Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Gaoyang Li; Sourabh Patil; Yanxia Xing; Wolfgang Belzig; Gaomin Tang

doi:10.1103/ydwg-y4f8

Paper details

Research paper

TheoreticalComputational Kinetic Model

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Gaoyang Li, Sourabh Patil, Yanxia Xing, Wolfgang Belzig et al.

arXiv·2025·10.1103/ydwg-y4f8·arXiv:2505.01330

Samples

Each sample groups how it was prepared, characterized, and measured. Click a card to expand.

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

10 properties

SimulatedCStudied MaterialIsing superconductorStudied Materialferromagnetic layerCatalyst Substrate

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

6 properties

SimulatedCStudied MaterialIsing superconductorStudied Materialferromagnetic layerCatalyst Substrate

Materials

graphene

Studied Material

studied material

Ising superconductor

Studied Material

Also known as

Ising superconducting electrode

Why these are connected

Related documents with shared materials, methods, properties, or citations.

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction | Matter42 Literature

Properties

Type	Label	Value	Material	Sample	Source
Critical Temperature	Tc	8K	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Superconducting Gap	Delta0	1.22meV	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Dimensionless Ratio	beta_so / Delta0	5	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Exchange Field	J	3Delta0	ferromagnetic layer	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Temperature	T	0.08K	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Broadening Parameter	eta	0.0122meV	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Effective Superconducting Gap	Delta_eff	0.42Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Mirage Gap Edge	epsilon1	5.6Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Mirage Gap Edge	epsilon2	6.1Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Dimensionless Energy Window	chemical-potential range for observing SAR	0 < \|mu\| < epsilon2	C	Two-terminal graphene–Ising superconductor junction used to	—

Properties

Type	Label	Value	Material	Sample	Source
Critical Temperature	Tc	8K	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Superconducting Gap	Delta0	1.22meV	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Dimensionless Ratio	beta_so / Delta0	5	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Exchange Field	J	3Delta0	ferromagnetic layer	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Temperature	T	0.08K	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Broadening Parameter	eta	0.0122meV	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Effective Superconducting Gap	Delta_eff	0.42Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Mirage Gap Edge	epsilon1	5.6Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Mirage Gap Edge	epsilon2	6.1Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Dimensionless Energy Window	chemical-potential range for observing SAR	0 < \|mu\| < epsilon2	C	Two-terminal graphene–Ising superconductor junction used to	—

Properties

Type	Label	Value	Material	Sample	Source
Critical Temperature	Tc	8K	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Superconducting Gap	Delta0	1.22meV	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Dimensionless Ratio	beta_so / Delta0	5	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Exchange Field	J	3Delta0	ferromagnetic layer	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Temperature	T	0.08K	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Broadening Parameter	eta	0.0122meV	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Effective Superconducting Gap	Delta_eff	0.42Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Mirage Gap Edge	epsilon1	5.6Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Mirage Gap Edge	epsilon2	6.1Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Dimensionless Energy Window	chemical-potential range for observing SAR	0 < \|mu\| < epsilon2	C	Two-terminal graphene–Ising superconductor junction used to	—

Properties

Type	Label	Value	Material	Sample	Source
Critical Temperature	Tc	8K	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Superconducting Gap	Delta0	1.22meV	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Dimensionless Ratio	beta_so / Delta0	5	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Exchange Field	J	3Delta0	ferromagnetic layer	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Temperature	T	0.08K	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Broadening Parameter	eta	0.0122meV	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to Four-terminal graphene nanoribbon junction with two Ising su	—
Effective Superconducting Gap	Delta_eff	0.42Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Mirage Gap Edge	epsilon1	5.6Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Mirage Gap Edge	epsilon2	6.1Delta0	Ising superconductor	Two-terminal graphene–Ising superconductor junction used to	—
Dimensionless Energy Window	chemical-potential range for observing SAR	0 < \|mu\| < epsilon2	C	Two-terminal graphene–Ising superconductor junction used to	—

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Samples

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

Materials

Why these are connected

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Samples

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

Materials

Why these are connected

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Samples

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

Materials

Why these are connected

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Samples

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

Materials

Why these are connected

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Samples

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

Materials

Why these are connected

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Samples

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

Materials

Why these are connected

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Samples

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

Materials

Why these are connected

Specular-Andreev reflection and Andreev interference in an Ising superconductor junction

Samples

Two-terminal graphene–Ising superconductor junction used to analyze retro-Andreev and specular-Andreev reflection under an in-plane exchange field.

Four-terminal graphene nanoribbon junction with two Ising superconducting electrodes and exchange fields, used to study Andreev interference.

Materials

Why these are connected

Properties

Simulations

Properties

Simulations

Properties

Simulations

Properties

Simulations