updated Oktober 2023
Number in front is the number of the storyline as is presented in the index
1 | grav14.html#gra9
and sea4.html#sea3 |
Renormalization procedure is every subsequent moment set up as new, without accumulation from one moment to the next, in grav14.html#gra9. There should be no building-up effect from one moment to the next. However, in sea4.html#sea3 paragraph RenormalizationARGUMENTS 1 and 2 point out the routes traversed by the virtual particles may or may be not dragged along in the act of gravity. Decision is not yet possible. |
2 | seaexp2#exper2 | Speed of branching of localities/universes |
2 | seaexp2#exper1 | There is one more peculiarity to view |
2 | seaexp4 | solution of the riddle |
4 | timedir6 | create [Figure] in middle of text of What is a coupling |
4 | timedir9 | implement Possibility 3 (at the end of the paragraph) |
4 | timedir13 | Very unfinished and pretty scary too |
5 | netreal3, netreal4 | retype Turbo Pascal PROGRAM BertKlaasDeeltjes |
8 | qqd9#qqd92 | Each of these two quarks has color too and each color consists of two Pauli matrices |
9 | netqcd6#qcd53 | Conjecture: in a sense that there is no net Higgs field absorption and thus no gravitation and no time |
9 | netqcd6#qcd59 | The h-c conjecture |
9 | netqcd10 | p8 of QCD, Color confinement. Reread & revise. |
9 | netqcd16#qcd2 | An early effort - Work out & finish diagram with 3 colors |
10 | mass2 | Here I am |
11 | grav8#grav81 | The sagging in of shells at vacuum marble level |
11 | grav8#grav82 | The sagging in of shells propagation speed |
11 | grav1 | Incorporate the uncertainty relations as superposition of states; the 3 actions of QED |
12 | grav7#grav72 | (2.7) - (2.9) Does the black glueball have mass? |
12 | grav9.html#grav80 | Construct the vacuum from sole color 1 spin 0 gluons. But this trick can be applied to the sole color -1 spin 0 gluon too and that's not what we want. |
12 | grav3.html#grav86 | If Pauli matrices determine color AND spin, then when one multiplication order is forbidden, because e.g. yielding -i, then also one spin is forbidden, e.g. spin down. This is the hallmark of the weak force. |
12 | grav10 | Is Neutrino 1 and Neutrino 2 solved by the view of qg4 and qg5? |
13 | grav2#grav23 | Transform disordered motion into an orderly expansion |
13 | grav2#grav29 | Gas cooling by highly negative curvature? (column at the right) |
13 | expan2.html#expan13 | The sink drain |
13 | expan2.html#expan4 | The bouncing ball |
13 | expan2.html#expan7 | The only clue for dark matter (column at the right) |
13 | expan3.html | tekst in this font |
13 | expan3.html#expan33 | Dark matter and inflation: black and white glueballs |
14 | sr8.html | Deriving SR from QM |
14 | sea3.html#sea32 | Gluons and photons outside of time |
21 | cir12.html | Calculations (column at the right) |