Francisco G. Pérez-Gutiérrez

Pump-probe imaging of nanosecond laser-induced bubbles in agar gel

In this paper we show results of Nd:YAG laser-induced bubbles formed in a one millimeter thick agar gel slab. The nine nanosecond duration pulse with a wave length of 532 nm was tightly focused inside the bulk of the gel sample. We present for the first time a pump-probe laser-flash shadowgraphy system that uses two electronically delayed Nd:YAG lasers to image the the bubble formation and shock wave fronts with nanosecond temporal resolution and up to nine seconds of temporal range. The shock waves generated by the laser are shown to begin at an earlier times within the laser pulse as the pulse energy increases. The shock wave velocity is used to infer a shocked to unshocked material pressure difference of up to 500 MPa. The bubble created settles to a quasi-stable size that has a linear relation to the maximum bubble size. The energy stored in the bubble is shown to increase nonlinearly with applied laser energy, and corresponds in form to the energy transmission in the agar gel. We show that the interaction is highly nonlinear, and most likely is plasma-mediated.

Time-resolved study of the mechanical response of tissue phantoms to nanosecond laser pulses

We present a time-resolved study of the interaction of nanosecond laser pulses with tissue phantoms. When a laser pulse interacts with a material, optical energy is absorbed by a combination of linear (heat generation and thermoelastic expansion) and nonlinear absorption (expanding plasma), according to both the laser light irradiance and material properties. The objective is to elucidate the contribution of linear and nonlinear optical absorption to bubble formation. Depending on the local temperatures and pressures reached, both interactions may lead to the formation of bubbles. We discuss three experimental approaches: piezoelectric sensors, time-resolved shadowgraphy, and time-resolved interferometry, to follow the formation of bubbles and measure the pressure originated by 6 ns laser pulses interacting with tissue phantoms. We studied the bubble formation and pressure transients for varying linear optical absorption and for radiant exposures above and below threshold for bubble formation. We report a rapid decay (of 2 orders of magnitude) of the laser-induced mechanical pressure measured (by time-resolved shadowgraphy) very close to the irradiation spot and beyond 1 mm from the irradiation site (by the piezoelectric sensor). Through time-resolved interferometry measurements, we determined that bubble formation can occur at marginal temperature increments as low as 3°C.

Short and ultrashort laser pulse induced bubbles on transparent and scattering tissue models.

Bubble formation is a well identified phenomenon within short (ns) and ultrashort (fs) laser pulses-aqueous media interactions. Bubble formation might be produced by three different mechanisms: (1) optical breakdown, (2) rarefraction wave and (3) overheating of the material. Experiments where transparent and scattering tissue models that mimic biological tissue were irradiated with a Q-switched, 532 nm, 5 nanosecond, Nd:YAG and Ti:sapphire femtosecond laser systems. The type of bubble (transient or permanent) and initial bubble diameter were characterized as a function of time as well as the number of pulses and repetition rate at which they were delivered. Threshold fluence for bubble formation in scattering tissue model was also studied. Two types of bubbles were identified depending on the number of pulses and the repetition rate at which they were delivered: transient (type 1) and permanent (type 2) bubbles. There is an insignificant difference in the fluence required to form a bubble in transparent tissue models regardless of the depth at which the beam was focused; in contrast, for scattering tissue models, the fluence required to form a bubble in deep positions is significantly higher than that of more superficial beam focus positions.

Experimental study of mechanical response of artificial tissue models irradiated with Nd:YAG nanosecond laser pulses

Nanosecond long laser pulses are used in medical applications where precise tissue ablation with minimal thermal and mechanical collateral damage is required. When a laser pulse is incident on a material, optical energy will be absorbed by a combination of linear and nonlinear absorption according to both: laser light irradiance and material properties. In the case of water or gels, the first results in heat generation and thermoelastic expansion; while the second results in an expanding plasma formation that launches a shock wave and a cavitation/boiling bubble. Plasma formation due to nonlinear absorption of nanosecond laser pulses is originated by a combination of multiphoton ionization and thermionic emission of free electrons, which is enhanced when the material has high linear absorption coefficient. In this work, we present three experimental approaches to study pressure transients originated when 6 ns laser pulses are incident on agar gels and water with varying linear absorption coefficient, using laser radiant exposures above and below threshold for bubble formation: (a) PVDF sensors, (b) Time-resolved shadowgraphy and (c) Time-resolved interferometry. The underlying hypothesis is that pressure transients are composed of the superposition of both: shock wave originated by hot expanding plasma resulting from nonlinear absorption of optical energy and, thermoelastic expansion originated by heat generation due to linear absorption of optical energy. The objective of this study is to carry out a comprehensive experimental analysis of the mechanical effects that result when tissue models are irradiated with nanosecond laser pulses to elucidate the relative contribution of linear and nonlinear absorption to bubble formation. Furthermore, we investigate cavitation bubble formation with temperature increments as low as 3 °C.

Reconstruction of laser-induced cavitation bubble dynamics based on a Fresnel propagation approach.

