Journal List > Korean J Androl > v.29(2) > 1033068

Kim and Moon: Basic Principles of Laser for Prostate Surgery

Abstract

Recent advances in laser technology have provided a varied arsenal for endoscopic treatment of benign prostatic hyperplasia. Laser is a collimated coherent radiation of photons generated by stimulated emission of gain media, allowing transfer of selective, controlled and focused energy to the targeted tissue. The application of laser to prostate surgery developed hand-in-hand with refinements to the equipment. Earlier lasers were low powered modalities with no significant tissue selectivity, aimed at thermal coagulation and resulted in significant side effects and recurrence. Since then, prostate lasers have developed towards a more high-powered and selective modality that allowed complete ablation of the tissue with fewer complications. Fiber technology has also developed to allow efficient and safe transfer of a continuously increasing energy output. It is important for the surgeon to understand these fundamental principles of laser and prostate surgery, not only to select the proper tools, but also to properly implement the technique as well.

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Fig. 1.
Lasers are generated by stimulated emission, brought about by pumping the gain medium to an excited state. Released photons oscillate within the optical resonator to emit a collimated, coherent monochromatic electromagnetic radiation.
kja-29-101f1.tif
Fig. 2.
Tissue effect can also vary with the depth of penetration, due to different levels of temperature achieved within the affected zone.42
kja-29-101f2.tif
Fig. 3.
Laser wavelength and mode of emission can affect the depth of penetration, leading to a varied profile of energy density (HPS: high performance system, CW: continuous wave).42
kja-29-101f3.tif
Fig. 4.
Chromophores allow selective absorption of specific wavelengths, vastly improving the tissue effect of certain lasers. Early Nd:YAG lasers are generally nonspecific to either water or hemoglobin. Modern green light lasers are highly absorbed by hemoglobin, while modern infrared lasers are highly absorbed by water.5
kja-29-101f4.tif
Fig. 5.
Increased power allows the beam to be more collimated. The tissue laser interaction not only benefits from more power, but also from a more focused high intensity transfer of energy (HPS: high performance system, PV: photo vaporization).44
kja-29-101f5.tif
Fig. 6.
Laser fibers also develop to accommodate the increased laser energy. Newer fibers are designed to allow more flexibility, less loss of energy and greater safety.41
kja-29-101f6.tif
Table 1.
Different tissue effects appear by level of energy transfer42
<40oC Photobiomodulation
42∼45oC 45∼50oC Hyperthermia Desiccation
50∼100oC Coagulation, irreversible
>60oC Protein denaturation
>100oC Carbonization, vaporization
Table 2.
Prostate laser developed from the early low power Nd:YAG to the contemporary modalities through increased power and optimized wavelengths29,37,43,44
Year Method Laser
1917 Theory of stimulated emission of electromagnetic radiation
1960 First functional Laser Ruby
1993 VLAP Nd:YAG
1994 CELAP Nd:YAG+Ho:YAG
1995 ILC Nd:YAG, Diode (70 W)
1995, 1996, 1997 HoLAP, HoLRP, HoLEP Ho:YAG
1998 PVP KTP (60∼80 W)
2005 Thulium laser resection of prostate Tm:YAG
2007 Laser vaporization of the prostate Diode (120∼200 W, 980 nm)
2008 PVP HPS: KTP or LBO (120 W)

VLAP: visual laser ablation of the prostate, CELAP: combined endoscopic laser ablation of the prostate, ILC: interstitial laser coagulation, HoLAP: holmium laser ablation of the prostate, HoLRP: holmium laser resection of the prostate, HoLEP: holmium laser enucleation of the prostate, PVP: photovaporization of the prostate, HPS: high performance system.

Table 3.
Different lasers are characterized primarily by wavelengths. However, interactions with different chromophores, and modes of generation also affect tissue interactions and depth of tissue effect10,20,37
Wavelength (nm) Chromophore Extinction length (mm) Wave mode Tissue interaction
Nd:YAG 1,064 - 10 Pulse or CW Coagulation
Ho:YAG 2,100 Water 0.4 Pulse Vaporization
KTP 532 Hemoglobin 0.8 Quasi-pulse Vaporization
Tm:YAG 2,000 Water 0.25 CW Vaporization
Diode 940/980/1,470 Water and hemoglobin Variable Pulse or CW Vaporization
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