From e2ab723d66342562b365a31a5c7fb15889e4cd23 Mon Sep 17 00:00:00 2001
From: Luca Ghiringhelli
Date: Sun, 4 Feb 2018 22:25:12 +0100
Subject: [PATCH] Edited QSHI yaml
---
topological-quantum-phases/QSHI_trivial.demoinfo.yaml | 4 ++--
1 file changed, 2 insertions(+), 2 deletions(-)
diff --git a/topological-quantum-phases/QSHI_trivial.demoinfo.yaml b/topological-quantum-phases/QSHI_trivial.demoinfo.yaml
index 33eeab9..ae07408 100644
--- a/topological-quantum-phases/QSHI_trivial.demoinfo.yaml
+++ b/topological-quantum-phases/QSHI_trivial.demoinfo.yaml
@@ -1,6 +1,6 @@
title: "Prediction of topological quantum phase transitions"
logicalPath: "/data/shared/tutorialsNew/topological-quantum-phases/QSHI_trivial.bkr"
-authors: ["Ahmetcik, Emre", "Ziletti, Angelo", "Ouyang, Runhai", "Ghiringhelli, Luca", "Scheffler, Matthias"]
+authors: ["Mera Acosta, Carlos", "Ahmetcik, Emre", "Carbogno, Christian", "Ouyang, Runhai", "Fazzio, Adalberto", "Ghiringhelli, Luca", "Scheffler, Matthias"]
editLink: "/notebook-edit/data/shared/tutorialsNew/topological-quantum-phases/QSHI_trivial.bkr"
isPublic: true
username: "tutorialsNew"
@@ -8,7 +8,7 @@ description: >
This tutorial shows how to find descriptive parameters (short formulas) for the prediction of
topological phase transitions. As an example, we address the topological classification of
two-dimensional functionalized honeycomb-lattice materials, which are formally described by
- the $Z_2$ topological invariant, i.e., $Z_2=0$ for trivial (normal) insulators and $Z_2=1$ for two-dimensional
+ the Z2 topological invariant, i.e., Z2=0 for trivial (normal) insulators and Z2=1 for two-dimensional
topological insulators (quantum spin Hall insulators).
Using a recently developed machine learning based on compressed sensing, we then derive a map of
these materials, in which metals, trivial insulators, and quantum spin Hall insulators are separated
--
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