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Book Chapter
Series: AIPP Books, Methods
Published: November 2022
10.1063/9780735424197_007
EISBN: 978-0-7354-2419-7
ISBN: 978-0-7354-2416-6
... as well, where some materials seek to minimize the effects of the applied pressure through structural changes and even amorphization. In this chapter, we take a look at various real examples to highlight how non-ambient experiments can inform us about the structure–property relations within real energy...
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Schematics of (top) octahedral distortion in <span class="search-highlight">non</span>-cubic structures as compar...
Published: March 2023
FIG. 2.1 Schematics of (top) octahedral distortion in non-cubic structures as compared to the cubic oxides; (bottom) various grain boundary structures and c-Si. Reproduced with permission from Raghunathan et al., Nano Lett. 14 , 4943–4950 (2014). Copyright 2014 American Chemical Society. More about this image found in Schematics of (top) octahedral distortion in non-cubic structures as compar...
Book Chapter
Series: AIPP Books, Principles
Published: November 2022
10.1063/9780735425194_003
EISBN: 978-0-7354-2519-4
ISBN: 978-0-7354-2508-8
...Wang, D. F., Han, H., Zhao, Z., Liu, S., Chen, B., Wang, X., Fang, Y., Lv, M., Fan, L., Zhu, X., Itoh, T., and Maeda, R., “Non-invasive passive resonant electric current sensors for EVs,” in Advanced Sensors and Sensing Technologies for Electric Vehicles, edited by W. Cao and S. Lu (AIP...
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(a) Strictly <span class="search-highlight">non</span>-blocking 2D N × N switch requiring N<sup>2</sup> single ax...
Published: March 2023
FIG. 7.23 (a) Strictly non-blocking 2D N × N switch requiring N2 single axis mirrors ( Stepanovsky, 2019 ; and Horsley et al., 2005 ). (b) A 3-axis micromirror array capable of N × N routing using 2 N mirrors ( Stepanovsky, 2019 ). (c) An N × N planar switch implemented using tunable directional couplers ( Han et al., 2015 ; and Stepanovsky, 2019 ). More about this image found in (a) Strictly non-blocking 2D N × N switch requiring N2 single ax...
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Microstructural evolution in a thin film system with <em>A<sub>Z</sub></em>...
Published: March 2023
FIG. 8.10 Microstructural evolution in a thin film system with AZ = 1. From top left, in the clockwise direction, the microstructures correspond to (non-dimensional) time units: t = 2600, t = 3000, t = 4000, and t = 11 700, respectively. More about this image found in Microstructural evolution in a thin film system with AZ...
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Microstructural evolution in a thin film system with      A  Z   =    1  3 ...
Published: March 2023
FIG. 8.9 Microstructural evolution in a thin film system with A Z = 1 3 . From top left, the microstructures correspond to (non-dimensional) time units: t = 9600, t = 11 400, t = 23 600 and t = 489 400, respectively. More about this image found in Microstructural evolution in a thin film system with A Z = 1 3 ...
Book Chapter
Series: AIPP Books, Methods
Published: March 2023
10.1063/9780735425743_frontmatter
EISBN: 978-0-7354-2574-3
ISBN: 978-0-7354-2572-9
... of technical challenges by using state-of-the-art systematic methods. It covers a broad range of energy topics, including traditional fossil fuels, renewable energy, clean energy production and storage, emerging non-traditional energy sources such as oil sands, shale gas, and natural gas hydrates, and energy...
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Microstructural evolution in a thin film system with      A  Z   =    1  3 ...
Published: March 2023
FIG. 8.11 Microstructural evolution in a thin film system with A Z = 1 3 in 3D. From top left, in the clockwise direction, the microstructures correspond to (non-dimensional) time units: t = 100, t = 500, t = 1000, and t = 11 700 for the left and right columns, respectively. More about this image found in Microstructural evolution in a thin film system with A Z = 1 3 ...
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Microstructural evolution in a thin film system with isotropic elasticity a...
Published: March 2023
FIG. 8.5 Microstructural evolution in a thin film system with isotropic elasticity and two films in the simulation cell; the far-field composition is 0.01. From top left, the microstructures correspond to (non-dimensional) time units: t = 105 200, t = 109 600, t = 112 200, and t = 142 200, respectively. More about this image found in Microstructural evolution in a thin film system with isotropic elasticity a...
