WO1997013458A1 - Radiation-delivery device - Google Patents

Radiation-delivery device Download PDF

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Publication number
WO1997013458A1
WO1997013458A1 PCT/US1996/016217 US9616217W WO9713458A1 WO 1997013458 A1 WO1997013458 A1 WO 1997013458A1 US 9616217 W US9616217 W US 9616217W WO 9713458 A1 WO9713458 A1 WO 9713458A1
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WO
WIPO (PCT)
Prior art keywords
radiation
reflective
housing
emitted
irradiating device
Prior art date
Application number
PCT/US1996/016217
Other languages
French (fr)
Inventor
Richard Rox Anderson
Original Assignee
The General Hospital Corporation
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by The General Hospital Corporation filed Critical The General Hospital Corporation
Priority to EP96939444A priority Critical patent/EP0955884A4/en
Priority to AU76621/96A priority patent/AU7662196A/en
Publication of WO1997013458A1 publication Critical patent/WO1997013458A1/en

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Classifications

    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B18/00Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body
    • A61B18/18Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body by applying electromagnetic radiation, e.g. microwaves
    • A61B18/20Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body by applying electromagnetic radiation, e.g. microwaves using laser
    • A61B18/203Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body by applying electromagnetic radiation, e.g. microwaves using laser applying laser energy to the outside of the body
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B18/00Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body
    • A61B2018/00315Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body for treatment of particular body parts
    • A61B2018/00452Skin
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B18/00Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body
    • A61B2018/00315Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body for treatment of particular body parts
    • A61B2018/00452Skin
    • A61B2018/00476Hair follicles
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61NELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
    • A61N5/00Radiation therapy
    • A61N5/06Radiation therapy using light
    • A61N2005/0664Details
    • A61N2005/0665Reflectors
    • A61N2005/0666Reflectors for redirecting light to the treatment area

