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A simply connected superconductor is shown with a “hole” within. C denotes a contour of integration in Eq. (4.13).
Published: December 2022
FIG. 4.7 A simply connected superconductor is shown with a “hole” within. C denotes a contour of integration in Eq. ( 4.13 ). More about this image found in A simply connected superconductor is shown with a “hole” w...
Images
Magnetic phase diagrams for type-I superconductors are shown. There is a direct transition from the superconductor to the normal phase in type-I superconductors.
Published: December 2022
FIG. 4.9 Magnetic phase diagrams for type-I superconductors are shown. There is a direct transition from the superconductor to the normal phase in type-I superconductors. More about this image found in Magnetic phase diagrams for type-I superconductors are shown. There is a di...
Images
Magnetic phase diagrams for type-II superconductors are shown. In type-II materials, there is an intermediate phase that interrupts a direct transition, where the flux lines penetrate.
Published: December 2022
FIG. 4.10 Magnetic phase diagrams for type-II superconductors are shown. In type-II materials, there is an intermediate phase that interrupts a direct transition, where the flux lines penetrate. More about this image found in Magnetic phase diagrams for type-II superconductors are shown. In type-II m...
Images
Different types of Josephson junctions, namely, (a) Tunnel junction, superconductor-insulator-superconductor (SIS) junction, (b) Proximity junction, superconductor-normal-superconductor (SNS) junction, (c) Constriction (Microbridge), (d) Point-contact junction.
Published: December 2022
FIG. 4.34 Different types of Josephson junctions, namely, (a) Tunnel junction, superconductor-insulator-superconductor (SIS) junction, (b) Proximity junction, superconductor-normal-superconductor (SNS) junction, (c) Constriction (Microbridge), (d) Point-contact junction. More about this image found in Different types of Josephson junctions, namely, (a) Tunnel junction, superc...
Images
Uemura plot showing the superconducting transition temperature, Tc vs the Fermi temperature, TF (both in log scale). The positions of different superconductors are shown. The conventional (BCS) superconductors lie far away from unconventional superconductors.
Published: December 2022
FIG. 4.28 Uemura plot showing the superconducting transition temperature, Tc vs the Fermi temperature, TF (both in log scale). The positions of different superconductors are shown. The conventional (BCS) superconductors lie far away from More about this image found in Uemura plot showing the superconducting transition temperature, T...
Book Chapter
Book cover for Strain Engineering in Functional Materials and Devices

Series: AIPP Books, Principles
Published: March 2023
0
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
.../S1431927615013732 Feighan , J. P. F. , Kursumovic , A. , and MacManus-Driscoll , J. L. , “ Materials design for artificial pinning centres in superconductor PLD coated conductors ,” Supercond. Sci. Technol.   30 , 123001-1-16 ( 2017 ). 10.1088/1361-6668/aa90d1 Foltyn , S. R...
Book Chapter
Book cover for Strain Engineering in Functional Materials and Devices
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590_005
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... and (d) defect formation energy of the GB obtained from first-principles calculation ( Sato et al., 2006 ). Nanostrain effect in superconductors REBa2Cu3O7−y coated conductors Superconductors have been considered promising candidates for electric-power...
Images
A schematic diagram of the dispersion E vs k corresponding to the Andreev reflection at the normal-superconductor (N-S) junction is shown. A cooper pair is created at the boundary, which can propagate at low bias inside a superconductor. The electron is specularly reflected as a hole on the metallic side.
Published: December 2022
FIG. 4.27 A schematic diagram of the dispersion E vs k corresponding to the Andreev reflection at the normal-superconductor (N-S) junction is shown. A cooper pair is created at the boundary, which can propagate at low bias inside a superconductor. The electron is specularly More about this image found in A schematic diagram of the dispersion E vs k...
Images
The zero field cooled (left panel) and field cooled (right panel) cases for a superconductor conductor are shown schematically.
Published: December 2022
FIG. 4.5 The zero field cooled (left panel) and field cooled (right panel) cases for a superconductor conductor are shown schematically. More about this image found in The zero field cooled (left panel) and field cooled (right panel) cases for...
Images
The behaviour of the specific heat is schematically shown as a function of the reduced temperature T/θD for both conventional (Cu and Pb) and unconventional (cuprate) superconductors.
Published: December 2022
FIG. 4.14 The behaviour of the specific heat is schematically shown as a function of the reduced temperature T/θD for both conventional (Cu and Pb) and unconventional (cuprate) superconductors. More about this image found in The behaviour of the specific heat is schematically shown as a function of ...
Images
Schematic demonstration of the behavior of an external magnetic field is presented. The field strength falls by a factor 1/e inside the superconductor, which is defined as the penetration depth.
Published: December 2022
FIG. 4.6 Schematic demonstration of the behavior of an external magnetic field is presented. The field strength falls by a factor 1/e inside the superconductor, which is defined as the penetration depth. More about this image found in Schematic demonstration of the behavior of an external magnetic field is pr...
Book Chapter
Book cover for Strain Engineering in Functional Materials and Devices

