Laser beam, first introduced in the field of ophthalmology in 1964 has been a powerful tool in medicine, plastic or general surgery, dermatology, gynaecology, oncology,
Laser pulses with a sufficient spatial resolution can introduce a physical gate in either a membrane or a cell wall under physiological environment such that one could deliver a foreign material into the cell and bring about selective manipulation of subcellular components without demolishing the cell’s integrity. It has been reported that in Japonica rice (
It is important to understand the developmental process of a pollen including germination of a receptive stigma and consequent tube growth as a basic sexual mechanism in flowering plants for the manipulation of plant production (Taylor & Hepler, 1997). Pollen transformation is also considered as an alternative strategy for the genetic engineering. Pollen acts as a natural vector for direct gene transfer due to its involvement in the normal sexual process in flowering plants and hence, transformed pollen has been used to generate numerous transgenic plants such as Tobacco, Scots pine etc., (Van der Leede-Plegt et al., 1995; Touraev et al., 1997; Aronen et al., 2003). In addition to several other potential advantages of this technology like rapid propagation with reduced somaclonal variation, pollen transformation does not require any
In first section of this chapter, we are discussing the application of ultrafast laser optoperforation to make a transient hole on lily (
We will devote the latter part of this chapter to explain the ultrafast laser-assisted optoperforation of endothelial cell membrane. In order to induce the transient perturbation on the live-cell plasma membrane for the efficient delivery of foreign materials, including drugs or genetic material, into the live cells (such as embryonic stem cell), numerous chemical or physical methods have been employed (Kobayashi et al., 2005). Also, it’s an ever chasing challenge waiting for us to elucidate the mechanism involved in the self-healing process of the perforated live cell plasma membranes. The mechanism for laser-mediated foreign material transfer as well as other perturbation methods was hypothesized with a limited understanding of the structure and functions of membrane lipids (Engelman, 2005). Recently, the fundamental mechanisms of fs-laser interaction with an aqueous media are extensively studied by Vogel et al. (Vogel et al., 2005). The most frequently invoked explanation was based on the assumption that the physicochemical methods used in the specific cases may either perforate the surface of the cell membranes or enhance the permeability of the foreign materials, enabling a transient transfer of foreign molecules into the cytosol (Kobayashi et al., 2005; Zeira et al., 2003). Manipulation and operation using ultrafast laser pulses have been introduced as a promising tool for the cellular nanosurgery and the transfer of foreign molecules into live cells under
2. Ultrafast laser optoperforation of lily (
Lilium hybrid cv Shiberia) pollen
2.1. Materials and method
Mature pollens were obtained from the anthers of
Near-infrared laser beam from amplified Ti:sapphire femtosecond laser at a repetition rate of 1 kHz (Quantronix) was focused on the pollen exine through objective lens (N.A. = 0.6) so that we could selectively puncture a wall inside an ornament. Petri dish containing the pollen grains was mounted on a motorized XYZ – translation stage, which is used to manipulate the sample to expose a fresh pollen grain surface at each laser pulse. The images obtained during the fs-laser irradiation on the pollen’s surface were fed into a personal computer for further data analysis. Laser fluence was attenuated by a variable neutral density filter. All the laser exposers were conducted under a single shot configuration by using a fast mechanical shutter with a opening time constant of 0.6 ms, which is synchronized with the laser. After optoperforation, the viability of the operated pollen grains was checked by measuring the germination rate of pollen tube by intrusion of propidium iodide (PI). The glass coverslips with grids marked on the surface, were used to cover over the pollens for the localization of the irradiated pollen grains.
For the pollen transformation study, a foreign DNA with a construct, encoding F1TPae-γ mitochondrial targeting sequence fused to RFP; was added into the culture medium before the laser optoperforation (Lee et al., 2001). MitoTracker Green FM (Molecular probes, invitrogen) was further used to confirm the RFP expression. MitoTracker Green FM is a conventional fluorescent marker used for tracking of the mitochondria (Lovy-Wheeler et al., 2007).
Pollen germination as well as its response to optoperforation was characterized with an optical microscope and a fluorescent microscope (Axioskop, Zeiss). In order to confirm the hole size, the intact pollen surface treated with laser beam was imaged by atomic force microscope (XE-120, PSIA) without any further treatments.
2.2. Results and discussion
It was observed that size of lily pollen grain increased during pollen re-hydration process. Before pollen tube starts to grow, a laser beam was precisely focused into the interior of the ornament of pollen surface. Figure 1 shows sequential optical microscopic images captured from the movie file obtained during fs-laser optoperforation of lily pollen walls. Immediately, after laser pulse irradiation on pollen wall surface, a cytoplasmic content of the pollen oozes out from the pollen grains.
This observation is consistent with the previous reports stating that UV laser pulses treatment causes release of cytoplasmic content either from the pollen itself or its tube (Hoffmann, 1996). This abrupt extrusion of cytoplasm from the treated pollen can be explained in terms of a high turgor pressure inside the hydrated pollen, which ranges between 0.1 and 0.4 MPa, and the mean value being 0.21 ± 0.06 MPa. (Benkert et al., 1997). Unless the buffering osmotic pressure is against the turgor pressure, the pressure inside the cell will no longer sustain due to the presence of hole on the wall. Following the cytoplasmic extrusion, a large vesicle with a diameter of about 10 μm was also flushed out from the pollen grain through the hole. The excluded large structure was apparently distinct from the concomitant flushed contents, as seen under optical microscope. The distinct boundary was rather rigid in nature and it remains intact without any bursting phenomenon.
