Proceedings Volume 2391

Laser-Tissue Interaction VI

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Proceedings Volume 2391

Laser-Tissue Interaction VI

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Volume Details

Date Published: 22 May 1995
Contents: 18 Sessions, 74 Papers, 0 Presentations
Conference: Photonics West '95 1995
Volume Number: 2391

Table of Contents

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Table of Contents

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  • Ocular Laser Effects I
  • Ocular Laser Effects II
  • Ocular Laser Effects III
  • Ocular Laser Effects IV
  • Photothermal Mechanisms
  • Photomechanical Mechanisms
  • Photochemical Mechanisms
  • Photo-Photo!
  • Imaging Transient Phenomena
  • Ablation I
  • Ablation II
  • Ablation III
  • Optical Dynamics
  • Thermal Effects I
  • Thermal Effects II
  • Hemothological Research
  • Basic Research
  • Hemothological Research
  • Clinical Research
  • Hemothological Research
  • Optical Dynamics
  • Thermal Effects II
  • Ablation III
Ocular Laser Effects I
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Retinal threshold studies for nanosecond and picosecond visible laser pulses
William P. Roach, Cheryl Dawn DiCarlo, Gary D. Noojin, et al.
Threshold measurements for Minimum Visible Lesions (MVL) at the retina are reported for 60 picoseconds (ps) and 4 nanoseconds (ns), single laser pulses in rhesus monkey eyes using a visible wavelength of 532 nanometers (nm) from a doubled Nd:YAG laser. The 50% probability for damage (ED50) dosages are calculated for 1 hour and 24 hour post exposures using 95% fiducial limits. For both pulsewidths, the threshold values calculated by probit analysis decrease between the 1 hour and 24 hour ophthalmoscopic evaluations. The ED50 value determined for the 60 ps pulsewidth was less than half the value at 4 ns (0.43 (mu) J/60 ps vs. 0.90 (mu) J/4 ns at 24 hours) for both readings. Of the 136 exposures for pulse energies ranging from 0.03 to 5.0 (mu) J no hemorrhagic lesions were produced for either pulsewidth studied. However, at 6.6 (mu) J one intraretinal hemorrhagic lesion was observed for 60 ps. The slope of the probit curve was higher for 60 ps when compared with the 4 ns value (3.03 at 60 ps vs. 2.68 at 4 ns). MVL threshold doses calculated are comparable with those reported in the literature. However, the 4 ns MVL values is less than one order of magnitude (a factor 4.7) above the Maximum Permissible Exposure (MPE) level as defined by the 'American National Standard For The Safe Use Of Lasers', ANSI Z136.1-19932. We present the current MVL data as it compares with previous data obtained for picosecond and femtosecond laser pulse thresholds and provide a preliminary assessment of how the ANSI MPE standard might be amended.
In vivo imaging of the development of linear and nonlinear retinal laser effects using optical coherence tomography in correlation with histopathological findings
Reginald Birngruber, Michael R. Hee, Stephen A. Boppart, et al.
Optical Coherence Tomography (OCT) is a new, non-invasive diagnostic technique for high resolution optical 3D imaging, which was developed and applied to several different biological materials during the lasi; five years [1, 2, 3]. A unique application ofthis technique is the microscopical cross-sectional imaging ofpostenor structures ofthe eye which are not accessable with other high resolution techniques in-vivo neither with x-ray-imaging nor with high frequency ultrasound scanning. The superior spatial resolution on the order ofabout lOtm laterally and axially, the high signal-to-noise ratio ofmore than 100 db and the fast acquisition-time of one second for a two dimensional scan provides a technique for cross-sectional in-vivo-momtoring ofintraocular structures and therefore the possibility to study the time course of anatomical and pathological developments in the eye. The acute morphological changes of ocular structures and their biological healing response after shortterm impacts such as high-intensity laser exposures are ofparticular interest for the understanding of the mechanisms responsible for therapeutic laser-application in ophthal-mology as well as for laser injury to the eye. A correlation between cross-sectional OCT-images and structural findings using classical histopathological techniques facilitates a better interpretation ofthe characteristic patterns seen in OCTimages and defines the sensitivity ofthe OCT-technique to image morphological details. On the other hand preparational artefacts not avoidable in all histological procedures can be identified and analyzed by comparing histological micrographs with OCT-images of exactly the same structure. First results of an experimental study where retinal effects were produced in monkey eyes using laser pulses from 200 ms to 130 fs in duration are presented in this article. The applied energies from 5tJ to 50 mJ were able to induce the whole spectrum of biological effects possible in the eye, ranging from intraretinal microruptures to extensive thermal denaturation and massive preretinal hemorrhages [4, 5, 6].
Ocular Laser Effects II
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Ultrashort pulse laser induced bubble creation thresholds in ocular media
The measurement and characterization of laser induced breakdown (LIB) in ocular media for ultrashort (< 1 ns) laser pulses is important in understanding both eye damage mechanisms and various ophthalmic applications. In particular, the American National Standards Institute laser safety standards (ANSI Z136.1-1993) have included only guidance but no definitive safety limits due to lack of both experimental data and quantitative understanding of the damage processed induced by ultrashort pulses. Moreover, LIB needs to be understood fully for the growing number of ophthalmic applications which employ LIB in beneficial ways, such as in capsulotomies and iridotomies. The threshold for gas bubble creation from a plasma induced by 100 fs, 400 fs, and 2.4 ps laser pulses at 0.58 micrometers was determined for various ocular media. Bubble creation was used as the endpoint for indication of LIB at these pulse durations due to the absence of broadband visible light emission (plasma spark) that is normally the indication of LIB at longer pulse durations. In addition, light emitted from the focal region was shown to come from gas breakdown within the bubbles produced by previous pulses when the laser was fired at 10 Hz. The difference in endpoints observed for ultrashort pulses and endpoints observed for longer pulses (> 30 ps) may result from aberrations in the optical setup, in particular the focusing optics. However, the nonlinear phenomena involved may play an important role in the observation of a different type of plasma. The cause and reduction of aberrations and the endpoints for LIB threshold studies are discussed.
In vivo laser-induced breakdown in the rabbit eye
Clarence P. Cain, Cheryl Dawn DiCarlo, Paul K. Kennedy, et al.
Threshold measurements for femtosecond laser pulsewidths have been made for retinal minimum visible lesions (MVLs) in Dutch Belted rabbit and rhesus monkey eyes. Laser-induced breakdown (LIB) thresholds in biological materials including vitreous, normal saline, tap water, and ultrapure water have been measured and reported using an artificial eye. We have recorded on video the first LIB causing bubble formation in any eye in vivo using albino rabbit eyes (New Zealand white) with 120- femtosecond (fs) pulses and pulse energies as low as 5 microjoules ((mu) J). These bubbles were clearly formed anterior to the retina within the vitreous humor and, with 60 (mu) J of energy, they lasted for several seconds before disappearing and leaving no apparent damage to the retina. We believe this to be true LIB because of the lack of pigmentation or melanin granules within the albino rabbit eye (thus no absorptive elements) and because of the extremely high peak powers within the 5-(mu) J, 120-fs laser pulse. These high peak powers produce self-focusing of the pulse within the vitreous. The bubble formation at the breakdown site acts as a limiting mechanism for energy transmission and may explain why high-energy femotsecond pulses at energies up to 100 (mu) J sometimes do not cause severe damage in the pigmented rabbit eye. This fact may also explain why it is so difficult to produce hemorrhagic lesions in either the rabbit or primate eye with 100-fs laser pulses.
First-order model for computation of laser-induced breakdown thresholds in condensed media
An analytic, first-order model has been developed to calculate irradiance thresholds for laser-induced breakdown (LIB) in condensed media, including fluids and ocular media. The model is derived from the simple rate equation formalism of Shen for cascade breakdown in solids and from the theory of multiphoton ionization in condensed media developed by Keldysh. Analytic expressions have been obtained for the irradiance thresholds corresponding to multiphoton breakdown, to cascade breakdown, and to initiation of cascade breakdown by multiphoton ionization of seed electrons (multiphoton initiation threshold). The model has been incorporated into a computer code and code results compared to experimentally measured irradiance thresholds for breakdown of ocular media, saline, and water by nanosecond, picosecond, and femtosecond laser pulses in the visible and near-infrared. Theoretical values match experiment to within a factor of 2 or better, over a range of pulsewidths spanning five orders of magnitude, a reasonably good match for a first order model.
Laser-induced bubble formation in the retina
Bernard S. Gerstman, Charles R. Thompson, Steven L. Jacques, et al.
Bubble formation in the retinal pigment epithelium by submicrosecond laser pulses may be a source of laser induced retinal damage. Heat conduction away from absorbing melanin granules requires timescales on the order of microseconds. For pulses of shorter duration, all energy absorbed is effectively absorbed as a (delta) -function in time, and energy concentration may be high enough to cause vaporization of the surrounding medium. This occurs at lower fluences than required for thermal denaturation of a significant volume of cellular material. The adiabatic nature of the absorption and subsequent expansion is used to develop expressions for the calculation of maximum bubble size as a function of laser intensity and melanosome properties such as radius and absorption coefficients. We describe the analysis that went into the development of the bubble size expression and also present the results for representative calculations of maximum bubble radius. We find that our expression leads to a threshold for the formation of bubbles in the retinal pigment epithelium that is close to the ED50 experimentally measured for laser induced retinal damage.
Ocular Laser Effects III
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Experimental investigations and numerical modeling of shock wave emission and cavitation bubble generation by picosecond and nanosecond optical breakdown
Alfred Vogel, Ulrich Parlitz, Stefan Busch
We present experimental investigations and numerical calculation of the shock wave emission and cavitation bubble expansion after optical breakdown in water with Hd:YAG laser pulses of 30 ps and 6 ns duration. The experimental investigations were done by time-resolved photography with a time resolution of 30 ps, or 6 ns, respectively, and a spatial resolution of 4 micrometers . Position and velocity of both the shock front and the bubble wall were determined, and the shock wave pressure p(r) was then calculated from the shock velocity. Calculations of the bubble formation and shock wave emission were performed using the Gilmore model of cavitation bubble dynamics. The calculations yield the dynamics of the bubble wall, the pressure evolution p(t) inside the bubble, and pressure profiles in the surrounding liquid at fixed times after the start of the laser pulse. The maximal shock wave pressure was measured to be 2400 MPa after a 1 mJ ns-pulse, and 1700 MPa after a ps-pulse of the same energy. The initial shock wave duration was slightly shorter for the ns-pulse than for the ps-pulse, and had a (calculated) value of 30 ns and 46 ns, respectively. Due to nonlinear effects, the duration increased to about 75 ns (measured for the ps-pulse) during propagation of the first few millimeters. A formation phase of the shock front was observed after the ns-pulse, but not after the ps-pulse, where the shock front arose within less than 100 ps after the end of the laser pulse. After shock front formation, the pressure decay was approximately proportional to r-2. The maximal bubble wall velocity was 1850 m/s after the 1 mJ ns-pulse, and 780 m/s after the ps-pulse. In general, good agreement was observed between the results of the calculations and the experimental data. The Gilmore model is therefore well suited to calculate the shock wave emission and the initial phase of bubble expansion after laser-induced plasma generation. Since it can cover a wide parameter range, it may serve as a tool for the optimization of laser parameters in medical laser applications.