Definitions

  • This invention relates to radiation-delivery devices.
  • Radiation sources such as lasers
  • lasers are used in a variety of medical applications because of their ability to generate precise, self-cauterizing incisions and locally heat tissue without contacting the patient.
  • laser light is used in a variety of der atological therapies, such as to remove tatoos, port- wine stains, and unwanted hair.
  • radiation is typically delivered through a fiber optic system to a lens, which subsequently images the radiation onto the region of interest.
  • the radiation is absorbed by a portion of the skin or hair (e.g., the melanin or blood vessels) , resulting in optical absorption and localized heating.
  • Webb describes an optical concentrator for manipulating the cross-sectional area and reducing speckle of an incident laser beam.
  • a spherical or hemispherical mirror is used to return laser light scattered from a diffusely reflective surface back onto the point of incidence. Lenses are then used to produce an output beam by collecting light from the point of incidence.
  • the invention provides a method for irradiating a material.
  • the method includes the step of first exposing the material with radiation (e.g., optical radiation). Following the exposing step, radiation is partially re-emitted (e.g., scattered, reflected, or both scattered and reflected) from the material. The material is then re-exposed with the re- emitted radiation.
  • the material is a patient's tissue.
  • tissue is meant any collection of cells or any specific organ in the patient (e.g., human skin) .
  • the method of the invention is carried out with an irradiating device configured receive radiation from a radiation delivery means.
  • the radiation delivery means delivers radiation from a radiation source to the material, and is preferably connected to a reflective housing.
  • the housing includes an opening or surface for placement over the material and a reflective component proximal to the opening or surface.
  • the radiation delivery means is a fiber optic waveguide or an articulated arm, and the radiation source is a laser.
  • the re-emitted radiation is received and reflected by a reflective device to re- expose the material.
  • the reflective device can be a reflective housing positioned proximal to the material prior to the exposing step.
  • the reflective housing is substantially hemispherical in shape, and the material is positioned substantially near the center of the hemisphere.
  • the reflective housing is substantially elliptical in shape, and the material is positioned substantially near a focus of the ellipse.
  • the reflective housing may also be substantially spherical in shape, with the opening disposed on a surface of the sphere.
  • the reflective housing is substantially cone-shaped and includes an opening at the base of the cone. During operation, the material is positioned near this opening.
  • the method of the invention can also be carried out with an irradiating device which includes an optically transparent plate featuring a reflective coating on one of its surfaces.
  • the reflective coating is disposed on the plate to transmit normally incident radiation (i.e., radiation angled at between about 80° and 100° relative to the surface of the reflective coating) , receive radiation re-emitted from the material, and reflect any re-emitted radiation back onto the material.
  • the reflective coating contains a dielectric material or multiple layers of dielectric materials which exhibit angularly dependent reflective properties.
  • substantially hemispherical a reflective housing which is shaped, respectively, in the form of a hemisphere, ellipse, or sphere so that it reflects incident light to a well- defined area. Preferably, this area is not more that a few millimeters in radius.
  • substantially cone-shaped means at least a portion of the housing is conically shaped.
  • center of the hemisphere is meant the geometrical center of the sphere composed of two identical hemispheres.
  • substantially near the center or “substantially near the focus” is meant a position within a few millimeters of, respectively, the actual center or focus.
  • substantially transparent and substantially reflects” means that, respectively, at least 80% of the radiation is either transmitted or reflected.
  • the reflective housing preferably includes a reflective coating for reflecting the re-emitted radiation.
  • the coating for example, may be a reflective film, such as a metallic or dielectric film.
  • the dielectric film may be reflective in only a portion of the electromagnetic spectrum, thereby allowing direct visualization of the material through the film.
  • the reflective housing features an array of grooves configured to reflect the re-emitted radiation. These grooves have reflective properties similar to those of corner cubes, retroreflectors, or similar optical components which reflect radiation by internal reflection. Other reflecting materials, such as white paint or reflecting tapes, may be used to reflect radiation within the housing.
  • the reflective housing may take on any shape.
  • the housing may be formed in the shape of a cylindrical tube, with the reflective material disposed on portions of the tube's inner surface.
  • the opening for irradiating the tissue is positioned on one of the flat surfaces of the tube.
  • the irradiation device is used during a medical therapy to irradiate a patient's tissue.
  • the device is used in combination with standard medical procedures normally employed when radiation is delivered to tissue.
  • the radiation used in the therapy is optical radiation, and the therapy is used to treat human skin.
  • Examples of such therapies include optical removal of tatoos, port- wine stains, abnormal blood vessels, psoriatic skin, unwanted hair, pigmented lesions, skin cancers and other lesions treated by laser surgery, phototherapy, photochemotherapy or photodynamic therapy.
  • the invention has a number of advantages.
  • it increases the efficiency of a laser-based surgical procedure by treating the tissue of interest with radiation which is normally not utilized. Scattered or reflected light, lost during conventional procedures, is effectively "recycled” and used to re-expose and treat the tissue. In this way, optical fluences can be kept relatively low during treatment, thereby enhancing the accuracy and flexibility of the therapy.
  • the invention provides a gain of optical energy available to the tissue by a factor of up to (1-R) -1 , where R is the wavelength-dependent fraction of incident light re-emitted from the tissue.
  • R is the wavelength-dependent fraction of incident light re-emitted from the tissue.
  • the invention can also effectively increase the exposure spot diameter of the radiation. In many applications in which the "target" for therapy is deep within the skin (e.g., during the removal of tattoos, port-wine stains, or hair) , such a larger exposure spot diameter is advantageous.
  • the invention by collecting and then re-exposing the tissue of interest with the re-emitted radiation, the invention generates a more spatially uniform field during therapy. This gives the operator more control over the amount of heat delivered to the tissue, and thus improves the accuracy of the therapy.
  • the invention also increases the safety of laser- based therapies.
  • the device can be made small and compact, and can be used interchangeably with conventional laser-based surgical instruments.
  • the device can additionally be fabricated with relatively inexpensive, disposable materials; a new, sterilized device can therefore be used for each procedure.
  • Fig. 1 is a top view of an irradiating device of the invention being used to irradiate a patient's skin
  • Fig. 2 is a cross-sectional side view of an irradiating device in contact with the patient's skin
  • Figs. 3A-3C are, respectively, cross-sectional side views of the irradiating device during initial irradiation of the skin, after radiation is initially re- emitted from the skin surface, and after the re-emitted radiation is reflected off the reflective housing and back towards the skin surface;
  • Figs. 4A and 4B are cut-away cross-sectional side views of, respectively, a reflective housing including a radiation-reflecting coating, and a reflective housing including an array of retro-reflecting grooves;
  • Fig. 5 is a cross-sectional side view of an irradiating device including a reflective housing featuring a hemispherical top portion and a tapered bottom portion;
  • Fig. 6 is a cross-sectional side view of an irradiating device containing a reflective housing featuring two hemispherical top portions and a straight bottom portion;
  • Fig. 7 is a cross-sectional side view of an irradiating device containing an elliptical reflective housing
  • Fig. 8 is a cross-sectional side view of an irradiating device including a cone-shaped reflective housing; and,
  • Fig. 9 is a side view of a irradiating device featuring a flat, optically transparent plate coated with a reflecting dielectric film.
  • an irradiating device 10 delivers radiation during a therapy to an area of a patient's tissue 14.
  • the device 10 is configured so that radiation which is normally re-emitted from the tissue after irradiation (and is thus wasted during the therapy) can be collected and imaged back onto the originally irradiated area.
  • the device includes a fiber optic waveguide 12 coupled to a laser or other radiation source (not shown in the figure) .
  • a distal end 20 of the fiber optic waveguide is housed in a delivery handpiece 18 and an input port 16 so that radiation from the fiber can be delivered to the device 10.
  • the input port 16 is connected to a hemispherically shaped reflective housing 13 which surrounds the tissue to be irradiated and is configured to reflect radiation.
  • radiation is delivered from the fiber optic waveguide 12 to the tissue. Portions of the delivered radiation are either absorbed by the tissue, leading to radiation- induced heating, or are re-emitted from the irradiated area. The re-emitted radiation propagates away from the tissue, and is collected by the hemispherically shaped reflective housing 13.
  • a template 22 connected to the housing 13 is used to position the device on the patient's tissue and facilitate alignment of the radiation.
  • the template is especially useful for aligning radiation onto tissue containing rough or curved surfaces, such as the skin.
  • the reflective housing 13 includes a transparent porthole 24 for viewing the irradiated region.
  • Figs. 2, 4A and 4B show cross-sectional views of the irradiation device 10 and the reflective housing 13.
  • the delivery handpiece 18 and input port 16 connected to the housing each enclose portions of the fiber optic waveguide 12.
  • the distal end 11 of the waveguide 12 extends into the device and is surrounded by the hemispherically shaped reflective housing 13.
  • the housing 13 is connected to the template 22 which, in turn, is placed in contact with a patient's tissue 14.
  • the template 22 includes an opening 21 positioned above a portion 17 of the tissue and in the center of the hemispherical reflective housing.
  • the opening 21 and distal end 11 of the waveguide are aligned so that, during therapy, radiation from the waveguide passes through the template and onto the tissue.
  • the reflective housing includes a reflective coating 30 on its inner surface so that during therapy radiation scattered or reflected from the tissue is collected and imaged back onto the originally irradiated portion of tissue.
  • the reflective coating 30 can be any reflective material and can be made using any of a number of techniques known in the art.
  • the coating may be deposited as a thin reflective film on the inner surface of a transparent substrate 32.
  • the coating may also be deposited on the substrate's outer surface.
  • the coating may be a thin metallic film composed of materials such as aluminum, silver, or gold.
  • the reflective properties of these materials are dependent on the material composition and the film thickness, and are well known in the optical arts.
  • Dielectric films may also serve as reflective coatings. These materials have particularly desirable reflectivities at visible and infrared wavelengths, and can be used to coat the inner or outer surfaces of the substrate material 32.
  • Dielectric coatings have the additional advantage that they can be made transparent to visible wavelengths or radiation at certain angles of incidence; thus, when used with transparent substrates, these materials allow the operator to directly view the procedure without the need for a porthole.
  • the reflective housing is preferably shaped so that re-emitted radiation is collected and imaged onto a region contained in the originally irradiated area. In this way, the spatial extent of the irradiated area is not significantly increased by the reflective process, and thus the accuracy of the procedure is maintained. This is particularly important during therapies requiring small radiation spot sizes, such as during the treatment of small vascularized regions in human skin.
  • the housing preferably has a hemispherical shape, and the irradiated region is located as close as possible to the center of the hemisphere. In this configuration, the re-emitted radiation incident on the tissue is evenly distributed, and "hot spots" in the irradiated area are avoided.
  • the reflective housing is hemispherical, and radiation (indicated by the arrow 33) incident on the coating 30 is reflected back towards the tissue (arrow 34) with a slight angular deviation. This angle is such that the re-exposed region of tissue lies substantially within the originally exposed area.
  • the coating 30 is deposited on the outer surface 35 of the substrate 32, radiation reflected back towards the tissue propagates through the substrate twice before re-exposing the tissue.
  • the housing can also be made reflective by cutting right-angle grooves 36 into the transparent substrate 32.
  • each groove 36 has two orthogonal reflective faces 35a, 35b and serves as an individual "corner cube” or “retroreflector” for reflecting the incident radiation.
  • an array of concentric grooves, each positioned at different cross-sectional slices of the hemisphere, are cut into the substrate.
  • Other patterns of grooves may also be used.
  • the grooves are spaced together as closely as possible.
  • the substrate For total internal reflection to occur at the air/substrate interface 38 of each groove, the substrate must be composed of a material having the appropriate refractive index.
  • optically transparent materials such as glasses or plastics having refractive indices greater than 1.4
  • incident radiation indicated by the arrow 40
  • the reflected radiation is displaced by an amount equal to the propagation distance between the two orthogonal faces 35a, 35b of the groove. In this way. - li ⁇ the irradiated area of tissue is kept small.
  • the radiation is reflected by the grooves directly back towards its point of origin regardless of the shape of the reflective housing.
  • irradiation devices employing reflecting grooves have the additional advantage that they can be formed into arbitrary shapes. This is particularly desirable for irradiating devices configured to irradiate hard-to-reach areas of tissue.
