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Surface Quality of Femtosecond Dissected Posterior Human Corneal Stroma Investigated With Atomic Force Microscopy

Lombardo M, De Santo MP, Lombardo G, Schiano Lomoriello D, Desiderio G, Ducoli P, Barberi R, Serrao S.
Cornea. 2012 Dec;31(12):1369-75. doi: 10.1097/ICO.0b013e31823f774c.
PMID: 22262224
DOI: 10.1097/ICO.0b013e31823f774c

Abstract

PURPOSE:

To investigate and compare the surface roughness and morphology of posterior stromal lenticules created with a femtosecond laser using various pulse energies to that obtained with a mechanical microkeratome.

METHODS:

A 150 kHz femtosecond laser platform (IntraLase iFS; Abbott Medical Optics) was programmed to create an 8.5-mm-diameter posterior stromal lenticule in 12 human corneal tissues. Specimens were dissected using different pulse energies (1.00, 0.75, 0.65, and 0.50) and fixed 2 μm spot separations. Three additional posterior corneal lenticules were prepared using a mechanical microkeratome (Moria Evolution 3; Moria). After the procedure, each corneal tissue was examined by atomic force microscopy (Autoprobe CP; Veeco).

RESULTS:

Femtosecond laser-treated tissues revealed similar morphological features, however, with significant differences in surface roughness in relation to the energy pulse used for lamellar dissection (P<0.001). The most regular stromal surface was achieved when using 0.50 μJ pulse energy; on the contrary, the roughest specimens were those dissected using 1.00 μJ pulse energy. No differences in surface roughness were measured between mechanically resected tissues and those treated using 0.50 μJ pulse energy (P>0.05).

CONCLUSIONS:

Atomic force microscopy submicron analysis of femtosecond-dissected donor tissues provided quantitative demonstration of the relation between pulse energy and stromal surface roughness. Surface quality of posterior corneal lenticules, comparable with that provided by mechanical microkeratome, is significantly improved when setting pulse energy for lamellar dissection of 0.50-μJ and 2-μm spot separations.

Adaptive Optics Technology for High-Resolution Retinal Imaging

Marco Lombardo, Sebastiano Serrao, Nicholas Devaney, Mariacristina Parravano, and Giuseppe Lombardo
Sensors (Basel). 2013 Jan; 13(1): 334–366. Published online 2012 Dec 27. doi: 10.3390/s130100334
PMID: 23271600
PMCID: PMC3574679
This article has been cited by other articles in PMC.

Abstract

Adaptive optics (AO) is a technology used to improve the performance of optical systems by reducing the effects of optical aberrations. The direct visualization of the photoreceptor cells, capillaries and nerve fiber bundles represents the major benefit of adding AO to retinal imaging. Adaptive optics is opening a new frontier for clinical research in ophthalmology, providing new information on the early pathological changes of the retinal microstructures in various retinal diseases. We have reviewed AO technology for retinal imaging, providing information on the core components of an AO retinal camera. The most commonly used wavefront sensing and correcting elements are discussed. Furthermore, we discuss current applications of AO imaging to a population of healthy adults and to the most frequent causes of blindness, including diabetic retinopathy, age-related macular degeneration and glaucoma. We conclude our work with a discussion on future clinical prospects for AO retinal imaging.

Keywords: adaptive optical systems, optical sensors, biomedical imaging techniques, eye

Optimal Parameters to Improve the Interface Quality of the Flap Bed in Femtosecond Laser-assisted Laser in Situ Keratomileusis

Serrao S, Buratto L, Lombardo G, De Santo MP, Ducoli P, Lombardo M.
J Cataract Refract Surg. 2012 Aug;38(8):1453-9. doi: 10.1016/j.jcrs.2012.05.021.
PMID: 22814052
DOI: 10.1016/j.jcrs.2012.05.021

Abstract

PURPOSE:

To analyze the interface quality of the anterior stroma after femtosecond laser flap creation using atomic force microscopy.

SETTING:

IRCCS Fondazione G.B. Bietti, Rome, Italy.

