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2D Database

Although graphene has captured a lot of attention recently, there are many other layered materials show similar promise. The non-chemical specific nature of the bonding between layers allows a combinatorial approach to designing new materials, similar to shuffling a deck of cards allowing the design and optimization of new materials. Database of 2D materials. Elastic binding analysis of -A-B-A-B- stacked 2D layers. Sliding energy surface calculations. Binding energy profile for layer rotation.

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2D Database | 2d.materials-mine.com Reviews
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Although graphene has captured a lot of attention recently, there are many other layered materials show similar promise. The non-chemical specific nature of the bonding between layers allows a combinatorial approach to designing new materials, similar to shuffling a deck of cards allowing the design and optimization of new materials. Database of 2D materials. Elastic binding analysis of -A-B-A-B- stacked 2D layers. Sliding energy surface calculations. Binding energy profile for layer rotation.
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1 2d materials design
2 calculated data
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5 data sharing
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2D Database | 2d.materials-mine.com Reviews

https://2d.materials-mine.com

Although graphene has captured a lot of attention recently, there are many other layered materials show similar promise. The non-chemical specific nature of the bonding between layers allows a combinatorial approach to designing new materials, similar to shuffling a deck of cards allowing the design and optimization of new materials. Database of 2D materials. Elastic binding analysis of -A-B-A-B- stacked 2D layers. Sliding energy surface calculations. Binding energy profile for layer rotation.

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2d.materials-mine.com 2d.materials-mine.com
1

Heusler Database

http://www.2d.materials-mine.com/elements.php

Abundance % by weight. DFT energy per atom. Relaced structure, lattice vectors (Ang). 3570,0.000,0.000;-1.785,3.092,0.000;0.000,0.000,5.830;. 2418,0.000,-0.000;1.208,2.093,0.000;1.208,0.698,1.973;. 1776,1.776,-0.000;1.776,0.000,1.776;0.000,1.776,1.776;. 3196,0.000,0.000;1.598,2.768,0.000;1.598,0.923,2.610;. 8506,-0.000,0.000;-1.755,8.324,-0.000;-3.387,-4.176,12.595;. 1386,1.386,1.386;1.386,-1.386,1.386;1.386,1.386,-1.386;. 3324,0.000,0.000;-1.081,3.144,0.000;1.163,1.542,2....3500,0.000,0.000;1&#4...3238,...

2

Data sharing

http://www.2d.materials-mine.com/data_sharing.html

Created by Thomas Archer, Trinity College, Dublin - -.

3

Heusler Database

http://www.2d.materials-mine.com/monolayers.php

Stress fit (a(x-1) 2). Binding energy meV.Ang -2. Created by Thomas Archer, Trinity College, Dublin - -.

4

Heusler Database

http://www.2d.materials-mine.com/2Dmaterials.php

Relaxed structure, lattice vectors (Ang). 3882,-0.000,-0.000;-1.941,3.362,0.000;-0.000,0.000,6.173;. 2168,-1.252,0.000;-0.000,2.504,0.000;0.000,-0.000,6.688;. 4021,0.000,-0.000;0.000,4.395,-0.000;-0.000,-0.000,11.203;. 3158,-0.000,0.000;-1.579,2.735,0.000;-0.000,0.000,12.043;. 3698,0.000,-0.000;-1.849,3.203,-0.000;-0.000,-0.000,6.005;. 3639,0.000,-0.000;2.808,2.314,-0.000;2.808,1.008,2.083;. 3296,-0.000,0.000;1.648,2.854,-0.000;1.614,0.932,6.339;. Created by Thomas Archer, Trinity College, Dublin - -.

5

Heusler Database

http://www.2d.materials-mine.com/AB_materials.php

Results here are extrapolated from calculations of the monolayers described in this document. Energy is plotted as a binding energy ( in meV Å. Where anything above 0 is unlikely to occur. If the bulk binding energy for system A is E bulk binding(A) and the elastic contribution is E elastic(A), we write the binding energy of the composite per layer as E bulk(-A-B-A-B-) = ( E bulk binding(A) E bulk binding(B) E elastic(A) E elastic(B) )/2. Estimate of the bulk energy of an -A-B-A-B- composite.

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2D Database

Although graphene has captured a lot of attention recently, there are many other layered materials show similar promise. The non-chemical specific nature of the bonding between layers allows a combinatorial approach to designing new materials, similar to shuffling a deck of cards allowing the design and optimization of new materials. Database of 2D materials. Elastic binding analysis of -A-B-A-B- stacked 2D layers. Sliding energy surface calculations. Binding energy profile for layer rotation.

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