  • the substrate is composed of a material which is transparent to the incident radiation.
  • the substrate can be composed of transparent glasses, plastics, or other suitable materials known in the art.
  • plastic materials are desirable, as they can be manufactured in high quantities for relatively low costs. Such materials are formed using techniques well-known in the art, such as injection molding or machining. Irradiation devices, and particularly those made from plastic materials, can be sterilized and are disposable.
  • the substrate can be substantially composed of a reflecting material, thereby obviating the need for inner or outer surface coatings.
  • the substrate can be composed of a diffusely reflecting white plastic, frosted glass, or a related material. These materials have lower reflectivities than metallic or dielectric- coated materials, and function essentially as optical "integrating spheres." Materials of this type have the advantage of irradiating an area with a particularly uniform field after reflecting the re-emitted radiation.
  • the reflecting housing may be covered on its inner or outer surface with reflecting tape, paint, or any other material which can be used to reflect radiation, and particularly optical radiation.
  • the reflecting material reflects at least 80% and most preferably, at least 90% of the remitted radiation. Since the most preferred applications involve the use of optical radiation, the coating preferably exhibits the above-mentioned reflectivities for wavelengths in the range of 200 nm to 5 microns.
  • the reflective housing is configured to reflect optical wavelengths which are typically used in dermatological applications, i.e., 500 - 1100 nm.
  • the template connected to the housing can be replaced with a plate which is transparent to the incident radiation.
  • the transparent plate is used to position the device on the patient's tissue and facilitate alignment of the radiation.
  • the plate is particularly effective in aligning radiation onto tissue containing rough or curved surfaces, such as the skin.
  • Figs. 3A-3C illustrate in more detail the propagation characteristics of the radiation during a typical therapy.
  • This same air/skin interface also scatters incident radiation away from the skin's outer surface.
  • Optical scattering within the skin such as scattering from collagens in the dermis, cells in the epidermis, and other skin structures, additionally directs radiation away from the originally irradiated area. Radiation propagating away from the tissue surface is collected by the reflective housing 13. Reflection off the housing redirects the re-emitted radiation 19'' back towards the tissue surface, where it irradiates the same or nearby region within the originally irradiated area. Here, radiation is again partially absorbed and partially re-emitted. Although a single reflection is indicated in the figures, radiation may undergo multiple reflections in the housing before being reflected back towards the originally irradiated area. As described above, to keep the irradiated area at a minimum, the reflective housing preferably has a hemispherical shape, with the irradiated region positioned at the hemisphere's center.
  • this iterative process of exposing and re-exposing the tissue is repeated until all the radiation propagating in the irradiation device 10 is absorbed.
  • losses due primarily to the reflectivity of the reflective housing and the fact that some components in the irradiation device (e.g., the fiber optic waveguide and the porthole) are non- reflective result in finite increases (i.e., gain) in the amount of delivered radiation.
  • the gain due to the irradiation device represents between about 25% and 300% of the amount of radiation orginally delivered to the tissue. This gain will depend on the wavelength, tissue properties, device reflectance, device size, and device shape.
  • the actual gain in the radiation energy is determined by comparing the method according to the invention to conventional means for delivering radiation to tissues.
  • the energy E 0 of the radiation available for treatment is:
  • R ⁇ is a coefficient indicative of the amount of radiation re-emitted from the tissue and E incident is the energy of the incident radiation.
  • R s is wavelength- dependent and has a value which is less than one: a low value of R B means that the majority of incident radiation is absorbed by the tissue, while a high value indicates a large amount of radiation re-emission.
  • the radiation energy E available for therapy when the irradiation device is employed can be expressed mathematically as:
  • R s and E 0 are the quantities expressed above and R_ is the collective reflectance of the reflective housing. Like R B , R_ is wavelength-dependent and has a value less than one.
  • the amount of radiation available for therapy increases as the collective reflectance of the reflective housing increases. Most preferably, therefore, this reflectance is made as high as possible.
  • Table 1 shown below, lists the increases in available optical radiation as a function of the radiation wavelength and the tissue remittance for human skin. In all cases, R_ is 0.9 and R ⁇ is the reflectance value of the skin at the optical wavelength. Increases in optical energy are calculated relative to conventional therapies performed without the irradiating device.
  • optical radiation near 700 nm is subjected to a gain of approximately 170% when used in combination with the irradiating device.
  • This wavelength is easily obtainable using conventional light sources (e.g., ruby, dye, diode and Ti:sapphire lasers) .
  • the irradiating device effectively triples the effective amount of radiation available for therapy.
  • Optical radiation at 1064 nm (a wavelength generated using conventional Nd:YAG lasers) is also subject to a high gain (117% increase) when used in combination with the irradiation device.
  • the distribution of radiation reflected from the irradiated area of tissue towards the reflective housing is typically diffuse.
  • skin which is an isotropic medium functioning essentially as a Lambertian reflector.
  • the intensity of re-emitted light varies as cos( ⁇ ), where ⁇ is the angle relative to the normal vector of the skin surface.
  • the reflective housing it is particularly important for the reflective housing to have adequate reflective properties in the regions where the reflected radiation is concentrated (i.e., around 45° from the angle of incidence and preferably the region of 0-60°) . Coatings in the regions of low radiation concentrations (e.g., 90°) are less important.
  • the reflective housing includes a hemispherically shaped upper portion 102 and a conical lower portion 104 connected directly to a template 106.
  • the template can be reduced in size or removed.
  • the device with its tapered lower portion occupying a relatively small area, is particularly effective in delivering radiation to hard-to-reach places.
  • the irradiated area 103 of tissue 105 is positioned substantially at the center of the upper portion 102 of the reflective housing 112.
  • the upper portion 102 extends at an angle of at least 60° from the angle of incidence of the input radiation.
  • the reflective housing only contains reflective portions in regions where the contribution from re-emitted radiation intensity is high; no reflecting portion is present in the regions where the reflected radiation intensity is low, i.e., from about an angle of 60° to 90° from the angle of incidence. Note that the small amount of light which is re-emitted at these angles will be reflected by the lower portion 104 of the housing towards the upper portion 102, where it - 19 - will then be reflected back towards the original area of irradiation.
  • the delivery handpiece 108 and input port 110 for this device are the same as those described for the embodiment of Fig. 1.
  • the reflective and substrate materials in this embodiment are the same as those described above.
  • the figure shows a reflective coating 114 deposited on the inner surface of a substrate 115.
  • Other types of reflective housings, such as those containing grooves, may also be used with the irradiation device.
  • an irradiating device 120 features a reflective housing 121 including first 131 and second 122 hemispherical portions and first 127 and second 124 tapered portions.
  • the reflective housing 121 is in contact with a template 126 and is configured to deliver re-emitted radiation to an area 128 of tissue 130.
  • Each portion of the housing is coated with a reflective film 125 as in previous embodiments.
  • re-emitted radiation is reflected by the coating back towards the originally irradiated region so that the amount of radiation delivered to the area 128 is increased.
  • the first and second hemispherical portions have different diameters; the irradiated area 128 is positioned at the coincident centers of the two hemispheres. Separating the housing into first and second hemispherical portions results in a smaller amount of the re-emitted optical intensity irradiating the non- reflective region containing the fiber optic waveguide 132 and the input port 134. This is because re-emitted radiation spatially diverges after the incident beam irradiates the tissue, and thus the spatial concentration of radiation decreases as a function of distance from the irradiated region 128.
  • Fig. 7 shows another embodiment of the invention in which the irradiating device 130 includes a reflective housing 132 shaped as an ellipse.
  • An area 136 of tissue 138 is irradiated with an incident beam delivered by the fiber optic waveguide 140.
  • the elliptical housing is positioned with respect to a template 134 so that one of its foci is coincident with the irradiated area 136. In this way, as indicated by the arrow 133, re-emitted radiation is returned to the originally irradiated area after being reflected multiple times by the housing.
  • the template connected to the housing can be replaced with a plate which is transparent to the incident radiation.
  • the transparent plate is used to position the device on the patient's tissue and facilitate alignment of the radiation.
  • the plate is particularly effective in aligning radiation onto tissue containing rough or curved surfaces, such as the skin.
  • Fig. 8 shows a cross-sectional view of an irradiating device 148 where an optical fiber 150 delivering optical radiation (indicated by the arrow 152) attaches directly to a cone-shaped, diffusely reflective housing 154.
  • the housing 154 includes an upper opening 156 which houses the fiber, and a lower opening 158 placed in direct contact with a patient's tissue 160 (e.g., the skin).
  • the housing 154 is preferably constructed entirely of a diffusely reflecting material, such as a white plastic, to form a highly reflecting cavity.
  • the housing may be formed from a plastic, metal, glass material coated on its inner surface with a diffusely reflecting coating (e.g., a white paint or roughened metallic coating) .
  • a diffusely reflecting coating e.g., a white paint or roughened metallic coating.
  • a portion of the radiation impinging the tissue is randomly re-emitted and propagates back towards the housing 154. There, the radiation is either reflected back onto the tissue or onto another portion of the housing.
  • These processes increase the gain, or total amount of radiation which is absorbed by the tissue. In theory, the reflection process continues until all the incident light is either absorbed by the tissue or is sent back through the fiber 150. It is therefore desirable to increase the ratio between the areas of the lower 158 and upper 156 openings, as this will increase the actual amount of light redirected towards the tissue.
  • Fig. 9 shows another irradiating device 168 of the invention where the reflective housing consists of a optically transparent plate 170 coated on its upper surface with a dielectric coating 172.
  • the plate 170 directly contacts the patient's tissue 160.
  • the reflectivity of a dielectric coating depends on the angle and wavelength of the incident optical beam, and can maximized or minimized by varying the thickness and refractive index (i.e., the material composition) of the coating's dielectric layers 170a, 170b.
  • the 'bandwidth' of the coating i.e., the range of wavelengths or incident angles which are transmitted or reflected, depends on the refractive index and number of the layers.
  • the device 168 preferably includes a narrow-band, high-efficiency coating which transmits normally incident radiation (indicated by the arrow 174) and radiation which deviates from normal by less than about 15°. After this radiation impinges the tissue 160, re-emitted radiation impinging the coating's bottom surface at angles greater than about 15° (indicated by the arrows 175) , is reflected back towards the tissue by the coating to increase the gain. As is described above, re-emitted radiation typically leaves the tissue at an angle of about 45°. This process of reflecting re-emitted radiation continues until all the radiation is either absorbed by the tissue or is transmitted through the coating.
  • the dielectric coating can be on the bottom surface of the glass plate. The plate can also be attached directly to a faceplate or handpiece for ease of use. Therapies and Other Applications
  • the irradiation device can be used in combination with any known radiation-based therapy to increase the gain of the radiation.
  • therapies include optical removal of tatoos, port-wine stains, abnormal blood vessels, psoriatic skin, unwanted hair, pigmented lesions, skin cancers and other lesions treated by laser surgery, phototherapy, photochemotherapy or photodynamic therapy.
  • Additional radiation-based therapies, particularly those used in dermatology, are described in Honigsmann et al., Dermatology in General Medicines, 3rd edition, T.B. Fitzpatrick et al. (eds.) 1728-1754 (1987) , the contents of which are incorporated herein by reference.
  • the opening of the template or the transparent plate is placed over the area to be irradiated.
  • the therapy is then conducted according to standard procedures used in the optical and medical arts.
  • the fluence of the radiation is between about 0.1 and 100 W/cm 2 .
  • the spatial intensity profile of the radiation can be adjusted to vary the amount at radiation-induced heat delivered to the region of interest. Radiation spot diameters of between 10 microns and 1 cm are typically used.
  • a laser is the preferred light source for optical radiation.
  • the laser is chosen according to the desired optical wavelength.
  • Preferred lasers include ion, dye, solid-state (e.g., Nd:YAG, Nd:YLF, Ti:Sapphire) holmium, C0 2 , metal-vapor, excimer, and diode lasers.
  • Other light sources such as fluorescent bulbs, may also be used.
  • the light source may be continuous-wave or pulsed.
  • the irradiation device can also be used in non- medical applications to increase the gain of the incident radiation.
  • the device can be used with a laser to cut or process materials.
  • the device may also be used to drive photochemical reactions in certain materials, such as light-sensitive films.

