User contributions for Giacomo.sesti
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23 May 2023
- 10:1810:18, 23 May 2023 diff hist −64 Quasi-particles of a 2D system →Step 2: GW parallel strategies
- 10:0910:09, 23 May 2023 diff hist 0 Quasi-particles of a 2D system →Step 3: Running on GPU
- 10:0910:09, 23 May 2023 diff hist +38 Quasi-particles of a 2D system →Step 3: Running on GPU
- 10:0710:07, 23 May 2023 diff hist −796 Quasi-particles of a 2D system →Step 3: Running on GPU
- 08:3908:39, 23 May 2023 diff hist −4 Quasi-particles of a 2D system →Step 2: GW parallel strategies
- 08:3808:38, 23 May 2023 diff hist +4,329 Quasi-particles of a 2D system →Step 2: GW parallel strategies on a cluster
22 May 2023
- 22:3422:34, 22 May 2023 diff hist +12 Quasi-particles of a 2D system →Step 2: GW parallel strategies on a cluster
- 22:3322:33, 22 May 2023 diff hist +16 Quasi-particles of a 2D system →Step 2: GW parallel strategies on a cluster
- 22:2222:22, 22 May 2023 diff hist −18 Quasi-particles of a 2D system →Step 2: GW parallel strategies on a cluster
- 20:4720:47, 22 May 2023 diff hist −38 Quasi-particles of a 2D system →Step 2: GW parallel strategies on a cluster
- 20:4620:46, 22 May 2023 diff hist +1 Quasi-particles of a 2D system →Step 2: GW parallel strategies on a cluster
- 20:4620:46, 22 May 2023 diff hist +182 Quasi-particles of a 2D system →Step 2: GW parallel strategies on a cluster
- 20:4320:43, 22 May 2023 diff hist +103 Quasi-particles of a 2D system →Step 2: GW parallel strategies on a cluster
- 20:4120:41, 22 May 2023 diff hist −11,394 Quasi-particles of a 2D system →Step 2: GW parallel strategies
- 15:4515:45, 22 May 2023 diff hist 0 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:4515:45, 22 May 2023 diff hist +2 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:4515:45, 22 May 2023 diff hist 0 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:4415:44, 22 May 2023 diff hist +73 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:4315:43, 22 May 2023 diff hist +35 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:4215:42, 22 May 2023 diff hist +6 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:4215:42, 22 May 2023 diff hist −5 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:4015:40, 22 May 2023 diff hist −1 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:3915:39, 22 May 2023 diff hist +1 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:3715:37, 22 May 2023 diff hist +131 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:3515:35, 22 May 2023 diff hist +449 GW on h-BN (standalone) →Beyond the plasmon pole approximation: a full frequency approach - real axis integration
- 15:2215:22, 22 May 2023 diff hist −102 Quasi-particles of a 2D system →Running on GPUs
- 15:1115:11, 22 May 2023 diff hist +4 Quasi-particles of a 2D system →Step 2: GW parallel strategies
- 15:1015:10, 22 May 2023 diff hist +2,761 Quasi-particles of a 2D system →Step 2: GW parallel strategies
- 15:0315:03, 22 May 2023 diff hist +7 GW on h-BN (standalone) →Converging Screening Parameters
- 15:0115:01, 22 May 2023 diff hist −2 GW on h-BN (standalone) →Step 3: Interpolating Band Structures
21 May 2023
- 18:2518:25, 21 May 2023 diff hist −2 Rome 2023 →DAY 2 - Tuesday, 23 May
- 18:2318:23, 21 May 2023 diff hist +158 Rome 2023 →DAY 2 - Tuesday, 23 May
- 18:2018:20, 21 May 2023 diff hist +4 Rome 2023 →DAY 2 - Tuesday, 23 May
- 18:2018:20, 21 May 2023 diff hist −1 Rome 2023 →DAY 2 - Tuesday, 23 May
- 18:2018:20, 21 May 2023 diff hist −9 Rome 2023 →DAY 2 - Tuesday, 23 May
- 18:1518:15, 21 May 2023 diff hist +545 Rome 2023 →DAY 2 - Tuesday, 23 May
- 18:1118:11, 21 May 2023 diff hist 0 Quasi-particles of a 2D system →Step 3: GW parallel strategies
- 18:1118:11, 21 May 2023 diff hist −5 Quasi-particles of a 2D system →Step 1: Speeding up the self-energy convergence
- 18:1018:10, 21 May 2023 diff hist −16 Quasi-particles of a 2D system →Step 1: Speeding up the self-energy convergence
- 18:1018:10, 21 May 2023 diff hist +46 Quasi-particles of a 2D system →Step 2: Speeding up the self-energy convergence
- 18:0918:09, 21 May 2023 diff hist −345 Quasi-particles of a 2D system →Step 1: Initialization
- 18:0718:07, 21 May 2023 diff hist +72 Rome 2023 →DAY 2 - Tuesday, 23 May
- 16:5316:53, 21 May 2023 diff hist −2 Quasi-particles of a 2D system →Step 1: Initialization
- 16:5216:52, 21 May 2023 diff hist −1 Quasi-particles of a 2D system →MPI parallelization
- 16:5116:51, 21 May 2023 diff hist −2 Quasi-particles of a 2D system →Step 1: Initialization
- 16:5016:50, 21 May 2023 diff hist −392 Quasi-particles of a 2D system →Step 1: Initialization
- 16:4616:46, 21 May 2023 diff hist +93 Quasi-particles of a 2D system →RIM-W
- 16:4516:45, 21 May 2023 diff hist +1 Quasi-particles of a 2D system →RIM-W
- 16:4416:44, 21 May 2023 diff hist +89 Quasi-particles of a 2D system →RIM-W
- 16:4216:42, 21 May 2023 diff hist −2 Quasi-particles of a 2D system →RIM-W