Dental hard tissue modification and removal using sealed transverse excited atmospheric-pressure lasers operating at lambda=9.6 and 10.6 microm.

Pulsed CO(2) lasers have been shown to be effective for both removal and modification of dental hard tissue for the treatment of dental caries. In this study, sealed transverse excited atmospheric pressure (TEA) laser systems optimally tuned to the highly absorbed 9.6 microm wavelength were investigated for application on dental hard tissue. Conventional TEA lasers produce an initial high energy spike at the beginning of the laser pulse of submicrosecond duration followed by a long tail of about 1-4 micros. The pulse duration is well matched to the 1-2 micros thermal relaxation time of the deposited laser energy at 9.6 microm and effectively heats the enamel to the temperatures required for surface modification at absorbed fluences of less than 0.5 J/cm(2). Thus, the heat deposition in the tooth and the corresponding risk of pulpal necrosis from excessive heat accumulation is minimized. At higher fluences, the high peak power of the laser pulse rapidly initiates a plasma that markedly reduces the ablation rate and efficiency, severely limiting applicability for hard tissue ablation. By lengthening the laser pulse to reduce the energy distributed in the initial high energy spike, the plasma threshold can be raised sufficiently to increase the ablation rate by an order of magnitude. This results in a practical and efficient CO(2) laser system for caries ablation and surface modification.

[1]  Martin Frenz,et al.  Bone-ablation mechanism using CO2 lasers of different pulse duration and wavelength , 1993 .

[2]  Joseph T. Walsh,et al.  Effect of the CO2 laser (9.6μm) on the dental pulp in humans , 2000, Photonics West - Biomedical Optics.

[3]  Daniel Fried,et al.  IR laser ablation of dental enamel : mechanistic dependence on the primary absorber , 1998 .

[4]  Daniel Fried,et al.  Treating occlusal pit and fissure surfaces by IR laser irradiation , 2000, Photonics West - Biomedical Optics.

[5]  H. Goodis,et al.  Histologic evaluation of the pulpal response to temperature probe placement in the Macaca fascicularis monkey. , 1991, Oral surgery, oral medicine, and oral pathology.

[6]  Daniel Fried,et al.  Effect of pulse duration and repetition rate on CO2 laser inhibition of caries progression , 1996, Photonics West.

[7]  Daniel Fried,et al.  Rational choice of laser conditions for inhibition of caries progression , 1995, Photonics West.

[8]  Gerhard J. Mueller,et al.  Hard-tissue ablation with pulsed CO2 lasers , 1993, Photonics West - Lasers and Applications in Science and Engineering.

[9]  P. Hering,et al.  Wet bone ablation with mechanically Q-switched high-repetition-rate CO2 laser , 1998 .

[10]  Daniel Fried,et al.  Optical properties of dental enamel in the mid-IR determined by pulsed photothermal radiometry , 1999 .

[11]  P. Bélanger,et al.  Complex index of refraction of dental enamel at CO(2) laser wavelengths. , 1987, Applied optics.

[13]  G. Marshall,et al.  Sterilization of Teeth by Gamma Radiation , 1994, Journal of dental research.

[14]  J L Fox,et al.  Initial Dissolution Rate Studies on Dental Enamel after CO2 Laser Irradiation , 1992, Journal of dental research.

[15]  Daniel Fried,et al.  Optical properties of dental enamel at 9 to 11 um derived from time-resolved radiometry , 1997, Photonics West - Biomedical Optics.

[16]  R. H. Stern Laser beam effect on dental hard tissues , 1964 .

[17]  Daniel Fried,et al.  Mechanism of laser-induced solubility reduction of dental enamel , 1997, Photonics West - Biomedical Optics.

[18]  L ZACH,et al.  PULP RESPONSE TO EXTERNALLY APPLIED HEAT. , 1965, Oral surgery, oral medicine, and oral pathology.

[19]  A. Sagi,et al.  A numerical model for temperature distribution and thermal damage calculations in teeth exposed to a CO2 laser , 1984 .