Abstract

A method and apparatus (10) for irradiating material (14), such as tissue in a patient, is described. The method features the step of first exposing the tissue (14) with a radiation. Following the exposing step, the radiation is partially re-emitted (e.g., reflected or scattered) from the tissue (14). The re-emitted radiation is then collected and imaged back onto the tissue (14) using an external irradiating device (13), containing, for example a hemispherically shaped reflective housing (13). The housing contains a reflective coating (30) disposed on one of its surfaces.

Description

RADIATION-DELIVERY DEVICE Background
This invention relates to radiation-delivery devices.
Radiation sources, such as lasers, are used in a variety of medical applications because of their ability to generate precise, self-cauterizing incisions and locally heat tissue without contacting the patient. In particular, laser light is used in a variety of der atological therapies, such as to remove tatoos, port- wine stains, and unwanted hair. In these applications, radiation is typically delivered through a fiber optic system to a lens, which subsequently images the radiation onto the region of interest. The radiation is absorbed by a portion of the skin or hair (e.g., the melanin or blood vessels) , resulting in optical absorption and localized heating.
In nearly all laser-based surgical procedures, it is desirable to maximize the amount of radiation delivered to the tissue, and minimize the amount of radiation which is re-emitted (e.g., reflected or back¬ scattered) from the tissue. This is particularly difficult to achieve during dermatological procedures, as the turbid optical quality of the skin tends to scatter incident light in all directions. In addition, reflection due to differences in the refractive indices of the skin (n = 1.5) and the air (n = 1.0) leads to further losses. To compensate for radiation lost through these processes, the operator is forced to increase the output power of the light source. This often decreases the accuracy of the procedure, or may, in fact, be impossible if the light source is operating at its maximum power output. Several references teach optical systems which manipulate laser beams to generate more desirable light fields for medical therapies. In U.S. Patent 5,309,339, for example, Webb describes an optical concentrator for manipulating the cross-sectional area and reducing speckle of an incident laser beam. In Webb's device, a spherical or hemispherical mirror is used to return laser light scattered from a diffusely reflective surface back onto the point of incidence. Lenses are then used to produce an output beam by collecting light from the point of incidence.
Summary In general, in one aspect, the invention provides a method for irradiating a material. The method includes the step of first exposing the material with radiation (e.g., optical radiation). Following the exposing step, radiation is partially re-emitted (e.g., scattered, reflected, or both scattered and reflected) from the material. The material is then re-exposed with the re- emitted radiation. Preferably, the material is a patient's tissue. By "tissue" is meant any collection of cells or any specific organ in the patient (e.g., human skin) .
The method of the invention is carried out with an irradiating device configured receive radiation from a radiation delivery means. The radiation delivery means delivers radiation from a radiation source to the material, and is preferably connected to a reflective housing. The housing includes an opening or surface for placement over the material and a reflective component proximal to the opening or surface. Most preferably, the radiation delivery means is a fiber optic waveguide or an articulated arm, and the radiation source is a laser. In preferred embodiments, the re-emitted radiation is received and reflected by a reflective device to re- expose the material. For example, the reflective device can be a reflective housing positioned proximal to the material prior to the exposing step. Preferably, the reflective housing is substantially hemispherical in shape, and the material is positioned substantially near the center of the hemisphere. Alternatively, the reflective housing is substantially elliptical in shape, and the material is positioned substantially near a focus of the ellipse. The reflective housing may also be substantially spherical in shape, with the opening disposed on a surface of the sphere. In still other embodiments, the reflective housing is substantially cone-shaped and includes an opening at the base of the cone. During operation, the material is positioned near this opening.
The method of the invention can also be carried out with an irradiating device which includes an optically transparent plate featuring a reflective coating on one of its surfaces. The reflective coating is disposed on the plate to transmit normally incident radiation (i.e., radiation angled at between about 80° and 100° relative to the surface of the reflective coating) , receive radiation re-emitted from the material, and reflect any re-emitted radiation back onto the material. Preferably, the reflective coating contains a dielectric material or multiple layers of dielectric materials which exhibit angularly dependent reflective properties.
Here, by "substantially hemispherical", "substantially elliptical", or "substantially spherical" is meant a reflective housing which is shaped, respectively, in the form of a hemisphere, ellipse, or sphere so that it reflects incident light to a well- defined area. Preferably, this area is not more that a few millimeters in radius. "Substantially cone-shaped" means at least a portion of the housing is conically shaped. By "center of the hemisphere" is meant the geometrical center of the sphere composed of two identical hemispheres. By "substantially near the center" or "substantially near the focus" is meant a position within a few millimeters of, respectively, the actual center or focus. "Substantially transparent" and substantially reflects" means that, respectively, at least 80% of the radiation is either transmitted or reflected.
The reflective housing preferably includes a reflective coating for reflecting the re-emitted radiation. The coating, for example, may be a reflective film, such as a metallic or dielectric film. The dielectric film may be reflective in only a portion of the electromagnetic spectrum, thereby allowing direct visualization of the material through the film. In other preferred embodiments, the reflective housing features an array of grooves configured to reflect the re-emitted radiation. These grooves have reflective properties similar to those of corner cubes, retroreflectors, or similar optical components which reflect radiation by internal reflection. Other reflecting materials, such as white paint or reflecting tapes, may be used to reflect radiation within the housing. In these embodiments, the reflective housing may take on any shape. For example, in addition to the embodiments described above, the housing may be formed in the shape of a cylindrical tube, with the reflective material disposed on portions of the tube's inner surface. In this case, the opening for irradiating the tissue is positioned on one of the flat surfaces of the tube. In preferred embodiments, the irradiation device is used during a medical therapy to irradiate a patient's tissue. In this case, the device is used in combination with standard medical procedures normally employed when radiation is delivered to tissue. Preferably, the radiation used in the therapy is optical radiation, and the therapy is used to treat human skin. Examples of such therapies include optical removal of tatoos, port- wine stains, abnormal blood vessels, psoriatic skin, unwanted hair, pigmented lesions, skin cancers and other lesions treated by laser surgery, phototherapy, photochemotherapy or photodynamic therapy.
The invention has a number of advantages. In particular, it increases the efficiency of a laser-based surgical procedure by treating the tissue of interest with radiation which is normally not utilized. Scattered or reflected light, lost during conventional procedures, is effectively "recycled" and used to re-expose and treat the tissue. In this way, optical fluences can be kept relatively low during treatment, thereby enhancing the accuracy and flexibility of the therapy.
The invention provides a gain of optical energy available to the tissue by a factor of up to (1-R)-1, where R is the wavelength-dependent fraction of incident light re-emitted from the tissue. For example, when R is 0.7 (a typical value for red light re-emitted from fair skin) the energy available to the skin using the irradiation device may be as large as three times that available without the device. In addition to increasing the amount of radiation available for therapy, the invention can also effectively increase the exposure spot diameter of the radiation. In many applications in which the "target" for therapy is deep within the skin (e.g., during the removal of tattoos, port-wine stains, or hair) , such a larger exposure spot diameter is advantageous.
Moreover, by collecting and then re-exposing the tissue of interest with the re-emitted radiation, the invention generates a more spatially uniform field during therapy. This gives the operator more control over the amount of heat delivered to the tissue, and thus improves the accuracy of the therapy.
The invention also increases the safety of laser- based therapies. Light reflected or scattered from the tissue, as well as ablated tissue which can be hazardous to the operators, is contained within a well-defined area by the irradiating device. Moreover, the device can be made small and compact, and can be used interchangeably with conventional laser-based surgical instruments. The device can additionally be fabricated with relatively inexpensive, disposable materials; a new, sterilized device can therefore be used for each procedure.
These and other advantages will be apparent from the following detailed description, and from the claims.
Brief Description of the Drawings Fig. 1 is a top view of an irradiating device of the invention being used to irradiate a patient's skin; Fig. 2 is a cross-sectional side view of an irradiating device in contact with the patient's skin; Figs. 3A-3C are, respectively, cross-sectional side views of the irradiating device during initial irradiation of the skin, after radiation is initially re- emitted from the skin surface, and after the re-emitted radiation is reflected off the reflective housing and back towards the skin surface;
Figs. 4A and 4B are cut-away cross-sectional side views of, respectively, a reflective housing including a radiation-reflecting coating, and a reflective housing including an array of retro-reflecting grooves;
Fig. 5 is a cross-sectional side view of an irradiating device including a reflective housing featuring a hemispherical top portion and a tapered bottom portion;
Fig. 6 is a cross-sectional side view of an irradiating device containing a reflective housing featuring two hemispherical top portions and a straight bottom portion;
Fig. 7 is a cross-sectional side view of an irradiating device containing an elliptical reflective housing;
Fig. 8 is a cross-sectional side view of an irradiating device including a cone-shaped reflective housing; and,
Fig. 9 is a side view of a irradiating device featuring a flat, optically transparent plate coated with a reflecting dielectric film.
Detailed Description
Device Structure
Referring first to Fig. 1, an irradiating device 10 delivers radiation during a therapy to an area of a patient's tissue 14. The device 10 is configured so that radiation which is normally re-emitted from the tissue after irradiation (and is thus wasted during the therapy) can be collected and imaged back onto the originally irradiated area.
The device includes a fiber optic waveguide 12 coupled to a laser or other radiation source (not shown in the figure) . A distal end 20 of the fiber optic waveguide is housed in a delivery handpiece 18 and an input port 16 so that radiation from the fiber can be delivered to the device 10. The input port 16 is connected to a hemispherically shaped reflective housing 13 which surrounds the tissue to be irradiated and is configured to reflect radiation. During operation, radiation is delivered from the fiber optic waveguide 12 to the tissue. Portions of the delivered radiation are either absorbed by the tissue, leading to radiation- induced heating, or are re-emitted from the irradiated area. The re-emitted radiation propagates away from the tissue, and is collected by the hemispherically shaped reflective housing 13. A template 22 connected to the housing 13 is used to position the device on the patient's tissue and facilitate alignment of the radiation. The template is especially useful for aligning radiation onto tissue containing rough or curved surfaces, such as the skin. The reflective housing 13 includes a transparent porthole 24 for viewing the irradiated region.
Figs. 2, 4A and 4B show cross-sectional views of the irradiation device 10 and the reflective housing 13. The delivery handpiece 18 and input port 16 connected to the housing each enclose portions of the fiber optic waveguide 12. The distal end 11 of the waveguide 12 extends into the device and is surrounded by the hemispherically shaped reflective housing 13. The housing 13 is connected to the template 22 which, in turn, is placed in contact with a patient's tissue 14. The template 22 includes an opening 21 positioned above a portion 17 of the tissue and in the center of the hemispherical reflective housing. The opening 21 and distal end 11 of the waveguide are aligned so that, during therapy, radiation from the waveguide passes through the template and onto the tissue.
The reflective housing includes a reflective coating 30 on its inner surface so that during therapy radiation scattered or reflected from the tissue is collected and imaged back onto the originally irradiated portion of tissue. The reflective coating 30 can be any reflective material and can be made using any of a number of techniques known in the art. For example, the coating may be deposited as a thin reflective film on the inner surface of a transparent substrate 32. The coating may also be deposited on the substrate's outer surface.
In particular embodiments, the coating may be a thin metallic film composed of materials such as aluminum, silver, or gold. The reflective properties of these materials are dependent on the material composition and the film thickness, and are well known in the optical arts. Dielectric films may also serve as reflective coatings. These materials have particularly desirable reflectivities at visible and infrared wavelengths, and can be used to coat the inner or outer surfaces of the substrate material 32. Dielectric coatings have the additional advantage that they can be made transparent to visible wavelengths or radiation at certain angles of incidence; thus, when used with transparent substrates, these materials allow the operator to directly view the procedure without the need for a porthole.
The reflective housing is preferably shaped so that re-emitted radiation is collected and imaged onto a region contained in the originally irradiated area. In this way, the spatial extent of the irradiated area is not significantly increased by the reflective process, and thus the accuracy of the procedure is maintained. This is particularly important during therapies requiring small radiation spot sizes, such as during the treatment of small vascularized regions in human skin. As described above, the housing preferably has a hemispherical shape, and the irradiated region is located as close as possible to the center of the hemisphere. In this configuration, the re-emitted radiation incident on the tissue is evenly distributed, and "hot spots" in the irradiated area are avoided.
In the embodiment shown in Fig. 4A, the reflective housing is hemispherical, and radiation (indicated by the arrow 33) incident on the coating 30 is reflected back towards the tissue (arrow 34) with a slight angular deviation. This angle is such that the re-exposed region of tissue lies substantially within the originally exposed area. When the coating 30 is deposited on the outer surface 35 of the substrate 32, radiation reflected back towards the tissue propagates through the substrate twice before re-exposing the tissue.
Referring now to Fig. 4B, the housing can also be made reflective by cutting right-angle grooves 36 into the transparent substrate 32. In this case, each groove 36 has two orthogonal reflective faces 35a, 35b and serves as an individual "corner cube" or "retroreflector" for reflecting the incident radiation. Preferably, an array of concentric grooves, each positioned at different cross-sectional slices of the hemisphere, are cut into the substrate. Other patterns of grooves may also be used. Preferably, in order to maximize the reflectance of the housing, the grooves are spaced together as closely as possible. For total internal reflection to occur at the air/substrate interface 38 of each groove, the substrate must be composed of a material having the appropriate refractive index. Typically, optically transparent materials, such as glasses or plastics having refractive indices greater than 1.4, are suitable. In the reflective housing 13 shown in Fig. 4B, incident radiation (indicated by the arrow 40) re-emitted from the tissue is reflected back towards its point of origin. The reflected radiation (arrow 42) is displaced by an amount equal to the propagation distance between the two orthogonal faces 35a, 35b of the groove. In this way. - li ¬ the irradiated area of tissue is kept small. Moreover, in the embodiment shown in Fig. 4B, the radiation is reflected by the grooves directly back towards its point of origin regardless of the shape of the reflective housing. Thus, irradiation devices employing reflecting grooves have the additional advantage that they can be formed into arbitrary shapes. This is particularly desirable for irradiating devices configured to irradiate hard-to-reach areas of tissue. Preferably, in the embodiments described above, the substrate is composed of a material which is transparent to the incident radiation. For example, for visible radiation, the substrate can be composed of transparent glasses, plastics, or other suitable materials known in the art. In particular, plastic materials are desirable, as they can be manufactured in high quantities for relatively low costs. Such materials are formed using techniques well-known in the art, such as injection molding or machining. Irradiation devices, and particularly those made from plastic materials, can be sterilized and are disposable.
