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 02:16:42 (NZT):

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

7 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
1213044	right	432164	T	3	f	1	b	Ti	47	f	22	f	C	12	b	6	b	Ar	38	b	18	b	4.734112
9518	none	2510	He	3	f	2	f	Ti	47	f	22	f	C	12	b	6	b	Ar	38	b	18	b	4.716200
1210758	none	516889	T	3	f	1	b	Ti	46	b	22	b	C	12	b	6	b	Cl	37	f	17	b	2.595402
9512	left	1434	He	3	f	2	f	Ti	46	b	22	b	C	12	b	6	b	Cl	37	f	17	b	2.577446
1213054	right	432174	T	3	f	1	b	Ti	49	f	22	f	C	12	b	6	b	Ar	40	b	18	b	1.427308
9534	none	2519	He	3	f	2	f	Ti	49	f	22	f	C	12	b	6	b	Ar	40	b	18	b	1.409400
9527	right	4643	He	3	f	2	f	Ti	48	b	22	b	C	12	b	6	b	K	39	f	19	b	0.245912

All Nuclides Appearing in Results Table (11):

id	A	Z	nBorF	aBorF	E	AMU	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar
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
38	37	17	f	b	Cl	36.9658960	8.5705207	SPN	50.0000	null	0.0000	24.4700	35.4815	null
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
42	39	19	f	b	K	38.9637140	8.5569203	SPN	50.0000	null	0.0000	93.1000	19457.9	null
52	46	22	b	b	Ti	45.9526330	8.6564016	SPN	50.0000	null	0.0000	7.9300	444.08	null
53	47	22	f	f	Ti	46.9517580	8.6612961	SPN	50.0000	null	0.0000	7.2800	407.68	null
54	48	22	b	b	Ti	47.9479480	8.7229436	SPN	50.0000	null	0.0000	73.9400	4140.64	null
55	49	22	f	f	Ti	48.9478670	8.7111863	SPN	50.0000	null	0.0000	5.5100	308.56	null