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21 May 2023
- 16:1216:12, 21 May 2023 diff hist −11 Linear response from real time simulations (density matrix only) →Results Analysis
- 15:5615:56, 21 May 2023 diff hist +276 Linear response from real time simulations (density matrix only) →Results Analysis
- 15:5515:55, 21 May 2023 diff hist −2,113 Linear response from real time simulations (density matrix only) →Approach based on the Berry Phase
- 15:4215:42, 21 May 2023 diff hist 0 Linear response from real time simulations (density matrix only) →Real-time dynamics at the independent particles level
- 15:4015:40, 21 May 2023 diff hist −320 Linear response from real time simulations (density matrix only) →Real-time dynamics at the independent particles level
- 15:3615:36, 21 May 2023 diff hist +796 Linear response from real time simulations (density matrix only) →Real-time dynamics at the independent particles level
- 15:3315:33, 21 May 2023 diff hist −4,829 Linear response from real time simulations (density matrix only) →Approach based on the Berry Phase
- 15:3015:30, 21 May 2023 diff hist +31 Linear response from real time simulations (density matrix only) →Real-time dynamics at the independent particles level
- 15:2915:29, 21 May 2023 diff hist 0 Linear response from real time simulations (density matrix only) →Real-time dynamics at the independent particles level
- 15:2815:28, 21 May 2023 diff hist +31 Linear response from real time simulations (density matrix only) →Real-time dynamics at the independent particles level
- 15:2715:27, 21 May 2023 diff hist −149 Linear response from real time simulations (density matrix only) →Real-time dynamics at the independent particles level
- 15:2315:23, 21 May 2023 diff hist −112 Linear response from real time simulations (density matrix only) →Real-time dynamics at the independent particles level
- 15:2215:22, 21 May 2023 diff hist 0 Linear response from real time simulations (density matrix only) →Introduction
- 15:2215:22, 21 May 2023 diff hist 0 Linear response from real time simulations (density matrix only) →Introduction
- 15:1715:17, 21 May 2023 diff hist +28 Linear response from real time simulations (density matrix only) →Introduction
- 15:1515:15, 21 May 2023 diff hist +2 Linear response from real time simulations (density matrix only) →Introduction
- 15:1515:15, 21 May 2023 diff hist +2 Real time approach to linear response →Introduction
- 15:1415:14, 21 May 2023 diff hist +86 Rome 2023 →DAY 3 - Wednesday, 24 May
- 15:1315:13, 21 May 2023 diff hist +14,910 N Linear response from real time simulations (density matrix only) Created page with "== Introduction == In this example, we will consider a single layer of hexagonal boron nitride (hBN). If you didn't before you can download input files and Yambo databases for this tutorial here: [http://www.yambo-code.org/educational/tutorials/files/hBN-2D-RT.tar.gz hBN-2D-RT.tar.gz]. and/or follow the instructions to generate the databases here: Prerequisites for Real Time propagation with Yambo Before proceeding with the real-time simulations it is useful to com..."
- 15:1215:12, 21 May 2023 diff hist +10 Prerequisites for Real Time propagation with Yambo →Setup again
- 15:1015:10, 21 May 2023 diff hist +3 Prerequisites for Real Time propagation with Yambo →Setup
- 15:0915:09, 21 May 2023 diff hist +2 Prerequisites for Real Time propagation with Yambo →Setup
- 15:0915:09, 21 May 2023 diff hist −1 Prerequisites for Real Time propagation with Yambo →Setup
- 15:0915:09, 21 May 2023 diff hist +123 Prerequisites for Real Time propagation with Yambo →Setup
- 15:0515:05, 21 May 2023 diff hist +87 Rome 2023 →DAY 3 - Wednesday, 24 May
- 15:0315:03, 21 May 2023 diff hist +177 Prerequisites for Real Time propagation with Yambo No edit summary
- 14:5614:56, 21 May 2023 diff hist +115 Rome 2023 →DAY 3 - Wednesday, 24 May
- 14:5414:54, 21 May 2023 diff hist −41 Rome 2023 →DAY 3 - Wednesday, 24 May
- 14:5314:53, 21 May 2023 diff hist +234 Rome 2023 →DAY 3 - Wednesday, 24 May
- 14:5114:51, 21 May 2023 diff hist +7 Rome 2023 →DAY 3 - Wednesday, 24 May
- 14:5014:50, 21 May 2023 diff hist +457 Rome 2023 →DAY 3 - Wednesday, 24 May
- 14:4614:46, 21 May 2023 diff hist −25 Rome 2023 →DAY 3 - Wednesday, 24 May
- 14:3714:37, 21 May 2023 diff hist +126 How to choose the input parameters →Convergence with the k-point mesh current
- 14:1114:11, 21 May 2023 diff hist +2 Rome 2023 →DAY 3 - Wednesday, 24 May
19 May 2023
- 17:0017:00, 19 May 2023 diff hist +34 How to choose the input parameters →Links
- 16:5916:59, 19 May 2023 diff hist +34 Bethe-Salpeter solver: SLEPC →Links current
- 16:5516:55, 19 May 2023 diff hist −6 Bethe-Salpeter solver: Lanczos-Haydock →Bethe-Salpeter solver runlevel
- 16:5016:50, 19 May 2023 diff hist +34 BSE solvers overview →Navigate current
- 16:4716:47, 19 May 2023 diff hist +4 BSE solvers overview →Full diagonalization solver
- 16:4216:42, 19 May 2023 diff hist +34 How to analyse excitons - ICTP 2022 school →Navigate current
- 16:3916:39, 19 May 2023 diff hist +137 How to analyse excitons - ICTP 2022 school →Plot the exciton spatial distribution
- 16:3416:34, 19 May 2023 diff hist +105 How to analyse excitons - ICTP 2022 school →Calculate the exciton oscillator strength and amplitude
- 16:3216:32, 19 May 2023 diff hist +3 How to analyse excitons - ICTP 2022 school →Calculate the exciton oscillator strength and amplitude
- 16:2416:24, 19 May 2023 diff hist +34 Bethe-Salpeter on top of quasiparticle energies →Navigate current
- 16:2116:21, 19 May 2023 diff hist +1 Bethe-Salpeter on top of quasiparticle energies →Reading the QP corrections from a previous GW calculation
- 16:1516:15, 19 May 2023 diff hist −1 Bethe-Salpeter solver: diagonalization →Choosing the input parameters current
- 16:0816:08, 19 May 2023 diff hist +22 Rome 2023 →DAY 3 - Wednesday, 24 May
- 14:0814:08, 19 May 2023 diff hist +34 Calculating optical spectra including excitonic effects: a step-by-step guide →Links current
- 14:0614:06, 19 May 2023 diff hist −135 Rome 2023 →DAY 3 - Wednesday, 24 May
- 13:5913:59, 19 May 2023 diff hist +783 Rome 2023 →Tutorials