User contributions for Maurizia
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- 17:14, 3 April 2022 diff hist +1 Hartree Fock
- 17:09, 3 April 2022 diff hist +151 Hartree Fock
- 16:36, 3 April 2022 diff hist −76 GW hBN Yambo Virtual 2021 version →Step 1: The Exchange Self Energy or HF quasi-particle correction
- 14:24, 7 April 2021 diff hist 0 GW hBN Yambo Virtual 2021 version →Step 3: Interpolating Band Structures
- 13:41, 7 April 2021 diff hist +2 GW hBN Yambo Virtual 2021 version →Step 3: Interpolating Band Structures
- 12:44, 6 April 2021 diff hist +1 GW hBN Yambo Virtual 2021 version →Converging Screening Parameters
- 12:43, 6 April 2021 diff hist −108 GW hBN Yambo Virtual 2021 version →Converging Screening Parameters
- 12:42, 6 April 2021 diff hist +136 GW hBN Yambo Virtual 2021 version →Converging Screening Parameters
- 09:24, 6 April 2021 diff hist +25 GW hBN Yambo Virtual 2021 version →Converging Screening Parameters
- 09:22, 6 April 2021 diff hist +1 GW hBN Yambo Virtual 2021 version →Convergence tests for a quasi particle calculation
- 08:32, 6 April 2021 diff hist −1 First steps: walk through from DFT(standalone) →Download the Files
- 08:24, 6 April 2021 diff hist −45 First steps: walk through from DFT(standalone) →Download the Files
- 08:20, 6 April 2021 diff hist +86 First steps: walk through from DFT(standalone) →Download the Files
- 08:19, 6 April 2021 diff hist +66 First steps: walk through from DFT(standalone) →Download the Files
- 08:17, 6 April 2021 diff hist +80 First steps: walk through from DFT(standalone) →Conversion to Yambo format
- 08:14, 6 April 2021 diff hist +20 First steps: walk through from DFT(standalone) →Download the Files
- 08:07, 6 April 2021 diff hist +101 First steps: walk through from DFT(standalone) →Download the Files
- 08:00, 6 April 2021 diff hist +299 First steps: walk through from DFT(standalone) →Download the Files
- 07:56, 6 April 2021 diff hist +2 First steps: walk through from DFT(standalone) →Download the Files
- 07:49, 6 April 2021 diff hist +29 First steps: walk through from DFT(standalone) →Download the Files
- 07:37, 6 April 2021 diff hist −6 GW hBN Yambo Virtual 2021 version →Input file generation
- 07:31, 6 April 2021 diff hist 0 GW hBN Yambo Virtual 2021 version →Input file generation
- 07:29, 6 April 2021 diff hist +83 Download →Getting the latest snapshot with git
- 07:09, 6 April 2021 diff hist +257 Hartree Fock →Calculation and analysis of output
- 06:56, 6 April 2021 diff hist 0 Hartree Fock →Input file generation
- 13:05, 2 April 2021 diff hist −1 First steps: walk through from DFT(standalone) →Verbosity
- 11:31, 2 April 2021 diff hist 0 First steps: walk through from DFT(standalone) →Allowed options
- 14:12, 29 January 2020 diff hist 0 Bethe-Salpeter solver: diagonalization →Prerequisites
- 14:12, 29 January 2020 diff hist +86 Bethe-Salpeter solver: diagonalization →Prerequisites
- 04:57, 21 January 2020 diff hist −24 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation current
- 04:56, 21 January 2020 diff hist 0 File:Alpha2D.gif Maurizia uploaded a new version of File:Alpha2D.gif current
- 04:54, 21 January 2020 diff hist +2 How to analyse excitons →Plot the exciton spatial distribution
- 19:36, 20 January 2020 diff hist +17 How to analyse excitons →Calculate the exciton oscillator strenght and amplitude
- 19:33, 20 January 2020 diff hist −2 How to analyse excitons →Calculate the exciton oscillator strenght and amplitude
- 19:32, 20 January 2020 diff hist +3 How to analyse excitons →Calculate the exciton oscillator strenght and amplitude
- 19:21, 20 January 2020 diff hist +326 N File:Strenght.png User created page with UploadWizard current
- 19:17, 20 January 2020 diff hist +66 How to analyse excitons →Sort the excitonic eigenvalues
- 18:48, 20 January 2020 diff hist +28 How to analyse excitons →Sort the excitonic eigenvalues
- 18:37, 20 January 2020 diff hist 0 File:BSE 2D cutnocut.png Maurizia uploaded a new version of File:BSE 2D cutnocut.png current
- 18:16, 20 January 2020 diff hist +326 N File:BSE 2D cutnocut.png User created page with UploadWizard
- 18:14, 20 January 2020 diff hist −5 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 15:54, 20 January 2020 diff hist +203 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 15:49, 20 January 2020 diff hist +27 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 15:37, 20 January 2020 diff hist 0 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 15:35, 20 January 2020 diff hist 0 File:Alpha2D.gif Maurizia uploaded a new version of File:Alpha2D.gif
- 15:31, 20 January 2020 diff hist +1 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 15:29, 20 January 2020 diff hist +4 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 15:26, 20 January 2020 diff hist +263 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 15:06, 20 January 2020 diff hist +87 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 15:02, 20 January 2020 diff hist −4 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 15:00, 20 January 2020 diff hist +71 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 14:59, 20 January 2020 diff hist 0 File:Lz.gif Maurizia uploaded a new version of File:Lz.gif current