In addition to the reflective surfaces shown in Figs. 4A and 4B, other reflective coatings and devices known in the art can be used with the irradiation device's reflective housing. For example, the substrate can be substantially composed of a reflecting material, thereby obviating the need for inner or outer surface coatings. In particular embodiments, the substrate can be composed of a diffusely reflecting white plastic, frosted glass, or a related material. These materials have lower reflectivities than metallic or dielectric- coated materials, and function essentially as optical "integrating spheres." Materials of this type have the advantage of irradiating an area with a particularly uniform field after reflecting the re-emitted radiation.
In other embodiments, the reflecting housing may be covered on its inner or outer surface with reflecting tape, paint, or any other material which can be used to reflect radiation, and particularly optical radiation. Preferably, the reflecting material reflects at least 80% and most preferably, at least 90% of the remitted radiation. Since the most preferred applications involve the use of optical radiation, the coating preferably exhibits the above-mentioned reflectivities for wavelengths in the range of 200 nm to 5 microns. In particularly preferred embodiments, the reflective housing is configured to reflect optical wavelengths which are typically used in dermatological applications, i.e., 500 - 1100 nm.
In still other embodiments, the template connected to the housing can be replaced with a plate which is transparent to the incident radiation. Like the template, the transparent plate is used to position the device on the patient's tissue and facilitate alignment of the radiation. The plate is particularly effective in aligning radiation onto tissue containing rough or curved surfaces, such as the skin.
Figs. 3A-3C illustrate in more detail the propagation characteristics of the radiation during a typical therapy. After being delivered from the fiber optic waveguide 12, incident radiation 19 enters the irradiation device, propagates through the opening 21 in the template 22, and irradiates the portion 17 of the patient's tissue 14. While some of the radiation is absorbed, refractive index differences between the surrounding air (n = 1) and the tissue (typically n = 1.5) cause a substantial fraction 19' of the incident radiation to be reflected. For example, for both black and white human skin, between 4% and 7% of optical radiation from 250 and 3000 nm is reflected off the stratum corneum (i.e., the skin's upper layer). This same air/skin interface also scatters incident radiation away from the skin's outer surface. Optical scattering within the skin, such as scattering from collagens in the dermis, cells in the epidermis, and other skin structures, additionally directs radiation away from the originally irradiated area. Radiation propagating away from the tissue surface is collected by the reflective housing 13. Reflection off the housing redirects the re-emitted radiation 19'' back towards the tissue surface, where it irradiates the same or nearby region within the originally irradiated area. Here, radiation is again partially absorbed and partially re-emitted. Although a single reflection is indicated in the figures, radiation may undergo multiple reflections in the housing before being reflected back towards the originally irradiated area. As described above, to keep the irradiated area at a minimum, the reflective housing preferably has a hemispherical shape, with the irradiated region positioned at the hemisphere's center.
In theory, this iterative process of exposing and re-exposing the tissue is repeated until all the radiation propagating in the irradiation device 10 is absorbed. In practice, however, losses due primarily to the reflectivity of the reflective housing and the fact that some components in the irradiation device (e.g., the fiber optic waveguide and the porthole) are non- reflective result in finite increases (i.e., gain) in the amount of delivered radiation. Typically, the gain due to the irradiation device represents between about 25% and 300% of the amount of radiation orginally delivered to the tissue. This gain will depend on the wavelength, tissue properties, device reflectance, device size, and device shape.
The actual gain in the radiation energy is determined by comparing the method according to the invention to conventional means for delivering radiation to tissues. In procedures where the irradiating device is not used, the energy E0 of the radiation available for treatment is:
E0 = Eincidβnt (l -Rg) ( 1 )
where Rβ is a coefficient indicative of the amount of radiation re-emitted from the tissue and Eincident is the energy of the incident radiation. Rs is wavelength- dependent and has a value which is less than one: a low value of RB means that the majority of incident radiation is absorbed by the tissue, while a high value indicates a large amount of radiation re-emission. Thus, if Rβ = .3, then E0 = 0.7 Eincidβnt, meaning that 70% of the incident light is absorbed by the tissue during treatment.
The radiation energy E available for therapy when the irradiation device is employed can be expressed mathematically as:
E = E0 [l + R,Ra ♦ R^) 2 + (2V?_)3 + ...] = { 1_EχA) (2)
where Rs and E0 are the quantities expressed above and R_ is the collective reflectance of the reflective housing. Like RB, R_ is wavelength-dependent and has a value less than one. By comparing equations 1 and 2, the gain due to the irradiation device is expressed as:
*ain - TOT ) (3)
Thus, using the device of the invention, the amount of radiation available for therapy increases as the collective reflectance of the reflective housing increases. Most preferably, therefore, this reflectance is made as high as possible.
Table 1, shown below, lists the increases in available optical radiation as a function of the radiation wavelength and the tissue remittance for human skin. In all cases, R_ is 0.9 and Rβ is the reflectance value of the skin at the optical wavelength. Increases in optical energy are calculated relative to conventional therapies performed without the irradiating device.
Table 1 - Gain as a Function of Skin Remittance and Optical Wavelength
Wavelength Application Rs Gain Increase in (n ) Optical Energy
510-532 vascular treatment, 0.3 1.37 37% tattoo and hair removal
585 vascular treatment 0.3 1.37 37%
694 tattoo and hair 0.7 2.70 170% remova1, pigment treatment
1064 tattoo and hair 0.6 2.17 117% removal I
From Table 1, it is evident that the gain of the radiation increases with the RgR,-, product. This product can be increased by choosing an irradiating wavelength which is re-emitted strongly by the tissue or, as described above, by maximizing the reflectance of the reflective housing for the irradiating wavelength.
As is evident from the Table, optical radiation near 700 nm is subjected to a gain of approximately 170% when used in combination with the irradiating device. This wavelength is easily obtainable using conventional light sources (e.g., ruby, dye, diode and Ti:sapphire lasers) . Thus, when used with these light sources, the irradiating device effectively triples the effective amount of radiation available for therapy. Optical radiation at 1064 nm (a wavelength generated using conventional Nd:YAG lasers) is also subject to a high gain (117% increase) when used in combination with the irradiation device.
During therapy, the distribution of radiation reflected from the irradiated area of tissue towards the reflective housing is typically diffuse. This is particularly true for skin, which is an isotropic medium functioning essentially as a Lambertian reflector. In this case, the intensity of re-emitted light varies as cos(θ), where θ is the angle relative to the normal vector of the skin surface. However, the amount of light collected by a hemispherical reflector varies as sin(θ) . Therefore, the contribution of a hemispherical reflector is most pronounced at Θ = 45°, i.e., the angle where the product sin(θ)cos(θ) is maximized. This means that although a large fraction of radiation is gathered at angles of between about 0° and 60° from the beam path of the incident radiation, the most significant region of reflected radiation typically occurs at 45° from the angle of incidence. The amount of radiation reflected at 90° from the angle of incidence is typically negligible. Thus, it is particularly important for the reflective housing to have adequate reflective properties in the regions where the reflected radiation is concentrated (i.e., around 45° from the angle of incidence and preferably the region of 0-60°) . Coatings in the regions of low radiation concentrations (e.g., 90°) are less important.
Fig. 5 shows an another embodiment of the invention in which the reflective housing 112 of the irradiation device 100 is designed to capture and reflect the re-emitted light over the important region of approximately θ = 0° - 60°. The reflective housing includes a hemispherically shaped upper portion 102 and a conical lower portion 104 connected directly to a template 106. The template can be reduced in size or removed. In this configuration, the device, with its tapered lower portion occupying a relatively small area, is particularly effective in delivering radiation to hard-to-reach places.
The irradiated area 103 of tissue 105 is positioned substantially at the center of the upper portion 102 of the reflective housing 112. Preferably, the upper portion 102 extends at an angle of at least 60° from the angle of incidence of the input radiation. In this configuration, the reflective housing only contains reflective portions in regions where the contribution from re-emitted radiation intensity is high; no reflecting portion is present in the regions where the reflected radiation intensity is low, i.e., from about an angle of 60° to 90° from the angle of incidence. Note that the small amount of light which is re-emitted at these angles will be reflected by the lower portion 104 of the housing towards the upper portion 102, where it - 19 - will then be reflected back towards the original area of irradiation.
The delivery handpiece 108 and input port 110 for this device are the same as those described for the embodiment of Fig. 1. Similarly, the reflective and substrate materials in this embodiment are the same as those described above. The figure shows a reflective coating 114 deposited on the inner surface of a substrate 115. Other types of reflective housings, such as those containing grooves, may also be used with the irradiation device.
Still other embodiments of the invention are shown in Figs. 6-9. In Fig. 6, an irradiating device 120 features a reflective housing 121 including first 131 and second 122 hemispherical portions and first 127 and second 124 tapered portions. The reflective housing 121 is in contact with a template 126 and is configured to deliver re-emitted radiation to an area 128 of tissue 130. Each portion of the housing is coated with a reflective film 125 as in previous embodiments. As indicated by the arrows 119 and 123, re-emitted radiation is reflected by the coating back towards the originally irradiated region so that the amount of radiation delivered to the area 128 is increased. In this case, the first and second hemispherical portions have different diameters; the irradiated area 128 is positioned at the coincident centers of the two hemispheres. Separating the housing into first and second hemispherical portions results in a smaller amount of the re-emitted optical intensity irradiating the non- reflective region containing the fiber optic waveguide 132 and the input port 134. This is because re-emitted radiation spatially diverges after the incident beam irradiates the tissue, and thus the spatial concentration of radiation decreases as a function of distance from the irradiated region 128.
Fig. 7 shows another embodiment of the invention in which the irradiating device 130 includes a reflective housing 132 shaped as an ellipse. An area 136 of tissue 138 is irradiated with an incident beam delivered by the fiber optic waveguide 140. The elliptical housing is positioned with respect to a template 134 so that one of its foci is coincident with the irradiated area 136. In this way, as indicated by the arrow 133, re-emitted radiation is returned to the originally irradiated area after being reflected multiple times by the housing.
In the embodiments shown in Figs. 6 and 7, the template connected to the housing can be replaced with a plate which is transparent to the incident radiation. Like the template, the transparent plate is used to position the device on the patient's tissue and facilitate alignment of the radiation. The plate is particularly effective in aligning radiation onto tissue containing rough or curved surfaces, such as the skin. Fig. 8 shows a cross-sectional view of an irradiating device 148 where an optical fiber 150 delivering optical radiation (indicated by the arrow 152) attaches directly to a cone-shaped, diffusely reflective housing 154. The housing 154 includes an upper opening 156 which houses the fiber, and a lower opening 158 placed in direct contact with a patient's tissue 160 (e.g., the skin). The housing 154 is preferably constructed entirely of a diffusely reflecting material, such as a white plastic, to form a highly reflecting cavity. Alternatively, the housing may be formed from a plastic, metal, glass material coated on its inner surface with a diffusely reflecting coating (e.g., a white paint or roughened metallic coating) . During operation, radiation emitted from the fiber 150 spatially diverges (typically at an angle of about 30°, as indicated by the dashed lines 162) until it impinges the tissue 160 and is absorbed. The height of the cone thus determines the radiation spot size on the tissue, as the radiation's divergence and area increase with cone height. Typically the cone height is chosen to be about 1.5 cm. As described above, a portion of the radiation impinging the tissue is randomly re-emitted and propagates back towards the housing 154. There, the radiation is either reflected back onto the tissue or onto another portion of the housing. These processes increase the gain, or total amount of radiation which is absorbed by the tissue. In theory, the reflection process continues until all the incident light is either absorbed by the tissue or is sent back through the fiber 150. It is therefore desirable to increase the ratio between the areas of the lower 158 and upper 156 openings, as this will increase the actual amount of light redirected towards the tissue.
Fig. 9 shows another irradiating device 168 of the invention where the reflective housing consists of a optically transparent plate 170 coated on its upper surface with a dielectric coating 172. The plate 170, in turn, directly contacts the patient's tissue 160. As is well known in the art, the reflectivity of a dielectric coating depends on the angle and wavelength of the incident optical beam, and can maximized or minimized by varying the thickness and refractive index (i.e., the material composition) of the coating's dielectric layers 170a, 170b. The 'bandwidth' of the coating, i.e., the range of wavelengths or incident angles which are transmitted or reflected, depends on the refractive index and number of the layers. For optimum performance, the device 168 preferably includes a narrow-band, high-efficiency coating which transmits normally incident radiation (indicated by the arrow 174) and radiation which deviates from normal by less than about 15°. After this radiation impinges the tissue 160, re-emitted radiation impinging the coating's bottom surface at angles greater than about 15° (indicated by the arrows 175) , is reflected back towards the tissue by the coating to increase the gain. As is described above, re-emitted radiation typically leaves the tissue at an angle of about 45°. This process of reflecting re-emitted radiation continues until all the radiation is either absorbed by the tissue or is transmitted through the coating. Other embodiments of the irradiating device of Fig. 9 are also possible. For example, the dielectric coating can be on the bottom surface of the glass plate. The plate can also be attached directly to a faceplate or handpiece for ease of use. Therapies and Other Applications
The irradiation device can be used in combination with any known radiation-based therapy to increase the gain of the radiation. Examples of such therapies include optical removal of tatoos, port-wine stains, abnormal blood vessels, psoriatic skin, unwanted hair, pigmented lesions, skin cancers and other lesions treated by laser surgery, phototherapy, photochemotherapy or photodynamic therapy. Additional radiation-based therapies, particularly those used in dermatology, are described in Honigsmann et al., Dermatology in General Medicines, 3rd edition, T.B. Fitzpatrick et al. (eds.) 1728-1754 (1987) , the contents of which are incorporated herein by reference.
During therapy, the opening of the template or the transparent plate is placed over the area to be irradiated. The therapy is then conducted according to standard procedures used in the optical and medical arts.
Because the effective amount of radiation which exposes the skin is increased using the irradiation device, it may be necessary to decrease the amount of radiation used during therapy. Typically, the fluence of the radiation is between about 0.1 and 100 W/cm2. The spatial intensity profile of the radiation can be adjusted to vary the amount at radiation-induced heat delivered to the region of interest. Radiation spot diameters of between 10 microns and 1 cm are typically used.
A laser is the preferred light source for optical radiation. The laser is chosen according to the desired optical wavelength. Preferred lasers include ion, dye, solid-state (e.g., Nd:YAG, Nd:YLF, Ti:Sapphire) holmium, C02, metal-vapor, excimer, and diode lasers. Other light sources, such as fluorescent bulbs, may also be used. The light source may be continuous-wave or pulsed. The irradiation device can also be used in non- medical applications to increase the gain of the incident radiation. For example, the device can be used with a laser to cut or process materials. The device may also be used to drive photochemical reactions in certain materials, such as light-sensitive films.
Still other embodiments are within the scope of the following claims.