[20]  J. M. White,et al.  Effects of Nd:YAG laser on pulps of extracted teeth , 1991 .

[21]  J. Featherstone,et al.  Artificial caries removal and inhibition of artificial secondary caries by pulsed CO2 laser irradiation. , 1999, American journal of dentistry.

[22]  Gregory B. Altshuler,et al.  Laser treatment of enamel and dentine by different Er lasers , 1994, Photonics West - Lasers and Applications in Science and Engineering.

[23]  Steven R. Visuri,et al.  Laser ablation of dental hard tissue: from explosive ablation to plasma-mediated ablation , 1996, Photonics West.

[24]  J. Featherstone,et al.  An infrared method for quantification of carbonate in carbonated apatites. , 1984, Caries research.

[25]  C Loiacono,et al.  Lasers in dentistry. , 1993, General dentistry.

[26]  James A. Harrington,et al.  Novel CO2 laser system for hard tissue ablation , 1994, Photonics West - Lasers and Applications in Science and Engineering.

[27]  J. Fox,et al.  Combined effects of laser irradiation/solution fluoride ion on enamel demineralization. , 1998, Journal of clinical laser medicine & surgery.

[28]  W. Seka,et al.  CO2 Laser Inhibition of Artificial Caries-like Lesion Progression in Dental Enamel , 1998, Journal of dental research.

[29]  Daniel Fried,et al.  Surface dissolution kinetics of dental hard tissue irradiated over a fluence range of 1 to 8 J/cm2 , 1998, Photonics West - Biomedical Optics.

[30]  Jeffrey L. Fox,et al.  Argon laser effect on demineralization of human enamel , 1992, Photonics West - Lasers and Applications in Science and Engineering.

[31]  J. Featherstone,et al.  Laser Effects On Dental Hard Tissues , 1987, Advances in dental research.

[32]  J. Featherstone,et al.  Scanning Electron Microscope Observations of CO2 Laser Effects on Dental Enamel , 1995, Journal of dental research.

[33]  M L Myers,et al.  Shear strength of composite bonded to laser-pretreated dentin. , 1988, The Journal of prosthetic dentistry.

[34]  Robert F. Boehm,et al.  Thermal Stress Effects and Surface Cracking Associated With Laser Use on Human Teeth , 1977 .

[35]  Daniel Fried,et al.  Permanent and transient changes in the reflectance of CO2 laser‐irradiated dental hard tissues at λ = 9.3, 9.6, 10.3, and 10.6 μm and at fluences of 1–20 J/cm2 , 1997 .

[36]  Daniel Fried,et al.  Dental hard tissue modification and removal using sealed TEA lasers operating at λ=9.6 and 10.6 μm , 1999, Photonics West - Biomedical Optics.

[37]  Ronald S. Dingus,et al.  Grüneisen-stress-induced ablation of biological tissue , 1991, Photonics West - Lasers and Applications in Science and Engineering.

[38]  Andrei V. Belikov,et al.  Optimum regimes of laser destruction of human tooth enamel and dentin , 1993, Photonics West - Lasers and Applications in Science and Engineering.

[39]  Steven R. Visuri,et al.  Shear test of composite bonded to dentin: Er:YAG laser versus dental handpiece preparations , 1995, Photonics West.

[40]  Daniel Fried,et al.  Backspallation due to ablative recoil generated during Q-switched Er:YAG ablation of dental hard tissue , 1998, Photonics West - Biomedical Optics.

[41]  Raimund Hibst,et al.  Effects of pulsed CO2 and Er:YAG lasers on enamel and dentin , 1993, Photonics West - Lasers and Applications in Science and Engineering.

[42]  J. Featherstone,et al.  Morphology, histology and crystallography of human dental enamel treated with pulsed low-energy infrared laser radiation. , 1987, Caries research.

[43]  Hamilton Ai,et al.  Cavity preparation with and without waterspray. Effects on the human dental pulp and additional effects of further dehydration of the dentine. , 1967 .

[44]  A. Welch,et al.  Time constants in thermal laser medicine , 1989, Lasers in surgery and medicine.