Effect of nonlinear optical phenomena on retinal damage
Recent studies of retinal damage due to ultrashort laser pulses have shown interesting behavior. Laser thresholds for retinal damage from ultrashort (i.e. <EQ 1 ns) laser pulses are produced at lower energies than in the nanosecond (ns) to microsecond (microsecond(s) ) laser pulse regime. We examine how nonlinear optical phenomena affect the characteristics of light impinging the retina and hence, changes the minimum energy required to produce damage. Nonlinear optical phenomena which occur in homogeneous materials like the ocular media include self-focusing, stimulated Brillouin scattering, supercontinuum generation, laser induced breakdown, and nonlinear absorption. We will discuss all relevant thresholds and determine which nonlinear optical phenomena play a role in mediating the reduction in energy required to produce minimum visible lesion damage to the retina.
Electron paramagnetic resonance spectroscopy of free radicals in corneal tissue following excimer laser irradiation
George H. Pettit M.D., Marwood N. Ediger, D. W. Hahn, et al.
Electron paramagnetic resonance spectroscopy (EPR) has been used to examine free radical formation during corneal tissue photoablation. Bovine corneal strips were frozen in liquid nitrogen, irradiated with excimer laser pulses, and assayed by EPR. Exposure conditions were varied to study radical formation dependence on laser intensity and repetition rate. Results were measured against a quantifiable standard to calculate radical quantum yield. EPR measurements indicate that corneal radical formation is largely a photochemical process driven by the 193 nm laser radiation. Reactive radical species are produced in substantial numbers, and likely have a significant clinical role.
Integrated light spectroscopy of laser-induced breakdown in aqueous media
David J. Stolarski, Jennifer M. Hardman, Craig M. Bramlette, et al.
In the scientific literature there is little information that describes the fundamental physical processes of laser induced breakdown (LIB) in transparent liquids. Our goal is to characterize these fundamental properties, which are critical to the understanding of retinal and other ophthalmic damage produced by ultrashort laser pulses. Laser pulses of 5.0 nanoseconds (ns) at less than 5.0 milli-Joules (mJ) per pulse and pulses of 80 picoseconds (ps) at 0.5 to 1.5 mJ per pulse from a Nd:YAG regenerative amplifier were used to produce LIB in a variety of aqueous media. These include physiological saline solution, triple-distilled water, and tap water. The resulting luminescent plasmas were analyzed using integrated light spectroscopy from a Chromex 0.25 meter (m) spectrograph. Plasmas were recorded in the wavelength region from 300 to 900 nm. Each spectrum obtained was analyzed using a Planck distribution for blackbody emission. The surface temperatures of the plasmas for the two pulse durations were computed to be in the 5000 K to 10,000 K range, depending on the pulse duration and energy. Also, the spectrographs from the saline solution included distinct spectral lines of emission over the broad band spectra, such as the 589 nm atomic emission line of sodium. We will discuss the time-integrated spectroscopy of LIB in various solution, and how LIB might mediate retinal damage induced by ultrashort laser pulses.
Ocular Laser Effects IV
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Ocular effects of penetrating IR laser wavelengths
Joseph A. Zuclich, Donald A. Gagliano, F. Cheney, et al.
This study is concerned with ocular effects of laser radiation in the wavelength range from approximately equals 1.1 micrometers to 2.0 micrometers which includes the so-called 'eye-safe' range where retinal and corneal damage thresholds are significantly higher than the corresponding thresholds for more common visible and far-IR lasers. Across this wavelength range, ocular safe exposure limits vary rapidly with wavelength and are up to approximately equals 6 orders of magnitude greater than exposure limits for visible wavelengths. However, recent developments in laser technology have yielded a variety of powerful near-IR laser sources. Such lasers are not 'eye safe' but, rather, may emit peak powers orders of magnitude above tissue-damaging levels. This report focuses on the unique aspects of laser-tissue interactions for 'eye-safe' wavelengths. In contrast to past experience where the laser energy is absorbed primarily in a thin layer (either at the corneal or skin surface for longer IR wavelengths or at the retinal pigment epithelium for visible wavelengths), 'eye- safe' wavelengths are attenuated gradually through a volume of tissue and may affect any one or several sites within the cornea, lens, and retina. The reaction of the irradiated organism to the volumetric heating associated with such penetrating laser wavelengths does not conform with expectations of an immediate or relatively early observable lesion. Rather, the observable consequences of the laser exposure may take days to become apparent and may involve degeneration across a wider expanse of tissue than that directly irradiated by the laser. For these reason, IR laser exposures bear close scrutiny to redefine both the usual tissue damage criteria and then the appropriate safe exposure limits.
Photoablation with the free-electron laser in the far IR in biological soft tissue (cornea)
Rudolf Walker, Manfred Ostertag, Thomas Bende, et al.
Wavelengths in the range from 12 micrometers up to 70 micrometers (far IR) have a water absorption coefficient in the same order as wavelengths used successfully for ablation near the 6 micrometers water absorption peak. Thus these wavelengths were considered to allow effective photothermal ablation of biological materials. The Free-Electron Laser (FEL) in Nieuwegein, NL (FELIX) is capable of delivering (far) IR laser light between 6 micrometers and 110 micrometers and was used for the first systematic investigation of the ablation quality (ablation depth per pulse and collateral damage beyond the surface) in the wavelength range between 12 micrometers and 70 micrometers . Porcine cadaver corneas were used as target material. Ablation depth per pulse as well as collateral thermal damage (extension of eosinophilic zone beyond the irradiated surface) were measured by histologic micrometry. It was found that the applied IR laser light can be used for an effective ablation of biological materials with a high water content. The experimental data are compared with theoretical values according to a previously described model for photoablation.
Optimizing photoablation parameters with FEL technology in the mid IR: predictive model for the description of experimental data
Manfred Ostertag, Rudolf Walker, Thomas Bende, et al.
An ablation model for pulsed laser ablation, based upon Lambert's law is presented. Ablation is assumed to be entirely the result of heating and subsequent evaporation of tissue water. The model predicts the ablation depth per pulse as well as the collateral damage beyond the surface as a function of the target material's absorption coefficient and allows variation of irradiance exposure per pulse to be taken into account. As a function of the wavelength of the applied laser light the ablation model was used to describe ablation data from the FEL at Vanderbilt University in Nashville, TN between the wavelengths of 2.7 micrometers and 6.5 micrometers and from the FEL at Rijnhuizen, NL (FELIX) between the wavelengths of 8 micrometers and 17 micrometers . Gelatine as well as procine cornea was used as target material. As a function of the absorption coefficient of the target material the ablation model was used to describe ablation data obtained with an Er:YAG laser (2.94 micrometers ) in corneas with different absorption coefficients. The corneas absorption coefficient was varied by substituting heavy water (D2O) for light water (H2O). It was found that the ablation depth per pulse decreases and the collateral damage beyond the surface increases with a decreasing absorption coefficient of the target material. Comparison of the experimental data with the ablation model indicates that around 3 micrometers heat conduction during pulse duration (FEL 4 microseconds; Er:YAG 250 microseconds), and between 6.5 micrometers and 10.5 micrometers the absorption not only by water but also e.g. by proteins must be taken into account.
Explosive vaporization and optical breakdown under the action of laser radiation pulses on the melanosomes
Energy absorption, heat transfer, thermodenaturation, explosive vaporization and optical breakdown under the action of laser radiation pulse on pigmented melanosomes in heterogeneous laminated biotissues are investigated theoretically.
Photothermal Mechanisms
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Thermally induced changes in tissue birefringence
Duncan J. Maitland, Joseph T. Walsh Jr.
We have previously demonstrated that the thermal denaturation of collagen results in a repeatable loss of linear birefringence (LB), which can be measured with birefringence compensation techniques or transmitted or remitted intensity measurements. Consequently, we have used LB to measure the kinetic changes in collagenous tissues. Analysis of the birefringence data results in the calculation of the kinetic parameters entropy, (Delta) S, enthalpy, (Delta) H and the rate constant, k. The birefringence data show that multiple kinetic processes are occurring during collagen denaturation. The most likely physical interpretation of the observed data is that structural changes are occurring on the molecular (tropocollagen) as well as the collagen fibril structural levels. Each of these structures contributes to the total birefringence. When a parallel kinetic model, which is composed of two first order exponential decay models, is applied to the birefringence data, excellent agreement between the data and model is seen. Moreover, the data also show that the relative contributions of the two constituent reactions to the total birefringence measured are in excellent agreement with reported values of intrinsic and form birefringence contributions in collagen. The knowledge that multiple reactions exist during collagen denaturation impacts the understanding of how denaturation occurs and what information can be utilized for the control of the heating process.
Imaging laser-induced thermal fields and effects
Laser light interaction with biological tissues is a combination of optical, thermal and mechanical effects depending on the energy applied per unit of volume per unit of time. Visualization of the phenomena with a high temporal and spatial resolution, contributes to a better understanding of the mechanism of action, especially when pulsed lasers are involved. For this goal, setups were developed based on Schlieren techniques to image the interaction of pulsed (CO2, Holmium and Excimer) and CW (CO2, Nd:YAG, Cu-vapor) lasers with physiological media and biological tissues. In a 'fast' Schlieren setup, images of shock waves and fast expanding and imploding vapor bubbles were captured using very short light flashes (10 ns-10 microseconds). These recordings suggest that these explosive vapor bubbles seem to be the main dynamism for tissue ablation. In a 'color' Schlieren setup, very small changes in optical density of the media induced by temperature gradients, were color coded. Calibration of the color images to absolute temperatures were performed by using calculated temperature distributions and by thermocouple measurements. Cameras with high speed shutters (0.1-50 ms) enabled the recording of dynamic images of the thermal relaxation and heat diffusion in tissues during variation of pulse length and repetition rate. Despite pulse lengths < ms, heat generation in tissue was considerable already at pulse repetition rates above a few Hz. Similar Schlieren techniques were applied to study the thermal characteristics of laser probes, e.g. for the treatment of Benign Prostatic Hyperplasia (BPH). In combination with thermal modeling an optimal therapy might be predicted. Schlieren techniques, generating high-speed and 'thermal' images, can provide a good understanding of the ablation mechanism and the thermo-dynamics during laser-tissue interaction with continuous wave and pulse lasers.
Effect of hydrogen bonding on far-ultraviolet water absorption and potential implications for 193-nm ArF excimer laser-tissue interaction
Joseph T. Walsh Jr., Paul T. Staveteig
The mechanisms causing transient 193-nm optical absorption of collagen during ablative-fluence ArF excimer pulses are poorly understood. The preponderance of hypotheses proposed to explain this phenomenon, such as ultrafast secondary-structure denaturation of proteins and transient free radical formation, focus on the protein matrix and ignore potential contributions from other tissue components such as water. A substantial body of spectroscopic literature places 193 nm adjacent to a steep absorption edge of water that rises to 60,000 cm-1 at 163 nm; other evidence shows that this absorption edge shifts toward 193 nm upon hydrogen-bond breakage. In this paper we show that heating of water from 20-100°C increases the liquid's absorption coefficient. Further investigations using an infrared pump laser show a significant increase in absorption by water of a 193-nm probe beam. Based on this evidence, we speculate that 193-nm laser ablation of tissue may contain a photothermal component related to dynamic absorption of incident radiation by water.