The extrusion of pollen’s cytoplasmic contents and the large organelle was strongly dependent on laser fluence. Figure 2 shows a series of optical microscopic images and a graph that represents the normalized germination percent of the pollen grains as a function of the laser fluence (0.11 – 7.10 J/cm2). With changing the laser fluence energy from 0.11 J/cm2 to 7.10 J/cm2, we perforate the pollen walls with single fs-laser pulse. Figure 2(a)
shows the exclusion of pollen’s cytoplasmic contents at progressive laser fluence energy levels. We observe that the hydrated lily pollens mostly begin to exclude cytoplasmic contents at the laser fluence energy level of 1.42 J/cm2. Sometimes we can observe the extrusion of the cytoplasmic contents even at the laser fluence less than 1.42 J/cm2. We have also compared the germinabilty rates of treated
We have cross-checked the viability of the pollen grains after optoperforation by the observation of intrusion of the PI (Propodium Iodide). About 150 out of 300 opto-perforated pollens were not stained with PI despite of the massive exclusion of the cytoplasmic contents, indicating that the fs-laser optoperforation of lily pollen wall hardly harms its viability. More interestingly, the excluded large organelle was not stained with PI, even though the organelle was not likely surrounded by pollen wall. This observation led us to assume that the organelle excluded from the pollen grains by the fs-laser processing still maintained its biological integrity without any observable perturbation.
Figure 4 exhibit a series of optical microscopic images during the
Subsequently, we emphasized our study on nucleus staining of the treated pollens to have a deeper understanding on the nature of excluded large organelles. Figure 5 shows bright-field optical image (a) and fluorescence image (b) of pollens stained with nucleic acid specific dye acridine orange after the fs-laser treatment (1, 2, and 3 labelled pollens). Cellular contents were massively extruded from all of the treated pollens upon illuminating rather at the high laser fluence (~8 μJ/pulse). Amongst them, only pollen “1” has been successfully
germinated to grow the pollen tube. It should be noted that an apparent fluorescent spot (arrow), indicating the presence of nucleic acid, was observed in the excluded contents in all the treated pollen grains. A faint emission indicated by an arrow head, which supposed to be a vegetative nucleus, was clearly observed in the pollen tube geminating from pollen “1”. Meanwhile, the nuclei excluded from the same pollen were obviously seen outside the pollen grain. Thus, it is most likely to state that the excluded large vesicle from the pollen “1” must either be a generative cell with its own nucleus or a sperm cell after the second mitotic division. In other words, the vegetative nucleus of treated pollen “1” is well trapped/tracked inside the tube, while the regenerative nucleus or sperm cell stayed outside the pollen. Vervaeke et al. suggested that the vegetative nucleus (VN) and the generative cell (GC) form a functional assemblage to generate callose plugs (Vervaeke et al., 2005; Strubinska & Sniezko, 2000). However, our findings clearly indicate that the close physical contact between the vegetative nucleus and the generative cell is not a necessary requisite for the pollen germination. Instead, it suggests a kind of chemical connection between the two constituents. Even if it is not known as how the two constituents are connected physically or chemically, the extrusion of generative cell from lily pollen grains by fs-laser optoperforation does not alter the growth of pollen tube or vegetative nucleus movement to a greater extent.
We have further performed the transformation studies for the fs-laser treated
mitochondria and results in the expression of green fluorescence. Exact matching of RFP fluorescence image with that of mitochondria in pollen tube led us to conclude that, the foreign DNA with a construct encoding F1TPae-γ mitochondrial targeting sequence fused RFP was delivered into pollen and expressed as designed. Statistically, 42 pollens out of 206 treated pollens were germinated. Amongst the germinated pollens, foreign DNA expression in mitochondria delivered by fs-laser optoperforation was observed in 9 pollen tubes out of 42 germinated pollens. As a result, the transformation efficiency of lily pollen by fs-laser optoperforation was about 4.4 %. However, in case of germinated pollens, the efficiency was about 21.4 %. This transformation efficiency was higher than that of American chestnut pollen transformation based on particle bombardment method to transiently express GFP with an efficiency of 4.1 % (Fernado et al., 2006).
3. Ultrafast laser optoperforation of endothelial cell membranes
3.1. Experimental techniques and materials
The perforation of the plasma membrane of live cells was performed with a femtosecond amplifier system (Integra, Quantronix) with maximum output energy of 1 mJ/pulse at 780 nm, of which the pulse width and the repetition rate is 150 fs and 1 kHz, respectively (Jeoung et al., 2005). The laser beam was tightly focused on the membrane with a high-numerical-aperture objective lens (Nikon, X100, N.A = 1.3, oil immersion lens) mounted to an inverted microscope (Axiovert 200M, Zeiss). All the experiments were done under single-shot configuration by using a fast electrical shutter with an opening time constant less than 0.5 ms. In order to eliminate any desperate loss of laser energy during these experiments, the fast electrical shutter was perfectly synchronized with the laser. The laser energy before the objective lens was kept to be about 5 ~ 7 nJ/pulse by attenuating it with a neutral density filter.
