Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Chanaprom Cholsuk; Sujin Suwanna; Tobias Vogl

doi:10.3390/nano12142427/s1

Paper details

Research paper

Computational DFTComputed Band Structure

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Chanaprom Cholsuk, Sujin Suwanna, Tobias Vogl

arXiv preprint·2022·10.3390/nano12142427/s1·arXiv:2207.08506

Samples

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

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

1 property

Simulated Supercell DfthBNStudied Material

Materials

hexagonal boron nitride

hBN

Studied Material

Also known as

hBNboron nitride

studied material

Properties

Type	Label	Value	Material	Sample	Condition	Source
Count Studied Defect Complexes	defect complexes studied	267	hBN	7 × 7 × 1 hBN supercell used for point-defect calculations;		—
Optical Band Gap	band gap	5.99eV	hBN	—	—	—

Why these are connected

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

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications | Matter42 Literature

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Samples

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

Materials

Properties

Why these are connected

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Samples

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

Materials

Properties

Why these are connected

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Samples

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

Materials

Properties

Why these are connected

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Samples

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

Materials

Properties

Why these are connected

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Samples

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

Materials

Properties

Why these are connected

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Samples

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

Materials

Properties

Why these are connected

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Samples

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

Materials

Properties

Why these are connected

Tailoring the Emission Wavelength of Color Centers in Hexagonal Boron Nitride for Quantum Applications

Samples

7 × 7 × 1 hBN supercell used for point-defect calculations; relaxed unit cell used as the starting point, with a 15 Å vacuum layer and spin-polarized HSE06 DFT.

Materials

Properties

Why these are connected

Simulations

Simulations

Simulations

Simulations