Claims

CLAIMS :
1. A method for irradiating a material, said method comprising: exposing said material with radiation, the radiation, following said exposing, being partially re- emitted from the material, and re-exposing the material with the re-emitted radiation.
2. The method of claim 1, wherein the re-emitted radiation is reflected, scattered, or reflected and scattered from the material.
3. The method of claim 1, wherein the re-emitted radiation is reflected by a reflective device to re- expose the material.
4. The method of claim 3, wherein the reflective device is a reflective housing positioned proximal to the material.
5. The method of claim 4, wherein the reflective housing is comprised by an irradiating device placed proximal to the material prior to said exposing.
6. The method of claim 4, wherein the reflective housing is substantially hemispherical in shape, and the material is positioned substantially near the center of the hemisphere.
7. The method of claim 4, wherein the reflective housing is substantially elliptical in shape, and the material is positioned substantially near a focus of the ellipse.
8. The method of claim 4, wherein the reflective housing is substantially cone-shaped and comprises a bottom opening, and the material is positioned near the bottom opening.
9. The method of claim 4, wherein the reflective housing is an optically transparent plate comprising a reflective coating which is substantially transparent to normally incident radiation and substantially reflects radiation incident at an angle, and the material is positioned in contact with a surface of the transparent plate.
10. The method of claim 4, wherein the reflective housing comprises a reflective coating for reflecting the re-emitted radiation.
11. The method of claim 4, wherein said reflective housing comprises an array of grooves configured to reflect the re-emitted radiation.
12. The method of claim 1, wherein the radiation is optical radiation.
13. An irradiating device for delivering radiation to a material, comprising a reflective housing configured to receive radiation from a radiation delivery means, said housing comprising an opening or surface for placement over a material and a reflective component proximal to said opening or surface, said reflective housing being shaped to receive radiation re-emitted from the material and reflect the re-emitted radiation back onto the material.
14. The irradiating device of claim 13, wherein said reflective component is a reflective film.
15. The irradiating device of claim 14, wherein said reflective film comprises a metallic or dielectric material.
16. The irradiating device of claim 13, wherein said reflective component is an array of grooves formed in said reflective housing.
17. The irradiating device of claim 13, wherein said reflective housing is substantially hemispherical in shape and said opening is positioned at a center of the hemisphere.
18. The irradiating device of claim 13, wherein said reflective housing is substantially elliptical in shape and said opening is positioned at a foci of the ellipse.
19. The irradiating device of claim 13, wherein said reflective housing is substantially spherical in shape and said opening is disposed on a surface of the sphere.
20. The irradiating device of claim 13, wherein said reflective housing is substantially conical in shape and said opening is positioned at a base of the cone.
21. The irradiating device of claim 13, wherein said radiation delivery means is a fiber optic waveguide or an articulated arm.
22. The irradiating device of claim 15, wherein said radiation source is a laser.
23. An irradiating device for delivering radiation to a material, comprising an optically transparent plate comprising a reflective coating on a surface, said reflective coating being disposed on the plate to transmit normally incident radiation from a radiation delivery means, receive radiation re-emitted from a material, and reflect re- emitted radiation incident on the coating at an angle back onto the material.
24. The irradiating device of claim 23, wherein the reflective coating comprises a dielectric material.
25. The irradiating device of claim 24, wherein the reflective coating comprises multiple layers of dielectric materials.
PCT/US1996/016217 1995-10-12 1996-10-10 Radiation-delivery device WO1997013458A1 (en)

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Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1999046005A1 (en) * 1998-03-12 1999-09-16 Palomar Medical Technologies, Inc. System for electromagnetic radiation of the skin
EP1913972A1 (en) * 1999-09-20 2008-04-23 Susanne Johansson Laser probe for medical treatment
US8915948B2 (en) 2002-06-19 2014-12-23 Palomar Medical Technologies, Llc Method and apparatus for photothermal treatment of tissue at depth
US9028536B2 (en) 2006-08-02 2015-05-12 Cynosure, Inc. Picosecond laser apparatus and methods for its operation and use
US9780518B2 (en) 2012-04-18 2017-10-03 Cynosure, Inc. Picosecond laser apparatus and methods for treating target tissues with same
US9919168B2 (en) 2009-07-23 2018-03-20 Palomar Medical Technologies, Inc. Method for improvement of cellulite appearance
US10245107B2 (en) 2013-03-15 2019-04-02 Cynosure, Inc. Picosecond optical radiation systems and methods of use
US10434324B2 (en) 2005-04-22 2019-10-08 Cynosure, Llc Methods and systems for laser treatment using non-uniform output beam
US11418000B2 (en) 2018-02-26 2022-08-16 Cynosure, Llc Q-switched cavity dumped sub-nanosecond laser

