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Band diagrams of (a) valence band and (b) conduction band in the GaN/InGaN ...
Published: March 2023
FIG. 3.15 Band diagrams of (a) valence band and (b) conduction band in the GaN/InGaN pin structure. Carrier wavefunctions are not centrosymmetric due to polarization. E p and E n are the first bound states in the valence and conduction bands, respectively. (c) Induced sheet charge at the interfaces of QW due to polarization. More about this image found in Band diagrams of (a) valence band and (b) conduction band in the GaN/InGaN ...
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(a) shows the time-resolved current response of multilayers for a voltage p...
Published: March 2023
FIG. 10.9 (a) shows the time-resolved current response of multilayers for a voltage pulse of 500 ns pulse width. Inset shows the half input pulse profile for the input pulse of 1.8 V amplitude and 500 ns pulse width. (b) Polarization-time curves obtained by integrating the It curve of multilayer samples. (c) Voltage–time and current–time curve for individual BCZT film. (d) Polarization-time curve for individual BCZT film. More about this image found in (a) shows the time-resolved current response of multilayers for a voltage p...
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Band diagrams of the AlGaN/GaN heterostructure for HEMT. Strained AlGaN is ...
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) Schematic of the pseudocubic unit cell with indication of eight equival...
Published: March 2023
FIG. 7.2 (a) Schematic of the pseudocubic unit cell with indication of eight equivalent polarization directions of 〈111〉. (b) The projection of the spin tip on (111) plane of pseudocubic BFO and (c) schematic of the spin cycloidal antiferromagnetic arrangement. More about this image found in (a) Schematic of the pseudocubic unit cell with indication of eight equival...
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(a) The out-of-plane, (b) in-plane phase contrast image obtained from BFO w...
Published: March 2023
FIG. 7.10 (a) The out-of-plane, (b) in-plane phase contrast image obtained from BFO with tetragonal phase grown on LSMO∼2 nm, and (c) the corresponding out-of-plane domain contrast obtained from the phase field modeling indicating only 〈001〉 polarization dominating the domain pattern. More about this image found in (a) The out-of-plane, (b) in-plane phase contrast image obtained from BFO w...
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(a) The schematic of the pseudocubic unit cell of BFO indicating the polari...
Published: March 2023
FIG. 7.4 (a) The schematic of the pseudocubic unit cell of BFO indicating the polarization vector pointing toward [111] direction and the schematic of the PFM tip approaching from the top, (b) out-of-plane phase contrast, and (c) in-plane phase contrast obtained from a PFM for a BFO/STO superlatti... More about this image found in (a) The schematic of the pseudocubic unit cell of BFO indicating the polari...
Images
(a) The schematic of the pseudocubic unit cell of BFO indicating the polari...
Published: March 2023
FIG. 7.5 (a) The schematic of the pseudocubic unit cell of BFO indicating the polarization vector pointing toward [001] direction and the schematic of the PFM tip approaching from the top, (b) out-of-plane phase contrast, and (c) in-plane phase contrast obtained from a PFM for a BFO/STO superlatti... More about this image found in (a) The schematic of the pseudocubic unit cell of BFO indicating the polari...
Images
(a) The out-of-plane (b) in-plane phase contrast image obtained from BFO wi...
Published: March 2023
FIG. 7.11 (a) The out-of-plane (b) in-plane phase contrast image obtained from BFO with mixed phase (rhombohedral + tetragonal) grown on LSMO∼10 nm and (c) the corresponding out-of-plane domain contrast obtained from phase field modeling, indicating the components apart from 〈001〉 polarization eme... More about this image found in (a) The out-of-plane (b) in-plane phase contrast image obtained from BFO wi...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590_007
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... is an interesting property in a given material that arises due to its coupling between two important functional properties like electrical and magnetic property. Conventionally, both electric polarization and magnetization were dealt as mutually exclusive properties due to their origin in materials. The coupling...
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(a) Energetics and density of states of BaTiO<sub>3</sub> (BTO) and PbTiO...
Published: March 2023
FIG. 2.9 (a) Energetics and density of states of BaTiO3 (BTO) and PbTiO3 (PTO), (b) energetics, buckling (Δ) and polarization (P) of 1T MoS2, and (c) energetics, charge disproportionation, and octahedral distortion in Bi2−xSrxFeCrO6. Reproduced with permission from Cohen, Nature 358 , 136–138 (1992). Copyright 1992 Nature Publishing Group; Chanana and Waghmare, Phys. Rev. Lett. 123 , 037601 (2019). Copyright 2019 American Physical Society; and Rout and Srinivasan, Phys. Rev. Lett. 123 , 107201 (2019). Copyright 2019 American Physical Society. More about this image found in (a) Energetics and density of states of BaTiO3 (BTO) and PbTiO...
Book Chapter
Series: AIPP Books, Professional
Published: March 2023
10.1063/9780735425712_020
EISBN: 978-0-7354-2571-2
ISBN: 978-0-7354-2568-2
..., reflection and refraction, shadows, and color Polarization of light with final year high school students Geometric optics, light diffraction, and the photoelectric effect with Grade-12 students Geometric optics with university students Simple everyday light phenomena with primary school teachers...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590_006
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... Ginzburg–Landau–Devonshire (GLD) theory to define the total free energy of a ferroelectric material. GLD theory expresses the total free energy as the function of a vector-valued order parameter field, termed as spontaneous polarization field P ( r ). Note that all components of P go to zero...
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
... consisting of physically separated piezoelectric and magneto strictive materials are utilized ( Nan et al., 2008 ). The strain developed in either the piezoelectric and/or magnetostrictive phase is transferred to the other phase and eventually leads to a polarization and/or magnetization induced...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590_003
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... in periodic potential, also known as deformation potential. In polar semiconductors, an electric field is generated by the long-wavelength acoustic and optical phonons by moving and localizing the charged ions ( Yu and Cardona, 1996 ). In thin films grown on a foreign substrate, the strain, based...
Book Chapter
Series: AIPP Books, Professional
Published: March 2023
10.1063/9780735425477_005
EISBN: 978-0-7354-2547-7
ISBN: 978-0-7354-2544-6
... (at the source for the charge inside the insulator, at the boundary for the charge outside the insulator) and between one quarter and one-sixth of these students mentioned that there could only be an electric field where charges could move. Where students took polarization into account, they often appeared...
Book
Book Cover Image
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590_002
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... withstand up to 21%, 15%, and 4% uniaxial, biaxial and shear strains, respectively. Ferroelectric Polarization Materials that possess spontaneous polarization and exhibit a reversal of electric polarization under the influence of an externally applied electric field are called ferroelectrics...