Stanford University / SLAC National Accelerator Laboratory, USA and LMU Munich / Max Planck Institute of Quantum Optics, Germany

For contributions to the invention and fundamental principles of optical code-division multiple-access communication systems and of optical orthogonal codes

For outstanding technology and business leadership contributions to the industrial laser field and exemplary services to Optica and the photonics community

For outstanding and sustained contributions to the research and development of optical fiber based devices, particularly optical fiber grating technology

For sustained contributions towards the research and development of compound (III-V and II-VI) semiconductor-based optoelectronics

For the development of information-optimal imaging and sensing platforms across the electro­magnetic spectrum and service to the optics community

Circularlypolarized light

For outstanding and sustained contributions to the research and development of photonic glasses for lasing and sensing applications

For pioneering research and commercialisation in nonlinear optics and Bragg gratings, with applications in quantum science, sensors and optical fabrication

For outstanding contributions to ultrafast spectroscopy and pioneering ultralow cryogenic magneto-THz microscopy, unveiling significant light-matter quantum and coherent many-body phenomena

For groundbreaking scientific and technical leadership in metamaterial transition and in creating a paradigm shift in active denial technology

For pioneering research into high-dimensional quantum states of multimode optical fields and their use in quantum information science

For substantial contribution to the research and development of high-capacity optical switching and high-speed optical fiber transmission systems

For the development of optically biaxial and plasmonic colloidal liquid crystals, light-powered micro-motors, and light control by topologically nontrivial structures of optical axis

For outstanding contributions to nanophotonics and optomechanics, and to the understanding of photonic systems with broken spatiotemporal symmetries

For outstanding achievements in high-speed vertical-cavity surface-emitting lasers and pioneering work in optoelectronic integration with light-emitting transistors and transistor lasers

Linearly polarized light is a special case of elliptically polarized light.  If the light is linearly polarized, then the two components oscillate in phase,  for example Ex = E0xexp(i(kz - ωt)), Ey = E0yexp(i(kz - ωt)), φ = 0.  The direction of E and the direction of propagation define a plane.  The electric vector traces out a straight line.  For example, E = Ei = E0xexp(i(kz - ωt))i.

For pioneering contributions to the integration of optical imaging and artificial intelligence for biomedical applications and service to the optical community

For seminal contributions to field sampling at optical frequencies reaching attosecond temporal and nanometer spatial resolutions

For seminal and pioneering contributions in ultrafast laser plasma physics and the development of innovative applied spectroscopy technologies

The extraordinary ray violates both Snell’s Law and the Law of Reflection.  It is not necessarily confined to the plane of incidence.  Its speed changes with direction.  The index of refraction for the extraordinary ray is a continuous function of direction.  The index of refraction for the ordinary ray is independent of direction.  When the ordinary index of refraction is plotted against wavelength, the dispersion curve for the ordinary ray is a single unique curve.  The dispersion curve for the extraordinary ray is a family of curves with different curves for different directions.  A ray normally incident on a birefringent crystalline surface will be divided into two rays at the boundary, unless it is in a special polarization state or unless the crystalline surface is perpendicular to an optic axis.  The extraordinary ray will deviate from the incident direction while the ordinary ray will not.  The ordinary ray index n0 and the most extreme extraordinary ray index ne are together known as the principal indices of refraction of the material.  The direction of the lesser index is called the fast axis because light polarized in that direction has the higher speed.

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For significant contributions to the development of high-performance, reconfigurable all-dielectric metasurfaces and metadevices

For outstanding and sustained contributions to the research and development of quantum secure communication and fiber optic sensing

For the discovery of pseudo-dielectric heating, pioneering work on nanoparticle colloids in liquid crystals, and achievements in liquid-crystal photonic devices and bio-sensing

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For seminal contributions to nonlinear fiber optics and high-capacity optical communications, and for the pioneering invention of the all-optical regeneration method

For substantial contributions to the measurement of nonlinear optical coefficients and the design of devices from the room-temperature-bonding technique

For pioneering contributions to germanium-on-silicon integrated photonics and to erbium-in-silicon light-emitting devices

Electric polarization

When the sun is at a low angle in the sky, the sunlight reflecting off the surface of water is nearly 100% horizontally polarized because the angle of incidence is close to the Brewster angle.  Glare-reducing sunglasses are coated with a polarizer with a vertical transmission axis and therefore block the reflected light.

