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 26-May-2020 08:04:13 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H', 'O', 'N', 'C') and (A1 = 14 or A1 = 16 or A1 = 12) and E2 in ('Mg', 'Na', 'Cl', 'Ca', 'S', 'Fe') and (A2 = 26 or A2 = 35 or A2 = 40 or A2 = 37 or A2 = 24) and E4 in ('K') and E3 in ('H', 'O', 'C', 'N', 'S') and (A4 = 39) order by MeV desc limit 100"

5 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
65916	right	844	N	14	b	7	f	Mg	26	b	12	b	H	1	f	1	b	K	39	f	19	b	13.314771
81777	none	24841	O	16	b	8	b	Mg	24	b	12	b	H	1	f	1	b	K	39	f	19	b	7.844100
66019	right	6263	N	14	b	7	f	Cl	37	f	17	b	C	12	b	6	b	K	39	f	19	b	5.052418
66139	left	10352	N	14	b	7	f	Ca	40	b	20	b	N	15	f	7	b	K	39	f	19	b	1.871374
81821	none	25011	O	16	b	8	b	Cl	35	f	17	b	C	12	b	6	b	K	39	f	19	b	0.052200

All Nuclides Appearing in Results Table (11):

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar
3	1	1	f	b	H	1.00782503223	0.00000000000	0.00000000000	SPN	50.0000	null	0.0000	99.9850	1399.79	705700
13	12	6	b	b	C	12.00000000000	92.15904307956	7.67992025663	SPN	50.0000	null	0.0000	98.8900	197.78	3032
16	14	7	b	f	N	14.00307400443	104.65546588494	7.47539042035	SPN	50.0000	null	0.0000	99.6300	18.9297	1105
17	15	7	f	b	N	15.00010889888	115.48853186480	7.69923545765	SPN	50.0000	null	0.0000	0.3700	0.0703	null
18	16	8	b	b	O	15.99491461957	127.61572716061	7.97598294754	SPN	50.0000	null	0.0000	99.7590	459888.99	9592
26	24	12	b	b	Mg	23.98504169700	198.25166064327	8.26048586014	SPN	50.0000	null	0.0000	78.7000	18337.1	513
28	26	12	b	b	Mg	25.98259296800	216.67481175445	8.33364660594	SPN	50.0000	null	0.0000	11.1700	2602.61	79
37	35	17	f	b	Cl	34.96885268200	298.20192590959	8.52005502599	SPN	50.0000	null	0.0000	75.5300	109.5185	null
38	37	17	f	b	Cl	36.96590260200	317.09208263639	8.57005628747	SPN	50.0000	null	0.0000	24.4700	35.4815	null
42	39	19	f	b	K	38.96370648640	333.71525897689	8.55680151223	SPN	50.0000	null	0.0000	93.1000	19457.9	null
45	40	20	b	b	Ca	39.96259086300	342.04320940400	8.55108023510	SPN	50.0000	null	0.0000	96.9700	40242.55	60