Pulsed laser ablation of tissue: surface vaporization or thermal explosion?
In this paper we discuss the effects of laser-induced stresses and tissue chromophore targeting on the mechanism and dynamics of pulsed laser ablation. We argue that larger pulse durations and optical absorption coefficients reduce the contribution of photomechanical effects to the onset of material removal. Further we argue that if the structural integrity of the tissue extra-cellular matrix (ECM) is not compromised during irradiation, the ablation process will necessarily be explosive even if the heated tissue volume is allowed to mechanically equilibrate to the laser-induced stressed during irradiation. However, if the tissue is not inertially confined and the ECM is compromised during irradiation, the material removal is consistent with a process of rapid surface vaporization.
Photomechanical Mechanisms
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Free-electron laser as the ideal stress-wave generator
Don C. Lamb, Apostolos George Doukas, Thomas J. Flotte M.D., et al.
Laser-induced thermal-elastic stress waves are of importance both in therapeutic applications and in potential morbidity associated with laser surgical procedures. Recent experiments have shown that drug cytotoxicity can be enhanced with stress waves and that direct cell injury correlates with the stress gradient (stress rate of change). To systematically investigate the biological effects of stress waves, it is essential to vary individually the parameters of the stress wave. The Free Electron Laser (FEL) is the ideal laser for generating controllable stress waves. A unipolar stress wave can be characterized by its rise time, duration, peak pressure, and decay time. For short laser pulses, the rise time and decay time are dependent upon the absorption depth of the tissue and can be varied by changing the wavelength of the FEL. The duration of the stress wave can be changed by selecting a different number of micropulses from the FEL macropulse with Pockels cell. The peak pressure can be altered by varying the laser intensity. Results on water have confirmed that the individual parameters of the stress wave can be varied independently.
Laser-induced stress transients: applications for molecular delivery
Thomas J. Flotte M.D., Shun Lee, Hong Zhang, et al.
Lasers can be used to enhance the delivery of a number of molecules. Other investigators have demonstrated local release of molecules from liposomes following laser irradiation, microbeam disruption of the cell membrane to increase cell transport, microbeam ablation of the zona pellucida surrounding the ovum to increase the chances of fertilization, and increased transcutaneous transport following ablation of the stratum corneum. Our experiments have shown that laser-induced stress transients can be utilized as a vector for intracellular delivery of molecules that may or may not normally cross the cell membrane. These two conditions have been tested with Photofrin and DNA. This technology may have applications in cell and molecular biology, cancer therapy, gene therapy, and others.
High-pressure effects on bacteria
Douglas H. Bartlett
Laser treatment of tissues can generate elevated pressures in the kilobar range. This review will provide an overview of the known cellular and biochemical effects of elevated pressure. As an example of pressure effects on enzyme structure/function. I will present results on the effects of high pressure on the stability and activity of the enzyme DNA gyrase. Information will also be provided on the pressure shock response of the bacterium Escherichia coli to abrupt shifts in elevated hydrostatic pressure. Finally, I will describe an unusual group of organisms which have evolved specialized adaptations for life at high pressure. These are the deep-sea barophilic ('pressure loving') bacteria.
Photochemical Mechanisms
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Role of carotenoid excited states and radicals in antioxidant activities
Chris R. Lambert
Carotenoids are linear polyenes that occur in nature and are known to have powerful antioxidant properties. They react efficiently with the excited states of many organic molecules. In the photosynthetic apparatus of plants they quench reactive excited states that may be formed and release the energy as heat. In photodynamic therapy they may be used to ameliorate the associated skin photosensitivity that is a consequence of many photosensitizers. This protection may be either through reaction with the sensitizer triplet state or through quenching of singlet oxygen. Carotenoids also form relatively stable radical species and react efficiently with the hydroxyl radical, superoxide and the solvated electron. In cells they are associated with the lipid core of the cell membrane and are effective against lipid peroxidation. The importance of the thermodynamic properties of these compounds and their organization within biological systems is pivotal to understanding carotenoid antioxidant activity. The present paper reviews some recent work on the energy level of (beta) -carotene, electron transfer involving the one electron reduced species and the resonance Raman spectra of some carotenoids in micellar solution.
Comparison of photobleaching and fluence rate effects in PpIX and BPD-MA photosensitization of rat bladder tumor in vivo
Seiichi Iinuma, Georges A. Wagnieres, Kevin T. Schomacker, et al.
Photobleaching of 5-aminolevulinic acid (ALA) -induced protoporphyrin IX (PpIX) and benzoporphyrin derivative-monoacid ring A (BPD-MA) was investigated using an orthotopic rat bladder tumor model. For both photosensitizers used, the photobleaching rate constant was not fluence- rate-dependent under conditions that photodynamic response was fluence rate-dependent. These data suggest that photobleaching pathways may be independent of the photochemical paths involved in tissue destruction. The fluorescence spectrum was followed during irradiation by using laser-induced fluorescence method and a build-up of photoproducts of PpIX was observed whereas no fluorescence of photoproducts was obtained in the case of BPD-MA.
DMSO affects the efficiency of photolabeling of tetrabrominated rhodamine to collagen fibers
The ability to photolabel a compound, tetrabrominated rhodamine (TBR), onto collagen gels was tested. The influence of DMSO on the efficiency of photolabeling was determined. The DMSO enhances the photolabeling presumably by allowing the TBR to become more closely associated to the collagen fibers such that upon photon absorption which causes debromination to yield a radical, the radical can covalently link to the collagen.
Fluorescence imaging and spectroscopy of motile sperm cells and CHO cells in an optical trap (laser tweezers)
Karsten Koenig, Yagang Liu, Tatiana B. Krasieva, et al.
We describe fluorescence spectroscopy and imaging studies of optically trapped single Chinese hamster ovary (CHO) and motile human sperm cells. The NIR trapping beam was provided by a tunable, multimode continuous wave Ti:Sapphire laser. The beam was introduced into an inverted confocal laser scanning microscope. Fluorescence of cells in the single- beam gradient force optical trap was excited with a 488 nm microbeam (laser scanning microscopy) or with 365 nm radiation from a high- pressure mercury lamp. Modifications to NADH-attributed autofluorescence and Rhodamine- and Propidium Iodide-attributed xenofluorescence indicate a significant cell-damaging effect of 760 nm trapping beams. 760 nm effects produce a biological response comparable to UVA-induced oxidative stress and appear to be a consequence to two-photon absorption.
Photo-Photo!
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Photosensitized inactivation of infectious blood-borne human parasites
Millard M. Judy, Franklin M. Sogandares-Bernal, James Lester Matthews
Blood-borne viruses and protozoan parasites that are infectious to humans pose risk world-wide of infection transmission through blood and blood product transfusion. Blood-borne infectious viruses include human immunodeficiency virus (HIV-I), which causes AIDS; hepatitis C virus, which can cause chronic hepatitis; and cytomegalovirus, which can be dangerous to immunocompromised patients, e.g., the newborn, transplant recipients, and AIDS patients. Infectious blood-borne protozoan parasites include Trypanosoma cruzi, which causes Chagas' disease, endemic throughout Central and South America; the Trypanosoma species causing African sleeping sickness endemic in Central Africa; and Plasmodium falciparum, which causes malignant and increasingly drug- resistant human malaria prevalent throughout the tropics. Some researchers have focused on using photosensitizers to inactivate HIV-I and other viruses in whole blood, packed red cells, and platelet concentrates without compromising blood product function. Our group previously has reported photosensitized in vitro inactivation of P. falciparum and the mouse malaria organism Plasmodium berghei in whole blood using hematoporphyrin derivative (HPD) and of T. cruzi using benzoporphyrin derivatives BPDMA and BPDDA, dihematoporphyrin ether (DHE), and hydroxyethylvinyldeuteroporphyrin (HEVD). These results suggest that continued investigation is warranted to evaluate the potential for photosensitized inactivation of blood-borne parasites in blood banking.
Melanin may promote photooxidation of linoleic acid
Randolph D. Glickman, Kwok-Wai Lam
We have previously shown that laser-exposed melanin granules isolated from the retinal pigment epithelium (RPE) are capable of oxidizing ascorbic acid. We are now characterizing the reactions of light- activated melanin with other cellular components such as linoleic acid, a polyunsaturated fatty acid. Commercial linoleic acid, and melanin granules isolated from bovine RPE cells, are mixed and exposed to the broad band output of a 150 W Xenon arc lamp or the CW output of an Argon laser. Native linoleic acid is separated from its hydroperoxides by HPLC, and the relative amounts of each are detected by UV absorbance at 210 and 232 nm, respectively. Exposure of the linoleic acid alone to the xenon arc source results in production of linoleic hydroperoxides (LHP) in an intensity-dependent reaction that doubles in extent over the temperature range of 0° to 80°C. Addition of melanin granules at a density of 108 granules/ml reduces the production of LHP, probably because of light absorption and self-screening by the melanin. At or below a density of 107 granules/ml, however, the light-driven production of LHP is enhanced, especially during exposure to the blue- green output of the Argon laser. Physiological antioxidants (Vit. C,E protect the linoleic acid from photo-oxidation in the presence or absence of melanin. These observations support the hypothesis that light-activated melanin can react with some cellular components and thereby contribute to photochemical damage, especially if endogenous antioxidants are depleted.
Modeling of endovascular patch welding using the computer program LATIS
Michael E. Glinsky, Richard A. London, George B. Zimmerman, et al.
A new computer program, LATIS, being developed at Lawrence Livermore National Laboratory is used to study the effect of pulsed laser irradiation on endovascular patch welding. Various physical and biophysical effects are included in these simulations: laser light scattering and absorption, tissue heating and heat conduction, vascular cooling, and tissue thermal damage. The geometry of a patch being held against the inner vessel wall (500 micrometers inner diameter) by a balloon is considered. The system is exposed to light pulsed from an optical fiber inside the balloon. A minimum in the depth of damage into the vessel wall is found. The minimum damage zone is about the thickness of the patch material that is heated by the laser. The more ordered the tissue the thinner the minimum zone of damage. The pulse length which minimizes the zone of damage is found to be the time for energy to diffuse across the layer. The delay time between the pulses is determined by the time for the heated layer to cool down. An optimal pulse length exists which minimizes the total time needed to weld the patch to the wall while keeping the thickness of the damaged tissue to less than 100 micrometers . For the case that is considered, a patch dyed with light absorbing ICG on the side next to the vessel (thickness of the dyed layer is 60 micrometers ), the best protocol is found to be 65-200 ms pulses applied over 2 min.
