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Dive into the research topics where T. R. Carter is active.

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Featured researches published by T. R. Carter.


Optics Letters | 2010

Demonstration of polarization-independent resonant subwavelength grating filter arrays

David W. Peters; R. R. Boye; Joel R. Wendt; Rick A. Kellogg; Shanalyn A. Kemme; T. R. Carter; Sally Samora

We demonstrate a two-dimensional (2D) polarization-independent resonant subwavelength grating (RSG) in a filter array. RSGs, also called guided mode resonant filters, are traditionally one-dimensional gratings; however, this leads to TE and TM resonances at different wavelengths and with different spectral shape. A 2D grating can remove the polarization dependence at normal incidence, while maintaining the desirable RSG properties of high reflectivity, narrow passband, and low sidebands without ripple. We designed and fabricated 2D gratings with near-identical responses for both polarizations at normal incidence in the telecommunication band. Ninety percent reflectivity is achieved at the resonant wavelengths.


Applied Physics B | 2011

Integration of fluorescence collection optics with a microfabricated surface electrode ion trap

G. R. Brady; A. R. Ellis; D. L. Moehring; D. Stick; Clark Highstrete; K. M. Fortier; Matthew Glenn Blain; Raymond A. Haltli; A. A. Cruz-Cabrera; Ronald D. Briggs; Joel R. Wendt; T. R. Carter; Sally Samora; Shanalyn A. Kemme

We have successfully demonstrated an integrated optical system for collecting the fluorescence from a trapped ion. The system, consisting of an array of transmissive, dielectric micro-optics and an optical fiber array, has been intimately incorporated into the ion-trapping chip without negatively impacting trapping performance. Epoxies, vacuum feedthrough, and optical component materials were carefully chosen so that they did not degrade the vacuum environment, and we have demonstrated light detection as well as ion trapping and shuttling behavior comparable to trapping chips without integrated optics, with no modification to the control voltages of the trapping chip.


Journal of Vacuum Science & Technology B | 1999

Fabrication of high performance microlenses for an integrated capillary channel electrochromatograph with fluorescence detection

Joel R. Wendt; Mial E. Warren; William C. Sweatt; Christopher G. Bailey; Carolyn M. Matzke; Don W. Arnold; Andrew A. Allerman; T. R. Carter; Randolph E. Asbill; Sally Samora

We describe the microfabrication of an extremely compact optical system as a key element in an integrated capillary channel electrochromatograph with fluorescence detection. The optical system consists of a vertical cavity surface-emitting laser (VCSEL), two high performance microlenses and a commercial photodetector. The microlenses are multilevel diffractive optics patterned by electron beam lithography and etched by reactive ion etching in fused silica. The design uses substrate-mode propagation within the fused silica substrate. Two generations of optical subsystems are described. The first generation design has a 6 mm optical length and is integrated directly onto the capillary channel-containing substrate. The second generation design separates the optical system onto its own substrate module and the optical path length is further compressed to 3.5 mm. The first generation design has been tested using direct fluorescence detection with a 750 nm VCSEL pumping a 10{sup {minus}4}M solution of CY-7 dye. The observed signal-to-noise ratio of better than 100:1 demonstrates that the background signal from scattered pump light is low despite the compact size of the optical system and is adequate for system sensitivity requirements.


Optics Express | 2016

Four-channel optically pumped atomic magnetometer for magnetoencephalography.

Anthony P. Colombo; T. R. Carter; Amir Borna; Yuan Yu Jau; Cort N. Johnson; Amber L. Dagel; Peter D. D. Schwindt

We have developed a four-channel optically pumped atomic magnetometer for magnetoencephalography (MEG) that incorporates a passive diffractive optical element (DOE). The DOE allows us to achieve a long, 18-mm gradiometer baseline in a compact footprint on the head. Using gradiometry, the sensitivities of the channels are < 5 fT/Hz1/2, and the 3-dB bandwidths are approximately 90 Hz, which are both sufficient to perform MEG. Additionally, the channels are highly uniform, which offers the possibility of employing standard MEG post-processing techniques. This module will serve as a building block of an array for magnetic source localization.


