Interplay of wavelength, fluence and spot-size in free-electron laser ablation of cornea.

Infrared free-electron lasers ablate tissue with high efficiency and low collateral damage when tuned to the 6-microm range. This wavelength-dependence has been hypothesized to arise from a multi-step process following differential absorption by tissue water and proteins. Here, we test this hypothesis at wavelengths for which cornea has matching overall absorption, but drastically different differential absorption. We measure etch depth, collateral damage and plume images and find that the hypothesis is not confirmed. We do find larger etch depths for larger spot sizes--an effect that can lead to an apparent wavelength dependence. Plume imaging at several wavelengths and spot sizes suggests that this effect is due to increased post-pulse ablation at larger spots.

Wavelength-dependent conformational changes in collagen after mid-infrared laser ablation of cornea.

We ablated porcine corneas with a free electron laser tuned to either 2.77 or 6.45 microm, two matched wavelengths that predominantly target water and protein, respectively. The ejected nonvolatile debris and the crater left behind were examined by circular dichroism, Raman spectroscopy, and scanning electron microscopy to characterize the postablation conformation of collagen proteins. We found near-complete unfolding of collagen secondary and tertiary structure at either ablating wavelength. On the other hand, we found excess fibril swelling and evidence for excess cis-hydroxyproline in the 6.45-microm debris. These results support the hypothesis that the favorable ablative properties of protein-targeting wavelengths rest on selective heating of tissue proteins.

Wavelength-dependent collagen fragmentation during mid-IR laser ablation.

Mid-infrared free-electron lasers have proven adept in surgical applications. When tuned to wavelengths between 6 and 7 microm, such lasers remove defined volumes of soft tissue with very little collateral damage. Previous attempts to explain the wavelength-dependence of collateral damage have invoked a wavelength-dependent loss of protein structural integrity. However, the molecular nature of this structural failure has been heretofore ill-defined. In this report, we evaluate several candidates for the relevant transition by analyzing the nonvolatile debris ejected during ablation. Porcine corneas were ablated with a free-electron laser tuned to 2.77 or 6.45 microm-wavelengths with matched absorption coefficients for hydrated corneas that respectively target either tissue water or protein. The debris ejected during these ablations was characterized via gel electrophoresis, as well as Fourier transform infrared spectroscopy, micro-Raman and 13C-NMR spectroscopy. We find that high-fluence (240 J/cm2) ablation at 6.45 microm, but not at 2.77 microm, leads to protein fragmentation accompanied by the accumulation of nitrile and alkyne species. The candidate transition most consistent with these observations is scission of the collagen protein backbone at N-alkylamide bonds. Identifying this transition is a key step toward understanding the observed wavelength-dependence of collateral damage in mid-infrared laser ablation.

Time-resolved FTIR spectroscopy of the photointermediates involved in fast transient H+ release by proteorhodopsin.

Proteorhodopsin (pR) is a homologue of bacteriorhodopsin (bR) that has been recently discovered in oceanic bacterioplankton. Like bR, pR functions as a light-driven proton pump. As previously characterized by laser flash induced absorption spectroscopy (Krebs, R. A.; Alexiev, U.; Partha, R.; DeVita, A. M.; Braiman, M. S. BMC Physiol. 2002, 2, 5), the pR photocycle shows evidence of light-induced H(+) release on the 10-50 micros time scale, and of substantial accumulation of the M intermediate, only at pH values above 9 and after reconstitution into phospholipid followed by extensive washing to remove detergent. We have therefore measured the time-resolved FTIR difference spectra of pR intermediates reconstituted into DMPC vesicles at pH 9.5. A mixture of K- and L-like intermediates, characterized by a 1516 cm(-1) positive band and a 1742 cm(-1) negative band respectively, appears within 20 micros after photolysis. This mixture decays to an M-like state, with a clear band at 1756 cm(-1) due to protonation of Asp-97. The 50-70 micros rise of M at pH 9.5 is similar to (but a little slower than) the rise times for M formation and H(+) release that were reported earlier based on flash photolysis measurements of pR reconstituted into phospholipids with shorter acyl chains. We conclude that, at pH 9.5, H(+) release occurs while Asp-97 is still protonated; i.e., this aspartic acid cannot be the H(+) release group observed by flash photolysis under similar conditions.

Modeling amino acid side chains in proteins: 15N NMR spectra of guanidino groups in nonpolar environments.

Natural-abundance 15N NMR spectroscopy on dodecylguanidine reveals solvent and protonation effects that model those that could occur for the arginine side chain in proteins. Our results demonstrate that the 15N chemical shifts of the terminal guanine nitrogens strongly depend on the solvent chosen for measurements. A polar H-bond-donating solvent like water has strongly deshielding effects on the neutral guanidine group (with the latter acting predominantly as an H-bond acceptor). As a result, a substantial upfield shift occurs when neutral guanidine is dissolved instead in a non-H-bonding solvent (chloroform). These solvent effects can be as large as those induced by protonation changes. This limits the ability of 15N chemical shifts to distinguish the protonation state of the arginine side chain, at least without specific knowledge of its environment. These results help to reconcile previous interpretations about the protonation state arg-82 in the M state of bacteriorhodopsin based on FTIR and 15N NMR spectroscopy. That is, contrary to earlier conclusions from solid-state NMR, the side chain of arg-82 could undergo a deprotonation between the bR and M states, but only if it also experienced a significant decrease in the H-bonding character and polarity of its environment. In fact, the average 15N chemical shift of the two Neta of arg-82 in bacteriorhodopsin's M intermediate (from the previous NMR measurements) is 17 ppm upfield from the corresponding value for the deprotonated arginine side chain in aqueous solution at pH >14, but only 3 ppm upfield from the value for deprotonated dodecylguanidine in chloroform.

Role of arginine-82 in fast proton release during the bacteriorhodopsin photocycle: a time-resolved FT-IR study of purple membranes containing 15N-labeled arginine.

Arginine-82 has long been recognized as an important residue in bacteriorhodopsin (bR), because its mutation usually results in loss of fast H(+) release, an important step in the normal light-induced H(+) transport mechanism. To help to clarify the structural changes in Arg-82 associated with the H(+)-release step, we have measured time-resolved FT-IR difference spectra of wild-type bR containing either natural-abundance isotopes ((14)N-Arg-bR) or all seven arginines selectively and uniformly labeled with (15)N at the two eta-nitrogens ((15)N-Arg-bR). Comparison of the spectra from the two isotopic variants shows that a 1556 cm(-1) vibrational difference band due to the M photocycle intermediate of (14)N-Arg-bR loses substantial intensity in (15)N-Arg-bR. However, this isotope-sensitive arginine vibrational difference band is only observed at pH 7 and not at pH 4 where fast H(+) release is blocked. These observations support the earlier conclusion, based on site-directed mutagenesis and chemical labeling, that a strong C-N stretch vibration of Arg-82 can be assigned to a highly perturbed frequency near 1555 cm(-1) in the M state of wild-type bR [Hutson et al. (2000) Biochemistry 39, 13189-13200]. Furthermore, alkylguanidine model compound spectra indicate that the unusually low arginine C-N stretch frequency in the M state is consistent with a nearly stoichiometric light-induced deprotonation of an arginine side chain within bR, presumably arginine-82.