LOW LEVEL LASER THERAPY
Keywords:
surgical,
laser,
fiber,
Time:26-04-2016
Low level laser therapy (LLLT) is also known as “soft laser therapy” and
bio-stimulation. The use of LLLT in health care has been documented in the literature for more
than three decades. Numerous research studies have demonstrated that LLLT is effective for some
specific applications in dentistry [1].
The LLLT literature is large, with more than 1000 papers published on this topic. A problem in
dissecting this literature is the variation in methodology and dosimetry between different
studies. Not only have a range of different wavelengths been examined, but exposure times and
the frequency of treatments also vary. The inclusion of sham-irradiated controls in clinical
studies is an important element, since placebo effects can be important, particularly in terms
of the level of pain experienced and reported following treatment [1].
While broad band light can exert effects on cells [2-3], interest has been concentrated on using
lasers as a light source because of their greater therapeutic effect. While much of the initial
work with LLLT used the helium-neon gas laser (632.8 nm), nowadays most LLLT clinical procedures
are undertaken using semi-conductor diode lasers, for example, gallium arsenide-based diode
lasers operating at 830 nm or 635 nm wavelengths [4]. Since wavelength is the most important
factor in any type of photo-therapy, the clinician must consider which wavelengths are capable
of producing the desired effects within living tissues.
The typical power output for a low level laser device used for this therapy is in the order of
10-50 milliWatts, and total irradiances at any point are in the order of several Joules. Thermal
effects of LLLT on dental tissues are not significant [5], and do not contribute to the
therapeutic effects seen. The wavelengths used for LLLT have poor absorption in water, and thus
penetrate soft and hard tissues from 3 mm to up to 15 mm. The extensive penetration of red and
near-infrared light into tissues has been documented by several investigators [6]. As the energy
penetrates tissues, there is multiple scattering by both erythrocytes and microvessels. Because
of this, both blood rheology and the distribution of microvessels in the tissue influence the
final distribution pattern of laser energy [1].
2. Mechanism of action
The mechanisms of low level laser therapy are complex, but essentially rely upon the absorption
of particular visible red and near infrared wave lengths in photoreceptors within sub-cellular
components, particularly the electron transport (respiratory) chain within the membranes of
mitochondria [2,7]. The absorption of light by the respiratory chain components causes a
short-term activation of the respiratory chain, and oxidation of the NADH pool. This stimulation
of oxidative phosphorylation leads to changes in the redox status of both the mitochondria and
the cytoplasm of the cell. The electron transport chain is able to provide increased levels of
promotive force to the cell, through increased supply of ATP, as well as an increase in the
electrical potential of the mitochondria membrane, alkalization of the cytoplasm, and activation
of nucleic acid synthesis [8]. Because ATP is the "energy currency" for a cell, LLLT
has a potent action that results in stimulation of the normal functions of the cell. The
specific actions of LLLT are summarized in Table 1.
Karu, who has studied the bio-stimulative effects of light on cell cultures in great detail, has
demonstrated that cell cultures which are initially irradiated with laser light show a range of
biological effects [7,9,10]. Of importance, if these cultures are then irradiated with
nonmonochromatic and incoherent light, the previous laser-produced biological effects are almost
nullified. This suggests that there are more complex mechanisms at work than the simple
excitation of polarization-sensitive chromophores in the cell.
It is crucial to recognize the optical distinction between irradiating human tissues, in which
light will scatter very widely, and a thin transparent monolayer of cells in a laboratory. In
this context, a key issue is polarization of the light, since polarized and non-polarized light
can bring about different biological responses. In a thin layer of cells in culture, the
polarization of laser light is maintained through the entire thickness of the cell layer. The
work of Mester [11], which used leucocytes in the laboratory setting, indicates that both
polarized laser light and polarized incoherent light can evoke bio-stimulation, whilst no such
stimulation occurs with non-polarized incoherent light.