The changes in the topography and the optical images of plasma membrane induced by the ultrafast laser irradiations were simultaneously monitored with both an atomic force microscope (AFM) and a charge coupled device (CCD) detector, respectively. AFM (XE-120, PSIA) was slightly modified and combined to an optical microscope. AFM probe was carefully aligned to be aimed at same position of the focus of fs-laser beam. Contact imaging of the AFM was performed using a silicon nitride bio-cantilever (Bio-lever, Olympus, Japan), of which nominal force constant is 0.03 nN/m. The topographies have been obtained by optimising the AFM running parameters that gives the identical results to that of the two-way scanning configuration (Parpura et al., 1993& Velegol et al., 2003). The set point for loading force was kept to be very weak between 0.65 nN and 1 nN, to minimize the damage or the attractional movement caused by attraction force of the AFM tip. A successive scanning of the live cells exhibit no observable changes in its phenotypes.
The measurements of the velocity field responsible for the membrane motility after fs-laser perforation have been measured by a micro particle image velocimetry (μ-PIV) (Yahng et al., 2005). The visualization of membrane movements was figured out by attaching a fluorescent polystyrene bead (diameter ~ 200 nm) on the plasma membrane of a target cell. Just after the fs-laser irradiation on the surface of plasma membrane, two successive ns-laser pulses with a time lapse of 10 ms were employed to capture the two fluorescence images. Thereafter, the velocity fields of membrane motility were obtained by a cross correlation calculation with the two images. We have confirmed that there is no damage on the cells with the current volumetric excitation with the ns-laser pulses, where the laser fluence is kept explicitly low.
Neuroblastoma (Neuro2A) cells were used to investigate the dynamics of its plasma membrane and self-healing process. During the experiment, live cells were kept inside a sterile miniaturized cell chamber filled with Dulbecco's Modified Eagle's Media (DMEM, Gibco BRL) containing 10 % Fetal Bovine Serum (FBS, Gibco) and 1 % penicillin/streptomycin (Gibco) under humid atmosphere at 5 % CO2 partial pressure. Although the lid glass of the cell chamber was removed for AFM imaging or other measurements, no apparent change in its phenotypes was observed within time span of (1.5 hr) the current experiments.
As a consequence of single-pulse ultrafast laser irradiation on the cells surface (ca. 5 ~ 7 nJ), a circular area appears to be observed on its plasma membrane as shown in Fig. 8(a). The injured area increased relatively fast over several tens of seconds comparable to the percentage of cellular size. It is interesting to note that the initial circular type of injured membrane area changes to an elliptical one with a long axis parallel to the cell. After
reaching at its maxima of about 6.4 x 4.9 μm2, within several tens of seconds (Fig. 8(b)), the area starts decreasing spontaneously and then completely faded out in next 7 minutes (Fig. 8(c-d)). We have checked the cell viability using trypan blue-dye extrusion and found no evident change in laser treated cells compared to that of intact cells. AFM topography shown in Fig. 8(e-g) were taken with a time-laps after irradiation. Fig. 8(h) exhibit a typical cross-sectional height profiles along dotted line in Fig. 8(e). It shows the presence of a deep hole on the irradiated plasma membrane, of which diameter is about 1.6 μm at a full width at maximum. Meanwhile, the estimated initial size must be the upper limit due to the limitation of spatial resolution for optical detection as well as the limitation in scanning speed for topographical imaging by the AFM. However, the laser beam irradiations on the fixed cells under the similar experimental conditions leads to a submicron-sized selective ablation (for dissection) and hole drilling on the plasma membrane surface. With a repeated scanning of the injured membrane, the topographical image shows not only the spontaneous movement of the ruptured region on the plasma membrane but also the dynamic changes in its shape as well as its size.
While the presence of injured area was completely faded out in the optical images within a time span of several minutes after the perforation, further changes on the membrane surface were still observed in AFM topographical images as shown in Fig. 8 (f). The observations from the topographical images reveals that the highly localized irregular ruffled features along with small irregular movements after the laser irradiations are in-part an experimental observations for the self-healing process of the plasma membrane (Fig. 8 (f)). After about 1 hour, the plasma membrane was found to be fully recovered in its topographic feature and looks almost similar as that before the perforation. Accompanied with these dynamic changes in plasma membrane, a trace tailed to the operated cellular parts, which is initially absent as shown in Fig. 8 (e), appeared on the substrate surface after several minutes of the perforation. Close examination of the shape and position of the trace for laser perforations indicates a little cellular or cytosolic extrusion along with the progressive increment in hole-size.
Figure 9 exhibits the temporal behavior of the geometrically averaged radius of the hole induced by fs laser ablation. The temporal behavior of the injured area was found to be strongly dependent on the pulse energy and the irradiated position.
For all the cases, where the laser energy is in between 5 nJ and 7 nJ, a very small quantity of the cellular contents are extruded from the injured cells before complete disappearance of the changes at site of injured area. With the progressive rise in the laser fluence, initially there is a successive increase in the injured area verified by the increments in radius of perturbation. However, at the higher fluence levels, the cell contents are massively extruded from the cells results in the complete rupturing of the injured cells without any initiation of self healing process. Upon irradiating the cells towards the site of nucleus, the laser fluence even lower than 5 nJ results in complete rupturing of the plasma membrane. These observations suggest that geometrical factors of the plasma membrane of the live cells plays an important role in the dynamics of ruptured membrane of live cells, assuming that the physicochemical nature of the plasma membrane is isotropic across the entire live cell.
We have an access to the velocity field by attaching the fluorescent beads (diameter ~200 nm) on the surface of the plasma membrane with several time lapses (Fig. 10). After incubation of the cells with the beads for about 12 hours, a strong correlation between fluorescence and topographical image from the beads, led us to know that the beads were
not delivered into the cytosol but remain attached on the surface of plasma membranes. With an aid of applied force to the beads by AFM tip, we found that interaction force between the beads and plasma membrane is fairly high enough to visualize the membrane dynamics without any detachment of the beads during the dynamic membrane movements.
