Publications

Nanoletters

Sinclair, Michael B.; Peters, D.W.

Abstract not provided.

Kekatpure, Rohan D.; Peters, D.W.; Shaner, Eric A.

Abstract not provided.

Ginn, James C.; Clem, Paul G.; Sinclair, Michael B.; Peters, D.W.; Wendt, J.R.; Stevens, Jeffrey S.; Hines, Paul H.; Brener, Igal B.; Basilio, Lorena I.; Warne, Larry K.; Ihlefeld, Jon I.

Abstract not provided.

Science

Ginn, James C.; Clem, Paul G.; Sinclair, Michael B.; Peters, D.W.; Wendt, J.R.; Stevens, Jeffrey S.; Hines, Paul H.; Brener, Igal B.; Basilio, Lorena I.; Warne, Larry K.; Ihlefeld, Jon I.

Abstract not provided.

Passmore, Brandon S.; Wendt, J.R.; Peters, D.W.; Brener, Igal B.; Sinclair, Michael B.; Shaner, Eric A.; Ten Eyck, Gregory A.

Abstract not provided.

Ginn, James C.; Ten Eyck, Gregory A.; Brener, Igal B.; Peters, D.W.; Sinclair, Michael B.

Dielectric resonators are an effective means to realize isotropic, low-loss optical metamaterials. As proof of this concept, a cubic resonator is analytically designed and then tested in the long-wave infrared.

Proceedings of SPIE - The International Society for Optical Engineering

Gin, A.V.; Kemme, S.A.; Boye, Robert B.; Peters, D.W.; Ihlefeld, Jon I.; Briggs, R.D.; Wendt, J.R.; Ellis, A.R.; Marshall, L.H.; Carter, T.R.; Hunker, J.D.; Samora, S.

In this work, we describe the most recent progress towards the device modeling, fabrication, testing and system integration of active resonant subwavelength grating (RSG) devices. Passive RSG devices have been a subject of interest in subwavelength-structured surfaces (SWS) in recent years due to their narrow spectral response and high quality filtering performance. Modulating the bias voltage of interdigitated metal electrodes over an electrooptic thin film material enables the RSG components to act as actively tunable high-speed optical filters. The filter characteristics of the device can be engineered using the geometry of the device grating and underlying materials. Using electron beam lithography and specialized etch techniques, we have fabricated interdigitated metal electrodes on an insulating layer and BaTiO3 thin film on sapphire substrate. With bias voltages of up to 100V, spectral red shifts of several nanometers are measured, as well as significant changes in the reflected and transmitted signal intensities around the 1.55um wavelength. Due to their small size and lack of moving parts, these devices are attractive for high speed spectral sensing applications. We will discuss the most recent device testing results as well as comment on the system integration aspects of this project. © 2010 Copyright SPIE - The International Society for Optical Engineering.

Ginn, James C.; Ten Eyck, Gregory A.; Brener, Igal B.; Peters, D.W.; Sinclair, Michael B.

Abstract not provided.

Cruz-Cabrera, A.A.; Kemme, S.A.; Cich, Michael C.; Ellis, A.R.; Wendt, J.R.; Rowen, Adam M.; Martinez, Marino M.; Scrymgeour, David S.; Peters, D.W.

Abstract not provided.

Lentine, Anthony L.; Nielson, Gregory N.; Wright, Jeremy B.; Peters, D.W.; Zortman, William A.; McCormick, Frederick B.

The advent of high quality factor (Q) microphotonic-resonators has led to the demonstration of high-fidelity optical sensors of many physical phenomena (e.g. mechanical, chemical, and biological sensing) often with far better sensitivity than traditional techniques. Microphotonic-resonators also offer potential advantages as uncooled thermal detectors including significantly better noise performance, smaller pixel size, and faster response times than current thermal detectors. In particular, microphotonic thermal detectors do not suffer from Johnson noise in the sensor, offer far greater responsivity, and greater thermal isolation as they do not require metallic leads to the sensing element. Such advantages make the prospect of a microphotonic thermal imager highly attractive. Here, we introduce the microphotonic thermal detection technique, present the theoretical basis for the approach, discuss our progress on the development of this technology and consider future directions for thermal microphotonic imaging. Already we have demonstrated viability of device fabrication with the successful demonstration of a 20{micro}m pixel, and a scalable readout technique. Further, to date, we have achieved internal noise performance (NEP{sub Internal} < 1pW/{radical}Hz) in a 20{micro}m pixel thereby exceeding the noise performance of the best microbolometers while simultaneously demonstrating a thermal time constant ({tau} = 2ms) that is five times faster. In all, this results in an internal detectivity of D*{sub internal} = 2 x 10{sup 9}cm {center_dot} {radical}Hz/W, while roughly a factor of four better than the best uncooled commercial microbolometers, future demonstrations should enable another order of magnitude in sensitivity. While much work remains to achieve the level of maturity required for a deployable technology, already, microphotonic thermal detection has demonstrated considerable potential.

Basilio, Lorena I.; Johnson, William Arthur.; Warne, Larry K.; Langston, William L.; Peters, D.W.; Sinclair, Michael B.

Abstract not provided.

Peters, D.W.; Gin, Aaron G.; Kemme, S.A.; Ihlefeld, Jon I.; Briggs, R.D.; Wendt, J.R.

Abstract not provided.

