3,210 research outputs found

    NASA/ESACV-990 spacelab simulation. Appendix B: Experiment development and performance

    Get PDF
    Eight experiments flown on the CV-990 airborne laboratory during the NASA/ESA joint Spacelab simulation mission are described in terms of their physical arrangement in the aircraft, their scientific objectives, developmental considerations dictated by mission requirements, checkout, integration into the aircraft, and the inflight operation and performance of the experiments

    Focus 3D: Compressive Accommodation Display

    Get PDF
    We present a glasses-free 3D display design with the potential to provide viewers with nearly correct accommodative depth cues, as well as motion parallax and binocular cues. Building on multilayer attenuator and directional backlight architectures, the proposed design achieves the high angular resolution needed for accommodation by placing spatial light modulators about a large lens: one conjugate to the viewer's eye, and one or more near the plane of the lens. Nonnegative tensor factorization is used to compress a high angular resolution light field into a set of masks that can be displayed on a pair of commodity LCD panels. By constraining the tensor factorization to preserve only those light rays seen by the viewer, we effectively steer narrow high-resolution viewing cones into the user's eyes, allowing binocular disparity, motion parallax, and the potential for nearly correct accommodation over a wide field of view. We verify the design experimentally by focusing a camera at different depths about a prototype display, establish formal upper bounds on the design's accommodation range and diffraction-limited performance, and discuss practical limitations that must be overcome to allow the device to be used with human observers

    Physical properties of ESA Rosetta target asteroid (21) Lutetia: Shape and flyby geometry

    Full text link
    Aims. We determine the physical properties (spin state and shape) of asteroid (21) Lutetia, target of the ESA Rosetta mission, to help in preparing for observations during the flyby on 2010 July 10 by predicting the orientation of Lutetia as seen from Rosetta. Methods. We use our novel KOALA inversion algorithm to determine the physical properties of asteroids from a combination of optical lightcurves, disk-resolved images, and stellar occultations, although the latter are not available for (21) Lutetia. Results. We find the spin axis of (21) Lutetia to lie within 5 degrees of ({\lambda} = 52 deg., {\beta} = -6 deg.) in Ecliptic J2000 reference frame (equatorial {\alpha} = 52 deg., {\delta} = +12 deg.), and determine an improved sidereal period of 8.168 270 \pm 0.000 001 h. This pole solution implies the southern hemisphere of Lutetia will be in "seasonal" shadow at the time of the flyby. The apparent cross-section of Lutetia is triangular as seen "pole-on" and more rectangular as seen "equator-on". The best-fit model suggests the presence of several concavities. The largest of these is close to the north pole and may be associated with large impacts.Comment: 17 pages, 5 figures, 3 tables, submitted to Astronomy and Astrophysic

    Optical and Terahertz Energy Concentration on the Nanoscale in Plasmonics

    Get PDF
    We introduce an approach to implement full coherent control on nanometer length scales. It is based on spatiotemporal modulation of the surface plasmon polariton (SPP) fields at the thick edge of a nanowedge. The SPP wavepackets propagating toward the sharp edge of this nanowedge are compressed and adiabatically concentrated at a nanofocus, forming an ultrashort pulse of local fields. The profile of the focused waveform as a function of time and one spatial dimension is completely coherently controlled. We establish the principal limits for the nanoconcentration of the terahertz (THz) radiation in metal/dielectric waveguides and determine their optimum shapes required for this nanoconcentration. We predict that the adiabatic compression of THz radiation from the initial spot size of vacuum wavelength ~300 ΞΌm to the unprecedented final size of 100-250 nm can be achieved, while the THz radiation intensity is increased by a factor of 10 to 250. This THz energy nanoconcentration will not only improve the spatial resolution and increase the signal/noise ratio for THz imaging and spectroscopy, but in combination with the recently developed sources of powerful THz pulses, will allow the observation of nonlinear THz effects and a variety of nonlinear spectroscopies (such as two-dimensional spectroscopy), which are highly informative. This should find a wide spectrum of applications in science, engineering, biomedical research and environmental monitoring. We also develop a theory of the spoof plasmons propagating at the interface between a dielectric and a real conductor. The deviation from a perfect conductor is introduced through a finite skin depth. The possibilities of guiding and focusing of spoof plasmons are considered. Geometrical parameters of the structure are found which provide a good guiding of such modes. Moreover, the limit on the concentration by means of planar spoof plasmons in case of non-ideal metal is established. These properties of spoof plasmons are of great interest for THz technology

