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 originally created from Dr Parkhomov's spreadsheets.

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

But note that it and Fission and Fusion is each dedicated to querying only one of two tables.

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.

You may indicate which of the three neutrino conditions to include: "left" and/or "none" and/or "right". The default condition is include all three.

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 ('b') if its A number is even; if odd a Fermion ('f'). The atom itself is considered a Boson ('b') if its number of neutrons (A - Z) is even; if odd a Fermion ('f').

These parameters can be used either passively, by observing the distributions of 'b' and 'f' in inputs and/or outputs, and/or actively, by selecting 'b only', 'f only' or 'either' in the boxes below.

NB: To avoid unnecessary duplication in all TwoToTwo tables, two rules independently apply: A1 <= A2 and A3 <= A4. These rules also apply implicitly in that, if the input side of the Core Query only involves E1 and E2, only rows whose associated mass numbers obey A1 <= A2 will appear in the results. Similarly with E3 and E4 on the output side, only rows whose associated mass numbers obey A3 <= A4 will appear in the results.

Input used for this run on 22-Aug-2020 06:23:45 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('N') and E2 in ('N' ) and E3 in ('C') 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
65810	none	20738	N	14	b	7	f	N	14	b	7	f	C	12	b	6	b	O	16	b	8	b	10.776500
65817	none	20743	N	14	b	7	f	N	15	f	7	b	C	13	f	6	f	O	16	b	8	b	4.732900
65816	none	20742	N	14	b	7	f	N	15	f	7	b	C	12	b	6	b	O	17	f	8	f	3.927200
65811	left	10202	N	14	b	7	f	N	14	b	7	f	C	13	f	6	f	N	15	f	7	b	2.814977
75327	none	20745	N	15	f	7	b	N	15	f	7	b	C	12	b	6	b	O	18	b	8	b	0.983700

All Nuclides Appearing in Results Table:

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz
13	12	6	b	b	C	12.00000000000	92.15904307956	7.67992025663	SPN	50.0000	null	0.0000	98.8900	197.78	3032	null	null	null	null	null
14	13	6	f	f	C	13.00335483507	97.10512018346	7.46962462950	SPN	50.0000	null	0.0000	1.1100	2.22	37	1/2-	0.7023690000	null	1.0000	100.589
16	14	7	b	f	N	14.00307400443	104.65546588494	7.47539042035	SPN	50.0000	null	0.0000	99.6300	18.9297	1105	1+	0.4035730000	0.0204400000	null	null
17	15	7	f	b	N	15.00010889888	115.48853186480	7.69923545765	SPN	50.0000	null	0.0000	0.3700	0.0703	null	1/2-	-0.2830569000	null	0.0220	40.547
18	16	8	b	b	O	15.99491461957	127.61572716061	7.97598294754	SPN	50.0000	null	0.0000	99.7590	459888.99	9592	null	null	null	null	null
19	17	8	f	f	O	16.99913175650	131.75857496811	7.75050440989	SPN	50.0000	null	0.0000	0.0370	170.57	null	5/2+	-1.8935430000	-0.0256000000	0.0610	50.227
20	18	8	b	b	O	17.99915961286	139.80371388824	7.76687299379	SPN	50.0000	null	0.0000	0.2040	940.44	null	null	null	null	null	null