Just after the laser irradiation, the velocity field is found to be radial in approximately with a direction towards the edge of the cells. The magnitude of the velocity field decreased with increasing the distance from the position of irradiation. This suggests that all the lipids collected from the growing hole are almost homogeneously spread throughout the remaining area of plasma membrane. Furthermore, the absence of any rim collecting the lipids associated with a long-range flow of the membrane indicates a viscoelastic behavior of the membrane opening process. The velocity field of the membrane closer to the initial ruptured area turns to the opposite direction in next 0.7 seconds after the perforation, while the plasma membrane at a long distance from the irradiated area is keeps on expanding. Afterwards, the movement of velocity fields for the membrane looks randomized, as shown in Fig. 10(d) and (e). Followed to these interesting dynamical behaviors of the live cell membrane, overall pattern of the velocity field in both direction and magnitude resumed again, as observed just after the perforations previously (Fig. 10(f)). At a short span of time, the repeated change in direction of velocity field accompanied with an ultimate hole-size increment seems to be due to an elastic propagation. It behaves like a rubber, with fairly a high elastic modulus. After a long overall hole opening time, the velocity fields of membrane movement turned its direction towards the initially injured area, possibly be associated with the self-healing process of the created holes.
The simplest explanation for the mechanism of laser-mediated foreign material transfer is based on the assumption that the foreign material added to the transforming medium passively enters into the cell through the laser-induced membrane perforation. Furthermore, it successfully undergone with a rapid self-sealing process follows immediately with no subsequent and irreversible injury to the cell (Zeira et al., 2003). The results demonstrated in the current study made the above assumptions true for the Neuro 2A cells, where the cells were irradiated with an ultrafast laser in near infrared (NIR) region.
The dynamic behavior of the rapidly generated pores, either in organic films or in lipid vesicles has been widely studied (Debregeas et al., 1995& Sandre et al., 1999). These synthetic materials are quite different in many aspects from the current plasma membranes of the live cell. Especially, they are quite inhomogeneous in distribution of viscosity, having a different elastic modulus and three-dimensional shape, and lastly have a different lipid composition. Meanwhile the previous investigation suggests that the viscosity of the films plays a very important role in opening and closing dynamics of the perforated holes (Sandre et al., 1999). If viscous dissipation is associated with the generation of transient pores dominates the inertia due to the very high viscosity, the leak out or extrusion of the cytosolic components slows down; the pore reaches the size up to 10 m. The immersion of vesicles in a viscous environment allows visualization of transient pores in a membrane stretched by intense illumination or laser irradiations. Therefore, we have adapted a simple model to describe the dynamics of holes in the plasma membrane of live cells by an analogy with the opening of holes in viscous suspended long-chain polymer films and the dynamics of transient pores in stretched giant unilamellar vesicles (Sandre et al., 1999). The growth law of the hole is derived from a transfer of surface energy into viscous losses:
Following the model, we are proposing the dynamics of live-cell plasma membrane associated with perforation of a hole with an initial radius of
With opening of a hole at the radius
associated with the domination of restoring force of the hole due to the increment of line energy
Based on the above simple model, the dependence of the radius
For comparison, the opening time constant and closing speed for a synthetic unilamellar vesicles made of 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC) adhering on the substrate were reported to be 0.8 sec with
Finally, we would like to discuss some explanations for the irregular features observed from the topographical studies during the self-healing process (Fig. 8(f)). The topographical features were maintained for quite a long period even after the disappearance of optical signature of presence of holes on the cell membranes. The long lasting irregular ruffled structures of the membrane are likely to be associated with the final reconstruction of live cell membrane, to that of similar nature as present at the initial stages. Following the previous interpretations on the nature of films in the dynamic hole opening and closing behavior, the intracellular support network as well as the lipid molecules have been not reconstructed completely even though the cellular structures get close enough to do so. The chemistry and physics associated with the reconstruction process is still far from its complete understanding. We can suppose that a non-homogeneous reconstruction process at a relative slow reconstruction speed may result in the generation of irregular topographies at
the edge of colliding films on the surface of cells. In order to obtain qualitative information concerning on this supposition, the cells just after completing the closing process under bright field images were stained to know the actin network distribution. As shown in Fig. 12, the fluorescence image shows the lower intensity of Alexa Flour 635 Palloidin expression near to the perforated region rather than other parts of the cells. This observation partly supports our proposition that the reconstruction process of F-actin network might results in several tiny slices of lipid during sealing and interconnecting the dissected cell membrane at the final stage of self-healing process. Another possible interpretation on the observations might be the self-healing process of damaged surface membrane of live cells such as urchin’s egg and muscle cell by, so called, surface precipitation reaction mechanism proposed several tens of years ago (Heilbrunn, 1956; Gonzalez-Serrators et al., 1996). If this is the case, the piece of the lipid assembly should be together spontaneously to recover the injured surface membrane of live cells and resulted in the surface irregularity detected with only AFM techniques as shown in Fig. 8 (e)-(f). Even though no any conclusive remarks on the nature of the final reconstruction process of the damaged surface of the live cells will be given with the available information on the process, the irregular features observed should be strongly associated with reconstruction of not only the plasma membrane itself but also the actin network as an cytoskeleton structure of the live cells.