DESIGN:

Experimental study.

METHODS:

A 110 μm depth flap was created in 20 human corneal tissues using a femtosecond laser platform (Intralase iFS). Tissues were divided into 4 groups of various cutting parameters: pulse energy and spot separation of 0.75 μJ and 6 μm (Group 1), 0.65 μJ and 5 μm (Group 2), 0.55 μJ and 4 μm (Group 3), and 0.45 μJ and 4 μm (Group 4). Four additional tissue sections were cut using a motorized microkeratome (Hansatome). Atomic force microscopy (Autoprobe CP) analysis was performed on the stromal bed of each sample.

RESULTS:

The corneal tissues treated with higher pulse energies and wider spot separations (Groups 1 and 2) showed a rougher stromal bed interface (root mean square [RMS] rough = 0.23 μm ± 0.008 (SD) and 0.24 ± 0.009 μm, respectively) than tissues in Groups 3 and 4 (RMS rough = 0.18 ± 0.006 μm and 0.18 ± 0.008 μm, respectively; P<.001, 1-way analysis of variance). The stromal surface quality of tissues treated with pulse energies of 0.55 μJ or lower and 4 μm spot separation compared favorably with that of tissues cut by the microkeratome (RMS rough = 0.17 ± 0.006 μm; P>.05, Tukey).

CONCLUSIONS:

The femtosecond stromal interface quality was improved with pulse energy lower and spot separations narrower than those currently used in the clinical setting. The flap interface smoothness created by the femtosecond laser was comparable to that created by the microkeratome.

FINANCIAL DISCLOSURE:

No author has a financial or proprietary interest in any material or method mentioned.

Copyright © 2012 ASCRS and ESCRS. Published by Elsevier Inc. All rights reserved.

Adaptive Optics Photoreceptor Imaging

Lombardo M, Lombardo G, Ducoli P, Serrao S.
Ophthalmology. 2012 Jul;119(7):1498-1498.e2. doi: 10.1016/j.ophtha.2012.03.019.
PMID: 22749092
DOI: 10.1016/j.ophtha.2012.03.019

In the present study, we investigated the cone packing density distribution along the horizontal meridian passing through the fovea in a population of young healthy subjects using a compact Adaptive Optics (AO) retinal camera (rtx1, Imagine Eyes, Orsay, France).

Nineteen healthy volunteer subjects (5 men and 14 women; age range, 24–38 years) participated in this study and gave a written informed consent. All subjects had 20/20 or better monocular best-corrected visual acuity and the spherical equivalent refractive errors ranged from −0.25 to −5.75 diopters (D) with astigmatism less than −1.50 D when referenced to the spectacle plane. The axial length (AxL) ranged between 22.61 and 26.29 mm. The protocol had approval of the local Ethical Committee and adhered to the tenets of Declaration of Helsinki. Exclusion criteria for this study included any ocular or systemic diseases.

Adaptive Optics imaging sessions were conducted after the pupils were dilated with 1 drop each of 0.5% tropicamide and 10% phenylephrine hydrochloride. A program provided by manufacturer correlated and averaged the captured image frames to reduce noise artefacts and produce a final image. Image analysis of the photoreceptor mosaic was performed using Image J (version 1.45a; NIH, Bethesda, MD). Cone density (cells/mm2) was estimated within two 50×50 μm windows at specified eccentricities (250-, 420-, 760- and 1300-μm) from the foveal center (Fig 1; available https://www.aaojournal.org). The spectacle-corrected magnification factor (RMFcorr) was determined in all the eyes.

With the exception of the central fovea (<160 μm), the photoreceptor structure was well resolved in most of the eyes. Cones were in close proximity to each other at 200 μm from the foveal center; at increasing retinal eccentricities, cones tended to become progressively larger and the intercellular space was wider between cells, with rods intruding between cones (Fig 2; available at https://www.aaojournal.org), in accordance with the histologic studies of the human retina.1 A variation in brightness between adjacent areas of cones was seen in all the eyes. The mean cone density was 50 574±6031 cells/mm2 at 250 μm eccentricity, falling to 14 198±2114 cells/mm2 at 1300 μm eccentricity (analysis of variance [ANOVA]; P<0.05). In general, subjects with higher cone density close to the foveal center had higher cone density at increasing eccentricities. The intersubject variability in parafoveal cone density distribution, estimated by the coefficient of variation, was within 15%.