Journal of Micro-nanolithography Mems and Moems | 2006

Fabrication and measurement of wideband achromatic waveplates for the mid-infrared region using subwavelength features

R. R. Boye; Shanalyn A. Kemme; Joel R. Wendt; A. A. Cruz-Cabrera; Gregory A. Vawter; Charles Alford; T. R. Carter; Sally Samora

Subwavelength diffractive features etched into a substrate lead to form birefringence that can produce polarization sensitive elements such as wave plates. Using etched features allows for the development of pixelated devices to be used in conjunction with focal plane arrays in polarimetric imaging systems. Form birefringence exhibits dispersion that can be advantageous to the design of wave plates with an achromatic response. Taking advantage of this dispersion, diffractive wave plates with good achromatic characteristics can be designed for the 2- to 5-µm spectral region. Previous work in this area has produced good results over a subset of this wavelength band, but designing for this extended band is particularly challenging. The fabrication processes for the subwavelength features will be discussed and fabricated devices with a measured average phase retardation of 80.6 deg and rms variation of 9.41 deg will be presented.


Gradient Index, Miniature, and Diffractive Optical Systems III | 2003

Integration and tolerance issues for resonant subwavelength gratings

Shanalyn A. Kemme; David W. Peters; Joel R. Wendt; T. R. Carter; Sally Samora

A current micro-optical system project at Sandia National Laboratories employs an array of resonant subwavelength gratings (RSGs). An RSG functions as an extremely narrow wavelength and angular band reflector, or mode selector. Theoretical studies predict that the infinite, laterally-extended RSG can reflect 100% of the resonant light while transmitting the balance of the other wavelengths. Experimental realization of these remarkable predictions has been impacted primarily by fabrication challenges. Even so, we will present large area (1.0mm) RSG reflectivities as high as 100.2%, normalized to deposited gold. Broad use of the RSG will only truly occur in an accessible micro-optical system. The program at Sandia is a normal incidence array configuration of RSGs where each array element resonates with a distinct wavelength to act as a dense array of wavelength- and mode-selective reflectors. Because of the array configuration, RSGs can be matched to an array of pixels, detectors, or chemical/biological cells for integrated optical sensing. Micro-optical system considerations impact the ideal, large area RSG performance by requiring finite extent devices and robust materials for the appropriate wavelength. Experimental measurements are presented that demonstrate the component response as a function of decreasing RSG aperture dimension and off-normal input angular incidence.


Physics in Medicine and Biology | 2017

A 20-channel magnetoencephalography system based on optically pumped magnetometers

Amir Borna; T. R. Carter; Josh D Goldberg; Anthony P. Colombo; Yuan-Yu Jau; Christopher Berry; Jim McKay; Julia M. Stephen; Michael P. Weisend; Peter D. D. Schwindt

We describe a multichannel magnetoencephalography (MEG) system that uses optically pumped magnetometers (OPMs) to sense the magnetic fields of the human brain. The system consists of an array of 20 OPM channels conforming to the human subjects head, a person-sized magnetic shield containing the array and the human subject, a laser system to drive the OPM array, and various control and data acquisition systems. We conducted two MEG experiments: auditory evoked magnetic field and somatosensory evoked magnetic field, on three healthy male subjects, using both our OPM array and a 306-channel Elekta-Neuromag superconducting quantum interference device (SQUID) MEG system. The described OPM array measures the tangential components of the magnetic field as opposed to the radial component measured by most SQUID-based MEG systems. Herein, we compare the results of the OPM- and SQUID-based MEG systems on the auditory and somatosensory data recorded in the same individuals on both systems.