    A Low Temperature Nonlinear Optical Rotational Anisotropy Spectrometer for the Determination of Crystallographic and Electronic Symmetries

    Get PDF
    Nonlinear optical generation from a crystalline material can reveal the symmetries of both its lattice structure and underlying ordered electronic phases and can therefore be exploited as a complementary technique to diffraction based scattering probes. Although this technique has been successfully used to study the lattice and magnetic structures of systems such as semiconductor surfaces, multiferroic crystals, magnetic thin films and multilayers, challenging technical requirements have prevented its application to the plethora of complex electronic phases found in strongly correlated electron systems. These requirements include an ability to probe small bulk single crystals at the micron length scale, a need for sensitivity to the entire nonlinear optical susceptibility tensor, oblique light incidence reflection geometry and incident light frequency tunability among others. These measurements are further complicated by the need for extreme sample environments such as ultra low temperatures, high magnetic fields or high pressures. In this review we present a novel experimental construction using a rotating light scattering plane that meets all the aforementioned requirements. We demonstrate the efficacy of our scheme by making symmetry measurements on a micron scale facet of a small bulk single crystal of Sr2_2IrO4_4 using optical second and third harmonic generation.Comment: 8 pages, 5 figure

    Dynamics of the solar chromosphere. V. High-frequency modulation in ultraviolet image sequences from TRACE

    Full text link
    We search for signatures of high-frequency oscillations in the upper solar photosphere and low chromosphere in the context of acoustic heating of outer stellar atmospheres. We use ultraviolet image sequences of a quiet center-disk area from the Transition Region and Coronal Explorer (TRACE) mission which were taken with strict cadence regularity. The latter permits more reliable high-frequency diagnosis than in earlier work. Spatial Fourier power maps, spatially averaged coherence and phase-difference spectra, and spatio-temporal k-f decompositions all contain high-frequency features that at first sight seem of considerable intrinsic interest but actually are more likely to represent artifacts of different nature. Spatially averaged phase difference measurement provides the most sensitive diagnostic and indicates the presence of acoustic modulation up to f=20 mHz (periods down to 50 seconds) in internetwork areas.Comment: 9 pages, 8 figure

    νŽΈκ΄‘ 닀쀑화λ₯Ό μ΄μš©ν•˜μ—¬ ν–₯μƒλœ κΈ°λŠ₯을 μ œκ³΅ν•˜λŠ” λ„νŒŒκ΄€ 기반의 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄

    Get PDF
    ν•™μœ„λ…Όλ¬Έ (박사) -- μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› : κ³΅κ³ΌλŒ€ν•™ 전기·정보곡학뢀, 2021. 2. μ΄λ³‘ν˜Έ.This dissertation presents the studies on the optical design method that enhances the display performance of see-through waveguide-based near-eye displays (WNEDs) using the polarization multiplexing technique. The studies focus on the strategies to improve the crucial display performances without compromising a small form factor, the most attractive merit of the WNEDs. To achieve this goal, thin and lightweight polarization-dependent optical elements are devised and employed in the WNED structure. The polarization-dependent devices can allow multiple optical functions or optical paths depending on the polarization state of the input beam, which can break through the limitation of the waveguide system with the polarization multiplexing. To realize the function-selective eyepiece for AR applications, the proposed devices should operate as an optically transparent window for the real scene while performing specific optical functions for the virtual image. The proposed devices are manufactured in a combination structure in which polarization-dependent optical elements are stacked. The total thickness of the stacked structure is about 1 mm, and it can be attached to the waveguide surface without conspicuously increasing the form factor of the optical system. Using the proposed polarization-dependent devices, the author proposes three types of novel WNED systems with enhanced performance. First, the author suggests a compact WNED with dual focal planes. Conventional WNEDs have an inherent limitation that the focal plane of the virtual image is at an infinite distance because they extract a stream of collimated light at the out-coupler. By using the polarization-dependent eyepiece lens, an additional focal plane can be generated with the polarization multiplexing in addition to infinity depth. The proposed configuration can provide comfortable AR environments by alleviating visual fatigue caused by vergence-accommodation conflict. Second, the novel WNED configuration with extended field-of-view (FOV) is presented. In the WNEDs, the maximum allowable FOV is determined by the material properties of the diffraction optics and the substrate. By using the polarization-dependent steering combiner, the FOV can be extended up to two times, which can provide more immersive AR experiences. In addition, this dissertation demonstrates that the distortion for the real scene caused by the stacked structure cannot severely disturb the image quality, considering the acuity of human vision. Lastly, the author presents a retinal projection-based WNED with switchable viewpoints by simultaneously adopting the polarization-dependent lens and grating. The proposed system can convert the viewpoint according to the position of the eye pupil without mechanical movement. The polarization-dependent viewpoint switching can resolve the inherent problem of a narrow eyebox in retinal projection displays without employing the bulky optics for mechanical movement. In conclusion, the dissertation presents the practical optical design and detailed analysis for enhanced WNED based on the polarization multiplexing technique through various simulations and experiments. The proposed approaches are expected to be utilized as an innovative solution for compact wearable displays.