For significant contributions to broadband laser spectroscopy and applications to gas sensing, characterization of solids, and plasma diagnostics

For world-class scientific and engineering contributions in high-energy and high-peak-power laser systems, and key technical leadership at the National Ignition Facility

For exemplary volunteer leadership and outstanding contributions to silicon photonics research and technology including pioneering investigations in waveguide stress engineering

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For interdisciplinary work on integrated photonic-electronic systems including photonic deep neural networks for direct image classification and photonic-assisted microwave imaging

For leadership in biophotonics through technological advancement of nanosensitive and angiographic OCT technologies, and exceptional contributions to education and diversity and inclusion

Elliptical polarization

For pioneering contributions to nanophotonics and optical manipulation technologies, with wide-ranging applications in biology, health, energy, and information technology

For outstanding contributions to terahertz photonics, particularly terahertz metasurfaces, plasmonics, and manipulations

For significant contributions to 2D semiconductor opto­electronics, optical modulation spectroscopy, and optical properties of semiconductor materials and devices

For outstanding technical and program leadership in lasers and inertial confinement fusion in achieving fusion ignition in a laboratory setting

polarization中文

For outstanding contributions in leading research and development of integrated photonic products for optical communication

For pioneering contributions in the field of low-power optical information science and imaging, enabled by low-dimensional materials, nanophotonics, and meta-optics

For pioneering contributions to the research, development, and commercialization of zero-power wireless infrared sensors

For innovation and technological breakthroughs in photonic integrated circuits for applications in optical communication, microwave photonics, and optical computing

For outstanding advances in understanding retinal structure and function in individuals with inherited vision disorders through the application of non-invasive tools

Linear polarization example

For pioneering research in architectures and evolution strategies for optical access networks and long-standing leadership in the optical community

For more information, contact the Optica Awards Office (awards@optica.org; +1 202.416.1960) or visit optica.org/fellows.

For the development of optical SPPs nano-sensors/nano-biosensors and ultra-high resolution chemical imaging systems for biological and defense applications

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For pioneering and seminal contributions to non-Hermitian photonics, topological photonics, and nonlinear phenomena in laser physics

For outstanding support of optics worldwide through scientific publishing leadership and for extensively promoting the importance of photonics to society

Circular polarization

In other devices the changes in direction of propagation between the two rays is used to separate the incoming beam into two orthogonally polarized beams as in the Wollaston and Thompson beam-splitting prisms.

For outstanding contributions to the development of novel optoelectronic devices based on quantum-confined systems and photonic nanostructures

For outstanding and sustained contributions to nanophotonics research, particularly developing material platforms for tuning, switching, and programming of photonic devices

For pioneering contributions to the study of polarized light transport in biological media through experimental and computational approaches

For contributions to III-nitride semiconductor materials and optoelectronic devices, including material epitaxy and light emitting devices

For pioneering contributions to ultrafast and nonlinear effects in semiconductors and sustained global research in photonics and phononics

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For outstanding contributions in pioneering CARS imaging in medicine and high content microscopic screening for drug discovery and biological research

The figure below shows the trace of the field vector Ex = E0exp(i(kz - ωt)), Ey = E0exp(i(kz - ωt + φ)) in a plane perpendicular to the z-axis when looking towards the source.  (E0x = E0y = E0)

In the Glan-Taylor polarizing prism shown on the right the rejected (ordinary) ray is absorbed by black mounting material in the prism housing.

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For pioneering contributions to the physics and engineering of high-efficiency, high-power light-emitting-diode illumination sources

For outstanding achievements in the research and development of advanced microscale optoelectronic devices for energy and biomedical applications

For pioneering the application of tunable-laser spectroscopy to atmospheric measurements of Earth, Mars, Venus, and the outer planets

A half-wave plate δ = π can be used to rotate the plane of linearly polarized light.  The angle of rotation is 2θ, where θ is the angle between the angle of polarization and the wave plate's fast axis.

For pioneering contributions to optical switching and sensing systems utilizing micro-electro-mechanical system (MEMS) actuation principles and nanophotonics

For leadership in the photonics and quantum technology community and pioneering technical contributions in the area of narrow-linewidth lasers

For scientific advances in quantum confined semiconductors, micro-opto-mechanical systems, waveguides, integrated photonics, and their development for DOD applications

For pioneering advancements in parallel OCT imaging technologies and the development of non-invasive optogenetic pacing techniques in animal models

For significant achievements in integrated nonlinear quantum photonics from fundamentals to applications, and a deep commitment to education and mentorship

For seminal contributions to design methodologies for silicon photonics and to research on programmable photonic circuits

For pioneering contributions to nonlinear optical microscopy and imaging in biomedicine, materials science, and cultural heritage

The electric field vector E can always be resolved into two perpendicular components.  The light is elliptically polarized, then the two components have a constant phase difference, and the tip of the electric field vector traces out an ellipse in the plane perpendicular to the direction of propagation.

