Laser selective cutting by impulsive heat deposition in the ir wavelength range for direct-drive ablation

Abstract

A method of laser processing of materials and specifically laser induced ablation processes for laser removal of material by impulsive heat deposition (IHD) by direct and specific excitation of short lived vibrations or phonons of the material in such a way as to not generate highly reactive and damaging ions through multiphoton absorption. The heat deposition and ensuing ablation is achieved faster than heat transfer to surrounding tissue by either acoustic or thermal expansion or thermal diffusion. The deposited laser energy is channeled into the ablation process to drive the most efficient ablation process possible with minimal damage to surrounding areas by either ionizing radiation or heat effects.

Description

CROSS REFERENCE TO RELATED U.S PATENT APPLICATION[0001]This patent application is a Divisional application of U.S. patent application Ser. No. 11 / 321,057 entitled LASER SELECTIVE CUTTING BY IMPULSIVE HEAT DEPOSITION IN THE IR WAVELENGTH RANGE FOR DIRECT-DRIVE ABLATION filed on Dec. 30, 2005, which relates to U.S. provisional patent application Ser. No. 60 / 640,092 filed on Dec. 30, 2004 entitled LASER SELECTIVE CUTTING BY WAVELENGTH AND TEMPORAL TUNING IR PULSES TO PROVIDE MOLECULAR LEVEL OPTIMIZATION OF IMPULSIVE HEAT DEPOSITION PROFILES FOR ABLATION, filed in English, all of which are incorporated herein by reference in their entirety.FIELD OF THE INVENTION[0002]The present invention relates to a method of material removal using pulsed lasers. Impulsive heat deposition (IHD) through direct excitation of mechanical degrees of freedom (short lived vibrations or phonons) of the target material provides a novel ablation process that leads to a minimum of damage to the surrounding mater...

AI Technical Summary

Benefits of technology

[0013]This invention provides a method of laser processing of materials that is based on a new understanding of the ablation process and the dynamics of energy transduction of vibrational energy into heat. The invention disclosed herein provides a new methodology in which one can efficiently achieve material ablation with the minimum of collateral damage through either ion formation or thermal accumulation. This is accomplished by impulsive heat deposition (IHD), a novel method that combines both thermally and photomechanically driven ablation mechanisms, in which most of the absorbed energy remains in the ablated material. The laser energy is effectively coupled directly to the mechanical degrees of freedom that lead to ablation and in so doing performs this task at optimal efficiency, which is key to minimizing collateral damage.

[0017]ii) a pulse duration time and wavelength that meets requirements for impulsive heat deposition such that the pulse duration time is shorter than a time required for thermal diffusion out of the laser irradiated volume and shorter than a time required for a thermally driven expansion of the laser irradiated volume, and

[0023]ii) a pulse duration time and wavelength that meets requirements for impulsive heat deposition such that the pulse duration time is shorter than a time required for thermal diffusion out of the laser irradiated volume of tissue and shorter than a time required for a thermally driven expansion of the laser irradiated volume of tissue, and

[0029]ii) a pulse duration time and wavelength that meets requirements for impulsive heat deposition such that the pulse duration time is shorter than a time required for thermal diffusion out of the laser irradiated volume of material and shorter than a time required for a thermally driven expansion of the laser irradiated volume of material, and

Problems solved by technology

However, the problem to date with methods of laser surgery has been the deleterious collateral damage to surrounding tissue, which has limited the widespread use of lasers as a replacement for mechanical surgical tools.

In the case of photomechanical spallation, the energy deposited must not exceed the vaporization threshold, and must be deposited quickly enough that shockwaves due to sudden thermal expansion lead to mechanical breakdown and ejection of the material.

However, photomechanical spallation is notoriously inefficient, and it has been found that “ .

. . for most tissues, material removal using IR laser pulses cannot be achieved via a laser-induced spallation mechanism.” [1]

In the case of biological materials, the temperature gets so hot that the material actually burns.

This latter process not only damages the surrounding tissue but actually blocks healing.

However, the material must still get hot enough to ablate in the irradiate volume and the excess heat which accumulates in the surrounding material leads to the tissue damage is the same.

Excess heating of this magnitude still severely harms the adjacent tissue and thus has prevented the general use of conventional long pulse lasers in medical surgery.

The longer it takes the incident laser energy to be converted to heat the more time thermal diffusion and thermal expansion have to transfer energy to surrounding material and increase collateral damage.

In the case of short laser pulses, it is possible to deposit the laser energy much faster than the ablation process, but realization of this is complicated by other deleterious effects as discussed below.

For a given amount of laser energy, the smaller the amount of material absorbing the light, the higher the temperature of the lattice rises in the irradiated zone, and the less total heat is available for transport to adjacent material to cause heat induced damage.

However, this wavelength range leads to radiation damage by UV photochemistry and ionization of the material.

This photochemistry is undesired in many applications and is a particularly serious problem in most medical and dental applications where ionizing effects and collateral photochemistry must be avoided in order to promote healing.

In this short pulse limit, there is also rapid heat deposition.

However, this process creates highly reactive intermediates.

Even in the absence of excessive heating in this short pulse limit of femtosecond durations, the effect of ion formation leads to damage that blocks healing and is unacceptable for most medical applications.

This problem has been identified by control studies of live animals in which it was found that even though femtosecond laser pulses cut without excess heating, the healing process was not invoked.

There was sufficient damage to adjacent cells to kill them but not enough to trigger normal healing mechanisms.

In the case of sensitive materials such as semiconductors, insulators, catalysts, etc., the ion induced chemistry will also lead to highly undesirable changes in material properties, such as the creation of surface states / defects.

This effect again is most undesirable in any kind of medical or dental application.

In the case of dental applications, the formation of highly reactive ions will have the potential for forming organic mercuric compounds from ablation of amalgam fillings that are incredibly toxic.

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