Random-walk methodology for determining optical properties of tissue from reflection and transmission measurements
A new iterative inverse method to calculate the absorption and scattering coefficients of optically turbid media from total reflectance and transmittance measured by integrating spheres is proposed and evaluated. Random walk methodology is used to calculate the total reflectance and transmittance of light from highly turbid slabs whose refractive index differs from that of the surrounding medium. Photon migration near index-mismatched boundaries is inferred from Monte-Carlo simulations that take into account significant angularly-dependent internal reflection. An inverse method is used to determine the optical coefficients, (mu) a and (mu) s', from diffuse reflectance and transmittance measurements on suspensions of polystyrene latex beads, the optical absorbance being varied by adding dyes to the suspension medium. The nominal optical coefficient ((mu) a from 0.01-0.09 mm-1 and (mu) s' from 1-2 mm-1) are found to agree on average within 8% of the values calculated by the inverse method. The use of the method for tissue characterizations is illustrated by determining the optical parameters of samples of bovine myocardium and human breast.
Imaging Transient Phenomena
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Streak-photographic investigation of shock-wave emission after laser-induced plasma formation in water
Joachim Noack, Alfred Vogel
The shock wave emission after dielectric breakdown in water was investigated to assess potential shock wave effects in plasma mediated tissue ablation and intraocular photodisruption. Of particular interest was the dependence of shock wave pressure as a function of distance from the plasma for different laser pulse energies. We have generated plasmas in water with a Nd:YAG laser system delivering pulses of 6 ns duration. The pulses, with energies between 0.4 and 36 mJ (approximately equals 180 times threshold), were focused into a cuvette containing distilled water. The shock wave was visualized with streak photography combined with a schlieren technique. An important advantage of this technique is that the shock position as a function of time can directly be obtained from a single streak and hence a single event. Other methods (e.g. flash photography or passage time measurements between fixed locations) in contrast rely on reproducible events. Using the shock wave speed obtained from the streak images, shock wave peak pressures were calculated providing detailed information on the propagation of the shock. The shock peak pressure as a function of distance r from the optical axis was found to decrease faster than 1/r2 in regions up to distances of 100-150 micrometers . For larger distances it was found to be roughly proportional to 1/r. The scaling law for maximum shock pressure p, at a given distance was found to be proportional to the square root of the laser pulse energy E for distances of 50-200 micrometers from the optical axis.
Ultrafast time-resolved imaging of stress transient and cavitation from short-pulsed laser irradiated melanin particles
Charles P. Lin, Michael W. Kelly
Melanins are naturally occurring pigment particles which strongly absorb visible and near infrared radiation in many pigmented tissues including the eye and the skin. When irradiated by short laser pulses, stress transients and cavitation can be generated from these micrometer-sized particles. The photoacoustic effect is a potential mechanism for short pulse laser injury to the retina. We report here direct observations of the stress wave and cavitation from irradiated melanin particles using the technique of fast time-resolved imaging. Melanin granules were isolated from fresh bovine retina suspended in gels, and irradiated with 100 psec laser pulses at 1.064 micrometers . Stress transients were imaged under a microscope using a delayed visible strobe pulse. With incident laser fluences of about 1 J/cm2 (near the threshold fluence for retinal injury), a spherical pressure wavefront and a cavitation bubble were observed around each irradiated melanin particle. By measuring the radius of the wavefront as a function of strobe delay time the propagation velocity of the stress wave was determined. We observed in initial supersonic shock front which rapidly decays to an acoustic wave within a few nanoseconds. Because the melanin granules are densely packed inside the 10 micrometers diameter RPE cells, the shock range of a few microns is potentially sufficient for creating injury in the retina.
Laser flash photography of cold cavitation-driven ablation in tissues
Plasma mediated ablation of collagen gels and porcine cornea was studied at various laser pulse durations in the range from 350 fs to 1 ns at 1053 nm wavelength. A time resolved stress detection technique was employed to measure transient stress profiles and amplitudes. Optical microscopy was used to characterize ablation craters qualitatively, while a wide band acoustic transducer helped to quantify tissue mechanical response and the ablation threshold. The ablation threshold was measured as a function of laser pulse duration and linear absorption coefficient. For nanosecond pulses the ablation threshold was found to have a strong dependence on the linear absorption coefficient of the material. As the pulse length decreased into the subpicosecond regime the ablation threshold became insensitive to the linear absorption coefficient. The ablation efficiency was found to be insensitive to both the laser pulse duration and the linear absorption coefficient. High quality ablation craters with no thermal or mechanical damage to surrounding material were obtained with 350 fs laser pulses. The mechanism of optical breakdown at the tissue surface was theoretically investigated. In the nanosecond regime, optical breakdown proceeds as an electron collisional avalanche ionization initiated by thermal seed electrons. These seed electrons are created by heating of the tissue by linear absorption. In the ultrashort pulse range, optical breakdown is initiated by the multiphoton ionization of the irradiated medium (6 photons in case of tissue irradiated at 1053 nm wavelength), and becomes less sensitive to the linear absorption coefficient. The energy deposition profile is insensitive to both the laser pulse duration and the linear absorption coefficient.
Monitoring of KrF excimer laser ablation for burn scars: a comparative study of transient reflection measurement and time-resolved photography of ablation plume
Akio Nakajima, Tsunenori Arai, Makoto Kikuchi, et al.
A simple laser ablation monitoring during burn scar removal by KrF laser irradiation was studied to control laser fluence in real-time. Because, to obtain suitable surface for auto skin-graft, the laser fluence should be precisely controlled at each laser shot. We employed simple probe transmission method which could detect ejected material/phenomena from irradiated surface. The time-course of measured probe intensity contained a couple of attenuated peaks, which might corresponded to a shock wave front and debris plume. The delay time from laser irradiation to the debris plume peak appearance varied with the ablation fluence. The delay time of 1 J/cm2 (near ablation threshold) case prolonged 25% from 8 J/cm2 (far above threshold) case. Therefore, we think the delay time measurement by means of the simple probe transmission method may be available to attain the laser fluence control for nonuniform burn scar removal. The time-resolved photography and probe reflection method were also studied to understand the measured time-course of the transmitted probe intensity.
Ablation I
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Photomechanical basis of laser ablation of biological tissue
Lev T. Perelman, Douglas Albagli, Marta Dark, et al.
The photomechanical picture of laser ablation of biological tissue asserts that ablation is initiated when the laser-induced tensile stress exceeds the ultimate tensile strength of the target. We have developed a three-dimensional theoretical model of the thermoelastic response of tissue to short-pulsed laser irradiation which allows the time-dependent stress distribution to be calculated given the optical, thermal and mechanical properties of the target. In addition, we have developed a complimentary interferometric technique which can measure the laser- induced thermoelastic expansion of a material with nanometer spatial resolution on a nanosecond time scale. The complex features of this expansion allow the needed optical, thermal, and mechanical properties of the target to be determined, which then allows the stress distribution to be calculated. This work has led to several significant results which support the photomechanical model of ablation of biological tissue. First, unlike the one-dimensional model predicts the development of significant tensile stressed on the surface of the target, precisely where ablation is observed to occur. Experimental results from bone are consistent with mechanical fracture caused by laser-induced stresses. Experimental results from human meniscus, a representative soft tissue, show additional behavior consistent with the growth and collapse of cavitation bubbles within the tissue caused by laser-induced stresses.
Mechanism of dye-enhanced enamel ablation by Alexandrite laser radiation
Insufficient light absorption in hard dental tissues makes laser ablation in near UV, visible or near IR spectral ranges very inefficient to be employed for tooth cavity preparations. We used deposition of a liquid absorber, indocyanine green (ICG) dye, to overcome this problem. Experiments employed Alexandrite laser anticipating that future near IR diode laser technology will replace existing medical lasers. Ablation kinetics and mechanisms for both free-running and Q-switched modes of Alexandrite laser were studied with the aim to determine optimal parameters of laser irradiation and optimal volume of the dye. Four experimental parameters were monitored during each ablation event: (1) incident laser fluence, (2) temporal profile of the laser pulse, (3) temporal profile and magnitude of laser-induced stress transients, (4) temporal profile and spectrum of plasma emission. We also examined kinetics of plume by probing ablation products with CW He-Ne laser beam. Results depicted ablation process as a complex multistage phenomenon. Two distinct stages associated with the tooth ablation are revealed in the free-running mode: (1) ablation of a dye droplet from a tooth surface by the first laser micropulse of a 250-microsecond(s) macropulse, (2) plasma mediated ablation of a melted layer of enamel produced by thermal explosion of the dye. Plasma jet formation was delayed 10-100 microsecond(s) against the beginning of free-running pulse. Ablation stages and their efficiency are defined by laser irradiation parameters, dye concentration and its total volume. In contrast, Q-switched (nanosecond) laser ablation occurs as a one stage process, and, therefore, less efficient. In addition, Q-switched mode irradiation induces shock waves amplitudes that are about an order of magnitude higher compared with that induced by the free-running irradiation. Experimental comparison of Q-switched and free-running modes of irradiation is evident in favor of free-running mode that produces a nice smooth crater without noticeable thermomechanical damage to surrounding tissues.
Effect of spot size, pulse energy, and repetition rate on microsecond ablation of gelatin under water
Ujwal S. Sathyam, Alan Shearin, Scott A. Prahl
The efficiency of laser ablation of thrombus depends on spot size, pulse energy and repetition rate. A 1 microsecond(s) pulsed dye laser (504 nm) was used to ablate a gelatin-based thrombus model containing an absorbing dye under water. The gelatin was confined in 3 mm inner diameter tubes and pulse energies of 25-100 mJ were delivered via 300, 600, and 1000 micrometers core diameter fibers. The experiments were conducted at pulse repetition rates of 3 Hz and 10 Hz. The amount of gelatin removed was measured using a spectrophotometric method and ablation efficiency was defined as mass removed per pulse per unit energy. Flash photography was used to visualize the ablation process in 1 cm cuvettes. Results: More material was removed using bigger fibers in the 3 mm tubes at similar pulse energies. The amount of gelatin removed per pulse increased linearly with pulse energy. There was no significant change in the amount removed at pulse repetition rates of 3 Hz and 10 Hz. In the 1 cm cuvettes, the ablation mass was roughly the same with both the 300 micrometers and 1000 micrometers fibers. Flash photography of the ablation process in 1 cm cuvettes showed that less than 1% of the laser energy went into formation of a vapor bubble. The mass removed increased roughly linearly with bubble energy. Conclusions: Ablation mass increases linearly with pulse energy, but does not have a direct relationship with radiant exposure. It is independent of the repetition rate under 10 Hz.
Scanning electron microscopy of holmium:YAG ablated lamellar bone
Eric Mun-Wight Cheung, Brian Jet-Fei Wong M.D., Lih-Huei L. Liaw, et al.
