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Merge pull request #273 from Exabyte-io/docs/SOF-7376
SOF-7376: SOC tutorial
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lang/en/docs/tutorials/dft/electronic/spin-magnetic-qe.json

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"endTime": "00:00:11.000"
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"text": "Performing a materials simulation involves following steps in our web platform. First, <break time='0.5' /> we need to specify the material system by creating or uploading a material structure. <break time='0.5' /> Second, <break time='0.5' /> we have to specify the workflow steps. These two steps can be carried out in any order. You may either create the structure first and then workflow or the other way around. <break time='0.5' /> Note that you may skip the above steps if you already have the required structure or workflow in you library. You may also find the structure and workflow you are looking for in our extensive materials and workflows banks, respectively.",
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"text": "Performing a materials simulation involves following steps in our web platform. First, <break time='0.5'/> we need to specify the material system by creating or uploading a material structure. <break time='0.5'/> Second, <break time='0.5'/> we have to specify the workflow steps. These two steps can be carried out in any order. You may either create the structure first and then workflow or the other way around. <break time='0.5'/> Note that you may skip the above steps if you already have the required structure or workflow in you library. You may also find the structure and workflow you are looking for in our extensive materials and workflows banks, respectively.",
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"text": "For today's demonstration, We will generate the material structure using materials designer in our web platform. Navigate to materials tab. <break time='1.5' /> Click create. <break time='3.0' /> We will clone the existing structure and then modify. Let's create iron oxide with cubic structure. <break time='3.0' /> Set the lattice constant. <break time='3.5' /> Set the atomic positions. <break time='2.0' /> There are two iron and two oxygen atoms in each unit cell. Notice that we have added label 1 and 2 to two iron atoms so that we can specify different spin states to them in antiferromagnetic spin calculation. <break time='1.0' />Finally, <break time='0.5' /> save the structure.",
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"text": "For today's demonstration, we will generate the material structure using materials designer in our web platform. Navigate to materials tab. <break time='1.5'/> Click create. <break time='3.0'/> We will clone the existing structure and then modify. Let's create iron oxide with cubic structure. <break time='3.0'/> Set the lattice constant. <break time='3.5'/> Set the atomic positions. <break time='2.0'/> There are two iron and two oxygen atoms in each unit cell. Notice that we have added label 1 and 2 to two iron atoms so that we can specify different spin states to them in antiferromagnetic spin calculation. <break time='1.0'/>Finally, <break time='0.5'/> save the structure.",
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"text": "Click edit workflow unit. <break time='1.0' /> Expand the details pane.",
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"text": "Click edit workflow unit. <break time='1.0'/> Expand the details pane.",
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"text": "Finally, we need to do the postprocessing of bands obtained in the above steps. Add another unit. <break time='4.0' /> This time select bands dot x executable.",
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"text": "Finally, we need to do the postprocessing of bands obtained in the above steps. Add another unit. <break time='4.0'/> This time select bands dot x executable.",
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"text": "The same way, we add another unit to process the down spin component. <break time='4.0' />Set the spin component equal to 2 for that.",
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"text": "The same way, we add another unit to process the down spin component. <break time='4.0'/>Set the spin component equal to 2 for that.",
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"text": "Navigate to jobs tab, <break time='0.5' />click create new job. <break time='3.0' />Import materials and select iron oxide. <break time='3.0' />Import workflow and select spin magnetic that we just created.",
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"text": "Navigate to jobs tab, <break time='0.5'/>click create new job. <break time='3.0'/>Import materials and select iron oxide. <break time='3.0'/>Import workflow and select spin magnetic that we just created.",
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"text": "Once finished, let's navigate to the results tab. We will see separate plots for both up and down spin components of bandstructure. <break time='1.0' /> We can zoom in to see the bands near the Fermi energy more clearly.",
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"text": "Once finished, let's navigate to the results tab. We will see separate plots for both up and down spin components of bandstructure. <break time='1.0'/> We can zoom in to see the bands near the Fermi energy more clearly.",
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{
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"descriptionLinks": [
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"How to incorporate spin-orbit coupling in Quantum ESPRESSO: https://docs.mat3ra.com/tutorials/dft/electronic/soc-qe/"
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],
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"description": "In this tutorial, we walk you through the steps of incorporate spin-orbit coupling effect in bandstructure calculation using Quantum ESPRESSO.",
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"tags": [
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{
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"...": "../../../metadata/general.json#/tags"
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},
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{
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"...": "../../../models-directory/dft.json#/tags"
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},
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{
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"...": "../../../software-directory/modeling/quantum-espresso.json#/tags"
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},
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"bandstructure",
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"slab",
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"soc",
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"spin",
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"spin-orbit-coupling",
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"supercell",
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"surface-state",
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"topological-insulator"
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],
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"title": "Mat3ra Tutorial: How to incorporate spin-orbit coupling in Quantum ESPRESSO",
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"youTubeCaptions": [
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{
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"text": "We would like to increase the density of k grid for self consistent field calculation.",
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"startTime": "00:00:06.000",
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"endTime": "00:00:11.000"
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},
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{
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"text": "Navigate to the compute tab.",
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"startTime": "00:00:14.000",
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"endTime": "00:00:15.500"
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},
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"text": "Here we can adjust time limit <break time='1.0'/>, cluster <break time='2.0'/>, queue <break time='3.0'/>, number of nodes <break time='1.0'/>, and number of processor cores. <break time='2.0'/> Save and exit job designer.<break time='2.0'/> Finally, click the run button to submit job.",
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"startTime": "00:00:17.000",
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"endTime": "00:00:38.000"
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},
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"text": "Once the job is finished, navigate to the results tab. Here we will find summary of various result including the bandstructure plot. If we zoom in, we can see the bands near the Fermi energy more clearly. Note the bandstucture we are currently looking at, was obtained with coarse convergence criterion. You need to increase the k grid density and stringent energy threshold to see the topological Dirac states clearly. You can compare the bandstructure for slab and bulk calculation, and identify the surface states.",
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"startTime": "00:00:39.000",
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"endTime": "00:01:07.000"
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},
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{
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"text": "All output files can be found under the files tab for further analysis.",
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"startTime": "00:01:08.000",
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"endTime": "00:01:13.000"
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},
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{
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"text": "Thank you for watching this tutorial. Now, explore more yourself at platform dot matera dot com.",
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"startTime": "00:01:14.000",
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"endTime": "00:01:19.000"
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}
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],
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"youTubeId": "Zr1jcalLYPU"
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}

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