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Martini 3 CG model of caffeine. (a) The 14 <span class="search-highlight">non</span>-hydrogen atoms are described...
Published: January 2023
FIG. 1.2 Martini 3 CG model of caffeine. (a) The 14 non-hydrogen atoms are described by a 7 T-bead model; the indices used for the beads in the CG topology file are also shown. (b) Rendering of the CG model: apolar aromatic and intermediately polar beads are displayed in silver (TC5, TN1) and blue... More about this image found in Martini 3 CG model of caffeine. (a) The 14 non-hydrogen atoms are described...
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Microstructural evolution in a thin film system with isotropic elasticity a...
Published: March 2023
FIG. 8.7 Microstructural evolution in a thin film system with isotropic elasticity and two films in the simulation cell; the far-field composition is 0.01. From the top left, the microstructures correspond to (non-dimensional) time units: t = 78 800, t = 84 800, t = 100 800 and t = 251 000, respectively. Note that relatively, the break-up is faster for two films as compared to the case of a single film in the simulation cell. More about this image found in Microstructural evolution in a thin film system with isotropic elasticity a...
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Microstructural evolution in a thin film system with isotropic elasticity, ...
Published: March 2023
FIG. 8.6 Microstructural evolution in a thin film system with isotropic elasticity, the far-field composition is 0.05 leading to growth along with film break-up. From the top left, the microstructures correspond to (non-dimensional) time units: t = 114 600, t = 122 800, t = 133 800 and t = 205 800, respectively. These times indicate that the growth slows down the break-up dynamics compared to the previous case of (near) static break-up. More about this image found in Microstructural evolution in a thin film system with isotropic elasticity, ...
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Microstructural evolution in a thin film system with isotropic elasticity a...
Published: March 2023
FIG. 8.8 Microstructural evolution in a thin film system with isotropic elasticity and two films in the simulation cell, the far-field composition is 0.05 leading to growth along with film break-up. From top left, the microstructures correspond to (non-dimensional) time units: t = 110 800, t = 122 800, t = 143 400, and t = 270 800, respectively. These times indicate that the growth slows down the break-up dynamics compared to the previous case of (near) static break-up. More about this image found in Microstructural evolution in a thin film system with isotropic elasticity a...
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(a) Strain in the waveguide resulting in a change in the effective index. (...
Published: March 2023
FIG. 7.12 (a) Strain in the waveguide resulting in a change in the effective index. (b) Cross-sectional views of different phase shifters implemented using the relative movement of a non-phase matched loading section resulting in a change in the effective index or attenuation due to proximity. (c)... More about this image found in (a) Strain in the waveguide resulting in a change in the effective index. (...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735424395_frontmatter
EISBN: 978-0-7354-2439-5
ISBN: 978-0-7354-2436-4
... through its interdisciplinary approach Identifies recent technologies from MEMS sensors domains and their efficacy in real-life applications Covers relevant topics for the expert as well as foundational information for non-specialists in MEMS technologies MEMS Applications in Electronics...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735424395_index
EISBN: 978-0-7354-2439-5
ISBN: 978-0-7354-2436-4
... interdisciplinary approach Identifies recent technologies from MEMS sensors domains and their efficacy in real-life applications Covers relevant topics for the expert as well as foundational information for non-specialists in MEMS technologies MEMS Applications in Electronics and Engineering...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425613_003
EISBN: 978-0-7354-2561-3
ISBN: 978-0-7354-2560-6
... systems. Similarly, Junsangsri and Lombardi (2010) showed that time, temperature, and irradiance have a high influence but in a double-diode model because the solar cell efficiency is affected. AlHajri et al. (2012) formulated the solar cell parameter estimation problem as a multivariate non...
Book Chapter
Series: AIPP Books, Professional
Published: March 2023
10.1063/9780735425477_010
EISBN: 978-0-7354-2547-7
ISBN: 978-0-7354-2544-6
... Thread Computerized tutoring systems Conceptual scaffolding Thread 2: Problem Solving in the Practice of Learning and Making Sense of Physics Dynamical accounts of intuition, understanding, and problem solving A non-procedural role for mathematics Epistemic games Epistemology in problem solving...
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