Surface features of Holmium:YAG (2.12 micrometers ) ablated lamellar bone were characterized using scanning electron microscopy (SEM). Porcine lamellar bone was harvested from the parietal and frontal regions of domestic pigs and machined into uniform specimens of 0.8 mm thickness. Ablation studies were performed under physiologic conditions (fresh bone) and on bone that had been serially dehydrated with graded alcohol baths. A Holmium:YAG laser at 4 Hz pulse repetition rate was used with an average energy density of 9 J/cm2 per pulse. Ablation was terminated at specific intervals corresponding to visibly observed changes in the ablation process. These included the initiation of ablation without plasma, the onset of plasma, prolonged plasma-mediated ablation, and through ablation to the other side of the specimen. Both wet and dry bone specimens were prepared for SEM. SEM was performed on selected ablation craters at magnifications varying from 75x to 5000x. Several features distinguish the ablation craters in wet versus dry bone. In general, ablated dehydrated bone exhibited very smooth surface features in which the heated bone appeared to melt and coalesce so as to form disc-like condensations. Often, successive discs were formed so that they stacked on top of each other. Fresh bone formed distinctly globular formations although some discs were also encountered at various energy settings. The overall globular structure was far more compact than that observed in the respective dehydrated samples. The results are discussed with relevance to ablation rates and surface temperature measurements.
Ablation II
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Characterization of handpieces to control tissue ablation with pulsed CO2 laser
Focusing handpieces used for CO2 beam delivery allow large variation of the power density in the spot depending on the distance to the tissue and hence the effect on the tissue. In contrast to the cw CO2 laser, the pulsed CO2 laser vaporized tissue water instantly (: equals ablation threshold), leaving a charless crater in the tissue surface. Only if the fluence is below or near threshold, the tissue effects are comparable with the cw laser. The threshold and tissue effects were studied for focusing (f equals 119 mm) and collimating (3 mm) handpieces coupled to an ultrapulsed CO2 laser. Using a special thermal imaging setup based on Schlieren techniques, the ablation threshold was determined depending on spotsize and pulse energy (1-200 mJ). In the focus of the handpiece, the threshold was already exceeded at 1 mJ, creating holes that were larger than the theoretical expected spotsize. The ablation threshold (J/cm2) increased for larger spotsizes. Below threshold, there is heating of the tissue resulting in coagulation. Above threshold, the exploding water vapor consumed thermal energy suppressing heating of the surrounding tissue. The gaussian shape of the collimated beam results in relatively more thermal effects. Focusing handpieces provide a wide range in power density and thus require experience from the surgeon. Collimated handpieces might be more easy to handle but offer less flexibility in tissue effect and a larger thermal zone.
Surface characteristics of argon laser-ablated bone in the presence and absence of an initiator
Brian Jet-Fei Wong M.D., Mark Russell Dickinson, Belinda Simonian, et al.
Argon lasers are widely used in neurotologic surgery for hard tissue ablation. They are used in stapes bone surgery to treat surgically correctable hearing loss. While the Argon laser has been shown to be effective in performing the stapedotomy operation, few studies exist which focus on the deleterious effects of this laser in a model that is relevant to clinical practice and laser-tissue interactions. This study focuses on surface temperature changes in otic capsule and cortical bone in the presence and absence of an initiator. For tissues which are poor absorbers at visible wavelengths, such as bone, an initiator can be applied to the surface. It then absorbs the applied laser energy and initiates ablation by creating a carbonized surface over the tissue in question. Clinically, blood or burnt tissue is used to initiate ablation over bone in ear surgery. In this study black ink was used as the initiator substance. We also studied the effect of multiple lasers pulses on these bone tissues. Fresh porcine otic capsule and cortical bone was machined to a uniform thickness of 0.8 mm. A coherent 920 Argon laser was used with a focusing lens as a delivery system (200 micrometers spot size, 100 msec pulse duration, 514 nm). A Hg-Cd-Te thermal camera system was used to measure surface temperature. Hot spot temperatures were recorded along with the full width-half maximum (FWHM) of the spatial thermal disturbance at that time. The time for the hot spot to return to ambient temperature was also measured. Minimal surface temperature elevation was recorded in the absence of an initiator. No surface modification was observed by light microscopy. In contrast, the addition of an initiator resulted in marked temperature elevations and significant surface carbonization. Surface changes were studied with scanning EM and an interferometric surface analyzer. The role of an initiator, mechanisms of tissue destruction, and clinical relevance of these findings will be discussed.
Holmium laser ablation of cartilage: effects of cavitation bubbles
Thomas Asshauer, Thomas Jansen, Thorsten Oberthur, et al.
The ablation of fresh harvested porcine femur patellar groove cartilage by a 2.12 micrometers Cr:Tm:Ho:YAG laser in clinically used irradiation conditions was studied. Laser pulses were delivered via a 600 micrometers diameter fiber in isotonic saline. Ablation was investigated as a function of the angle of incidence of the delivery fiber with respect to the cartilage surface (0-90 degrees) and of radiant exposure. Laser pulses with energies of 0.5, 1.0 and 1.5 J and a duration of 250 microseconds were used. A constant fiber tip-tissue distance of 1 mm was maintained for all experiments. The dynamics of the induced vapor bubble and of the ablation process was monitored by time resolved flash videography with a 1 microseconds illumination. Acoustic transients were measured with a piezoelectric PVDF needle probe hydrophone. Bubble attachment to the cartilage surface during the collapse phase, leading to the direct exposition of the cartilage surface to the maximal pressure generated, was observed in all investigated irradiation conditions. Maximal pressure transients of up to 200 bars (at 1 mm distance from the collapse center) were measured at the bubble collapse at irradiation angles >= 60 degrees. No significant pressure variation was observed in perpendicular irradiation conditions as a function of radiant exposure. A significant reduction of the induced pressure for irradiation angles
Effect of Young's modulus on bubble formation and pressure waves during pulsed holmium ablation of tissue phantoms
E. Duco Jansen, Thomas Asshauer, Martin Frenz, et al.
Mechanical injury during pulsed laser ablation of tissue is caused by rapid bubble expansions and collapse or by laser-induced pressure waves. In this study the effect of material elasticity on the ablation process has been investigated. Polyacrylamide tissue phantoms with various water concentrations (75-95%) were made. The Young's moduli of the gels were determined by measuring the stress-strain relationship. An optical fiber (200 or 400 micrometers ) was translated into the clear gel and one pulse of holmium:YAG laser radiation was given. The laser was operated in either the Q-switched mode (tau) p equals 500 ns, Qp equals 14 +/- 1 mJ, 200 micrometers fiber, Ho equals 446 mJ/mm2) or the free-running mode ((tau) p equals 100 microsecond(s) , Qp equals 200 +/- 5 mJ, 400 micrometers fiber, Ho equals 1592 mJ/mm2). Bubble formation inside the gels was recorded using a fast flash photography setup while simultaneously recording pressures with a PVDP needle hydrophone (40 ns risetime) positioned in the gel, approximately 2 mm away from the fibertip. A thermo-elastic expansion wave was measured only during Q-switched pulse delivery. The amplitude of this wave (approximately equals 40 bar at 1 mm from the fiber) did not vary significantly in any of the phantoms investigated. Rapid bubble formation and collapse was observed inside the clear gels. Upon bubble collapse, a pressure transient was emitted; the amplitude of this transient depended strongly on bubble size and geometry. It was found that (1) the bubble was almost spherical for the Q-switched pulse and became more elongated for the free-running pulse, and (2) the maximum bubble size and thus the collapse amplitude decreased with an increase in Young's modulus (from 68 +/- 11 bar at 1 mm in 95% water gel to 25 +/- 10 bar at 1 mm in 75% water gel).
Ablation III
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Photoacoustic drug delivery: the effect of laser parameters on the spatial distribution of delivered drug
HanQun Shangguan, Lee W. Casperson, Alan Shearin, et al.
Photoacoustic drug delivery is a technique for delivering drugs to localized areas by timing laser-induced pressure transients to coincide with a bolus of drug. This study explores the effects of target material, laser energy, absorption coefficient, fiber size, repetition rate, and number of pulses on the spatial distribution of delivered drug. A microsecond flash-lamp pumped dye laser delivered 30-100 mJ pulses through optical fibers with diameters of 300-1000 micrometers . Vapor bubbles were created 1-5 mm above clear gelatin targets submerged in mineral oil containing a hydrophobic dye (D&C Red#17). The absorption coefficient of the oil-dye solution was varied from 50-300 cm-1. Spatially unconfined geometry was investigated. We have found that while the dye can be driven a few millimeters into the gels in both the axial and radial directions, the penetration was less than 500 micrometers when the gel surface remained macroscopically undamaged. Increasing the distance between the fiber tip and target, or decreasing the pulse energy reduced the extend of the delivery.
Modeling and experimental observation of photomechanical effects in tissue-like media
Guenther Paltauf, Heinz Schmidt-Kloiber
To investigate the contribution of photomechanical fracture to tissue ablation with short laser pulses, we performed a study in which experimental phenomena were compared to results of a theoretical model. In this mode the generation and one-dimensional propagation of thermoelastic stress waves caused by a laser pulse of finite duration is simulated and the dynamics of cavitation induced by the negative components of these stress waves are calculated. To experimentally observe the cavitation dynamics in water and gelatine, an optical pump- probe technique together with time-resolved imaging and stress detection methods was employed. With the pump-probe technique the lifetimes of individual cavitation bubbles until the first collapse could be measured. At low fluence values a good agreement between experiment and simulation was observed. At higher fluences, where the bubbles do not move independently from each other as it is assumed in the model, the experimental lifetimes were longer than the calculated ones. Additional properties of photomechanical damage such as the dependence of the cavitation process on the time-integral over the stress wave, the spatial occurrence of cavitation bubbles and the influence of viscosity in gelatine are demonstrated in the simulation.
Modeling of ablation by photospallation using the computer program PUFF/DFRACT
Tarabay H. Antoun, Lynn Seaman, Michael E. Glinsky
In general, macroscopic material failure is a manifestation of irreversible changes at the microscopic level. Many tissues, which may appear to be macroscopically homogeneous, are, at a fundamental microscopic level, a composite material. For example, cornea is composed of a hyaluronic acid matrix in which layers of collagen fibers are overlaid in a crossing pattern. The points where the collagen fibers intersect are potential nucleation sites for microscopic defects, which under the action of tensile stress, nucleate, grow and coalesce to form macroscopic failure planes, or spall planes. Using a model based on microstructural evolution, this paper examines the failure process during photoablation. Specifically, the paper describes a physically motivated, micromechanical model based on the nucleation and growth of spherical voids. This model is then used to simulate photoablation of cornea. Potential for using this model to predict the stress wave and material damage measured by experiment is discussed.
Ultrashort pulse laser microsurgery on cell
He Zhou Wang, Xu Guang Huang, Xiguang Zheng, et al.
