User contributions for Pmelo
15 October 2024
- 12:4112:41, 15 October 2024 diff hist −5 Time-evolution algorithm →Independent-particle approximation
- 12:3712:37, 15 October 2024 diff hist −30 LANCZOSTHR No edit summary
- 12:1812:18, 15 October 2024 diff hist +404 Category:Bethe-Salpeter equations →Time evolution
- 12:0212:02, 15 October 2024 diff hist +400 IBSE No edit summary
14 October 2024
- 15:5315:53, 14 October 2024 diff hist +53 Time-evolution algorithm →The macroscopic-dielectric function as a time-dependent integral
- 15:4515:45, 14 October 2024 diff hist +36 Time-evolution algorithm No edit summary
- 15:2315:23, 14 October 2024 diff hist −16 IBSE No edit summary
3 October 2024
- 16:3316:33, 3 October 2024 diff hist +132 Time-evolution algorithm No edit summary
- 14:5914:59, 3 October 2024 diff hist +110 Time-evolution algorithm No edit summary
- 14:5614:56, 3 October 2024 diff hist +100 Time-evolution algorithm →Related tags and articles
- 14:5514:55, 3 October 2024 diff hist +157 Time-evolution algorithm →Related tags and articles
- 10:0610:06, 3 October 2024 diff hist +15 LANCZOSTHR No edit summary
2 October 2024
- 14:2414:24, 2 October 2024 diff hist +822 N LANCZOSTHR Created page with "{TAGDEF|LANCZOSTHR|[real]}} {{DEF|LANCZOSTHR| <math>10^{-3}</math> | }} Description: {{TAG|LANCZOSTHR}} is used by the BSE Lanczos algorithm to stop the iterative procedure, once the dielectric function has reached numerical convergence. The difference between the dielectric function at two consecutive iterations, <math>i</math> and <math>i+1</math> is computed as root-mean-square over the frequency grid sampling ::<math> \mathrm{RMS}[\epsilon] = \sqrt{\sum_{j=1}^N\le..."
- 13:5213:52, 2 October 2024 diff hist +451 Category:Bethe-Salpeter equations No edit summary
- 13:2113:21, 2 October 2024 diff hist +201 IBSE No edit summary
30 September 2024
- 16:3216:32, 30 September 2024 diff hist +904 Category:Bethe-Salpeter equations No edit summary
10 August 2024
- 11:0111:01, 10 August 2024 diff hist +731 Time-evolution algorithm No edit summary
8 August 2024
19 July 2024
- 16:2716:27, 19 July 2024 diff hist +434 Time-evolution algorithm →Comparison to other methods
- 16:1616:16, 19 July 2024 diff hist +532 Time-evolution algorithm →Perturbing all transitions with a delta-like potential
17 July 2024
- 16:1016:10, 17 July 2024 diff hist +12 Time-evolution algorithm →Choosing the direction of perturbation
- 15:5915:59, 17 July 2024 diff hist −10 Time-evolution algorithm →Hartree exchange potential
- 15:5815:58, 17 July 2024 diff hist −16 Time-evolution algorithm →Hartree exchange potential
- 15:4315:43, 17 July 2024 diff hist +401 Category:Dielectric properties →Other dielectric properties
12 July 2024
- 13:3413:34, 12 July 2024 diff hist +2 Time-evolution algorithm →The many-body terms in the hamiltonian
11 July 2024
- 13:5613:56, 11 July 2024 diff hist 0 Time-evolution algorithm →Step 2: time-evolution run
- 13:5613:56, 11 July 2024 diff hist +10 Time-evolution algorithm →Step 2: time-evolution run
- 13:5513:55, 11 July 2024 diff hist +204 Time-evolution algorithm →Step 2: time-evolution run
- 13:3213:32, 11 July 2024 diff hist −1 Time-evolution algorithm →The many-body terms in the hamiltonian
- 13:3113:31, 11 July 2024 diff hist −127 Time-evolution algorithm →Ladder diagrams from many-body perturbation theory
- 13:3113:31, 11 July 2024 diff hist +281 Time-evolution algorithm →The many-body terms in the hamiltonian
- 13:0613:06, 11 July 2024 diff hist 0 Time-evolution algorithm →The many-body terms in the hamiltonian
- 13:0513:05, 11 July 2024 diff hist −8 Time-evolution algorithm →The many-body terms in the hamiltonian
- 13:0513:05, 11 July 2024 diff hist +204 Time-evolution algorithm →The many-body terms in the hamiltonian
- 13:0313:03, 11 July 2024 diff hist +559 Time-evolution algorithm →Ladder diagrams from many-body perturbation theory
- 12:5912:59, 11 July 2024 diff hist +1,061 Time-evolution algorithm →Exchange-correlation effects from time-dependent density functional theory
- 12:4412:44, 11 July 2024 diff hist +93 Time-evolution algorithm →Hartree exchange potential
- 12:2412:24, 11 July 2024 diff hist +849 Time-evolution algorithm →Hartree exchange potential
- 12:1712:17, 11 July 2024 diff hist +4 Time-evolution algorithm →Independent-particle approximation
- 12:1412:14, 11 July 2024 diff hist 0 Time-evolution algorithm →Ladder diagrams from many-body perturbation theory
- 12:1112:11, 11 July 2024 diff hist +5 Time-evolution algorithm →Ladder diagrams from many-body perturbation theory
- 12:1012:10, 11 July 2024 diff hist −2 Time-evolution algorithm →The many-body terms in the hamiltonian
- 12:0912:09, 11 July 2024 diff hist +246 Time-evolution algorithm →The many-body terms in the hamiltonian
- 11:5511:55, 11 July 2024 diff hist +285 Time-evolution algorithm →The many-body terms in the hamiltonian
- 11:5211:52, 11 July 2024 diff hist +435 Time-evolution algorithm →Independent-particle approximation
- 11:3811:38, 11 July 2024 diff hist −3 Time-evolution algorithm →Choosing the direction of perturbation
- 11:3711:37, 11 July 2024 diff hist +5 Time-evolution algorithm →Setting up the bands
- 11:3211:32, 11 July 2024 diff hist +951 Time-evolution algorithm →Choosing the direction of perturbation
- 10:1410:14, 11 July 2024 diff hist +517 Time-evolution algorithm →Setting up the time-step
- 09:5809:58, 11 July 2024 diff hist +1,063 Time-evolution algorithm →Step 2: time-evolution run