4. Ultrafast laser- assisted optoperforation of primary retinal blood vessels
4.1. Experimental techniques and materials
Furthermore, these extensive studies on single cell and plasma membrane dynamics open up the new scenarios, to apply this technology in a real surgical world, such as retinal blood vessel occlusions.
Experimental porcine eyes obtained from a local abattoir were deposited in ice cold Hanks’s Balanced Salt Solution (HBSS) and transported to the laboratory on ice (4 oC) within 1 hr after the slaughter. After a precise incision of the porcine eyes behind the ora serrata, cornea and lens, the retina tissues were carefully peeled off from pigmented epithelium and put it onto the Whatmann 2 paper. Before proceeding further for the fs-laser irradiations, the retina segments with size of about 3 X 5 mm2 were prepared and to closely mimic the
The fs-laser system used in this study consists of a regenerative amplified Ti: Sapphire ( = 810 nm) laser, delivering a 150-fs pulse at a repetition rate of 1 kHz (Quantronix, USA). The laser beam is focused on the retina surface with an objective lens of N.A. 0.4 and the estimated laser beam diameter at the retinal surface is about 1.3 μm. Similar to the previous setups, the retina tissues are mounted onto a motorized XYZ translation stage, which is used to manipulate the samples to expose a fresh area of tissue to each laser pulse (Fig. 13). The laser fluence used in the current work is in the range of 1.4 J/cm2 ~ 99.4 J/cm2. With 13 different porcine eyeballs, 20 - 25 laser treatments for each eye ball were conducted at intervals of 100 m on the surface of retinal blood vessels. Blood vessels used in the experiments were primary in nature and were classified on the basis of the location and the
diameter of the vessel. All the experiments were conducted under a single-shot configuration by using a mechanical shutter with an opening time constant of 0.6 ms, which is synchronized with the laser, allows an accurate delivery of single pulse- irradiations into the samples. (Sidhu et al., 2009)
After optoperforation of blood vessel epithelium, the location of each laser lesion was carefully mapped. Just after laser treatment, the retina segments were immersed and fixed in 2%
With changing laser fluence from 1.4 J/cm2 to 99.4 J/cm2, we produce a series of lesions on the blood vessel walls with a single fs-laser pulse. Laser irradiation on the surface of the retinal blood vessels with the fluence higher than about several tens of J/cm2 results in an apparent disruption of the vessel walls, followed by a continuous outflow of blood within 2 ~ 3 seconds, as shown in Fig. 14. The red color of the vessels fades out after about 5 minutes. After ~ 10 minutes, the bleeding is almost stopped. However, at lower laser fluence, the bleeding is stopped within one minute after extrusion of a little blood. (Sidhu et al., 2009)
To examine the blood vessels of a porcine retina after fs-laser irradiation, we sequentially sectioned the retina segment with primary blood vessels with a thickness of 20 m. Figure 15 represents histological images of the sectioned slices. The laser irradiations at lower fluence cause damage on the surface of the blood vessels with a low probability. At higher laser fluence, however, almost all the retinal segments exhibit apparent disruption of the ILM, which mainly consists of a Glial cell layer. Apparent disruptions of the ILM in the sectioned slices of the retina treated at 14.2 J/cm2 could be observed in the first and the fifth slices without any visible alterations in other sequential slices. No apparent disruption in the
surface of the blood vessels endothelial layer and no bleeding after laser irradiation were observed. If the slice thickness of 20 m in the sectioning procedure is considered, the interval between slices with an apparent disruption is 100 m, which is quite consistent with the distance between laser-irradiated points on the retina tissue. This observation suggests that from the histological analysis, the lateral damage of the retina upon fs-laser exposure is limited to 20 m range. In fact, the diameter of the laser lesions on the surface of treated retina, examined via scanning electron microscopy, is found to be less than 4 m (Fig. 16). With increasing laser fluence to 28.4 J/cm2, single-pulse laser irradiation induces complete optoperforation on the blood vessel wall. With further increment in the laser fluence to 52.6 J/cm2, the frequency of sequential slices with observed prominent damage on the blood vessels increases. This reveals that the diameter of the induced lesion is larger than 20 m under these rather higher laser fluences. The data suggest that up to 85.2 J/cm2, there is no observable alteration in underlying retina cell layers, except for disruptions in both the blood vessel walls and the ILM. Under a higher fluence of 99.4 J/cm2, however, a slight distortion is observed in the underlying tissue (Fig. 15(J)). (Sidhu et al., 2009)
The cryosections of the retina segments irradiated with a single-shot ultrafast laser were tentatively grouped into three types of lesions: no change, ablation only at the ILM and optoperforation of blood vessel walls (Fig 17). Correlation statistics of these different types of lesions is shown in Fig. 18 as a function of laser fluence. The optoperforation probability of blood vessels increased in the fluence range of 3.6 J/cm2 ~ 99.4 J/cm2. We determined the laser fluence to damage the ILM layer, found to be in the range between 1.4 J/cm2 and 3.6 J/cm2. However, perforation of the blood vessels is apparently caused by femtosecond-laser irradiation with a higher fluence between 3.6 J/cm2 and 7.1 J/cm2. If the percent probability at low fluence is extrapolated, the fluence at zero probability of alteration of the ILM and the perforation of the blood vessels are estimated to be 2.19 ± 1.08 J/cm2 and 5.85 ± 1.49 J/cm2, respectively. (Sidhu et al., 2009)
Recent development in advanced laser technology transiently facilitates to perform transaction, ablation, and coagulation of tissues via delivery of laser irradiation into a small focal volume are providing an attractive possibilities for new laser surgical technologies. The laser beam is a potential candidate that has already undergone a multi-center clinical trial to evaluate the feasibility for its use in vitreoretinal surgery (Schastak et al., 2007). Limited precision and significant damage by lasers with relative long pulse durations does not allow partial or selective tissue ablation with high precision. If such damage is to be overcome, infrared laser sources, such as CO2, Er:YAG and Holmium:YAG lasers, have undergone several trials via optical fiber delivery in intraocular surgery. However, apparent collateral damage to surrounding tissue due to significant thermal and shockwave effects have been reported (Paula- Yu et al., 2006).