λ³Έ λ°•μ‚¬ν•™μœ„ λ…Όλ¬Έμ—μ„œλŠ” νŽΈκ΄‘ 닀쀑화 기법을 μ΄μš©ν•˜μ—¬ λ„νŒŒκ΄€ 기반의 μ¦κ°•ν˜„μ‹€ κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄μ˜ μ„±λŠ₯을 ν–₯μƒμ‹œν‚€λŠ” κ΄‘ν•™ 섀계 및 이에 λŒ€ν•œ 뢄석에 λŒ€ν•΄ λ…Όμ˜ν•œλ‹€. λ³Έ μ—°κ΅¬λŠ” λ„νŒŒκ΄€ 기반 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄μ˜ κ°€μž₯ 큰 μž₯점인 μ†Œν˜• 폼 νŒ©ν„°λ₯Ό μœ μ§€ν•˜λ©΄μ„œ λ””μŠ€ν”Œλ ˆμ΄ μ„±λŠ₯을 κ°œμ„ ν•˜λŠ” 것에 쀑점을 λ‘”λ‹€. 이λ₯Ό μœ„ν•΄ κΈ°μ‘΄ κ΄‘ν•™ μ†Œμžμ— λΉ„ν•΄ 맀우 가볍고 얇은 νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμžκ°€ μƒˆλ‘­κ²Œ μ œμ•ˆλ˜λ©°, μ΄λŠ” μž…μ‚¬κ΄‘μ˜ νŽΈκ΄‘ μƒνƒœμ— 따라 독립적인 κ΄‘ 경둜 μ œμ–΄λ₯Ό κ°€λŠ₯μΌ€ ν•˜μ—¬ νŽΈκ΄‘ 닀쀑화λ₯Ό 톡해 ν–₯μƒλœ μ„±λŠ₯을 제곡 ν•  수 μžˆλ‹€. λ˜ν•œ μ‹€μ œ μ˜μƒμ˜ 빛은 κ·ΈλŒ€λ‘œ 투과 μ‹œν‚΄μœΌλ‘œμ¨ μ¦κ°•ν˜„μ‹€μ„ μœ„ν•œ μ†Œμžλ‘œ ν™œμš© κ°€λŠ₯ν•˜λ‹€. λ³Έ μ—°κ΅¬μ—μ„œ μ œμ•ˆν•˜λŠ” νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° κ΄‘ν•™ μ†ŒμžλŠ” κΈ°ν•˜ν•™μ  μœ„μƒ(geometric phase, GP)에 κΈ°λ°˜ν•˜μ—¬ λ™μž‘ν•œλ‹€. GP 기반의 κ΄‘ν•™μ†Œμžκ°€ μ„œλ‘œ μ§κ΅ν•˜λŠ” μ›ν˜• νŽΈκ΄‘ μž…μ‚¬κ΄‘μ— λŒ€ν•΄ 상보적인 κΈ°λŠ₯을 μˆ˜ν–‰ν•˜λŠ” 것을 μ΄μš©ν•˜μ—¬, 두 개 μ΄μƒμ˜ GP μ†Œμžμ™€ νŽΈκ΄‘ μ œμ–΄λ₯Ό μœ„ν•œ κ΄‘ν•™ 필름듀을 쀑첩 μ‹œν‚΄μœΌλ‘œμ¨ μ¦κ°•ν˜„μ‹€ κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμžλ₯Ό κ΅¬ν˜„ν•  수 μžˆλ‹€. 이듀 κ΄‘ν•™μ†ŒμžλŠ” 맀우 μ–‡κΈ° λ•Œλ¬Έμ—, λ³Έ μ—°κ΅¬μ—μ„œ μ œμž‘λœ νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμžμ˜ 총 λ‘κ»˜λŠ” 1 mm μˆ˜μ€€μœΌλ‘œ 폼 νŒ©ν„° μ œμ•½μœΌλ‘œλΆ€ν„° μžμœ λ‘­λ‹€. λ˜ν•œ ν‰ν‰ν•œ 필름 ν˜•νƒœμ΄λ―€λ‘œ, ν‰νŒν˜• λ„νŒŒκ΄€μ— λΆ€μ°©ν•˜κΈ° μ‰½λ‹€λŠ” 이점을 μ§€λ‹Œλ‹€. κ³ μ•ˆλœ νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμžλ₯Ό μ‚¬μš©ν•˜μ—¬ μ„Έ 가지 μœ ν˜•μ˜ μƒˆλ‘œμš΄ λ„νŒŒκ΄€ 기반의 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄ ꡬ쑰λ₯Ό μ œμ•ˆν•œλ‹€. 첫 λ²ˆμ§ΈλŠ” μž…μ‚¬κ΄‘μ˜ νŽΈκ΄‘ μƒνƒœμ— 따라 투λͺ… κ΄‘ν•™ μ°½ λ˜λŠ” 였λͺ© 렌즈둜 μž‘λ™ν•˜λŠ” νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° 렌즈λ₯Ό μ μš©ν•˜μ—¬ 가상 μ˜μƒμ— λŒ€ν•΄ 이쀑 μ΄ˆμ λ©΄μ„ μ œκ³΅ν•˜λŠ” μ‹œμŠ€ν…œμ΄λ‹€. μ œμ•ˆλœ κ΅¬μ‘°λŠ” 기쑴의 λ„νŒŒκ΄€ 기반 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄κ°€ λ¬΄ν•œλŒ€ μœ„μΉ˜μ— 단일 μ΄ˆμ λ©΄μ„ μ œκ³΅ν•¨μœΌλ‘œμ¨ λ°œμƒν•˜λŠ” μ‹œκ°μ  ν”Όλ‘œ 및 νλ¦Ών•œ μ¦κ°•ν˜„μ‹€ μ˜μƒμ˜ 문제λ₯Ό μ™„ν™”ν•  수 μžˆλ‹€. 두 λ²ˆμ§Έλ‘œλŠ” μž…μ‚¬κ΄‘μ˜ νŽΈκ΄‘ μƒνƒœμ— 따라 κ΄‘ 경둜λ₯Ό 쒌츑 λ˜λŠ” 우츑으둜 μ œμ–΄ν•  수 μžˆλŠ” νŽΈκ΄‘ 격자λ₯Ό ν™œμš©ν•˜μ—¬ 가상 μ˜μƒμ˜ μ‹œμ•Όκ°μ„ 기쑴보닀 μ΅œλŒ€ 2λ°°κΉŒμ§€ ν™•μž₯ν•  수 μžˆλŠ” μ‹œμŠ€ν…œμ„ μ œμ•ˆν•œλ‹€. μ΄λŠ” 단일 λ„νŒŒκ΄€ 기반 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄μ—μ„œ μ˜μƒ κ²°ν•©κΈ° (imaging combiner)둜 ν™œμš©λ˜λŠ” 회절 μ†Œμžμ˜ 섀계 λ³€μˆ˜μ— μ˜ν•΄ μ œν•œλ˜λŠ” μ‹œμ•Όκ° ν•œκ³„μ μ„ λŒνŒŒν•  수 μžˆλŠ” ꡬ쑰둜 μ»΄νŒ©νŠΈν•œ 폼 νŒ©ν„°λ‘œ λ”μš± λͺ°μž…감 μžˆλŠ” λŒ€ν™”λ©΄ μ¦κ°•ν˜„μ‹€ μ˜μƒμ„ μ œκ³΅ν•  수 μžˆλ‹€. λ§ˆμ§€λ§‰μœΌλ‘œ μœ„μ—μ„œ μ œμ•ˆλœ 두 가지 νŽΈκ΄‘ μ˜μ‘΄ν˜• κ΄‘ν•™ μ†Œμžλ₯Ό λͺ¨λ‘ μ‚¬μš©ν•˜μ—¬ μ‹œμ  μ „ν™˜μ΄ κ°€λŠ₯ν•œ λ„νŒŒκ΄€ 기반의 망막 νˆ¬μ‚¬ν˜• λ””μŠ€ν”Œλ ˆμ΄ ꡬ쑰λ₯Ό μ œμ•ˆν•œλ‹€. νŽΈκ΄‘ 닀쀑화λ₯Ό 톡해 닀쀑 μ΄ˆμ λ“€μ„ μ„ νƒμ μœΌλ‘œ ν™œμ„±ν™”ν•¨μœΌλ‘œμ¨, ν™•μž₯된 μ‹œμ²­μ˜μ—­μ„ μ œκ³΅ν•˜λŠ” λ™μ‹œμ— 동곡 크기 λ³€ν™” λ˜λŠ” μ›€μ§μž„μ— μ˜ν•œ 이쀑 μ˜μƒ 문제λ₯Ό μ™„ν™”ν•  수 μžˆλ‹€. λ˜ν•œ 기계적 μ›€μ§μž„ 없이 μ‹œμ  κ°„μ˜ 고속 μ „ν™˜μ΄ κ°€λŠ₯ν•˜λ‹€λŠ” μž₯점을 μ§€λ‹ˆκ³  μžˆλ‹€. λ³Έ λ°•μ‚¬ν•™μœ„ λ…Όλ¬Έμ—μ„œ μ œμ‹œν•œ νŽΈκ΄‘ 닀쀑화λ₯Ό ν™œμš©ν•œ μƒˆλ‘œμš΄ κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμž 및 κ΄‘ν•™ ꡬ쑰듀은 λ„νŒŒκ΄€ 기반 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄μ˜ ν–₯μƒλœ μ„±λŠ₯을 μ œκ³΅ν•˜λŠ” ν•΄κ²°μ±… 및 μƒˆλ‘œμš΄ κ°€λŠ₯μ„±μœΌλ‘œ μ œμ‹œν•  수 μžˆμ„ 것이라 κΈ°λŒ€λœλ‹€.Abstract i Contents iii List of Tables vi List of Figures vii Chapter. 