For contributions to silicon photonics integrated circuits including optical phased arrays, coherent lidar, and laser phase noise reduction

For pioneering work developing light field cameras, as well as seminal contributions in 3D view synthesis and human visual perception

For pioneering contributions, in terms of both original discoveries and knowledge dissemination, in the fields of plasmonics and metamaterials

For transformative and sustained contributions in photonic applications of nanomaterials and pioneering ultraminiaturised computational spectrometers

For innovative contributions to terahertz photonics including metasurfaces, antennas, and integrated platforms for sensing and communications

For significant contributions to 3D optical metrology, student training, and the advancement of science in Mexico and Latin America

For technical leadership at NRL in imaging through turbulence and scattering media, and for outstanding service to Optica

Congratulations to the 2024 class of Optica Fellow Members, who will be recognized throughout the year for scientific, engineering and technological contributions, as well as industry leadership and service to Optica and the global optics community.

A quarter-wave plate δ = π/2 can be used to convert linearly polarized light to circularly polarized light.  The incident linearly polarized light must be oriented at 45o to the wave plate's axes.  A half-wave plate δ = π can be used to rotate the plane of linearly polarized light.  The angle of rotation is 2θ, where θ is the angle between the angle of polarization and the wave plate's fast axis.

If a beam of linearly polarized monochromatic light enters a birefringent crystal along a direction not parallel to the optical axis of the crystal, the beam will may be divided into two separate beams.  Each will be polarized at right angles to the other, and they will travel in different directions.  The intensity of the original beam will be divided between the two new beams in a manner which depends on the original orientation of the electric field vector with respect to the crystal.  The ratio or the intensities of the two orthogonally polarized beams can have any value.

For pioneering mathematical and physical research to advance design methods for imaging and non-imaging optics, and industrial leadership in lighting

For advancements in precision optical metrology, namely the pioneering development and successful commercialization of novel substrate-transferred crystalline optical interference coatings

For outstanding contributions to ultrafast THz science and technology, particularly in developing high-energy THz sources and functional THz devices

For demonstrated quantum machine-learning, and the implementation of quantum noise reduction for the advanced gravitational wave detectors, and the development of quantum noise squeezing

For pioneering contributions to our understanding of the role of crystal anisotropy, phonons, and electron-phonon coupling for IR nanophotonics

For contributions to the fields of organic optoelectronics, particularly for innovative application of structures and materials into photovoltaic devices

For outstanding contributions to the field of ultrafast optics and spectroscopy, and for actively serving the optics community

For pioneering innovations in the technology and applications of large-aperture optics used for fusion and chirped-pulse-amplification lasers

For contributions to quantum information science and quantum optics, including fundamental tests of quantum phenomena and development of quantum networks

For pioneering contributions to strong-field and attosecond physics in condensed matter, including nonperturbative high-harmonic generation from band-insulators and quantum materials

Polarization

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For innovations in biomedical optics, including miniature microscopes for surgical guidance and non-destructive 3D pathology and analysis for clinical decision support

For research excellence and scientific leadership in atmospheric remote sensing using applied spectroscopy, as well as extensive contributions to professional service and public outreach

For seminal contributions to the ultra-high gain phototransistors and next-generation organic and perovskite photovoltaics

For pioneering and critical contributions to innovative fabrication techniques, interrogation methods, and applications of optical fiber sensors for harsh environments

For pioneering contributions to silicon photonics from science to technology deployment, and for global advocacy of engineering education enrichment

For establishing an international design, fabrication, and test ecosystem in silicon photonics, and developing high-performance and photonic integrated circuit components

For innovative leadership in tissue optical clearing imaging as well as serving the biomedical optics community and the society

For pioneering use of poly(trimethylene terephthalate) polymer in flexible nanofibers and cell-based living nano­probes in optical trapping and manipulation

Polarization oflight

For pioneering contributions to Brillouin slow light and Brillouin dynamic grating with significant impact on signal processing and sensing

For outstanding contributions to ultrafast optics including generation, characterization, and application of isolated attosecond pulses and few-cycle infrared pulses

For contributions to understanding quantum and coherent states in multifunctional materials and educating researchers from underrepresented groups in science

For foundational contributions to the all-digital control of structured light, and for outstanding service to the international optics community

The two beams within the birefringent crystal are referred to as the ordinary and extraordinary ray, respectively.  The polarization of the extraordinary ray lies in the plane containing the direction of propagation and the optic axis, and the polarization of the ordinary ray is perpendicular to this plane.

For outstanding and sustained contributions to nonlinear and ultrafast spectroscopy in condensed materials, nonlinear fiber optics, and optical communications

Congratulations to the 2024 class of Optica Fellow Members, who will be recognized throughout the year for scientific, engineering and technological contributions, as well as industry leadership and service to Optica and the global optics community.