Laser ablation of tissues could be described using either an optical breakdown model or a thermal confinement models. The optical breakdown model considers plasma formation and subsequent shock wave formation, cavitation, and tissue disruption. The thermal confinement model recognizes the competing thermal effects of the vaporization of water driving an explosive ablation and thermal diffusion leading to collateral damage. This model accounts for the observation that collateral damage is limited if the pulse duration is less than the thermal relaxation time of the ablated tissue volume (Vogel et al., 2003; Apitz et al., 2005).
The process of plasma formation through laser induced breakdown in transparent biological media is schematically depicted in Fig. 19. It essentially consists of the formation of quasi-free electrons by interplay of photoionization and avalanche ionization. It’s a well known fact that the optical breakdown threshold in water is very similar to that in ocular and other biological media (Docchio et al., 1986). Irradiation by an intense ultrafast laser beam further leads to multiphoton excitation of a target material. The absorbed energy might be transported to the electrons without thermal diffusion to adjacent material because the pulse width is shorter than the vibrational relaxation time constant of several picoseconds. As a result, thermal damage on the surrounding tissues could be minimized, and the biological tissue remains unaffected by the subsequent photoinduced mechanical shock process. This effectively renders the fs-laser surgical process non-thermal. The formation of a high density of free electrons could result in a local plasma formation in the targeted materials. This hot plasma formation results in a permanently damaged region, even inside a cell with a sub-micron size (Vogel et al., 2005). Furthermore, a previous on tissues like the corneal stroma revealed that the ablation threshold fluence decreased with increasing pulse width of the applied laser (Preuss et al., 1995). These uniquely show that ultrafast lasers can be utilized for precise treatment of tissues while minimizing any apparent thermal damage or shock pressure to biological tissues (Kohli et al., 2005). The results illustrated in the current work made the above hypothesis true for the retinal tissues, where retinal blood vessels were selectively perforated with wide range of laser fluence (1.42 ~ 99.4 J/cm2) with an ultra fast laser in near infra red region.
From the past literature values for the ablation thresholds for various tissues, including the corneal stroma, axons, the eye’s anterior chamber, and hard tissue (under a single-shot configuration, as in current work), the ablation threshold of the corneal stroma for an ultrafast laser is in the range of 1 J/cm2 to 2 J/cm2. Meanwhile, the ablation threshold for axons of
The thickness of the ILM, which is essentially a basement membrane consists of retina müller cells, is only 6 µm to 10 µm. The thickness of the ILM is thinnest at the fovea region of the retina. However, the thickness is larger at the posterior pole of retina (Hoerauf et al., 2006). Furthermore, the ILM is also present over the retinal blood vessels. If only the ILM is to be ablated selectively without any alterations in the underlying layers, the energy delivered by the laser irradiation must be confined in thin layers without any apparent diffusion of the deposited energy into other parts of the retina. To evoke this topic, we have examined the dependence of the ablation depth for transparent materials, like retinal tissue, on the laser fluence (Fig. 20). If there is high free electron density due to optical absorption processes, we suppose that the underlying mechanism for the ablation by fs-laser irradiation is not directly governed by the optical and the electronic properties of the materials. Even if the absorption mechanism of the NIR fs-laser is dependent on the optical band gap of each material, two different slopes under fs laser irradiation have already been reported for metals, semiconductors, and dielectrics (Nolte et al., 1997; Furusawa et al., 1999). For a lower laser fluence, F, the ablation depth can be described by the expression L =
With increasing laser fluence, however, the mechanism underlying the retina ablation can no longer be expressed by the optical penetration depth. As shown in Figure 16, the retina surface treated with a high laser fluence of 99.4 J/cm2 is very much roughened compared to the surface treated with a low fluence of 7.1 J/cm2. Based on the changes in the slopes of the semi-logarithmic plot of the ablation depth as function of the fluence, we have supposed that at laser fluence higher than 25.3 J/cm2, the electronic heat diffusion process plays an important role, even in an ultrafast laser ablation. The ablation depth in this region can be described with the expression of L =
The probability of retina blood vessel damage shows a linear relationship with the laser fluence. With the progressive increase in the laser fluence, selective ablations of concerted retina layers even including primary blood vessels is possible without any apparent damage to the underlying layers of the porcine retina. The threshold fluence to perforate the walls of the primary blood vessels embedded in the porcine retina is estimated to be 5.85 ± 1.49 J/cm2. If the ablation depth depends on the laser fluence as
In summary, all the observations from the present work reveals that fs-laser irradiation on pollen walls to make an evident physical hole with an outside diameter of about 1 μm well conserves the physiological state of the cell including its viability and pollen tube germination capability. Furthermore, from the successful delivery of foreign DNA into pollen through the hole reveals that the current method has an evident potential in the field of plant genetic engineering.