A laser microbeam system has been set up for microsurgery on cell. The relations of laser wavelength, pulse duration and pulse energy to punching effects and self-healing are studied. The experimental results demonstrate that picosecond pulse laser microbeam offers many advantages in cell microsurgery. The mechanism of punching by picosecond microbeam is high field puncture instead of heat effect, and is irrelevant to cell kinds and colors. The diameter and depth of microsurgery can therefore be easily controlled by adjusting the laser pulse energy. The diameter of the minimum aperture is about 0.1 micrometers , much smaller than the theoretical limit ((lambda) /2) for optical microscope due to self- focusing effect. With ultrashort pulse laser microbeam, we can easily cut off any part of a cell. An example is that eight nuclei in the center of unicellular parasite Pneumocystis Carinii can be destroyed one by one by ultrashort pulse laser microbeam without cell wall injury. The holes can also be punched by ultrashort pulse laser microbeam from cell wall to cell nucleus. In a fraction of a second to several seconds after punching, the hole on cell wall or cell membrane can self-heal. Exogenous DNA can be introduced into the cell before its self- healing.
Optical Dynamics
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Role of dynamic changes in blood perfusion and optical properties in thermal coagulation of the prostate
Beop-Min Kim, Steven L. Jacques, Sohi Rastegar, et al.
The dynamic evolution of the coagulation front in laser irradiated prostate tissue is simulated using a nonlinear finite element method (NFEM) which takes into account the temperature and thermal damage dependence of blood perfusion rate and optical properties. Using this nonlinear model, it was found that the hyperemic ring formed at the periphery of the coagulation front reduces heat penetration significantly and the increased scattering near the tissue surface reduces the light energy deposition in the deep region. The final damage depth would be overestimated by about 50% if the effect of temperature and damage dependence of blood perfusion and optical properties modeling is disregarded.
Optical changes of porcine brain tissue after thermal coagulation
Hans-Joachim Schwarzmaier M.D., Thomas Goldbach, Ilya V. Yaroslavsky, et al.
Porcine brain tissue is a model for human brain structures in laser induced thermo-therapy. However, its optical properties including possible heat-related changes were basically unknown so far. To simulate laser coagulation, 12 specimens (6 grey and 6 white matter) were heated in a saline bath (80°C, 2 hours) and compared to 11 untreated samples (5 grey and 6 white matter). The optical constants were obtained from transmission (total and collimated) and reflection (diffuse) measurements using the inverse Monte-Carlo method. The absorption coefficient ((mu) a) of untreated grey substance decreased from 0.35 +/- 0.06/mm (340 nm) to 0.03 +/- 0.02/mm (800 nm). The scattering coefficient ((mu) s) varied between 20.42 +/- 3.65/mm (340 nm) and 6.85 +/- 2.07/mm (800 nm). The anisotropy factor (g) increased from 0.848 +/- 0.013 (340 nm) to 0.889 +/- 0.009 (800 nm). Coagulation increased (mu) a up to a factor of 2 (340-540 nm; p < 0.05), and (mu) s by a factor up to 3 (340-800 nm, all data p < 0.001) while g was decreased up to 18% (340-560 nm; p < 0.05). White substance exhibited a (mu) a between 0.24 +/- 0.07/mm (340 nm) and 0.04 +/- 0.02/mm (800 nm) while (mu) s varied between 26.72 +/- 9.10/mm (340 nm) and 21.78 +/- 3.88/mm (800 nm). The g-value increased from 0.561 +/- 0.180 (340 nm) to 0.834 +/- 0.068 (800 nm). Coagulation increased (mu) a by a factor up to 2 (340-800 nm; all data p < 0.05) while (mu) s and g remained unchanged. Thermal denaturation changes the absorption and scattering properties of porcine brain significantly.
Measurement of time-dependent changes in optical transmission characteristics of biological tissues
Uwe Vogel, Juergen Uhlemann, Andreas Melchner, et al.
The results of several measurements of optical tissue properties often show a wide range of variety. This could be a reason for neglecting time-dependent alterations after the preparation or during the measurement procedure itself. To combine the opportunities optical tomography offers (i.e. structural and functional imaging) with two- or even three-dimensional spectroscopy without using any contrast means of fluorescence dyes, we measured several transmission spectra of various tissues of biological specimen. To prove reproducibility three consecutive measurements were carried out. Generally, a variation in the transmission or extinction could be seen. Their value and direction usually depends on the type of biological specimen. Living cells, freshly taken from the nutritive medium, showed a significant decrease in transmission in contrast to various types of originally frozen animal tissue, which revealed an increase in transmission. But here the value of increase was found to be dependent on the tissue, too. Furthermore, we have made investigations on the dependence of transmission alterations by changing the tissue preparation, e.g. the cutting area in regard to tissue properties. In general, the relative spectral response remained the same, thus resulting in a shift to higher or lower transmissions. The investigations were made with tissue of a thicknesses between 300 micrometers and 1 mm. Details will be explained in this paper. These measurements allow the conclusion, that thin biological specimen are subject to changes of optical properties at the time after having taken them out of a stable in vitro state. These changes are probably due to varying anisotropy. Finally, this leads to the conclusion, that for thin biological specimen the rules of geometrical optics have to be preferred rather than making radiation transport calculations. Optical rules should be part of common methods to determine optical properties of tissue.
Thermal Effects I
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Tissue fluorescence changes and protein coagulation after Nd:YAG interstitial laser photocoagulation
Stephen Thomas Flock, Scott Ferguson, Lewis Krain M.D., et al.
In attempting to identify a tissue response suitable for monitoring interstitial laser photocoagulation (ILP) during treatment, we observed that the lesions produced in tissue by interstitial irradiation with the 1064 nm radiant energy produced by an Nd:YAG laser fluoresce when exposed to the long-wave ultraviolet light produced by a handheld UV fluorescent lamp. The visual extent of the fluorescence was correlated to the irradiation time and energy fluence rate. Fluorescence spectra of four tissue chromophores, serum albumin, Type 1 collagen, nicotinamide adenine dinucleotide (NADH) and flavin adenine dinucleotide (FAD) exhibited similar spectra to the fluorescence of solubilized tissue. No significant changes in the fluorescent spectra were observed upon heating to 70°C for 5 minutes the chromophores or tissue sample prior to solubilization. In another experiment, the tissue was thermally damaged by immersion in phosphate buffered saline from 60-100°C for 30-90 seconds. The reflectance from 400-800 nm of the intact tissue was noted to increase with increasing thermal damage up to 80°C, and the decrease at 90°C and 100°C. Activation energies calculated from this data was suggestive of thermal damage to blood and other tissue constituents. In order to see if changes in electrophoretic mobility occurred upon heating, nondenaturing polyacrylamide gel electrophoresis (native PAGE) was done on heated that were solubilized by ultrasonication. The gels showed a quantitative loss of tissue proteins with increasing thermal damage, and the irreversible formation of heavy protein coagulums.
Fluorescence measurement of diode (805 nm) laser-induced release of 5,6-CF from DSPC liposomes for monitoring of temperature: an in vivo study in rat liver using indocyanine green potentiation
Serge R. Mordon, Thomas Desmettre, Jean-Marie Devoisselle, et al.
This in-vivo study examines the validity of fluorescence measurement of laser-induced release of temperature sensitive liposome-encapsulated dye for monitoring of temperature and prediction of tissue thermal damage. It is performed in rat liver after i.v. injection of liposomes loaded with a fluorescent dye and i.v. injection of Indocyanine Green (ICG) for diode laser potentiation. Temperature sensitive liposomes (DSPC: Di- Stearoyl-Phosphatidyl-Choline) are loaded with 5,6-Carboxyfluorescein (5,6-CF). These liposomes (1.5 ml solution) and ICG (1.5 ml solution-5 mg/kg) are injected to adult male wistar rats. Two hours later, the liver is exposed and irradiated with a 0.8 W diode laser using pulses lasting from 1 s to 6 s (fluence ranging from 16 to 98 J/cm+2)). Simultaneously, the fluorescence emission is measured with a fluorescent imaging system. Results show that the fluorescence intensity increases linearly form 18 J/cm2 up to 75 J/cm2. These fluences correspond to surface temperatures between 42°C to 64°C. The measurements appear to be highly reproducible. In this temperature range, the accuracy is +/- 3°C. The maximum intensity is observed immediately after the laser is switched off and a decrease of the fluorescence intensity is observed (27% in 20 minutes) due to the 5.6-CF clearance. However, the ratio (IF/Ibck) remains almost stable over this period of time and the determination of the temperature is still possible with a good accuracy even 20 minutes after laser irradiation. In conclusion, temperature monitoring by using fluorescence measurement of laser-induced release of liposome-encapsulated dye is clearly demonstrated. This procedure could conceivably prove useful for controlling the thermal coagulation of biological tissues.
Microthermometry of laser-heated Chinese hamster ovary cells and sperm cells
Yagang Liu, Gregory J. Sonek, Curtis F. Chapman, et al.
Microthermometric measurements on optically-trapped Chinese Hamster Ovary (CHO) cells and sperms cells re reported, using a noninvasive microfluorometric detection technique. Within an optical tweezer system that has been outfitted with a spectral fluorescence excitation and detection capability, the changes in temperature induced by the process of sample confinement by a focused laser beam has been quantified over micron-sized spatial regions of both motile and immotile cells. Our measurement technique is based on the use of environmentally sensitive fluorophores that can be incorporated into the cell membrane and used to sense local changes in temperature when the cell membrane is perturbed optically or via other environmental stress factors. Using a cw 1.064 micrometers Nd:YAG laser for trapping CHO and human sperm cells, a temperature increase of approximately equals 1°C per 100 mW laser power was observed. At this infrared wavelength, cellular heating as result of laser confinement appears to be mainly due to radiation absorption by water.
Thermal Effects II
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Ultrasonic detection of photothermal interaction of lasers with tissue using a pulsed Doppler system
Hao Ying, Aamer Azeemi, Craig J. Hartley, et al.
Thermal therapy using various heating sources such as lasers or microwaves to destroy benign and malignant lesions has recently gained widespread acceptance. However, the accurate prediction of thermal damage in tissue according to theoretical or computer modeling is difficult and unreliable due to target variability with respect to physical properties, geometry, and blood perfusion. Thus, one of the major obstacles to application of thermal therapies has been the lack of a noninvasive, real-time method that could determine the extent and geometry of treated tissue. To evaluate the effects of laser heating on tissue, we have developed an analog-digital hybrid Doppler ultrasound system to measure the phase and amplitude of ultrasonic echoes returned from the heated tissue. The system consists of an eight-gate pulsed Doppler detector, a 16-channel 12-bit A/D converter, and a signal analysis and visualization software package. In vitro studies using canine liver showed two distinct types of modulation of the echoes along the ultrasound beam path during laser irradiation using an 810 nm diode laser. Type 1 signals showed a small and slow variation in amplitude and phase, and were attributed to tissue coagulation. Type 1 signals showed a small and slow variation in amplitude and phase, and were attributed to tissue coagulation. Type 2 signals showed large and rapid variations in amplitude and phase which usually appeared after tissue surface explosion and were indicative of tissue ablation. We hypothesize that the observed phase changes in type 1 signals are due to thermal effects within the tissue consistent with tissue expansion and contraction while the phase changes in type 2 signals are likely due to formation and motion of gas bubbles in the tissue. A further development of the Doppler ultrasound technique could lead to the generation of feedback information needed for monitoring and automatic control of thermal treatment using various heating modalities such as laser, high intensity focused ultrasound, microwaves, or radio frequency waves.