Families Citing this family (99)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6214034B1 (en) * 1996-09-04 2001-04-10 Radiancy, Inc. Method of selective photothermolysis
IL119683A (en) * 1996-11-25 2002-12-01 Rachel Lubart Method and device for light irradiation into tissue
US8182473B2 (en) 1999-01-08 2012-05-22 Palomar Medical Technologies Cooling system for a photocosmetic device
US6517532B1 (en) 1997-05-15 2003-02-11 Palomar Medical Technologies, Inc. Light energy delivery head
US6653618B2 (en) 2000-04-28 2003-11-25 Palomar Medical Technologies, Inc. Contact detecting method and apparatus for an optical radiation handpiece
JP4056091B2 (en) 1997-05-15 2008-03-05 パロマー・メディカル・テクノロジーズ・インコーポレーテッド Dermatological treatment method and apparatus
US6104959A (en) 1997-07-31 2000-08-15 Microwave Medical Corp. Method and apparatus for treating subcutaneous histological features
AU752968B2 (en) * 1997-12-31 2002-10-03 Radiancy Inc. Apparatus and method for removing hair
US6004344A (en) * 1998-02-04 1999-12-21 Sun Medical Co., Ltd. Infrared ray irradiation apparatus and infrared ray irradiation source used therein
AU3363999A (en) 1998-03-27 1999-10-18 General Hospital Corporation, The Method and apparatus for the selective targeting of lipid-rich tissues
US5997530A (en) * 1998-04-13 1999-12-07 The Regents Of The University Of California Apparatus and method to control atmospheric water vapor composition and concentration during dynamic cooling of biological tissues in conjunction with laser irradiations
US6514242B1 (en) * 1998-12-03 2003-02-04 David Vasily Method and apparatus for laser removal of hair
US7041094B2 (en) * 1999-03-15 2006-05-09 Cutera, Inc. Tissue treatment device and method
US6290713B1 (en) 1999-08-24 2001-09-18 Thomas A. Russell Flexible illuminators for phototherapy
IL150604A0 (en) * 2000-01-25 2003-02-12 Palomar Medical Tech Inc Method and apparatus for medical treatment utilizing long duration electromagnetic radiation
US6457365B1 (en) * 2000-02-09 2002-10-01 Endosonics Corporation Method and apparatus for ultrasonic imaging
US7083610B1 (en) 2000-06-07 2006-08-01 Laserscope Device for irradiating tissue
US7384797B1 (en) 2000-10-12 2008-06-10 University Of Utah Research Foundation Resonant optical cavities for high-sensitivity high-throughput biological sensors and methods
CA2433022C (en) * 2000-12-28 2016-12-06 Palomar Medical Technologies, Inc. Method and apparatus for therapeutic emr treatment of the skin
US6723090B2 (en) 2001-07-02 2004-04-20 Palomar Medical Technologies, Inc. Fiber laser device for medical/cosmetic procedures
US6942658B1 (en) * 2001-08-24 2005-09-13 Boilase Technology, Inc. Radiation emitting apparatus with spatially controllable output energy distributions
US6811565B2 (en) * 2001-11-14 2004-11-02 Healing Machines, Inc. System and method for light activation of healing mechanisms
IL163946A0 (en) 2002-03-12 2005-12-18 Gen Hospital Corp Method and apparatus for hair growth managment
US20040034388A1 (en) * 2002-06-14 2004-02-19 Healing Machines, Inc. Apparatus and method for physiological treatment with electromagnetic energy
US7018397B2 (en) * 2002-09-25 2006-03-28 Ceramoptec Industries, Inc. Flexible device for topical application of PDT
EP2522293A2 (en) 2002-10-23 2012-11-14 Palomar Medical Technologies, Inc. Phototreatment device for use with coolants and topical substances
US11007373B1 (en) * 2002-12-20 2021-05-18 James Andrew Ohneck Photobiostimulation device and method of using same
US7703458B2 (en) * 2003-02-21 2010-04-27 Cutera, Inc. Methods and devices for non-ablative laser treatment of dermatologic conditions
US7981111B2 (en) 2003-02-25 2011-07-19 Tria Beauty, Inc. Method and apparatus for the treatment of benign pigmented lesions
US7413567B2 (en) 2003-02-25 2008-08-19 Spectragenics, Inc. Optical sensor and method for identifying the presence of skin
US7250045B2 (en) 2003-02-25 2007-07-31 Spectragenics, Inc. Self-contained, eye-safe hair-regrowth-inhibition apparatus and method
US7452356B2 (en) 2003-02-25 2008-11-18 Tria Beauty, Inc. Eye-safe dermatologic treatment apparatus
EP2604215B1 (en) 2003-02-25 2017-10-11 Tria Beauty, Inc. Eye-safe dermatologic treatment apparatus and method
ES2570987T3 (en) 2003-02-25 2016-05-23 Tria Beauty Inc Dermatological treatment device, based on diode laser and autonomous
CA2437638A1 (en) * 2003-08-20 2005-02-20 John Robert North Photodynamic therapy
US8777935B2 (en) 2004-02-25 2014-07-15 Tria Beauty, Inc. Optical sensor and method for identifying the presence of skin
JP5065005B2 (en) 2004-04-01 2012-10-31 ザ ジェネラル ホスピタル コーポレイション Method and apparatus for dermatological treatment and tissue remodeling
US7331954B2 (en) * 2004-04-08 2008-02-19 Omniguide, Inc. Photonic crystal fibers and medical systems including photonic crystal fibers
US20070179482A1 (en) * 2004-05-07 2007-08-02 Anderson Robert S Apparatuses and methods to treat biological external tissue
US20050251117A1 (en) * 2004-05-07 2005-11-10 Anderson Robert S Apparatus and method for treating biological external tissue
US8571648B2 (en) * 2004-05-07 2013-10-29 Aesthera Apparatus and method to apply substances to tissue
US7842029B2 (en) * 2004-05-07 2010-11-30 Aesthera Apparatus and method having a cooling material and reduced pressure to treat biological external tissue
US7837675B2 (en) 2004-07-22 2010-11-23 Shaser, Inc. Method and device for skin treatment with replaceable photosensitive window
ES2432140T3 (en) * 2004-08-06 2013-11-29 Syneron Beauty Ltd. Therapy device
US20060047281A1 (en) 2004-09-01 2006-03-02 Syneron Medical Ltd. Method and system for invasive skin treatment
US20060093561A1 (en) * 2004-11-02 2006-05-04 John Kennedy Method of treating microorganisms in the oral cavity
JP4717468B2 (en) * 2005-02-23 2011-07-06 浜松ホトニクス株式会社 Laser processing equipment
AU2006292526A1 (en) 2005-09-15 2007-03-29 Palomar Medical Technologies, Inc. Skin optical characterization device
CA2535276A1 (en) * 2006-02-06 2007-08-06 John Kennedy Therapy device and system and method for reducing harmful exposure to electromagnetic radiation
US20080031833A1 (en) * 2006-03-13 2008-02-07 Oblong John E Combined energy and topical composition application for regulating the condition of mammalian skin
US20080055755A1 (en) * 2006-08-31 2008-03-06 Searete Llc, A Limited Liability Corporation Of The State Of Delaware Electromagnetic device and method
US7963676B2 (en) * 2006-10-23 2011-06-21 Wu Kuohua Angus Reflector window for use in a light lamp
US20080172111A1 (en) 2007-01-16 2008-07-17 The General Hospital Corporation Method and apparatus for selective photothermolysis of veins
US20100211059A1 (en) 2007-04-19 2010-08-19 Deem Mark E Systems and methods for creating an effect using microwave energy to specified tissue
JP2010524589A (en) 2007-04-19 2010-07-22 ザ ファウンドリー, インコーポレイテッド Method, apparatus and system for non-invasive delivery of microwave therapy
US9241763B2 (en) 2007-04-19 2016-01-26 Miramar Labs, Inc. Systems, apparatus, methods and procedures for the noninvasive treatment of tissue using microwave energy
CN101711134B (en) 2007-04-19 2016-08-17 米勒玛尔实验室公司 Tissue is applied the system of microwave energy and in organized layer, produces the system of tissue effect
US9149331B2 (en) 2007-04-19 2015-10-06 Miramar Labs, Inc. Methods and apparatus for reducing sweat production
US20090012434A1 (en) * 2007-07-03 2009-01-08 Anderson Robert S Apparatus, method, and system to treat a volume of skin
EP2194899A4 (en) 2007-08-08 2012-11-28 Tria Beauty Inc Capacitive sensing method and device for detecting skin
US20090069795A1 (en) * 2007-09-10 2009-03-12 Anderson Robert S Apparatus and method for selective treatment of tissue
US20090093864A1 (en) * 2007-10-08 2009-04-09 Anderson Robert S Methods and devices for applying energy to tissue
AU2008335715B2 (en) 2007-12-12 2014-01-23 Miradry, Inc. Systems, apparatus, methods and procedures for the noninvasive treatment of tissue using microwave energy
ES2471971T3 (en) 2007-12-12 2014-06-27 Miramar Labs, Inc. System and apparatus for non-invasive treatment of tissue using microwave energy
US20090171422A1 (en) * 2007-12-31 2009-07-02 Searete Llc , A Limited Liability Corporation Of The State Of Delaware Radiation treatment device
AU2009205297A1 (en) 2008-01-17 2009-07-23 Syneron Medical Ltd. A hair removal apparatus for personal use and the method of using same
EP2237732A4 (en) 2008-01-24 2011-06-01 Syneron Medical Ltd A device, apparatus, and method of adipose tissue treatment
WO2009120876A2 (en) * 2008-03-27 2009-10-01 The General Hospital Corporation Apparatus and method for surface cooling
US20110224656A1 (en) * 2008-04-03 2011-09-15 The General Hospital Corporation Method and apparatus for selective photothermolysis of veins
JP5628792B2 (en) 2008-04-25 2014-11-19 トリア ビューティ インコーポレイテッド Optical sensor and method for distinguishing skin presence and skin pigmentation
US20100017750A1 (en) 2008-07-16 2010-01-21 Avner Rosenberg User interface
US9314293B2 (en) 2008-07-16 2016-04-19 Syneron Medical Ltd RF electrode for aesthetic and body shaping devices and method of using same
AU2009294227B2 (en) 2008-09-21 2012-07-19 Syneron Medical Ltd. A method and apparatus for personal skin treatment
US8606366B2 (en) 2009-02-18 2013-12-10 Syneron Medical Ltd. Skin treatment apparatus for personal use and method for using same
JP2012518459A (en) 2009-02-25 2012-08-16 トランスファーマ メディカル リミテッド Electrical skin regeneration
PL210631B1 (en) * 2009-04-08 2012-02-29 Politechnika Swietokrzyska Device for increasing of effectiveness of application of laser power
WO2011001344A2 (en) * 2009-06-30 2011-01-06 Koninklijke Philips Electronics N.V. Light treatment system
FR2951283B1 (en) * 2009-10-08 2013-02-15 Commissariat Energie Atomique METHOD AND DEVICE FOR DIFFUSED EXCITATION IN IMAGING
AU2010325682B2 (en) 2009-12-06 2014-09-11 Gilead Bar - Ilan A method and apparatus for personal skin treatment
US9063299B2 (en) 2009-12-15 2015-06-23 Omni Guide, Inc. Two-part surgical waveguide
FR2954690A1 (en) * 2009-12-29 2011-07-01 Ekkyo DEVICE FOR DERMATOLOGICAL TREATMENT BY LIGHT BEAM
US9314301B2 (en) 2011-08-01 2016-04-19 Miramar Labs, Inc. Applicator and tissue interface module for dermatological device
US10195458B2 (en) 2011-09-08 2019-02-05 Johnson & Johnson Consumer Inc. Light therapy platform enhanced controller
US9789333B2 (en) 2011-09-08 2017-10-17 Johnson & Johnson Consumer Inc. Light therapy platform system
US10090694B2 (en) 2011-09-08 2018-10-02 Johnson & Johnson Consumer Inc. Light therapy platform mobile phone charger
US10022554B2 (en) 2013-03-15 2018-07-17 Johnson & Johnson Consumer Inc. Light therapy bandage system
US10434325B2 (en) 2011-09-08 2019-10-08 Johnson & Johnson Consumer Inc. Light therapy platform mobile device applications
US8771328B2 (en) 2011-09-08 2014-07-08 La Lumiere Llc Light therapy platform system
US10213618B2 (en) 2011-09-08 2019-02-26 Johnson & Johnson Consumer, Inc. Light therapy platform combination mask
US10092770B2 (en) 2011-09-08 2018-10-09 Johnson & Johnson Consumer Inc. Light therapy spot applicator
US10272257B2 (en) 2011-09-08 2019-04-30 Johnson & Johnson Consumer, Inc. Light therapy platform inductive mask and charger
ES2937663T3 (en) * 2012-07-26 2023-03-30 Donna J Brezinski portable phototherapy device
CN108378984B (en) * 2013-06-25 2020-06-26 Tec晶体有限责任公司 Device for phototherapy of the eye
WO2015013502A2 (en) 2013-07-24 2015-01-29 Miramar Labs, Inc. Apparatus and methods for the treatment of tissue using microwave energy
EP3237968A1 (en) * 2014-12-22 2017-11-01 Teclens, LLC Improved uv application device
US20190336788A1 (en) * 2016-12-28 2019-11-07 Sharp Kabushiki Kaisha Light radiator and light shielding member
US11103724B2 (en) 2017-01-04 2021-08-31 Arbor Grace, Inc. Photo-treatment device
US11497930B2 (en) * 2018-11-28 2022-11-15 Ag Ip Holding Llc Phototherapy device and system
US11517765B2 (en) * 2019-12-31 2022-12-06 L'oreal Hands-free skin treatment system