A single laser-induced cavitation bubble in transparent liquids has been studied through a variety of experimental techniques. High-speed video with varying frame rate up to 20×10(7)   fps is the most suitable to study nonsymmetric bubbles. However, it is still expensive for most researchers and more affordable (lower) frame rates are not enough to completely reproduce bubble dynamics. This paper focuses on combining the spatial transmittance modulation (STM) technique, a single shot cavitation bubble and a very simple and inexpensive experimental technique, based on Fresnel approximation propagation theory, to reproduce a laser-induced cavitation spatial dynamics. Our results show that the proposed methodology reproduces a laser-induced cavitation event much more accurately than 75,000 fps video recording. In conclusion, we propose a novel methodology to reproduce laser-induced cavitation events that combine the STM technique with Fresnel propagation approximation theory that properly reproduces a laser-induced cavitation event including a very precise identification of the first, second, and third collapses of the cavitation bubble.

Cell damage extent due to irradiation with nanosecond laser pulses under cell culturing medium and dry environment

Cell mono-layers were irradiated with nanosecond laser pulses under two distinct scenarios: (a) with culturing medium positioning the beam waist at different stand-off distances γ and (b) without cell culturing medium, positioning the beam waist directly on top of the cell mono-layer. Damaged cells were marked with Trypan Blue, a vital cell marker. Three different zones of damage were identified: (1) a zone of complete cell clearance, surrounded by (2) a ring of dead cells marked with Trypan Blue and (3) the rest of the cell culture where the cells remain alive and viable. Different hydrodynamic mechanisms damage cells as it was shown by high speed video for γ=0 and comparison with time resolved imaging. The cell damage mechanism has its origin on the optical breakdown plasma formation. For the case with culturing medium, a combination of plasma formation and shear stresses are responsible for cell damage; wheras for the case without cell culturing medium, the plasma formation is the only mechanism of interaction between laser pulses and cells. The rapidly expanding plasma generates shock waves whose pressure is most likely responsible for the cell detachment observed.

TIME-RESOLVED STUDY OF LASER-INDUCED BUBBLES AND SHOCKWAVES IN AGAR GEL TISSUE PHANTOMS

Laser-tissue interactions have been extensively used in a number of biomedical treatments. However, the high optical absorption in tissue and the use of relatively long laser pulses or, in many cases, cw laser exposure, frequently results in excessive laser-heating producing undesirable collateral damage. Short pulsed lasers are one of the most precise tools for delivering energy and can allow for the greatest finesse [1]. Laser pulses with duration of only a few nanoseconds, and as short as a few hundreds of femtoseconds, seem to be a good alternative to minimize or even suppress laser-heating undesirable effects [2].Copyright

Study of ns and fs Pulse Laser‐Induced Effects in Biological‐Tissue Models and Corneal Tissue

This work presents a study of photo‐induced effects in biological‐tissue models made from agar gel and on porcine cornea samples. We used a Nd:YAG (5 ns) and a Ti:sapphire (90fs) lasers to irradiate the samples. The main objective in this study is to understand some aspects of the interaction between pulsed lasers and biological tissue, of especially interest for us are vascular and corneal tissues. Our research includes laser heating of vascular‐like tissue and laser‐induced cavitation bubble formation in cornea. We will present results of laser heating of vascular‐like tissue, and its dependence on laser fluence and pulse duration. Also, we will present results of cavitation bubble formation for agar gel and corneal tissues. Our results show that there exists a well determined threshold fluence for the onset of bubble formation; the laser‐induced bubbles on agar gel and cornea can be permanent or transient depending on the laser irradiation parameters. Some interesting dermatological and ophthalmic appl...

Passive cooling of cutaneous and subcutaneous tissues using phase changing materials: feasibility study using a numerical model

Abstract In many dermatological applications, lowering the temperature of skin and maintaining specific temperatures for extended periods of time are fundamental requirements for treatment; for example, in targeting adipose tissue and managing cutaneous pain. In this work, we investigate the feasibility of using phase changing materials (PCMs) as an alternative passive, open-loop, heat extraction method for cooling cutaneous and subcutaneous tissues. We used a finite difference parametric approach to model the spatial and temporal progression of the heat transferred from the skin to a PCM in contact with the skin surface. We modelled the thermal performance of different PCMs, including different thicknesses. In addition, we used our model to propose application strategies. Numerical simulations demonstrate the feasibility of using PCMs for extracting heat from the skin and upper fat layers, inducing and maintaining similar temperatures as those induced by active closed-loop cooling with a cold plate. In terms of development, the critical design parameters are the temperature range of solidification of the material, the thickness of the material, and the rate of melting. Our study suggests that PCM-based devices may offer an alternative skin and adipose tissue cooling method that is simple to implement and use.

Study of the effect of temperature on the optical properties of Latin skins

Photodynamic therapy (PDT) is a very effective technique for treatment of certain types of cancer, among the most common, skin cancer. PDT requires the presence of three elements: the photosensitizer, light and oxygen. Penetration depth of light into the tumor depends on both the characteristics of the tissue to be treated and the wavelength. As the light dose to be delivered in each lesion depends on the optical properties of the tissue, all the effects that change these properties should be considered in order to choose suitable doses. There are some studies that have determined the maximum dose of radiation tolerated for certain types of skin, but the influence of the temperature on the optical properties, especially for darker skin types, remains unknown. In this study, we analyzed the optical properties of skin in vivo of different Latin volunteers in order to study the influence of the temperature on the optical properties and thereby to define more precisely the dose of light to be received by each patient in a personalized way. The optical properties of skin in vivo were investigated using an optical system that included an integrating sphere, a tungsten lamp and a spectrophotometer. Such experimental set up-allowed to obtain spectra reflectance of various volunteers and from this measurement, the absorption coefficient was recovered by Inverse Adding Doubling (IAD) program.