1 Introduction 1 1.1 Augmented reality near-eye display 1 1.2 Key performance parameters of near-eye displays 4 1.3 Basic scheme of waveguide-based near-eye displays 22 1.4 Motivation and purpose of this dissertation 33 1.5 Scope and organization 37 Chapter 2 Dual-focal waveguide-based near-eye display using polarization-dependent combiner lens 39 2.1 Introduction 39 2.2 Optical design for polarization-dependent combiner lens 42 2.2.1 Design and principle of polarization-dependent combiner lens 42 2.2.2 Prototype implementation 48 2.3 Waveguide-based augmented reality near-eye display with dual-focal plane using polarization-dependent combiner lens 51 2.3.1 Implementation of the prototype and experimental results 51 2.3.2 Performance analysis and discussion 57 2.4 Conclusion 69 Chapter 3 Extended-field-of-view waveguide-based near-eye display via polarization-dependent steering combiner 70 3.1 Introduction 70 3.2 Optical design for polarization-dependent steering combiner 73 3.2.1 Principle of polarization grating 73 3.2.2 Principle of polarization-dependent steering combiner 76 3.2.3 Analysis and verification experiment for real-scene distortion 77 3.3 Waveguide-based augmented reality near-eye display with extended-field-of-view 81 3.3.1 Field-of-view for volume grating based waveguide technique 81 3.3.2 Implementation of the prototype and experimental results 84 3.3.3 Performances analysis and discussion 87 3.4 Conclusion 92 Chapter 4 Viewpoint switchable retinal-projection-based near-eye display with waveguide configuration 93 4.1 Introduction 93 4.2 Polarization-dependent switchable eyebox 97 4.2.1 Optical devices for polarization-dependent switching of viewpoints 97 4.2.2 System configuration for proposed method 100 4.2.3 Design of waveguide and imaging combiner 105 4.3 Compact retinal projection-based near-eye display with switchable viewpoints via waveguide configuration 114 4.3.1 Implementation of the prototype and experimental results 114 4.3.2 Performance analysis and discussion 118 4.4 Conclusion 122 Chapter 5. Conclusion 123 Bibliography 127 Appendix 135Docto

    Piezomorphic materials

    Get PDF
    The development of stress-induced morphing materials which are described as piezomorphic materials is reported. The development of a piezomorphic material is achieved by introducing spatial dependency into the compliance matrix describing the elastic response of a material capable of undergoing large strain deformation. In other words, it is necessary to produce an elastically gradient material. This is achieved through modification of the microstructure of the compliant material to display gradient topology. Examples of polymeric (polyurethane) foam and microporous polymer (expanded polytetrafluoroethylene) piezomorphic materials are presented here. These materials open up new morphing applications where dramatic shape changes can be triggered by mechanical stress
    • …
    corecore