Nielson, Gregory N.; Rakich, Peter T.; Zortman, William A.; Wright, Jeremy B.; Peters, D.W.; McCormick, Frederick B.

Abstract not provided.

Nano Letters

Peters, D.W.; McKenzie, Bonnie B.; Hsu, Julia W.

Abstract not provided.

Proceedings of SPIE - The International Society for Optical Engineering

Kemme, S.A.; Cruz-Cabrera, A.A.; Peters, D.W.; Ellis, A.R.; Carter, T.R.; Samora, S.

We present simulations and measurements of a technology that can manipulate thermal angular and wavelength emission. This work is representative of Sandia National Laboratories' efforts to investigate advanced technologies that are not currently accessible for reasons such as risk, cost, or limited availability. The goal of this project is to demonstrate a passive thermal emission management surface that can tailor the direction of emission as well as the wavelength bands of emission. This new proposed technology enables thermal emission pattern management by structuring the surface. This structuring may be in either the lateral or depth dimension. A lateral structuring consists of a shallow grating on a metal surface. This air/metal interface allows photon/plasmon coupling, which has been shown to coherently and preferentially emit at certain wavelengths.

Lentine, Anthony L.; McCormick, Frederick B.; Peters, D.W.; Nielson, Gregory N.

Abstract not provided.

Ruby, Douglas S.; Peters, D.W.; McKenzie, Bonnie B.; Hsu, Julia W.

Abstract not provided.

Kemme, S.A.; Cruz-Cabrera, A.A.; Peters, D.W.

Abstract not provided.

Cruz-Cabrera, A.A.; Peters, D.W.

Abstract not provided.

Proceedings of SPIE - The International Society for Optical Engineering

Kemme, S.A.; Boye, Robert B.; Peters, D.W.; Nellums, Robert N.

We present the design and initial fabrication for a wavelength-agile, high-speed modulator that enables a long-term vision for the THz Scannerless Range Imaging (SRI) sensor. This modulator takes the place of the currently utilized SRI micro-channel plate which is limited to photocathode sensitive wavelengths (primarily in the visible and near-IR regimes). The new component is an active Resonant Subwavelength Grating (RSG). 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. Previous experimental realization of these remarkable predictions has been impacted primarily by fabrication challenges. Even so, we have demonstrated large-area (1.0mm) passive RSG reflectivity as high as 100.2%, normalized to deposited gold. In this work, we transform the passive RSG design into an active laser-line modulator.

Sweatt, W.C.; Verley, Jason V.; Luk, Ting S.; El-Kady, I.; Peters, D.W.; McCormick, Frederick B.

Abstract not provided.

Subramania, Ganapathi S.; Sweatt, W.C.; El-Kady, I.; Peters, D.W.; Verley, Jason V.; Williams, John D.; McCormick, Frederick B.; Luk, Ting S.

Abstract not provided.

Peters, D.W.; Loui, Hung L.

Abstract not provided.

Proceedings of SPIE - The International Society for Optical Engineering

Williams, John D.; Arrington, C.; Sweatt, W.C.; Peters, D.W.; El-Kady, I.; Ellis, A.R.; Verley, Jason V.; McCormick, Frederick B.

The LIGA microfabrication technique offers a unique method for fabricating 3-dimensional photonic lattices based on the Iowa State "logpile" structure. These structures represent the [111] orientation of the [100] logpile structures previously demonstrated by Sandia National Laboratories, The novelty to this approach is the single step process that does not require any alignment. The mask and substrate are fixed to one another and exposed twice from different angles using a synchrotron light source. The first exposure patterns the resist at an angle of 45 degrees normal to the substrate with a rotation of 8 degrees. The second exposure requires a 180 degree rotation about the normal of the mask and substrate. The resulting pattern is a vertically oriented logpile pattern that is rotated slightly off axis. The exposed PMMA is developed in a single step to produce an inverse lattice structure. This mold is filled with electroplated gold and stripped away to create a usable gold photonic crystal. Tilted logpiles demonstrate band characteristics very similar to those observed from [100] logpiles. Reflectivity tests show a band edge around 5 μm and compare well with numerical simulations.

Kemme, S.A.; Peters, D.W.; Boye, Robert B.; Nellums, Robert N.

In this late-start LDRD, we will present a design for a wavelength-agile, high-speed modulator that enables a long-term vision for the THz Scannerless Range Imaging (SRI) sensor. It takes the place of the currently-utilized SRI micro-channel plate which is limited to photocathode sensitive wavelengths (primarily in the visible and near-IR regimes). Two of Sandia's successful technologies--subwavelength diffractive optics and THz sources and detectors--are poised to extend the capabilities of the SRI sensor. The goal is to drastically broaden the SRI's sensing waveband--all the way to the THz regime--so the sensor can see through image-obscuring, scattering environments like smoke and dust. Surface properties, such as reflectivity, emissivity, and scattering roughness, vary greatly with the illuminating wavelength. Thus, objects that are difficult to image at the SRI sensor's present near-IR wavelengths may be imaged more easily at the considerably longer THz wavelengths (0.1 to 1mm). The proposed component is an active Resonant Subwavelength Grating (RSG). Sandia invested considerable effort on a passive RSG two years ago, which resulted in a highly-efficient (reflectivity greater than gold), wavelength-specific reflector. For this late-start LDRD proposal, we will transform the passive RSG design into an active laser-line reflector.