Journal of Micro-nanolithography Mems and Moems | 2008

Fabrication and testing of finite aperture polarizers for determination of edge termination effects on polarimetric imaging applications at midwave infrared

A. A. Cruz-Cabrera; Shanalyn A. Kemme; Joel R. Wendt; R. R. Boye; T. R. Carter; Sally Samora

Polarimetric imaging applications at the 2-to-5-µm or midwave infrared range use large pixel-count focal plane arrays (FPAs) with small pixel sizes. We report on the design, fabrication, and characterization of micropolarizers for the 2-to-5-µm regime. These micropolarizers will be used in conjunction with a FPA and will be in the near field of the imaging device. The pixel pitches for some commercial FPAs are small enough that the finite apertures of the polarizing devices may significantly affect their performance, because their aperture dimension varies between three and five waves. We are interested in understanding the effect on the extinction ratio due to variations in the edge terminations of a polarizer with a small aperture. Edge terminations are the spaces between the first and last wire with the perimeter of the aperture of the polarizer. To verify these effects, we fabricated micropolarizers with apertures of 5 to 20 µm and with termination edge spaces of one-quarter and three-quarters of the wiregrids period. The devices measured extinction ratios from 50:1 for the smallest aperture to 200:1 for the largest. Simulations and measurements show that the extinction ratio is larger for the smaller termination edge spacing.


SPIE 1999 Symposium on Micromachining and Microfabrication, Santa Clara, CA (US), 09/20/1999--09/22/1999 | 1999

Integrated Micro-Optical Fluorescence Detection System for Microfluidic Electrochromatography

Mial E. Warren; William C. Sweatt; Joel R. Wendt; Christopher A. Bailey; Carolyn M. Matzke; Don W. Arnold; Shanalyn A. Kemme; Andrew A. Allerman; T. R. Carter; Randolph E. Asbill; Sally Samora

We describe the design and microfabrication of an extremely compact optical system as a key element in an integrated capillary-channel electrochromatograph with laser induced fluorescence detection. The optical design uses substrate-mode propagation within the fused silica substrate. The optical system includes a vertical cavity surface-emitting laser (VCSEL) array, two high performance microlenses and a commercial photodetector. The microlenses are multilevel diffractive optics patterned by electron beam lithography and etched by reactive ion etching in fused silica. Two generations of optical subsystems are described. The first generation design is integrated directly onto the capillary channel-containing substrate with a 6 mm separation between the VCSEL and photodetector. The second generation design separates the optical system onto its own module and the source to detector length is further compressed to 3.5 mm. The systems are designed for indirect fluorescence detection using infrared dyes. The first generation design has been tested with a 750 nm VCSEL exciting a 10-4 M solution of CY-7 dye. The observed signal-to-noise ratio of better than 100:1 demonstrates that the background signal from scattered pump light is low despite the compact size of the optical system and meets the system sensitivity requirements.


Proceedings of SPIE | 2004

Inadvertent and intentional subwavelength surface texture on micro-optical components

Shanalyn A. Kemme; David W. Peters; T. R. Carter; Sally Samora; Douglas S. Ruby; Saleem H. Zaidi

We will discuss the fabrication of several diffractive optical elements (DOEs) for projects at Sandia National Laboratories, which highlight the relative importance of subwavelength surface texture in the componentsi’ performance. This surface texture is in addition to the larger, anisotropic DOE features that manipulate the propagating orders, and is commonly referred to as grass. Surface texture on amorphous or multi-crystalline material is readily apparent in a scanning electron micrograph and is often an unavoidable consequence of the reactive ion etch (RIE) process. Contributing factors are mask erosion, self-masking, and material non-uniformity. In this presentation, we describe and quantify the effects of unavoidable and deliberate surface texture through several projects in progress at Sandia National Laboratories.

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Joel R. Wendt

Sandia National Laboratories

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Sally Samora

Sandia National Laboratories

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Shanalyn A. Kemme

Sandia National Laboratories

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David W. Peters

Sandia National Laboratories

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A. A. Cruz-Cabrera

Sandia National Laboratories

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R. R. Boye

Sandia National Laboratories

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Ronald D. Briggs

Sandia National Laboratories

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Mial E. Warren

Sandia National Laboratories

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Peter D. D. Schwindt

National Institute of Standards and Technology

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William C. Sweatt

Sandia National Laboratories

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