Media Summary: This is a simulation of the NLS equation for solidly rotating hexagonally arranged identical (S=1) Applied current density J = 0.0225 MA/cm^2 along x direction. B = 317 G (left), and B = 480 G (right) in z direction. Depth of the ... This is a simulation of the NLS/GPE equation for an

Controlling Vortex Chirality In Hexagonal - Detailed Analysis & Overview

This is a simulation of the NLS equation for solidly rotating hexagonally arranged identical (S=1) Applied current density J = 0.0225 MA/cm^2 along x direction. B = 317 G (left), and B = 480 G (right) in z direction. Depth of the ... This is a simulation of the NLS/GPE equation for an Applied current density J = 0.108 MA/cm^2 along x direction. B = 108 G (left), and B = 132 G (right) in z direction. Depth of the ... This speech was delivered by Dr. Alexey Snezhko during the International Conference on Magnetic Fluids that was held in Paris ... Applied current density J = 0.0344 MA/cm^2 along x direction. B = 450 G (left), and B = 594 G (right) in z direction. Depth of the ...

Original paper: Title: Robust and tunable coreless ICTP-SAIFR - Workshop on New Horizons in Quantum Correlated Materials August 15 - 19,2022 Speaker: Rodrigo Pereira ... MIT 8.851 Effective Field Theory, Spring 2013 View the complete course: Instructor: Iain Stewart In ...

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Controlling vortex chirality in hexagonal building blocks of artificial spin ice
Identical charge solidly rotating simulation of hexagonal vortex arrangement
Vortex dynamics in hexagonal pinscape, B = 317, 480 G, J = 0.0225 MA/cm^2, h = 12 nm
Vortex (S=-4) surrounded by identical charge hexagon vortices, centre breaks down to more vortices
Vortex dynamics in hexagonal pinscape, B = 108, 132 G, J = 0.108 MA/cm^2, h = 12 nm
Active magnetic spinner liquids: dynamic flocking, chirality switching vortices and transport
Vortex dynamics in hexagonal pinscape, B = 450, 594 G, J = 0.0344 MA/cm^2, h = 50 nm
Robust and tunable coreless vortices and fractional vortices in chiral $d$-wave supercon
Rodrigo Pereira: Spontaneous spin chirality versus magnetization in a zigzag chain
Chirality (physics)
NPCQD-2013: M. Faber "Vortices and chiral symmetry breaking"
7. Chiral Loops
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Controlling vortex chirality in hexagonal building blocks of artificial spin ice

Controlling vortex chirality in hexagonal building blocks of artificial spin ice

Video abstract for the article '

Identical charge solidly rotating simulation of hexagonal vortex arrangement

Identical charge solidly rotating simulation of hexagonal vortex arrangement

This is a simulation of the NLS equation for solidly rotating hexagonally arranged identical (S=1)

Vortex dynamics in hexagonal pinscape, B = 317, 480 G, J = 0.0225 MA/cm^2, h = 12 nm

Vortex dynamics in hexagonal pinscape, B = 317, 480 G, J = 0.0225 MA/cm^2, h = 12 nm

Applied current density J = 0.0225 MA/cm^2 along x direction. B = 317 G (left), and B = 480 G (right) in z direction. Depth of the ...

Vortex (S=-4) surrounded by identical charge hexagon vortices, centre breaks down to more vortices

Vortex (S=-4) surrounded by identical charge hexagon vortices, centre breaks down to more vortices

This is a simulation of the NLS/GPE equation for an

Vortex dynamics in hexagonal pinscape, B = 108, 132 G, J = 0.108 MA/cm^2, h = 12 nm

Vortex dynamics in hexagonal pinscape, B = 108, 132 G, J = 0.108 MA/cm^2, h = 12 nm

Applied current density J = 0.108 MA/cm^2 along x direction. B = 108 G (left), and B = 132 G (right) in z direction. Depth of the ...

Active magnetic spinner liquids: dynamic flocking, chirality switching vortices and transport

Active magnetic spinner liquids: dynamic flocking, chirality switching vortices and transport

This speech was delivered by Dr. Alexey Snezhko during the International Conference on Magnetic Fluids that was held in Paris ...

Vortex dynamics in hexagonal pinscape, B = 450, 594 G, J = 0.0344 MA/cm^2, h = 50 nm

Vortex dynamics in hexagonal pinscape, B = 450, 594 G, J = 0.0344 MA/cm^2, h = 50 nm

Applied current density J = 0.0344 MA/cm^2 along x direction. B = 450 G (left), and B = 594 G (right) in z direction. Depth of the ...

Robust and tunable coreless vortices and fractional vortices in chiral $d$-wave supercon

Robust and tunable coreless vortices and fractional vortices in chiral $d$-wave supercon

Original paper: https://arxiv.org/abs/2306.01202 Title: Robust and tunable coreless

Rodrigo Pereira: Spontaneous spin chirality versus magnetization in a zigzag chain

Rodrigo Pereira: Spontaneous spin chirality versus magnetization in a zigzag chain

ICTP-SAIFR - Workshop on New Horizons in Quantum Correlated Materials August 15 - 19,2022 Speaker: Rodrigo Pereira ...

Chirality (physics)

Chirality (physics)

A new paper on the

NPCQD-2013: M. Faber "Vortices and chiral symmetry breaking"

NPCQD-2013: M. Faber "Vortices and chiral symmetry breaking"

"

7. Chiral Loops

7. Chiral Loops

MIT 8.851 Effective Field Theory, Spring 2013 View the complete course: http://ocw.mit.edu/8-851S13 Instructor: Iain Stewart In ...

Optical Activity Explained: How Chiral Molecules Rotate Light (Polarimeter Demo)

Optical Activity Explained: How Chiral Molecules Rotate Light (Polarimeter Demo)

Chiral