Adaptive Optics technology opens a new frontier for the research in clinical Ophthalmology. The accurate measurements of retinal microscopic sized features in normal populations, according to age, refractive defects, etc., represents the basis for detecting early pathological changes of the photoreceptor layer. The cone density found in the present study could be considered representative of a healthy population of myopic adults. In previous works using AO- scanning laser ophthalmoscope (SLO), Li et al2 found an average decline in cone density from ∼120 000 to ∼45 000 cell/mm2 from 0.10– to 0.30–mm eccentricity from the foveal center in a population of 18 adult young subjects (23–43 years; AxL 22.86–28.31 mm). Chui et al3 found an average cone density of ∼35 000 cell/mm2 at 0.5 mm, ∼20 000 cell/mm2 at 1.0 mm, and ∼12 000 cell/mm2 at 1.5 mm eccentricity from the fovea respectively in 11 subjects (21–31 years; AxL: 22.00–28.00 mm). Song et al4 found a mean cone density of ∼70 000 cell/mm2 at 0.18 mm from the fovea falling to 37 000 cell/mm2 and 19 000 cell/mm2 at 0.5- and 1.1-mm eccentricity respectively in a population of 10 young adults (22–35 years; AxL, 22.10–26.30 mm).

We based our method of cone counting on the results of a previous work by Hirsch and Miller.5 The authors demonstrated that a 56×56 μm was less subject to error than smaller window sizes when estimating cone density across increasing eccentricity from the fovea. Previous authors recently used a 50×50 μm sampling window to locate cone photoreceptor positions,4 further showing a high repeatability in cone density estimates taken 6 months apart at the same retinal location.

Data on populations of healthy eyes are fundamental in characterizing the density, distribution, and appearance of normal photoreceptor cells in vivo. This will permit measurement of the normal ranges, which allows comparison with pathological photoreceptors, even in early stages of retinal diseases.

Variations in Image Optical Quality of the Eye and the Sampling Limit of Resolution of the Cone Mosaic with Axial Length in Young Adults

Lombardo M, Serrao S, Ducoli P, Lombardo G.
J Cataract Refract Surg. 2012 Jul;38(7):1147-55. doi: 10.1016/j.jcrs.2012.02.033.
PMID: 22727285
DOI: 10.1016/j.jcrs.2012.02.033

Abstract

PURPOSE:

To evaluate the variation in higher-order ocular wavefront aberrations and the Nyquist limit of resolution of the cone mosaic (N(c)) in a population of young healthy subjects and the relation to axial length (AL).

SETTING:

Fondazione G.B. Bietti IRCCS, Rome, Italy.

DESIGN:

Case series.

METHODS:

An adaptive optics retinal camera prototype (rtx1) was used to image the cone mosaic. Cone density and N(c) were calculated at fixed eccentricity between 260 μm and 600 μm from the foveal center. Ocular higher-order wavefront aberrations were measured using the OPD Scan II device. The coefficient of variation (CoV) was used to analyze the variation in optical and retinal parameters. The correlation of optical and retinal parameters with AL was performed using Pearson analysis.

RESULTS:

Twelve subjects (age 24 to 38 years; AL 22.61 to 26.63 mm) were evaluated. A high interindividual variation in the higher-order wavefront aberrations was found, ranging from 26% for corneal higher-order aberrations (HOAs) to 41% for intraocular HOAs. The CoV of cone density and N(c) were 16% and 5%, respectively. The decline in cone density and N(c) with AL was statistically significant at all retinal eccentricities (R(2) > 0.44, P<.001).