Topographical imaging as well as optical imaging of the plasma membranes led us to observe a self-healing process for live cells within several minutes of time after the fs-laser ablation on the live cells. A simple viscoelastic model for both the hole opening and closing process was found to be applicable to interpret its dynamics. The very slow dynamics could be explained in terms of high surface viscosity due to the presence of cytoskeleton network bound to the plasma membrane. The irregular feature in plasma topography observed in the final stage of the healing process might be due to a slice of the assembled lipid, which resulted from the reconstruction of not only the plasma membrane itself but also F-actin network as a cytoskeleton structure of live cells. Although two-dimensional plug flow model adapted in the current work fairly well interpret the experimental observations in macroscopically, the presence of transmembrane proteins, transbilayer interactions, and adhesion sites, etc., in addition to the bound cytoskeleton structure, produces a variety of restrictions on the flow dynamics of the plasma membrane through an alterations in many microscopic physico-chemical properties including thickness and hydrodynamic properties of the fluidic films.
We have developed a new method for elucidating more exact mechanism on the interesting topic of self-healing process based on ultrafast laser perforation of the plasma membrane of the animal cell. A mechanical stimulus to live-cell plasma membrane by the induced surface tension as well as surface line energy can be also applied by the current methods with high spatial resolution and unattainable speed of perforation. So interesting is the spatiotemporal characterization of the plasma membrane movement associated with the healing process that is closely related with the cell migration and transmission of the mechanical stimuli into biochemical signals, which might be mainly governed by cytoskeleton structure (Wang et al., 2005; Yamazaki et al., 2005; Supatto et al., 2005).
We have also successfully applied the current fs- laser technology to selectively perforate the retinal blood vessels without any apparent damage in the concerted retina layers. It provides a major breakthrough for the retinal vein occlusion therapy and removal of abnormal blood vessels (Choroidal Neovascularization (CNV)) grown during numerous retinal diseases.
This work was financially supported by the Ministry of Knowledge Economy of Korea and KRISS program.
Apitz I. Vogel A. 2005Material ejection in nanosecond Er: YAG laser ablation of water, liver, and skin, . A 81 329 338
Aronen T. S. Nikkanen T. O. Haggman H. M. 2003The production of transgenic Scots pine (Pinus sylvestris L.) via the application of transformed pollen in controlled crossing, . 12 375 378
Benkert R. Obermeyer G. Bentrup F. W. 1997The turgor pressure of growing lily pollen tubes, Protoplasm 198 1 8
Debregeas G. Martin P. Brochard-Wyart F. 1995Viscous bursting of suspended films, 75 3886 3889
Docchio F. Sachhi C. A. Marshall J. 1986Experimental investigation of optical breakdown thresholds in ocular media under single pulse irradiation with different pulse durations, 1 83 91
Engelman D. M. 2005Membrane are more mosaic than fluid, 438 578 570
Fernado D. D. Richards J. L. Kikkert J. R. 2006In vitro germination and transient GFP expression of American chestnut (Castanea dentate) pollen, . 25 450 456
Furusawa K. Takahashi K. Kumagai H. Midorikawa K. Obara M. 1999“Ablation characteristics of Au, Ag, and Cu metals using a femtosecond: Ti Sapphire laser, . 69(7), S 359-S366
Gonzalez-Serratos H. Rozycka M. Cordoba-Rodriguez R. Ortega A. 1996Membrane healing and restoration of contractility after mechanical injury in isolated skeletal muscle fibers of the frog, 93 5996 6001
Greulich K. O. Weber G. 1992The light microscope on its way from an analytical to a preparative tool, . 167 127 151
Heilbrunn L. V. 1956The surface precipitation reaction, In: 62 84, Academic, New York
Higashiyama T. Yabe S. Sasaki N. Nishimura Y. Miyagishima S. Kuroiwa H. Kuroiwa T. 2001Pollen Tube Attraction by the Synergid Cell, 293 1480 1483
Hoerauf H. Brix A. Winkler J. Droege G. Winter C. Birngruber R. Laqua H. Vogel A. 2006A Photoablation of inner limiting membrane and inner retinal layers using the Erbium: YAG-laser: An study, Lasers Surg. Med. 38(1), 52-61
Hoffmann F. 1996Laser microbeams for the manipulation of plant cells and subcellular structures, 113 1 11
Jeoung S. C. Kim H. S. Park M. I. Lee J. Kim C. S. Park C. O. 2005Preparation of room-temperature photoluminescent nanoparticles by ultrafast laser processing of single-crystalline Ge, 44 5278 5281
Jia T. Q. Chen H. X. Huang M. Zhao F. L. Li X. X. Xu S. Z. Sun H. Y. Feng D. H. Li C. B. Wang X. F. Li R. X. Xu Z. Z. He X. K. Kuroda H. 2006Ultraviolet-infrared femtosecond laser-induced damage in fused silica and CaF2 crystals 73 (5) 054105-1- 054105-9
Kobayashi N. Rivas-Carrillo J. D. Soto-Gutierrez A. Fukazawa T. Chen Y. Navarro-Alvarez N. Tanaka N. 2005Gene delivery to embryonic stem cells, 75 10 18
Kohli V. Elezzabi A. Y. Acker J. P. 2005Cell nanosurgery using ultrashort (femtosecond) laser pulses: applications to membrane surgery and cell isolation, Lasers Surg. Med. 37 227 230
König K. Riemann I. Fischer P. Halbhuber K. J. 1999Intracellular nanosurgery with near infrared femtosecond laser pulses, 45 195 201
Krautwig B. Lörz H. 1995Cereal protoplasts, 111 1 10
Lee Y. J. Kim D. H. Kim Y. Hwang I. 2001Identification of a signal that distinguishes between the chloroplast outer envelope membrane and the endomembrane system in vivo,” 13 2175 2190
Lovy-Wheeler A. Cardenas L. Kunkel J. G. Hepler P. K. 2007Differential organelle movement on the actin cytoskeleton in lily pollen tubes. . 64 217 232
Nelson J. S. Berm M. W. 1989Laser application in biomedicine. Part II: Clinical applications, 1 9 20
Nolte S. Momma C. Jacobs H. Tünnermann A. Chichkov B. N. Wellegehausen B. 1997Ablation of metals by ultrashort laser pulses B 14 2716 2722
Oliver J. M. King J. R. Mckinlay K. J. Brown P. D. Grant D. M. Scotchford C. A. Wood J. V. 2005Thin-film theories for two-phase reactive flow models of active cell motion, 22 53 98
Parpura V. Haydon P. G. Henderson E. 1993Three-dimensional imaging of living neurons and glia with the atomic force microscope, 104 427 432
Paula-Yu K. Miller J. Cringle S. J. Yu-Y D. 2006Experimental retinal ablation using a fourth-harmonic 266 nm laser coupled with an optical fiber probe, 47(4), 1587-1593.
