Clemson University

Rutgers, the State University of New Jersey

University of Illinois

Other

US Government As Represented by the Secretary of the Army

Northrop Grumman Systems Corporation

University of Central Florida Research Foundation Inc

Board of Trustees of the Univ. of Illiniois—urbana

Clomson University

John Ballato

Stephen H Foulger

Dennis Smith

Hiren Shah

David W Carroll

Peter Danny Dragic

Richard E Riman

Richard Czerw

Earl Wagener

Robert R Rice

David Loren Carroll

Jeffrey R DiMaio

Arthur D Ballato

Michael Bass

Michael G Wickham

Hiroshi Komine

Martin C Richardson

Ahmad Safari

Joseph William Kolis

Amit Bandyopadhyay

Colin D McMillen

Ping Jiang

Stephen C Danforth

Andrey Mironov

Remco Van Weeren

Timothy McComb

J Matthew Mann

Vikas Sudesh

Travis W Baughman

Anthony Siegman

Matthew Tuggle

Courtney Kucera

Thomasina Zaengle

Baris Kukuoz

Ursula Gibson

Hacop Injeyan

Thomas W Hawkins

William Hagemann

Suresh Kumar Manthati

Amanda C Lattam

Maxime Cavillon

Disclosed are methods for formation of a fiber and fibers that can be formed according to the methods. Formation methods incorporate a 'molten core flux method' whereby a solid primary core material is combined with a solid secondary flux material in a multi-phase preform core. In some embodiments, the multi-phase preform core has a liquidus temperature that is reduced relative to the melting temperature of at least the primary core material. A homogeneous liquid melt of the preform core can exhibit a sufficiently low vapor pressure such that a fiber preform incorporating the materials in the core can be thermally drawn. Upon cooling and solidification of the homogeneous core melt, separation of the core components can occur via recrystallization, with one phase being that of the desired primary core material. Methods can be particularly beneficial for forming fibers incorporating high vapor pressure semiconductor materials, e.g., ZnSe or GaAs, in the fiber core.

Molten core flux formation method and fibers formed therefrom

A fiber includes a core and cladding, both of which may have temperature dependent indices of refraction. The materials and size of the core and cladding may be selected such that as the temperature of the core and/or cladding is heated above room temperature, the fiber transitions from supporting multimode optical waveguiding to supporting single mode waveguiding.

Optical fiber with low thermo-optic coefficient

A microheater comprises an optical fiber including a rare earth-doped glass core surrounded by a glass cladding. The rare earth-doped glass core comprises a rare earth dopant at a concentration sufficient for luminescence quenching such that, when the rare earth dopant is pumped with light at an absorption band wavelength, at least about 90% of absorbed pump light is converted into heat.

Microheater comprising a rare earth-doped optical fiber

A rare earth-doped optical fiber comprises a fluorosilicate core surrounded by a silica cladding, where the fluorosilicate core comprises an alkaline-earth fluoro-alumino-silicate glass, such as a strontium fluoro-alumino-silicate glass. The rare earth-doped optical fiber may be useful as a high-power fiber laser and/or fiber amplifier. A method of making a rare earth-doped optical fiber comprises: inserting a powder mixture comprising YbF, SrF, and AlOinto a silica tube; after inserting the powder mixture, heating the silica tube to a temperature of at least about 2000&#xb0; C., some or all of the powder mixture undergoing melting; drawing the silica tube to obtain a reduced-diameter fiber; and cooling the reduced-diameter fiber. Thus, a rare earth-doped optical fiber comprising a fluorosilicate core surrounded by a silica cladding is formed.

Rare earth-doped multicomponent fluorosilicate optical fiber for optical devices

Disclosed is an optical fiber formed from a preform that includes a clad component and a core component. The core component includes one or more precursor core materials. The precursor core materials and the clad materials are selected such that that the photoelastic constants of at least one precursor core material and the clad material are of opposite sign resulting in a final glass optical fiber of tailored Brillouin performance. The clad material may include an oxide glass having a positive photoelastic constant and the core component may include a precursor core material that has a negative photoelastic constant. During formation, the precursor core material can melt and interact with clad material that precipitates into the core to form a glass of at least one tailored Brillouin property, such as very low Brillouin gain.

Low brillouin scattering optical fibers and formation methods thereof

Disclosed is an optical fiber formed from a preform that includes a clad material and a core material. The clad material includes an oxide glass and the core material includes as a primary component a semiconductor material that melts at a temperature below where the cladding glass draws into fiber. In addition, the core material includes a scavenger for oxide precipitates that can precipitate into the core from the adjacent clad material during the fiber formation process. During formation, the scavenger reduces oxide precipitate to form the core primary component, or a phase compatible with it, and volatile products. The volatile products evolve out of the system. The primary material of the core can melt during the fiber formation process and crystallize upon cooling leaving the formed optical fiber with a crystalline core and little or no impurities due to precipitation of oxide into the core.

