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Elma Baron (editor) - Light-Based Therapies for Skin of Color

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Elma Baron (editor) Light-Based Therapies for Skin of Color
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Light-Based Therapies for Skin of Color: summary, description and annotation

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Light-based therapies have been a major component of dermatologic practice. Historically, these treatment modalities have been mainly tailored to the treatment of patients with light skin. Principles governing use of light therapies in skin of color are less defined. However, there is a tremendous need to understand the benefits and limitations of these therapeutic options for dark-skinned patients as well. Demographic data in the United States alone indicate that the population and recipients of health care are rapidly changing with regard to skin phototype. Physicians who are involved in the delivery of care for patients with cutaneous problems that can be addressed by light treatments need to be able to fully understand the mechanisms, applications, risks, efficacy, adverse events, and other pertinent issues in considering treatment options for their patients with pigmented skin.

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Elma Baron (ed.) Light-Based Therapies for Skin of Color 10.1007/978-1-84882-328-0_1 Springer-Verlag London Limited 2009
1. Principles of Light-Skin Interactions
Marjorie F. Yang 1
(1)
Department of Dermatology, Indiana University School of Medicine, Indianapolis, IN, USA
(2)
Department of Optics and Biomedical Physics, Institute of Optics and Biophotonics, Saratov State University, Saratov, Russia
(3)
Wellman Center for Photomedicine and Department of Dermatology, Harvard Medical School and Massachusetts General Hospital, Boston, MA, USA
Marjorie F. Yang
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Anna N. Yaroslavsky (Corresponding author)
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Abstract
Skin is the largest human organ. It covers between 1.5 and 2 m2, comprising about one-sixth of total body weight. Skin performs a complex role in human physiology. It serves as a barrier to the environment and acts as a channel for communication to the outside world. For example, skin protects us from water loss, ultraviolet (UV) rays of the sun, friction, and impact wounds. It also helps in regulating body temperature and metabolism. All photobiological responses are influenced heavily by the optical properties of skin. Therefore, for the successful development of photomedicine, in-depth knowledge and understanding of light-skin interactions, specifically known as skin optics, is required. The transfer of optical radiation into human skin depends on the absorption and scattering properties of three functional skin layers: epidermis, dermis, and hypodermis. The structures and component chromophores of these layers determine the attenuation of radiation in skin. The enhanced penetration of optical radiation as well as selective targeting of pathology can be achieved by studying and analyzing the wavelength-dependent interactions of light with skin. For example, considering that melanin exhibits maximum absorption in the UV and blue spectral ranges, whereas blood preferentially absorbs blue and yellow light, the treatment protocol have been devised that target pigmented and vascular lesions, respectively. This chapter provides a brief summary and description of the properties of light, its interaction with human skin, the list of the medical light sources, and the diagnostic and/or therapeutic uses of currently available light-based devices within the visible to NIR spectral range in dermatology.
Introduction
Skin is the largest human organ. It covers between 1.5 and 2 m2, comprising about one-sixth of total body weight. Skin performs a complex role in human physiology. It serves as a barrier to the environment and acts as a channel for communication to the outside world. For example, skin protects us from water loss, ultraviolet (UV) rays of the sun, friction, and impact wounds. It also helps in regulating body temperature and metabolism. All photobiological responses are influenced heavily by the optical properties of skin. Therefore, for the successful development of photomedicine, in-depth knowledge and understanding of light-skin interactions, specifically known as skin optics, is required. The transfer of optical radiation into human skin depends on the absorption and scattering properties of three functional skin layers: epidermis, dermis, and hypodermis. The structures and component chromophores of these layers determine the attenuation of radiation in skin. The enhanced penetration of optical radiation as well as selective targeting of pathology can be achieved by studying and analyzing the wavelength-dependent interactions of light with skin. For example, considering that melanin exhibits maximum absorption in the UV and blue spectral ranges, whereas blood preferentially absorbs blue and yellow light, the treatment protocol have been devised that target pigmented and vascular lesions, respectively. This chapter provides a brief summary and description of the properties of light, its interaction with human skin, the list of the medical light sources, and the diagnostic and/or therapeutic uses of currently available light-based devices within the visible to NIR spectral range in dermatology.
Fundamental Properties of Light
Light can be described as the energy that is carried in the form of traveling wave composed of electric and magnetic fields. Electric and magnetic fields vary in intensity and are at right angles to each other and to the direction that the wave is propagating (Fig. ). Initially, light was defined as the electromagnetic waves in the visible spectral range. At present, however, light is defined as electromagnetic radiation between 100 and 10,000 nm. In photomedicine, this spectral range is subdivided in the following ways: UV light: UVC, 100280 nm; UVB, 280315 nm; and UVA, 315400 nm; visible: 400780 nm (violet, 400450 nm; blue, 450480 nm; green, 510560 nm; yellow, 560590 nm; orange, 590620 nm; and red, 620780 nm); infrared (IR) light: IRA, 0.781.4 m; IRB, 1.43.0 m; and IRC, 31000 m. In physics, the light is classified as UV, 100400 nm; visible, 400800 nm; NIR, 0.82.5 m; middle-IR (MIR), 2.550 m; and far-infrared (FIR), 502000 m.
Fig 11 a Propagating electromagnetic wave Arrow points toward the - photo 1
Fig. 1.1
(a) Propagating electromagnetic wave. Arrow points toward the direction of the propagation. (b) The wavelength, , is the distance between neighboring crests
Fig 12 The evolution of the electric field vector blue with time the - photo 2
Fig. 1.2
The evolution of the electric field vector (blue), with time (the vertical axes), as a particular point in space, along with its x and y components (red/left and green/right), and the path traced by the tip of the vector in the plane (purple). (a) Linearly polarized light. (b) Circularly polarized light. (c) Elliptically polarized light
Fig 13 Electromagnetic spectrum Simultaneously light can also be - photo 3
Fig. 1.3
Electromagnetic spectrum
Simultaneously, light can also be described as a stream of particles, photons, which have a rest mass of zero, are electrically neutral, and carry certain amount of energy. In other words, the energy that is transported by EM wave is not continuously distributed over the wave front defined by crests. Energy is located at discrete points, photons, along the wave front. Photons are created inside the atoms of radiating body from which they receive their energy content. Photons move with velocity of light. When photons are absorbed by atoms of the matter, they lose their identity by transferring their energy to an atom. Energy content in photon is inversely proportional to its wavelength: E photon = hc /, where c is the velocity of light, the photon wavelength, h = 6.626 1034 Js the Plancks constant. Energy is measured in joules (J). Energy characterizes the ability of light to produce some work. Power is the rate of the energy delivery. It is normally measured in watts (W), that is, joules (J) per second (s). The efficiency of lighttissue interaction depends on the energy density, also called fluence. Light fluence is the energy, which propagates through a unit area, which is perpendicular to direction of light propagation. Fluence is measured in J/m2. Power density is power of light wave, which propagates through a unit area which is perpendicular to direction of propagation of light wave. A power density or intensity is measured in W/m2. Fluence ( F1 ) and intensity ( I 1) are proportional: F = I p, where p is the length of pulse (pulse width) or exposure time. Another important parameter that characterizes light is its fluence rate that is defined as the sum of the radiance over all angles at a point Picture 4
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