Charts to rapidly estimate temperature following laser irradiation
A recurring problem in laser applications is estimating the thermal response of target tissues to laser irradiation. This typically involves using an optical model to determine the distribution of absorbed laser energy and then using a thermal model to establish the temperature during and after laser irradiation. To avoid such modelling and yet allow one to obtain fast, accurate estimates of temperature, a series of charts for laser irradiation of semi-infinite homogeneous media with adiabatic boundaries is presented. These charts were created using analytic solutions of the temperature for absorbing-only media with simple pulsed source geometries. Through the use of nondimensional parameters, these charts allow one to make rapid estimates of the spatial and temporal thermal distributions following laser irradiation for arbitrary pulse durations and absorption coefficients.
In vitro interstitial laser (805 nm) photocoagulation (ILP): comparison of fiber tips
Xiaomei Shi, Abraham H. Dachman
We sought to study the effect of fiber tip modification on the size and shape of lesions created by the interstitial application of a 805 nm diode laser. In order to clarify conflicting results of other authors, we performed a large number of burns in order to obtain definitive statistically significant data. The plastic cladding and jacket were removed from the distal 5 mm of a hard polymer clad fused silica fiber of 600 micrometers . Three tip modifications were compared: a bare cut tip with and without precharring and a conical diffused tip. Continuous wave laser radiation was applied over a 1.0 to 2.5 watt range at 0.5 watt increments for a duration of 5, 10, and 15 minutes in vitro using fresh pig liver. The liver burns were thinly cut in cross-sections, and photographed. The sizes of the resultant cavity and lesion were measured and analyzed for statistical significance.
Hemothological Research
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Interactions of monochromatic visible light and near-IR radiation with cells: currently discussed mechanisms
Biological responses of cells to visible and near IR (laser) radiation occur due to physical and/or chemical changes in photoacceptor molecules, components of respiratory chains (cyt a/a3 in mitochondria, and cyt d in E. coli). As a result of the photoexcitation of electronic states, the following physical and/or chemical changes can occur: alteration of redox properties and acceleration of electron transfer, changes in biochemical activity due to local transient heating of chromophores, one-electron auto-oxidation and O2- production, and photodynamic action and 1O2 production. Different reaction channels can be activated to achieve the photobiological macroeffect. The primary physical and/or chemical changes induced by light in photoacceptor molecules are followed by a cascade of biochemical reactions in the cell that do not need further light activation and occur in the dark (photosignal transduction and amplification chains). These reactions are connected with changes in cellular homeostasis parameters. The crucial step here is thought to be an alteration of the cellular redox state: a shift towards oxidation is associated with stimulation of cellular vitality, and a shift towards reduction is linked to inhibition. Cells with a lower than normal pH, where the redox state is shifted in the reduced direction, are considered to be more sensitive to the stimulative action of light than those with the respective parameters being optimal or near optimal. This circumstance explains the possible variations in observed magnitudes of low-power laser effects. Light action on the redox state of a cell via the respiratory chain also explains the diversity of low-power laser effects. Beside explaining many controversies in the field of low-power laser effects (i.e., the diversity of effects, the variable magnitude or absence of effects in certain studies), the proposed redox-regulation mechanism may be a fundamental explanation of some clinical effects of irradiation, for example the positive results achieved in treating wounds, chronic inflammation, and ischemia, all characterized by acidosis and hypoxia.
Basic Research
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Allosteric enzyme behavior: the onset of oscillations EM field sustained
F. Causa, Michele Costato, Marziale Milani, et al.
The experimental set up is discussed for yeast fermentation monitoring in connection with irradiation procedures. The key role of the PFK enzyme is examined and a model for ATP-ADP competition is presented.
Does low intensity He-Ne laser radiation affect the intracellular pH of intact Escherichia coli cells?
Terence I. Quickenden, Lillian L. L. Daniels, Lyndsay T. Byrne
Claims that low levels of He-Ne laser light (cw, (lambda) equals 632.8 nm) can provide clinical benefits and can enhance in vitro cellular growth are still controversial (T.I. Quickenden and L.L. Daniels, 1993, Photochem. Photobiol. 57, 272-278; L.L. Daniels and T.I. Quickenden, 1994, Photochem. Photobiol., 60, 481-485). The present study tests the suggestion (T.I. Karu, 1988, Lasers life Sci. 2, 53-74; H. Friedmann, R. Lubart, I. Laulicht and S. Rochkink, 1991, J. Photochem. Photobiol. B: Biol. 11, 87-91) that red light stimulates mitosis by raising intracellular pH via absorption by chromophores in the respiratory chain. In order to search for photoinduced changes in intracellular pH, the effect of 5 mW He-Ne laser irradiation on cultures of E. coli was examined using a 300 MHz Nuclear Magnetic Resonance (NMR) spectrometer. The pH difference between the intracellular and extracellular fluid was monitored in the presence and absence of radiation by determining the difference in chemical shift for 31P resonances arising from the H2PO4- ⇔ HPO42- + H+ equilibrium in the two environments.
Action of low-energy monochromatic coherent light on the stability of retinal lysosomes
Irina P. Metelitsina, N. F. Leus M.D.
The data had been obtained during the experiment in vitro by irradiation of solubilized lysosomal enzymes, retinal homogenates and native lysosomes enabled us to conclude that the laser beam ((lambda) equals 632.8 nm, power density from 0.1 to 15.0 mWt/cm2) acts on the level of membranous structures of lysosomes. During irradiation of rabbits eyes in vitro with an unfocused laser beam (power density on the cornea aur face from 0.01 to 15.0 mWt/cm2 was shown, that low-energy, ranged from 0.01 to 1.0 mWt/cm2 promotes stabilization of lysosomal membranes. Irradiation with laser beam of 8.0 mWt/cm2 and more power induces destabilization of lysosomal membranes. We have also shown that vitamins A and E effecting membranotropic on lysosomes may be corrected by low-energy radiation of helium-neon laser. It is substantiated experimentally that the stabilizing effect of vitamin E may be intensified in case of the combined action of laser radiation on lysosomes. The labilizing effect of vitamin A on membranes of organelles, as was studied, may be weakened by application of laser radiation of low intensities.
Distant cells interaction via radiation in the visible region
Vasili A. Mostovnikov, Galina R. Mostovnikova, Vitali Yu Plavski, et al.
Optical set-up for the discovering of distant interaction between cells monolayers is proposed. This set-up allows to show with high degree of trustworthiness, that animal cells monolayer (monolayer-inductor) having its mitotic activity as a result of outer influence emits electromagnetic radiation that causes adequate alterations in the cells monolayer (monolayer-detector) placed at some distance from monolayer- inductor. It is established that distant interaction between cells monolayers (mitosis synchronization) is realized by the radiation of visible spectral range. The effect of distant synchronization mitosis in a inductor-detector pair observes both in the case of cells stimulation mitotic activity and in the case of activity inhibition. The mitosis synchronization is absent when a filter absorbing light in visible spectral range is used or optical contact between monolayer-inductor and monolayer-detector is disturbed.
Molecular mechanism of biological and therapeutical effect of low-intensity laser irradiation
Vasili A. Mostovnikov, Galina R. Mostovnikova, Vitali Yu Plavski, et al.
The investigations carried out in our group on biological systems of various organization level (enzyme molecules in solution, human and animal cell cultures), allowed us to conclude, that the light-induced changes of spatial structure of cells components form the basis of biological activity (and as a consequence therapeutic effect) of various wavelength low-intensity laser emission. Photophysical mechanism of these changes lies in the reorientation of highregulated anisotropic parts (domains) with the liquid-crystalline type of ordering of the cell components due to the interaction between the electric field and the light induced integral electric dipole of the domain. The mechanism of such reorientation is well established in physics of liquid crystals of nematic type and is known as light induced analogue of Frederix's effect. The following results enable us to draw the conclusion about the determining role of the orientations effects on the biological activity mechanism of low-intensity laser radiation: (i) the possibility of reversible modification of spatial structure and enzyme molecules functional activity under the influence of laser radiation outside the band of their own or admixture absorption; (ii) the dependence of biological effect of laser radiation on the functional activity of cells vs. polarization degree of the light with the maximum photobiological effects observed for linear-polarized radiation; (iii) the equivalence of a static magnetic field and low-intensity laser radiation in action on functional activity of the cells and the lowering of the laser field intensity for the achieving the difinite changes of the cell functional activity in the presence of static magnetic field.
Hemothological Research
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Adenylate pool and energy charge in human lymphocytes and granulocytes irradiated at 632 nm (HeNe laser)
Lorenzo Bolognani, T. Venturelli, N. Volpi, et al.
Aim of this report was to investigate the adenylate pool and the energy charge in human white blood cells exposed to increasing time (15, 30 and 60 min) of HeNe laser treatment. EDTA treated human blood diluted 1:1 with 0.88% KCl was added (1:5) with NaCl-dextran solution to allow sedimentation of red blood cells. 6 ml of the white cells floating in the supernatant were layered on 3 ml of Lymphoprep in plastic tubes and each tube was centrifuged (from 50 to 5000 X g for 5 min). Granulocytes were concentrated in the lower phase, whilst lymphocytes were in the intermediated phase. After further purification cytological homogeneity was tested by a cell counter. Granulocytes and lymphocytes were irradiated at +22°C with HeNe (Space, Valfivre equipment). On these population ATP was tested by luminometric procedure, the adenylate pool was separated by HPLC (Jasco) on neutralyzed perchloric extracts. ATP concentration increased in lymphocytes (+63.9%, p < 0.01) and in granulocytes (+25.0%, p < 0.05) after 60 min irradiation. The adenylate pool (tested by HPLC) does not change significatively in lymphocytes or granulocytes after 30 min irradiation, whilst in 60 min irradiated lymphocytes and granulocytes a significative increment was observed in nucleotide concentration. No changes were observed in energy charge according to Atkinson.
Laboratory research of laser-radiated blood therapy and its clinical application
Fu-Shou Yang, Xi-Cheng Yang, Hong-Lin Zhang
This paper deals with the therapy by the He-Ne laser of low power, modulated pulse and low dosage of 365 nm optic source. To radiate the blood in vitro of patient's, at the time, the blood was treated with addition of oxygen. The treated blood was then retransfusion into the same patient. From 1993 to 1994, we have cured 202 cases with prominent therapeutic effect. The results of clinic and laboratory research showed: It greatly increased the immunologic function of the body, the total effective ratio achived 95% (cerebral vascular diseases), and greatly decreased the drug reaction of patients after the tumors were treated by chemotherapy and radiotherapy.
Clinical Research
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Effect of low-power laser on wound healing at the site of tracheal anastomosis in rats
Koji Sensaki M.D., Tsunenori Arai, Susumu Tanaka M.D., et al.
