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 13-Oct-2021 02:42:08 (NZT):

Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and (E1 in ('Al') and E2 in ('Hg' ) and E3 in ('Br') ) order by MeV desc limit 1000"

One row was 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
175772	none	62880	Al	27	f	13	b	Hg	196	b	80	b	Br	81	f	35	b	Ce	142	b	58	b	113.617000

All Nuclides Appearing in Results Table: (4)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
32	27	13	f	b	Al	26.98153840800	224.94588197047	8.33132896187	SPN	50.0000	null	0.0000	100.0000	82300	58	5/2+	3.6407000000	0.1466000000	1170.0000	104.227	6.97627800
106	81	35	f	b	Br	80.91628820600	704.35343630503	8.69572143586	SPN	50.0000	null	0.0000	49.4600	1.18704	null	3/2-	2.2686000000	0.2620000000	277.0000	108.028	7.24977900
214	142	58	b	b	Ce	141.90924988400	1185.25222959520	8.34684668729	SPN	50.0000	null	0.0000	11.0700	7.36155	null	null	null	null	null	null	null
297	196	80	b	b	Hg	195.96583344400	1551.17232499070	7.91414451526	SPN	50.0000	null	0.0000	0.1460	0.0001241	null	null	null	null	null	null	null

All Elements Appearing in Results Table: (4)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
13	Al	Aluminium	3	13	26.98154	118	9.99316	933.47	2792	1.61	42.5	3	13	222316	2700	38	235	904	82300	null	Paramagnetic	null	0.00002110000
35	Br	Bromine	4	17	79.90656	94	25.61108	265.8	332	2.96	324.6	7	8	18600	3120	0	0.12	947.3	2.4	null	Diamagnetic	null	-0.00001530000
58	Ce	Cerium	6	4	140.10507	158	20.94559	1071	3633	1.12	50	4	6	7490	6689	1.4	11	192	66.5	null	Paramagnetic	null	0.00147160000
80	Hg	Mercury	6	12	200.60902	171	14.82260	234.32	629.88	2	0	4	3	3300	13534	1	8.3	139.5	0.085	null	Diamagnetic	null	-0.00002840000