Two To Two Reactions - data provided by Dr. Alexander Parkhomov

Conceived by R. W. Greenyer and coded by P. W. Power for the Martin Fleischmann Memorial Project

Version 5.0, Sep 28, 2019

This program enables SQL commands to query the TwoToTwo (2-2) tables created from Dr Parkhomov's two spreadsheets the latest of which includes the effects of neutrinos

To make full use of this and the other database tables, a good grasp of SQL is essential.

It replaces its orginal (and rather misnamed) version "FissionFusion.php".

But note that it and Fission and Fusion is each dedicated to querying only one table ("TwoToTwo", "Fission" and "Fusion" respectively).

The "universal" program All Tables can accept full SQL commands that query any of the 12 "Parkhomov" tables, together with the "ElementProperties", "Nuclides", "RadioNuclides" and "Atomic Radii" tables as well.

New Feature (1): In the checkbox, you may indicate which of the three tables you want effectively included. The resulting query is only on TwoToTwoAll but it uses the new field "neutrino" (setable to "left" and/or "none" and/or "right") to effectively select "TwoToTwoEoL" and/or "TwoToTwo" and/or "TwoToTwoEoR".

New Feature (2): In all the above tables except the Periodic, each atom, in either the input or the output, as well as its 'A' and 'Z' numbers now also has a 'nBorF' ('nuclear Boson or Fermion') and a 'aBorF' ('atomic Boson or Fermion') parameter associated with it.

An atom's nucleus is considered a Boson if its A number is even; if odd a Fermion (thus nBorF = 'b' or 'f'). The atom itself is considered a Boson if its number of neutrons (A - Z) is even; if odd a Fermion (thus aBorF = 'b' or 'f').

The above extra parameters can be used either passively by observing the distributions of 'b' and 'f' in inputs and/or outputs, and/or actively by the New Feature (3) of selecting 'b only', 'f only' or 'either' in the boxes below.

Input used for this run on 12-May-2020 02:16:50 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H', 'D', 'T', 'He') and E2 in ('Ar' ) and E3 in ('C') order by MeV desc"

8 rows were found.

Results Table:

id	neutrino	id_sub	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	E3	A3	nBorF3	Z3	aBorF3	E4	A4	nBorF4	Z4	aBorF4	MeV
9436	right	4638	He	3	f	2	f	Ar	40	b	18	b	C	12	b	6	b	P	31	f	15	b	4.332373
4356	right	4194	D	2	b	1	f	Ar	40	b	18	b	C	12	b	6	b	Si	30	b	14	b	2.538315
1213004	right	432124	T	3	f	1	b	Ar	38	b	18	b	C	12	b	6	b	Si	29	f	14	f	2.126860
9432	none	2474	He	3	f	2	f	Ar	38	b	18	b	C	12	b	6	b	Si	29	f	14	f	2.108900
1210725	none	516856	T	3	f	1	b	Ar	36	b	18	b	C	12	b	6	b	Al	27	f	13	b	1.921000
9426	left	1405	He	3	f	2	f	Ar	36	b	18	b	C	12	b	6	b	Al	27	f	13	b	1.903044
1213007	right	432127	T	3	f	1	b	Ar	40	b	18	b	C	13	f	6	f	Si	30	b	14	b	1.227968
9437	none	2477	He	3	f	2	f	Ar	40	b	18	b	C	13	f	6	f	Si	30	b	14	b	1.210000

All Nuclides Appearing in Results Table (12):

id	A	Z	nBorF	aBorF	E	AMU	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar
4	2	1	b	f	D	2.0141020	1.1122544	SPN	50.0000	null	0.0000	0.0150	0.21	23
5	3	1	f	b	T	3.0160492	2.8273630	SYN	1.0906	b-	0.0186	0.0000	0	null
6	3	2	f	f	He	3.0160300	2.5725468	SPN	50.0000	null	0.0000	0.0001	null	35
13	12	6	b	b	C	12.0000000	7.6802188	SPN	50.0000	null	0.0000	98.8900	197.78	3032
14	13	6	f	f	C	13.0033540	7.4699830	SPN	50.0000	null	0.0000	1.1100	2.22	37
29	27	13	f	b	Al	26.9815350	8.3317448	SPN	50.0000	null	0.0000	100.0000	82300	58
31	29	14	f	f	Si	28.9764910	8.4488277	SPN	50.0000	null	0.0000	4.7000	13254	34
32	30	14	b	b	Si	29.9737610	8.5210123	SPN	50.0000	null	0.0000	3.0900	8713.8	23
33	31	15	f	b	P	30.9737630	8.4812115	SPN	50.0000	null	0.0000	100.0000	1050	null
39	36	18	b	b	Ar	35.9675480	8.5199089	SPN	50.0000	null	0.0000	0.3370	null	77
40	38	18	b	b	Ar	37.9627250	8.6145286	SPN	50.0000	null	0.0000	0.0630	null	null
41	40	18	b	b	Ar	39.9623840	8.5953124	SPN	50.0000	null	0.0000	99.6000	null	null