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 29-Jan-2024 03:05:52 (NZT):

Full SQL Query: "select * from TwoToTwoAll where A1 = 16 and E2 in ('Cu') and E3 in ('Ar') and E4 in ('Ca' ) 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
82026	right	50006	O	16	b	8	b	Cu	65	f	29	b	Ar	38	b	18	b	Ca	43	f	20	f	1.114061

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
20	16	8	b	b	O	15.99491461960	127.61572713267	7.97598294579	SPN	50.0000	null	0.0000	99.7590	459888.99	9592	null	null	null	null	null	null
44	38	18	b	b	Ar	37.96273210400	327.33413710958	8.61405623973	SPN	50.0000	null	0.0000	0.0630	null	null	null	null	null	null	null	null
52	43	20	f	f	Ca	42.95876643000	369.81890795747	8.60043971994	SPN	50.0000	null	0.0000	0.1450	60.175	null	7/2-	-1.3173300000	-0.0408000000	null	null	-1.80306900
84	65	29	f	b	Cu	64.92778948700	569.19666729878	8.75687180460	SPN	50.0000	null	0.0000	30.9100	18.546	null	3/2-	2.3844000000	-0.2040000000	201.0000	113.669	7.60430000

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
8	O	Oxygen	2	16	15.99938	48	11196.20378	54.8	90.2	3.44	141	2	8	84078	1.429	null	0.02658	919	461000	10400	Paramagnetic	null	0.00000190772
18	Ar	Argon	3	18	39.94766	71	22392.18700	83.8	87.3	null	0	2	18	427066	1.784	null	0.01772	520.33	null	null	Diamagnetic	null	-0.00000001070
20	Ca	Calcium	4	2	40.07586	194	25.85539	1115	1757	1	2.37	2	20	527762	1550	29	200	631	41500	null	Paramagnetic	null	0.00002139000
29	Cu	Copper	4	11	63.54724	145	7.12413	1357.77	3200	1.9	118.4	4	29	1116105	8920	59	400	384.4	60	null	Diamagnetic	null	-0.00000963000