High purity crystalline core optical fibers and formation methods thereof

Disclosed are heterogeneous crystals for use in a laser cavity and methods of forming the crystals. A crystal can be a monolithic crystal containing regions that are based upon the same host material but differ from one another according to some material feature such that they can perform various functions related to lasing. Disclosed methods include hydrothermal growth techniques for the growth of differing epitaxial layers on a host. A host material can be doped in one region with a suitable active lasing ion and can be formed with another region that is undoped and can act as an endcap, a waveguide cladding layer, or a substrate to provide strength and/or contact to a heat sink. Regions can be formed with controlled thickness in conjunction. Following formation, a heterogeneous crystal can be cut, polished and coated with mirror films at each end for use in a laser cavity.

Hydrothermal growth of heterogeneous single crystals for solid state laser applications

One embodiment of the invention includes a method for forming an optical fiber. The method comprises providing a preform having a core material and a glass cladding material surrounding the core material. The method also comprises drawing the preform at a temperature that is greater than a melting temperature of the core material to form a drawn fiber. The method further comprises cooling the drawn fiber to form the optical fiber having a crystalline fiber core and a cladding that surrounds the crystalline fiber core and extends axially along a length of the crystalline fiber core.

Optical fiber systems and methods

The disclosure provides compositions prepared by combining nanomaterials with a halide-containing polymer, thereby forming a combined polymer matrix having dispersed nanomaterials within the matrix. The nanomaterials may be carbon-based nanotubes, in some applications. A halide-containing monomer is combined with nanotubes, and then polymerized in some compositions. In other applications, a halide-containing polymer is solution processed with nanotubes to form useful compositions in the invention. Also disclosed are probes for near field detection of radiation.

Halogen containing-polymer nanocomposite compositions, methods, and products employing such compositions

Optically transparent composite materials in which solid solution inorganic nanoparticles are dispersed in a host matrix inert thereto, wherein the nanoparticles are doped with one or more active ions at a level up to about 60 mole % and consist of particles having a dispersed particle size between about 1 and about 100 nm, and the composite material with the nanoparticles dispersed therein is optically transparent to wavelengths at which excitation, fluorescence or luminescence of the active ions occur. Luminescent devices incorporating the composite materials are also disclosed.

Optically transparent nanocomposite materials

Methods, systems and devices for a waveguide pumping gain guided index antiguided fiber laser having a fiber selected for a refractive index crossover at a wavelength between a pump wavelength and a laser emission wavelength. A waveguide pumping system pumps a light having a pump wavelength into the fiber allowing a laser light to be captured by a gain guided process in the core while the pump light, propagating in the cladding is coupled to the core. The fiber selection includes selecting a fiber with a cladding material having a refractive index less than a core material refractive index for a pump wavelength and a core refractive index at the laser emission wavelength is less than the cladding refractive index at the same laser emission wavelength to allow the pump light to propagate through the cladding as a conventional wave guided fiber laser, white the laser emission is captured within the core as an index antiguided, gain guided wave.

Waveguide-pumping gain guided index antiguided fiber laser

Recent theoretical investigations have predicted the existence of axially frozen modes that arise when light is incident upon an anisotropic two-dimensional photonic crystal. Such electromagnetic modes are of interest since they suggest a near-zero group velocity with extraordinary amplitudes. The present invention addresses the crystal physics associated with realizing such effects and provides for the development of materials suitable for use in the forming photonic crystals that can exhibit such effects.

Materials for freezing light

The present invention is directed to optical devices. More specifically, the disclosed devices include a film defining a periodic array of surface elements so as to give rise to surface plasmon polaritons. The film also includes at least a single aperture having a diameter less than the wavelength of light. In one embodiment, the surface elements can be an array of anisotropic apertures and the films can act as a polarizer. The disclosed devices can also include a material having a variable refractive index substantially adjacent to the metal film. For example, the refractive index of the adjacent material can vary according to some characteristic of the light incident to the device, for instance, the intensity or the angle of incidence of the light. In this embodiment, resonant coupling of incident light with the SPP, and hence transmittivity of the device, can depend upon the nature of incident light. The disclosed devices can be useful in, for example, remote polarizers, polarization mode dispersion, isolators, multi-color displays, switches, such as can be controlled according to incident sunlight, or optical filters, such as for eye protection devices, filtering out possibly harmful light.

Plasmon-photon coupled optical devices

Growing community of inventors

Clemson, SC, United States of America

John Ballato