicholas, College of Physical and Mathematical Sciences, CPMS Research School of Chemistry, RSC General, The Australian National University | en_AU |
| local.contributor.affiliation | Jin, Lu, College of Physical and Mathematical Sciences, CPMS Research School of Chemistry, RSC General, The Australian National University | en_AU |
| local.contributor.affiliation | Jaszewski, Adrian, College of Physical and Mathematical Sciences, CPMS Research School of Chemistry, RSC General, The Australian National University | en_AU |
| local.contributor.affiliation | Smith, Paul, College of Physical and Mathematical Sciences, CPMS Research School of Chemistry, RSC General, The Australian National University | en_AU |
| local.contributor.affiliation | Krausz, Elmars, College of Physical and Mathematical Sciences, CPMS Research School of Chemistry, RSC General, The Australian National University | en_AU |
| local.contributor.affiliation | Rutherford, Alfred W, CEA-Saclay, France | en_AU |
| local.contributor.affiliation | Pace, Ronald, College of Physical and Mathematical Sciences, CPMS Research School of Chemistry, RSC General, The Australian National University | en_AU |
| local.contributor.authoruid | u3286768 | en_AU |
| local.description.notes | Imported from ARIES | en_AU |
| local.identifier.absfor | 030606 | en_AU |
| local.identifier.absfor | 030699 | en_AU |
| local.identifier.ariespublication | u4217927xPUB417 | en_AU |
| local.identifier.citationvolume | 97 | en_AU |
| local.identifier.doi | 10.1016/j.bpj.2009.06.033 | en_AU |
| local.identifier.essn | 1542-0086 | en_AU |
| local.identifier.scopusID | 2-s2.0-70349928560 | |
| local.identifier.thomsonID | 000270586000025 | |
| local.publisher.url | http://www.biophysics.org/ | en_AU |
| local.type.status | Published Version | en_AU |