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 16-Dec-2021 11:37:04 (NZT):

Full SQL Query: "select * from TwoToTwoAllNewPlus where E1 in ('O') and E2 in ('W' ) and E4 IN ('Mo') and MeV > 110 limit 104"

One row was found.

Results Table:

id	neutrino	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	BEin	E3	A3	nBorF3	Z3	aBorF3	E4	A4	nBorF4	Z4	aBorF4	BEout	MeV
197206	none	O	16	b	8	b	W	180	b	74	b	1572.15484124	Zr	96	b	40	b	Mo	100	b	42	b	1689.41363719	117.258796

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
127	96	40	b	b	Zr	95.90827762100	828.96988821546	8.63510300224	UPN	19.3010	2 B-	3.4000	2.8000	4.62	null	null	null	null	null	null	null
135	100	42	b	b	Mo	99.90746797600	860.44374897168	8.60443748972	UPN	18.8923	2 B-	3.0350	9.1300	0.10956	null	null	null	null	null	null	null
273	180	74	b	b	W	179.94671343500	1444.53911410570	8.02521730059	UPN	18.2555	A	2.5090	0.1400	0.00175	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
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
40	Zr	Zirconium	5	4	91.22340	206	14.01066	2128	4682	1.33	41.1	4	6	9500	6511	2.4	23	278	165	null	Paramagnetic	null	0.00010900000
42	Mo	Molybdenum	5	6	95.21689	190	9.26234	2896	4912	2.16	71.9	6	30	154500	10280	20	139	251	1.2	null	Paramagnetic	null	0.00012030000
74	W	Tungsten	6	6	183.84152	193	9.55021	3695	5828	2.36	78.6	6	2	1700	19250	20	170	132	1.25	null	Paramagnetic	null	0.00008840000