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Book Chapter
Series: AIPP Books, Principles
Published: November 2022
10.1063/9780735424470_002
EISBN: 978-0-7354-2447-0
ISBN: 978-0-7354-2444-9
... with their target tissue for prolonged periods of time. Over this time, tissues and devices continue to interact at their interface. While this interaction can be minimally harmful, an improperly designed device can trigger a severe reaction in the tissue and potentially permanently destroy the target of its...
Book Chapter
Series: AIPP Books, Principles
Published: November 2022
10.1063/9780735424470_012
EISBN: 978-0-7354-2447-0
ISBN: 978-0-7354-2444-9
.... Bioelectronics can not only bring solutions for several of the current healthcare challenges, but also open new possibilities, for example, a brain–machine interface. Bioelectronics has neither been focused nor been applied to the same extent to plant systems. Many reasons may have contributed to this; plant...
Images
HRTEM image of PZT/SRO interface (Jia et al., 2007) showing the measured lattice parameters in the film and substrate. The thick arrow denotes the interface. dIL and dIS are the shift parameters as defined in Fig. 5.3(c).
Published: March 2023
FIG. 5.2 HRTEM image of PZT/SRO interface ( Jia et al., 2007 ) showing the measured lattice parameters in the film and substrate. The thick arrow denotes the interface. dIL and dIS are the shift parameters as defined in Fig. 5.3(c) . Reproduced More about this image found in HRTEM image of PZT/SRO interface ( Jia et al., 2007 ) show...
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(a) Dependence of nanostrain on the incoherent interface of nanoparticles and (b) dependence of normalized maximum isotropic pinning force on nanostrain of the YBCO–BMO sample (Coll et al., 2014).
Published: March 2023
FIG. 5.13 (a) Dependence of nanostrain on the incoherent interface of nanoparticles and (b) dependence of normalized maximum isotropic pinning force on nanostrain of the YBCO–BMO sample ( Coll et al., 2014 ). Reproduced with permission from Coll et al., Supercond. Sci More about this image found in (a) Dependence of nanostrain on the incoherent interface of nanoparticles a...
Images
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(a) Low magnification TEM images on BT-CFO, (b) high magnification image of CFO/BCZT interface, (d) BCZT/CFO interface, and (c) and (d) magnified image of (b) and (e), respectively, showing lattice fringes across the interface.
Published: March 2023
FIG. 10.3 (a) Low magnification TEM images on BT-CFO, (b) high magnification image of CFO/BCZT interface, (d) BCZT/CFO interface, and (c) and (d) magnified image of (b) and (e), respectively, showing lattice fringes across the interface. More about this image found in (a) Low magnification TEM images on BT-CFO, (b) high magnification image of...
Images
Schematic of typical Ga-faced HEMT device structure. A nucleation layer is grown on the substrate for accommodating lattice mismatch. 2DEG is formed at the interface of the AlGaN/GaN interface on the GaN side. Thin GaN is formed at the top to make better contact.
Published: March 2023
FIG. 3.18 Schematic of typical Ga-faced HEMT device structure. A nucleation layer is grown on the substrate for accommodating lattice mismatch. 2DEG is formed at the interface of the AlGaN/GaN interface on the GaN side. Thin GaN is formed at the top to make better contact. More about this image found in Schematic of typical Ga-faced HEMT device structure. A nucleation layer is ...
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SIMS depth profiles showing Si accumulation at the film/substrate interface for MOCVD grown films. After BHF etch, the Si peak at the interface decreases by up to one order of magnitude.
Published: February 2023
FIG. 3.3 SIMS depth profiles showing Si accumulation at the film/substrate interface for MOCVD grown films. After BHF etch, the Si peak at the interface decreases by up to one order of magnitude. More about this image found in SIMS depth profiles showing Si accumulation at the film/substrate interface...
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Schematic of perturbation at the free surface (denoted by γ). The regions where interface displacements are prescribed is denoted by Γ.
Published: March 2023
FIG. 8.3 Schematic of perturbation at the free surface (denoted by γ). The regions where interface displacements are prescribed is denoted by Γ. More about this image found in Schematic of perturbation at the free surface (denoted by γ...
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Band diagrams of the AlGaN/GaN heterostructure for HEMT. Strained AlGaN is grown pseudomorphically on relaxed GaN. A positive polarization charge (+σ) is induced at the interface, which attracts electrons and forms 2DEG.
Published: March 2023
FIG. 3.20 Band diagrams of the AlGaN/GaN heterostructure for HEMT. Strained AlGaN is grown pseudomorphically on relaxed GaN. A positive polarization charge ( + σ ) is induced at the interface, which attracts electrons and forms 2DEG. More about this image found in Band diagrams of the AlGaN/GaN heterostructure for HEMT. Strained AlGaN is ...
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(a) Lattice parameters, a and c, and (b) sublattice spacing, dIL and dIS, of PZT and SRO measured from HRTEM image (Jia et al., 2007). The dotted lines indicate the location of the PZT/SRO interface. The open and filled symbols denote the experimental and calculated values, respectively. (c) Schematic illustration of PZT and SRO unit cells with the definition of dIL and dIS. Panels (a) and (b) were reproduced with permission from Jia et al., Nat. Mater. 6, 64–69 (2007).
Published: March 2023
FIG. 5.3 (a) Lattice parameters, a and c, and (b) sublattice spacing, dIL and dIS, of PZT and SRO measured from HRTEM image ( Jia et al., 2007 ). The dotted lines indicate the location of the PZT/SRO interface. The open and filled More about this image found in (a) Lattice parameters, a and c, and (b) ...
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Nanostrain analysis for nanocomposite YBCO films (Llordés et al., 2012). (a) Williamson–Hall plots of the symmetric YBCO Bragg reflection, (b) dependence of the YBCO vertical nanostrain (determined from Williamson–Hall plots) on the incoherent specific interface of nanodots, (c) nanostrain anisotropy, and (d) dependence of coherent domain size on nanostrain along the c-axis in YBCO–BZO nanocomposites, as determined by Rietveld analysis of high-resolution XRD measurements.
Published: March 2023
FIG. 5.11 Nanostrain analysis for nanocomposite YBCO films ( Llordés et al., 2012 ). (a) Williamson–Hall plots of the symmetric YBCO Bragg reflection, (b) dependence of the YBCO vertical nanostrain (determined from Williamson–Hall plots) on the incoherent specific interface of nanodots More about this image found in Nanostrain analysis for nanocomposite YBCO films ( Llordés et al....
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590_010
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... the interface to be sharp and perfect, which is an ideal case. Bichurin et al. [R] constructed an interesting model by taking the interface quality into account and revised Eqns. ( 10.4 ) and ( 10.5 ) by introducing the coupling factor “k.” The coupling factor (k) represents the bonding strength...