Preuss S. Demchuk A. Stuke M. 1995Sub-picosecond UV laser ablation of metals, A 61 33 37
Sandre O. Moreaux L. Brochard-Wyart F. 1999Dynamics of transient pores in stretched vesicles, USA 96 10591 10596
Schastak S. Yafai Y. Yasukawa T. Wang Y. S. Hillrichs G. Wiedemann P. 2007Flexible UV light guiding system for intraocular laser microsurgery, Lasers Surg. Med. 39 353 357
Senz R. Miiller G. 1989Laser in Medicine, 93 269 277
Shen N. Datta D. Schaffer C. B. Le Duc P. Ingber D. E. Mazur E. 2005Ablation of cytoskeletal filaments and mitochondria in live cells using a femtosecond laser nanoscissor, 2 17 26
Sidhu M. S. Kim E. K. Woo S. Y. Song M. C. Jeoung S. C. Park Y. I. 2009Femtosecond- laser- assisted optoperforation of the primary retinal blood vessel and retina tissue of porcine eyes, 55(2) (in Press)
Singer S. J. Nicolson G. L. 1972The fluid mosaic model of the structure of cell membranes, 175 720 731
Strubinska J. Sniezko R. 2000Localization of vegetative nucleus and generative cell nuclei in branching pollen tubes of Oenothera hookeri L. grown in vitro, 42 107 112
Supatto W. Debarre D. Moulia B. Brouzes E. Martin J. L. Farge E. Beaurepaire E. 2005In vivo modulation of morphogenetic movements in Drosophila embryos with femtosecond laser pulses, 102 1047 1052
Tang W. Weidner D. A. Hu B. Y. Newton R. J. Hu X. H. 2006Efficient delivery of small interfering RNA to plant cells by a nanosecond pulsed laser-induced stress wave for posttranscriptional gene silencing, 171 375 381
Taylor L. P. Hepler P. K. 1997Pollen germination and tube growth, 48 461 491
Tirlapur U. K. König K. 2002Targeted transfection by femtosecond laser, 418 290 291
Touraev A. Stoger E. Voronin V. Heberle-Bors E. 1997Plant male germ line transformation, 12 949 956
Van der Leede-Plegt L. M. van den Ven. B. C. E. Schilder M. Franker J. van Tunen A. J. 1995Development of a pollen-mediated transformation method for Nicotiana glutinosa, . 4 77 86
Velegol S. B. Pardi S. Li X. Velegol D. Logan B. E. 2003AFM imaging artifacts due to bacterial cell height and AFM tip geometry, 19 851 857
Vervaeke I. Londers E. Piot G. Deroose R. Deproft M. P. 2005The division of the generative nucleus and the formation of callose plugs in pollen tubes of Aechmea fasciata (Bromeliaceae) cultured in vitro. 18 9 19
Vogel A. Venugopalan V. 2003Mechanism of pulsed laser ablation of biological tissues 103 577 644
Vogel A. Noack J. Huttman G. Paltauf G. 2005Mechanism of femtosecond laser nanosurgery of cells and tissues, B 81 1015 1047
Wang Y. Botvinick E. L. Zhao Y. Berns M. W. Usami S. Tsien R. Y. Chien S. 2005Visualizing the mechanical activation of Src, 434 1040 1045
Yahng J. S. Jeoung S. C. Choi D. S. Cho D. Kim J. H. Choi H. M. Paik J. S. 2005Fabrication of microfluidic devices by using a femtosecond laser micromachining techniques and μ-PIV studies on its fluid dynamics, 47 977 981
Yamazaki D. Kurisu S. Takenawa T. 2005Regulation of cancer cell motility through actin reorganization, 96 379 386
Zeira E. Manevitch A. Khatchatouriants A. Pappo O. Hyam E. Darash-Yahana M. Tavor E. Honigman A. Lewis A. Galun E. 2003Femtosecond infrared laser- An efficient and safe in vivo gene delivery system for prolonged expression, 8 342 350