CONCLUSIONS:

Although there appeared to be random variation in the eye's optical wavefront aberration from subject to subject, the cone-packing density and N(c) were highly correlated with AL. Although the eye's overall image optical quality in the emmetropic group and the myopic group was comparable, the spatial sampling of the cone mosaic decreased with increasing AL.

FINANCIAL DISCLOSURE:

No author has a financial or proprietary interest in any material or method mentioned.

Copyright © 2012 ASCRS and ESCRS. Published by Elsevier Inc. All rights reserved.

Femtosecond Laser Photodisruptive Effects on the Posterior Human Corneal Stroma Investigated with Atomic Force Microscopy

Abstract

PURPOSE:

To analyze the effects of femtosecond laser pulses on the posterior human corneal stroma with atomic force microscopy (AFM) and environmental scanning electron microscopy (ESEM).

METHODS:

A femtosecond laser (IntraLase iFS, Abbott, USA) was programmed to create a full posterior lamellar dissection in 9 human corneal tissues, using 3 different pulse energies (1.00 µJ, 0.75 µJ, and 0.50 µJ). Three corneal tissues were prepared in a similar fashion using a mechanical microkeratome (Moria Evolution 3, Moria, France). Six corneal tissues received an 8.00-mm diameter full cylindrical resection using either the femtosecond laser or the Barron trephine (Katena Products Inc., USA). The posterior corneal lenticules were first examined at AFM (Autoprobe CP, Veeco, USA). Both the posterior lenticules and the trephined corneal samples were scanned by ESEM (FEI Quanta 400, USA).

RESULTS:

Granules and crater-like features were observed on the stromal interface of all the laser dissected tissues, likely due to a secondary thermal effect of femtosecond laser dissection. Collagen fibers were seen only on samples treated with the 0.50 µJ pulse energy. Images of an even stromal surface were observed on the posterior stroma of mechanically dissected corneal samples.

CONCLUSIONS:

Mechanical and thermal effects, induced by femtosecond laser pulses on the human corneal stroma, were seen with AFM. Surface regularity of the photodisrupted stroma was inversely and non-linearly related to the pulse energy. The femtosecond laser provided high surface quality for lamellar resection of the posterior stroma comparable to those provided by mechanical devices.

Biomechanics of the Anterior Human Corneal Tissue Investigated with Atomic Force Microscopy

Lombardo M, Lombardo G, Carbone G, De Santo MP, Barberi R, Serrao S.
Invest Ophthalmol Vis Sci. 2012 Feb 29;53(2):1050-7. doi: 10.1167/iovs.11-8720.
PMID: 22266511
DOI: 10.1167/iovs.11-8720

Abstract

PURPOSE:

To investigate the biomechanics of the anterior human corneal stroma using atomic force microscopy (AFM).

METHODS:

AFM measurements were performed in liquid on the anterior stroma of human corneas, after gently removing the epithelium, using an atomic force microscope in the force spectroscopy mode. Rectangular silicon cantilevers with tip radius of 10 nm and spring elastic constants of 25- and 33-N/m were used. Each specimen was subjected to increasing loads up to a maximum of 2.7 μN with scan speeds ranging between 3- and 95-μm/s. The anterior stromal hysteresis during the extension-retraction cycle was quantified as a function of the application load and scan rate. The elastic modulus of the anterior stroma was determined by fitting force curve data to the Sneddon model.

RESULTS:

The anterior stroma exhibited significant viscoelasticity at micrometric level: asymmetry in the curve loading-unloading response with considerable hysteresis dependent both on the application load and scan rate (P < 0.01). The mean elastic modulus ranged between 1.14 and 2.63 MPa and was constant over the range of indentation depths between 1.0 and 2.7 μm in the stroma.

CONCLUSIONS:

At microscale level, the mechanical response of the most anterior stroma is complex and nonlinear. The microstructure (fibers' packing, number of cross-links, water content) and the combination of elastic (collagen fibers) and viscous (matrix) components of the tissue influence the type of viscoelastic response. Efforts in modeling the biomechanics of human corneal tissue at micrometric level are needed.