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3527932A (en) * 1967-11-16 1970-09-08 James J Thomas Transilluminating flashlight
US5108388A (en) * 1983-12-15 1992-04-28 Visx, Incorporated Laser surgery method
US5309339A (en) 1992-06-24 1994-05-03 The Schepens Eye Research Institute, Inc. Concentrator for laser light
US5380317A (en) * 1988-06-10 1995-01-10 Trimedyne Laser Systems, Inc. Medical device applying localized high intensity light and heat, particularly for destruction of the endometrium
US5505726A (en) * 1994-03-21 1996-04-09 Dusa Pharmaceuticals, Inc. Article of manufacture for the photodynamic therapy of dermal lesion
US5519534A (en) * 1994-05-25 1996-05-21 The Government Of The United States Of America As Represented By The Secretary Of The Department Of Health And Human Services Irradiance attachment for an optical fiber to provide a uniform level of illumination across a plane

Family Cites Families (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3602213A (en) * 1968-02-13 1971-08-31 Prototypes Inc Apparatus for photoelectric dermachromography
US3818914A (en) * 1972-04-17 1974-06-25 Spectroderm Inc Apparatus and method for treatment of skin disorders
GB1521585A (en) * 1975-09-09 1978-08-16 Perkin Elmer Corp Spectrophotometers
US4364033A (en) * 1979-10-31 1982-12-14 Tsay Yun Tyng Alarming seismometer
US4592726A (en) * 1983-01-03 1986-06-03 Herbert Brilliant Diagnostic mirror and light filter
ZA847338B (en) * 1983-09-19 1985-05-29 Amerace Corp Retroreflective sheeting and methods for making same
JPS6063039A (en) * 1983-09-19 1985-04-11 株式会社肌粧品科学開放研究所 Skin moisture measuring apparatus
JPH0137644Y2 (en) * 1985-07-10 1989-11-13
GB8816648D0 (en) * 1988-07-13 1988-08-17 Rowland A C Light delivery system
US5405368A (en) * 1992-10-20 1995-04-11 Esc Inc. Method and apparatus for therapeutic electromagnetic treatment
JP3027065B2 (en) * 1992-07-31 2000-03-27 日本電信電話株式会社 Display / imaging device

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3527932A (en) * 1967-11-16 1970-09-08 James J Thomas Transilluminating flashlight
US5108388A (en) * 1983-12-15 1992-04-28 Visx, Incorporated Laser surgery method
US5108388B1 (en) * 1983-12-15 2000-09-19 Visx Inc Laser surgery method
US5380317A (en) * 1988-06-10 1995-01-10 Trimedyne Laser Systems, Inc. Medical device applying localized high intensity light and heat, particularly for destruction of the endometrium
US5309339A (en) 1992-06-24 1994-05-03 The Schepens Eye Research Institute, Inc. Concentrator for laser light
US5505726A (en) * 1994-03-21 1996-04-09 Dusa Pharmaceuticals, Inc. Article of manufacture for the photodynamic therapy of dermal lesion
US5519534A (en) * 1994-05-25 1996-05-21 The Government Of The United States Of America As Represented By The Secretary Of The Department Of Health And Human Services Irradiance attachment for an optical fiber to provide a uniform level of illumination across a plane

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See also references of EP0955884A4 *

Cited By (23)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1566149A1 (en) * 1998-03-12 2005-08-24 Palomar Medical Technologies, Inc. System for electromagnetic radiation of the skin
WO1999046005A1 (en) * 1998-03-12 1999-09-16 Palomar Medical Technologies, Inc. System for electromagnetic radiation of the skin
EP1913972A1 (en) * 1999-09-20 2008-04-23 Susanne Johansson Laser probe for medical treatment
US8915948B2 (en) 2002-06-19 2014-12-23 Palomar Medical Technologies, Llc Method and apparatus for photothermal treatment of tissue at depth
US10556123B2 (en) 2002-06-19 2020-02-11 Palomar Medical Technologies, Llc Method and apparatus for treatment of cutaneous and subcutaneous conditions
US10500413B2 (en) 2002-06-19 2019-12-10 Palomar Medical Technologies, Llc Method and apparatus for treatment of cutaneous and subcutaneous conditions
US10434324B2 (en) 2005-04-22 2019-10-08 Cynosure, Llc Methods and systems for laser treatment using non-uniform output beam
US10849687B2 (en) 2006-08-02 2020-12-01 Cynosure, Llc Picosecond laser apparatus and methods for its operation and use
US9028536B2 (en) 2006-08-02 2015-05-12 Cynosure, Inc. Picosecond laser apparatus and methods for its operation and use
US11712299B2 (en) 2006-08-02 2023-08-01 Cynosure, LLC. Picosecond laser apparatus and methods for its operation and use
US10966785B2 (en) 2006-08-02 2021-04-06 Cynosure, Llc Picosecond laser apparatus and methods for its operation and use
US9919168B2 (en) 2009-07-23 2018-03-20 Palomar Medical Technologies, Inc. Method for improvement of cellulite appearance
US11095087B2 (en) 2012-04-18 2021-08-17 Cynosure, Llc Picosecond laser apparatus and methods for treating target tissues with same
US10581217B2 (en) 2012-04-18 2020-03-03 Cynosure, Llc Picosecond laser apparatus and methods for treating target tissues with same
US9780518B2 (en) 2012-04-18 2017-10-03 Cynosure, Inc. Picosecond laser apparatus and methods for treating target tissues with same
US11664637B2 (en) 2012-04-18 2023-05-30 Cynosure, Llc Picosecond laser apparatus and methods for treating target tissues with same
US10305244B2 (en) 2012-04-18 2019-05-28 Cynosure, Llc Picosecond laser apparatus and methods for treating target tissues with same
US10765478B2 (en) 2013-03-15 2020-09-08 Cynosurce, Llc Picosecond optical radiation systems and methods of use
US10245107B2 (en) 2013-03-15 2019-04-02 Cynosure, Inc. Picosecond optical radiation systems and methods of use
US10285757B2 (en) 2013-03-15 2019-05-14 Cynosure, Llc Picosecond optical radiation systems and methods of use
US11446086B2 (en) 2013-03-15 2022-09-20 Cynosure, Llc Picosecond optical radiation systems and methods of use
US11418000B2 (en) 2018-02-26 2022-08-16 Cynosure, Llc Q-switched cavity dumped sub-nanosecond laser
US11791603B2 (en) 2018-02-26 2023-10-17 Cynosure, LLC. Q-switched cavity dumped sub-nanosecond laser

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AU7662196A (en) 1997-04-30
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US5824023A (en) 1998-10-20
EP0955884A4 (en) 2001-02-07

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