- 14:57, 20 January 2020 diff hist +326 N File:Lz.gif User created page with UploadWizard
- 14:56, 20 January 2020 diff hist +2 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 14:53, 20 January 2020 diff hist 0 File:Alpha2D.gif Maurizia uploaded a new version of File:Alpha2D.gif
- 14:51, 20 January 2020 diff hist +262 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 14:29, 20 January 2020 diff hist +326 N File:Alpha2D.gif User created page with UploadWizard
- 14:27, 20 January 2020 diff hist 0 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 14:14, 20 January 2020 diff hist +12 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 14:10, 20 January 2020 diff hist +35 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 13:59, 20 January 2020 diff hist +12 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 13:56, 20 January 2020 diff hist −4 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 13:51, 20 January 2020 diff hist +4 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 13:29, 20 January 2020 diff hist +92 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 13:22, 20 January 2020 diff hist 0 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 13:21, 20 January 2020 diff hist +5 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 13:10, 20 January 2020 diff hist +2 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 10:05, 20 January 2020 diff hist +9 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 10:04, 20 January 2020 diff hist −20 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 10:00, 20 January 2020 diff hist 0 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 09:59, 20 January 2020 diff hist +2 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 09:27, 20 January 2020 diff hist 0 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 09:22, 20 January 2020 diff hist 0 How to treat low dimensional systems →Use the truncated coulomb potential in a G0W0-PPA calculation
- 09:12, 20 January 2020 diff hist −74 How to treat low dimensional systems →Use the truncated coulomb potential in a G0W0-PPA calculation
- 09:07, 20 January 2020 diff hist +40 How to treat low dimensional systems →Avoid numerical divergences using the Random Integration Method (RIM)
- 07:50, 20 January 2020 diff hist +26 Bethe-Salpeter solver: diagonalization →Background
- 21:51, 17 January 2020 diff hist −19 ICTP2020 →Wednesday 29 Jan HANDS-ON 3
- 20:17, 17 January 2020 diff hist 0 Bethe-Salpeter solver: Lanczos-Haydock →Convergence of the iterative procedure
- 19:59, 17 January 2020 diff hist +1 Bethe-Salpeter solver: Lanczos-Haydock →Bethe-Salpeter solver runlevel
- 19:53, 17 January 2020 diff hist +6 Bethe-Salpeter solver: Lanczos-Haydock →Bethe-Salpeter solver runlevel
- 18:44, 17 January 2020 diff hist −1 Bethe-Salpeter solver: diagonalization →Bethe-Salpeter solver runlevel
- 17:53, 17 January 2020 diff hist +17 Bethe-Salpeter kernel →Bethe-Salpeter kernel runlevel
- 17:49, 17 January 2020 diff hist +10 Bethe-Salpeter kernel →Choosing input parameters
- 17:20, 17 January 2020 diff hist +2 Bethe-Salpeter kernel →Background
- 17:17, 17 January 2020 diff hist −10 Bethe-Salpeter kernel →Background
- 17:16, 17 January 2020 diff hist −7 Bethe-Salpeter kernel →Background
- 17:15, 17 January 2020 diff hist +69 Bethe-Salpeter kernel →Background
- 15:25, 17 January 2020 diff hist +56 Static screening →Static screening runlevel
- 15:22, 17 January 2020 diff hist +15 Static screening →Static screening runlevel
- 14:40, 27 April 2017 diff hist −37 How to analyse excitons →Sort the excitonic eigenvalues
- 14:38, 27 April 2017 diff hist 0 How to analyse excitons →Sort the excitonic eigenvalues
- 14:34, 27 April 2017 diff hist +22 How to treat low dimensional systems →Analyze the differences with corresponding GW and BSE calculations without the use of a truncated coulomb potential
- 14:32, 27 April 2017 diff hist −15 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 14:31, 27 April 2017 diff hist −5 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 14:30, 27 April 2017 diff hist +6 How to treat low dimensional systems →Use the truncated coulomb potential in a BSE calculation
- 14:29, 27 April 2017 diff hist +6 How to treat low dimensional systems →Use the truncated coulomb potential in a G0W0-PPA calculation
- 14:28, 27 April 2017 diff hist −11 How to treat low dimensional systems →Generate a truncated coulomb potential
- 14:26, 27 April 2017 diff hist −11 How to treat low dimensional systems →Avoid numerical divergences using the Random Integration Method (RIM)
- 04:58, 26 April 2017 diff hist −28 How to analyse excitons →Plot the exciton spatial distribution
- 04:51, 26 April 2017 diff hist +104 How to analyse excitons →Plot the exciton spatial distribution