Photodissociation of isolated ferric heme and heme-His cations in an electrostatic ion storage ring.

Photodissociation of isolated Fe(III)-heme(+) and Fe(III)-heme(+)(His) ions in the gas phase has been investigated using an electrostatic storage ring. The experiment provides three pieces of information, namely fragmentation channels, dissociation times, and absorption spectra. After photoexcitation with either 390 or 532 nm light, we find that the fragmentation takes place on a microsecond to millisecond time scale, and the channels are CH(2)COOH loss (beta-cleavage reaction) and histidine loss from Fe(III)-heme(+) and Fe(III)-heme(+)(His), respectively. These channels were also observed by means of collision-induced dissociation. Significant information on the nonradiative processes that occur after photoexcitation was revealed from the decay spectra. At early times (first two to three milliseconds), the decay of the photoexcited ions is well-described by a statistical model based on an Arrhenius-type expression for the rate constant. The activation energy and preexponential factor are 1.9 +/- 0.2 eV and 1 x 10(17) to 1 x 10(21) s(-1) for heme(+) and 1.4 +/- 0.2 eV and 1 x 10(16) to 1 x 10(19) s(-1) for heme(+)(His). Decay on a longer time scale was also observed and is ascribed to the population of lower-lying states with higher spin multiplicity because intersystem crossing back to the electronic ground-state is a bottleneck for the dissociation. The measurements give lifetimes for these lower-lying states of about 10 ms after 390 nm excitation and we estimate the probability of spin flip to be 0.3 and 0.8 for heme(+) and heme(+)(His), respectively.

Photodissociation of protonated tryptophan and alteration of dissociation pathways by complexation with crown ether.

The behavior of protonated tryptophan (TrpH(+)) and its complex with 18-crown-6-ether (CE) after photoexcitation has been explored based on measurements of dissociation lifetimes, fragmentation channels, and absorption spectra using an electrostatic ion storage ring. A recent implementation of pulsed power supplies for the ring elements with microsecond response times allows us to identify the daughter ion fragment masses and to disentangle fragmentation that occurs from excited states immediately after photoexcitation from that occurring on a longer time scale of several microseconds to milliseconds. We find that attachment of crown ether significantly alters the dissociation channels since it renders the pisigma(*)(NH(3)) state inaccessible and hence prevents the N-H bond breakage which is an important fragmentation channel of TrpH(+). As a result, on a long time scale (>10 micros), photoexcited TrpH(+)(CE) decays exponentially whereas TrpH(+) displays a power-law decay. The only ions remaining in the latter case are Trp(+) radical cations with a broad internal energy distribution caused by the departing hydrogen. Large changes in the fragment branching ratios as functions of excitation wavelength between 210 and 290 nm were found for both TrpH(+) and TrpH(+)(CE).

A Soret marker band for four-coordinate ferric heme proteins from absorption spectra of isolated Fe(III)-Heme+ and Fe(III)-Heme+(His) ions in vacuo.

In this work, we report the absorption spectra in the Soret band region of isolated Fe(III)-heme+ and Fe(III)-heme+(His) ions in vacuo from action spectroscopy. Fe(III)-heme+ refers to iron(III) coordinated by the dianion of protoporphyrin IX. We find that the absorption of the five-coordinate complex is similar to that of pentacoordinate metmyoglobin variants with hydrophobic binding pockets except for an overall blueshift of about 16 nm. In the case of four-coordinate iron(III), the Soret band is similar to that of five-coordinate iron(III) but much narrower. These spectra serve as a benchmark for theoretical modeling and also serve to identify the coordination state of ferric heme proteins. To our knowledge this is the first unequivocal spectroscopic characterization of isolated 4c ferric heme in the gas phase.

A new technique for time-resolved daughter ion mass spectrometry on the microsecond to millisecond time scale using an electrostatic ion storage ring.

A new method for time-resolved daughter ion mass spectrometry is presented, based on the electrostatic ion storage ring in Aarhus, ELISA. Ions with high internal energy, e.g., as a result of photoexcitation, dissociate and the yield of neutrals is monitored as a function of time. This gives information on lifetimes in the microsecond to millisecond time range but no information on the fragment masses. To determine the dissociation channels, we have introduced pulsed supplies with switching times of a few microseconds. This allows rapid switching from storage of parent ions to storage of daughter ions, which are dumped into a detector after a number of revolutions in the ring. A fragment mass spectrum is obtained by monitoring the daughter ion signal as a function of the ring voltages. This technique allows identification of the dissociation channels and determination of the time dependent competition between these channels.

Electron-capture-induced dissociation of protoporphyrin IX ions.

Electron-capture induced dissociation of protoporphyrin cations and anions has been studied. The cations captured two electrons in two successive collisions and were converted to the corresponding even-electron anions. About one fifth of the ions lost a hydrogen atom to become radical anions but otherwise very little fragmentation was observed. The anions captured an electron to become dianions. No hydrogen loss occurred, and the only fragmentation channel observed was loss of CO2H, to give a doubly charged carbanion. Our results indicate that protoporphyrin ions are very efficient in accommodating one or even two electrons in the lowest unoccupied molecular orbital of the porphyrin macrocycle, and that electron capture induces only limited dissociation.