Series: AIPP Books, Principles
Published: March 2023
0
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... Phys.   8 , 337 – 354 ( 2017 ). 10.1146/annurev-conmatphys-031016-025458 Yan , B. , Jansen , M. , and Felser , C. , “ A large-energy-gap oxide topological insulator based on the superconductor BaBiO3 ,” Nat. Phys.   9 , 709 – 711 ( 2013 ). 10.1038/nphys2762...
Book
Book cover for Strain Engineering in Functional Materials and Devices
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
Images
Generic phase diagram showing temperature vs hole doping (per copper atom) for cuprate superconductors. The different phases are shown. The superconducting dome extends upto a doping of 0.3. In the underdoped regime, at high temperatures, one gets a “strange” metallic phase, which cannot be explained by the Fermi liquid theory, whereas the overdoped regime shows more familiar metallic features.
Published: December 2022
FIG. 4.31 Generic phase diagram showing temperature vs hole doping (per copper atom) for cuprate superconductors. The different phases are shown. The superconducting dome extends upto a doping of 0.3. In the underdoped regime, at high temperatures, one gets a “strange” metallic phase More about this image found in Generic phase diagram showing temperature vs hole doping (per copper atom) ...
Book Chapter
Book cover for Modern Perspectives in the Study of Electronic Systems

Series: AIPP Books, Perspectives
Published: December 2022
10.1063/9780735422537_004
EISBN: 978-0-7354-2253-7
ISBN: 978-0-7354-2251-3
... temperature phenomena until Bednorz and Müller discovered the onset of superconductivity in the copper oxide planes at larger temperatures. As years passed by, the discovery of a large number of copper oxide superconductors were made with larger and larger critical temperatures, which were thought to have far...
Book Chapter
Book cover for Strain Engineering in Functional Materials and Devices
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590_002
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... Phys.   8 , 337 – 354 ( 2017 ). 10.1146/annurev-conmatphys-031016-025458 Yan , B. , Jansen , M. , and Felser , C. , “ A large-energy-gap oxide topological insulator based on the superconductor BaBiO3 ,” Nat. Phys.   9 , 709 – 711 ( 2013 ). 10.1038/nphys2762...
Book
Book cover for Modern Perspectives in the Study of Electronic Systems
Series: AIPP Books, Perspectives
Published: December 2022
10.1063/9780735422537
EISBN: 978-0-7354-2253-7
ISBN: 978-0-7354-2251-3
Book Chapter
Book cover for Modern Perspectives in the Study of Electronic Systems
Series: AIPP Books, Perspectives
Published: December 2022
10.1063/9780735422537_frontmatter
EISBN: 978-0-7354-2253-7
ISBN: 978-0-7354-2251-3
... properties of superconductors, etc. Importantly, we present the BCS theory, in as much detail as possible, in an effort to provide a microscopic description of the thermodynamics and the electromagnetic phenomena. The finite momentum pairing and the FFLO states are hence described to compare and contrast...
Book Chapter
Book cover for Modern Perspectives in the Study of Electronic Systems

Series: AIPP Books, Perspectives
Published: December 2022
10.1063/9780735422537_003
EISBN: 978-0-7354-2253-7
ISBN: 978-0-7354-2251-3
..., the so-called Kitaev model in 1D the symmetry that protects the topological features is much more physical than the chiral symmetry. In fact, it is the particle-hole symmetry that plays a crucial role here, is also inherent to the mean field description of superconductors. Thus, the Kitaev chain...
Book Chapter

Series: AIPP Books, Methods
Published: December 2022
0
EISBN: 978-0-7354-2542-2
ISBN: 978-0-7354-2540-8
... Lu , X. , Stepanov , P. , Yang , W.   , “ Superconductors, orbital magnets and correlated states in magic-angle bilayer graphene ,” Nature   574 , 653 – 657 ( 2019 ). 10.1038/s41586-019-1695-0 Meitl , M. , Zhu , Z. T. , Kumar , V.   , “ Transfer printing by kinetic...