The effect of low power laser on the wound healing process was investigated at the site of anastomosis in rats. Tracheal reconstruction was performed after the tracheal transection and He-Ne laser (NEC,GLG5360, wavelength 632.8 nm)(3.3 X 10-3 W/cm2, 5 min) was irradiated to the site of anastomosis. Structural and functional recoveries were evaluated at 1 and 2 weeks postoperatively. Hydroxyproline content, epithelial condition, cellular infiltration, fiber proliferation, microstructure of cilia, mucociliary function and neovascularization were measured. Hydroxyproline was measured with Amino acid autoanalyzer (Hitachi 835-50). Microstructure of cilia was observed with scanning electron microscope (JSN-840, JEOL). Mucociliary function was evaluated by India ink movement. The hydroxyproline contents per 1 mg dry weight in irradiated group and control group were equivalent (approximately 20 (mu) g). Cellular infiltration of irradiated group was fewer than that of control group. The degree of mucociliary functional recovery in the irradiated group was better than that of control group. Among the cases that showed the structural recovery of cilia, the functional recovery was observed in whole irradiated group, and in 40% of control group. Neovascularization was more pronounced in irradiated group. From this study it is suggested that the laser irradiation may reduce the inflammation and promote the recovery of mucociliary function at the site of anastomosis.
Low-energy laser irradiation: a possible neuroprotective modality
Michal Schwartz, E. Yoles, Arieh S. Solomon M.D., et al.
We have tested the effects of early posttraumatic low-energy laser irradiation on injured neural tissues. Rat optic nerves were crushed by a calibrated forceps and the ensuing degenerative processes were followed up electrophysiologically and by on-line metabolism measurements, using nicotinamide adenine dinucleotide autofluorescence in response to anoxia. The irradiation not only decelerate the posttraumatic degenerative processes but also increased axonal survival as shown by visual evoked potential response recording. The irradiation also reduced significantly the very early posttraumatic reduction in the metabolic activity of the optic nerve. It seems that the low-energy irradiation, possibly by a photochemical mechanism and by modifying he cellular metabolism, prevents the spread of the injury effects from the injury site and along the axons. This action of low-energy laser irradiation is akin to the neuroprotective effects ascribed to various drugs, such as corticosteroids.
Confocal scanning laser evaluation of repeated Q-switched laser exposure and possible retinal NFL damage
Harry Zwick, Donald A. Gagliano, Joseph A. Zuclich, et al.
Repeated extended source Q-switched exposure centered on the macula has been shown to produce a Bullseye maculopathy. This paper provides a confocal scanning laser ophthalmoscopic evaluation with regard to the retinal nerve fiber layer (NFL) and deeper choroidal vascular network. Confocal imaging revealed that the punctate annular appearance of this lesion in the deeper retinal layers is associated with retinal nerve fiber bundle disruptions and small gaps in the retinal NFL. No choroidal dysfunction was noticed with Indocyanine green angiography. It is hypothesized that retinal NFL damage occurs either through disruption of retinal pigment epithelial cell layer support to the NFL or through direct exposure to high spatial peak powers within the extended source beam profile, causing direct microthermal injury to the NFL. The apparent sparring of the fovea reflects central retinal morphology rather than a lack of retinal damage to the fovea.
Exocrine and endocrine testicular function during the treatment of experimental orchitis and nonspecific orchoepididymitis by low-energy laser radiation
Leonid L. Reznikov M.D., Ludmila S. Pupkova, H. Bell, et al.
Investigations into the biological effects of low-energy laser radiation (LLR) are characterized by a score of challenges, which are due primarily to a cascade of laser-induced and sometimes antagonistic processes. To investigate these processes on various biologic levels, we analyzed local and general effects of LLR on the exocrine and endocrine functions of the accessory sex glands in experimentally induced orchitis and orchoepididymitis in rabbits, and in clinical studies on male patients. The results indicate that LLR may alter the inflammatory response, including the exudative reaction, macrophage migration, and fibroblast activity. Furthermore, LLR may result in changes in serum concentrations of LH, FSH, and ACTH, prolactin, testosterone, cortisol and aldosterone. Some of these changes may be at least partially responsible for the well-known anti-inflammatory effects of LLR.
Comparative study of neurohormonal effects of low-energy laser acupuncture and traditional reflex therapy in the treatment of male hypofertility
Ludmila S. Pupkova, Leonid L. Reznikov M.D., H. Bell, et al.
Reflex therapy is one of numerous applications of low-energy laser radiation in medical treatment. The advantages of this therapy in comparison with traditional acupuncture include technical simplicity, absence of pain, and, as a consequence of the complete noninvasiveness of the procedure, the absence of risk of contracting AIDS or other infectious diseases. However, no definitive results have been published regarding the comparative effectiveness of the two approaches to reflex therapy. In view of the neurohumoral role in the curative effects of reflex therapy, we compared laser acupuncture and the traditional needle technique in relation to changes in the serum concentrations of the principal sexual and gonadotropic hormones in hypofertile men.
Low-energy laser treatment of rheumatic diseases: a long-term study
Ciprian Antipa, Vladimir Moldoveanu, Nicolae Rusca, et al.
We tried to establish the efficiency of low energy (power) lasers (LEL), in various inflammatory and noninflammatory rheumatic diseases during five years. We treated 514 patients with osteoarthrosis, 326 patients with nonarticular rheumatism and 82 patients with inflammatory rheumatism, in four different ways: only with Galium-Aluminum-Arsenide (GaAs) infrared lasers; both GaAs lasers and Helium neon (HeNe) lasers; with placebo laser; with classical anti-inflammatory therapy. The results were analyzed using local objective improvements and the score obtained from a pain scale before and after the treatments. We also note some preliminary results obtained by the computer analysis of the evocated potentials after laser irradiation. We conclude that LEL (especially HeNe with GaAs) is obviously more efficient than placebo laser therapy and also had better or at least similar results, in most of the cases, than classical anti-inflammatory therapy.
Effects of low-power laser irradiation on the mitosis rate of the corneal epithelium
Varda Chen, Nahum Landshman M.D., Michael Belkin M.D.
The effect of repeated low power He-Ne laser on rabbit's corneal epithelium was studied after 3 daily sessions. Under certain irradiation parameters, low power He-Ne laser irradiation was found to change the mitotic rate in the basal layer of intact corneal epithelium. Three daily irradiations for 3 or 10 minutes increased the mitotic index while 30 minutes irradiations decreased it.
Hemothological Research
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Biological effects of low-energy laser and nonlaser light irradiation on fish embryos
Natalia B. Savchenko, Alexander V. Priezzhev, Borislav A. Levenko
The problems of choice of live models for the study of laser and nonlaser light irradiation effects on animal organisms are discussed. Fish embryos are shown to fit many requirements related to the performance of experiments in clearly defined conditions. Laser Doppler microscopy yielding quantitative data on the dynamic response of the embryos irradiation have proved to be an adequate technique. Preliminary experimental data on the biological effects of light on different types of embryos are presented.
Formation of secondary messengers by blood-formed elements in low-power laser irradiation
Gregory E. Brill, Olga V. Proshina, Valentina N. Zhigalina, et al.
Irradiation of heparinized rat blood by He-Ne laser light ((lambda) - 632.8 nm, power density - 5 mW/cm2) during 15 or 30 min was performed in vitro experiments. The complex of biochemical parameters of erythrocytes, plasma and cytochemical parameters of polymorphonuclear leucocytes was studied. Laser irradiation was stated to cause different metabolic changes in red blood cells and neutrophils depending on the dose. In both doses of irradiation glucose-6-phosphate dehydrogenase activity lowers in erythrocytes, succinate dehydrogenase activity and lysosomal cationic proteins content increase in neutrophils. Stimulation of oxygen active forms production in cellular membranes of blood formed elements results in plasma malonic dialdehyde level increase and in the change of the balance between primary and secondary lipid peroxidation products. Cooperative interaction between different blood cells in the process of realization of system response to laser exposure is supposed to exist.
Optical Dynamics
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Coupled light transport-heat diffusion model for laser dosimetry with dynamic optical properties
Richard A. London, Michael E. Glinsky, George B. Zimmerman, et al.
The effect of dynamic optical properties on the spatial distribution of light in laser therapy is studied via numerical simulations. A 2D, time dependent computer program called LATIS is used. Laser light transport is simulated with a Monte Carlo technique including anisotropic scattering and absorption. Thermal heat transport is calculated with a finite difference algorithm. Material properties are specified on a 2D mesh and can be arbitrary functions of space and time. Arrhenius rate equations are solved for tissue damage caused by elevated temperatures. Optical properties are functions of tissue damage, as determined by previous measurements. Results are presented for the time variation of the light distribution and damage within the tissue as the optical properties of the tissue are altered.
Thermal Effects II
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Effects of simultaneously fiber transmitted erbium and holmium radiation on the interaction with highly absorbing media
Martin Frenz, Hans Surya Pratisto, Michael Ith, et al.
Erbium and Holmium lasers have both been shown to be suitable for orthopedic surgery performed under water. Erbium lasers emitting in the 3 micrometers wavelength region corresponding to the maximum water absorption peak effectively ablated biological tissues with high precision and minimal thermal damage. Holmium laser radiation at 2 micrometers , due to a lower absorption coefficient, is characterized by a greater extent of thermal damage leading to hemostasis. To combine the special advantages of each system we simultaneously coupled their radiation into a zirconium fluoride fiber (ZrF4) which was protected with a quartz fiber tip. Pressure measurements performed in the liquid using a piezo electrical transducer, transmission measurements and video flash lamp schlieren imaging of the laser induced vapor bubble were used in order to determine optimum laser parameters. The cutting efficiency of the Erbium laser is drastically improved when a low energy Holmium laser pulse is additionally used which is just able to open a vapor channel through which the Erbium laser pulse can be transmitted. The dynamics of the channel formation, geometry and life time are measured as a function of the delay time between the two different laser pulses and the pulse energy applied. The combination of 2 micrometers and 3 micrometers radiation seems to be an ideal instrument for tissue treatment.
Ablation III
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Plasma-mediated ablation of biological tissues with ultrashort laser pulses
Plasma mediated ablation of collagen gels and porcine cornea was studied at various laser pulse durations in the range from 350 fs to 1 ns at 1053 nm wavelength. A time resolved stress detection technique was employed to measure transient stress profiles and amplitudes. Optical microscopy was used to characterize ablation craters qualitatively, while a wide band acoustic transducer helped to quantify tissue mechanical response and the ablation threshold. The ablation threshold was measured as a function of laser pulse duration and linear absorption coefficient. For nanosecond pulses the ablation threshold was found to have a strong dependence on the linear absorption coefficient of the material. As the pulse length decreased into the subpicosecond regime the ablation threshold became insensitive to the linear absorption coefficient. High quality ablation craters with no thermal or mechanical damage to surrounding material were obtained with 350 fs laser pulses. The mechanism of optical breakdown at the tissue surface was theoretically investigated. In the nanosecond regime, optical breakdown proceeds as an electron collisional avalanche ionization initiated by thermal seed electrons. These seed electrons are created by heating of the tissue by linear absorption. In the ultrashort pulse range, optical breakdown is initiated by the multiphoton ionization of the irradiated medium (6 photons in case of tissue irradiated at 1053 nm wavelength), and becomes less sensitive to the linear absorption coefficient. The energy deposition profile is insensitive to both the laser pulse duration and the linear absorption coefficient.