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 26-Jul-2022 12:23:16 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H', 'O', 'K') and E2 in ('Sr' ) and E3 in ('C') order by MeV desc limit 1000"

9 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
97403	none	26524	O	18	b	8	b	Sr	84	b	38	b	C	12	b	6	b	Zr	90	b	40	b	7.653200
90012	left	14020	O	17	f	8	f	Sr	84	b	38	b	C	12	b	6	b	Y	89	f	39	b	6.594980
97444	none	26603	O	18	b	8	b	Sr	86	b	38	b	C	12	b	6	b	Zr	92	b	40	b	3.567600
97404	left	14029	O	18	b	8	b	Sr	84	b	38	b	C	13	f	6	f	Y	89	f	39	b	3.494968
90095	none	26632	O	17	f	8	f	Sr	87	f	38	f	C	12	b	6	b	Zr	92	b	40	b	3.198800
90056	none	26589	O	17	f	8	f	Sr	86	b	38	b	C	12	b	6	b	Zr	91	f	40	f	2.928600
97475	right	6523	O	18	b	8	b	Sr	87	f	38	f	C	12	b	6	b	Nb	93	f	41	b	1.890927
90057	none	26590	O	17	f	8	f	Sr	86	b	38	b	C	13	f	6	f	Zr	90	b	40	b	0.670700
97476	none	26649	O	18	b	8	b	Sr	87	f	38	f	C	13	f	6	f	Zr	92	b	40	b	0.098700

All Nuclides Appearing in Results Table: (12)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
15	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	null
16	13	6	f	f	C	13.00335483521	97.10512005305	7.46962461947	SPN	50.0000	null	0.0000	1.1100	2.22	37	1/2-	0.7023690000	null	1.0000	100.589	6.72828600
21	17	8	f	f	O	16.99913175664	131.75857483770	7.75050440222	SPN	50.0000	null	0.0000	0.0370	170.57	null	5/2+	-1.8935430000	-0.0256000000	0.0610	50.227	-3.62806000
22	18	8	b	b	O	17.99915961284	139.80371390688	7.76687299483	SPN	50.0000	null	0.0000	0.2040	940.44	null	null	null	null	null	null	null
116	84	38	b	b	Sr	83.91341912000	728.89223431142	8.67728850371	SPN	50.0000	null	0.0000	0.5600	2.072	null	null	null	null	null	null	null
117	86	38	b	b	Sr	85.90926072631	748.90792839362	8.70823172551	SPN	50.0000	null	0.0000	9.8600	36.482	null	null	null	null	null	null	null
118	87	38	f	f	Sr	86.90887749615	757.33599207773	8.70501140319	SPN	50.0000	null	0.0000	7.0200	25.974	null	9/2+	-1.0931600000	0.3050000000	null	null	-1.16393800
121	89	39	f	b	Y	88.90584120500	775.52412059225	8.71375416396	SPN	50.0000	null	0.0000	100.0000	33	null	1/2-	-0.1372980000	null	null	null	-1.31627900
122	90	40	b	b	Zr	89.90469875800	783.87705705078	8.70974507834	SPN	50.0000	null	0.0000	51.4600	84.909	null	null	null	null	null	null	null
123	91	40	f	f	Zr	90.90564022300	791.07117469965	8.69308983186	SPN	50.0000	null	0.0000	11.2300	18.5295	null	5/2+	-1.3022000000	-0.1760000000	null	null	-2.49743000
124	92	40	b	b	Zr	91.90503532200	799.70572351514	8.69245351647	SPN	50.0000	null	0.0000	17.1100	28.2315	null	null	null	null	null	null	null
128	93	41	f	b	Nb	92.90637316100	805.74828761906	8.66396008193	SPN	50.0000	null	0.0000	100.0000	20	null	9/2+	6.1630000000	-0.3200000000	2740.0000	97.904	6.56740000

All Elements Appearing in Results Table: (6)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
6	C	Carbon	2	14	12.01114	67	5.31466	3823	4300	2.55	153.9	4	6	47277	2260	0.1	140	710	200	4600	Diamagnetic	null	-0.00001400000
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
38	Sr	Strontium	5	2	87.61644	219	33.31424	1050	1655	0.95	5.03	2	11	31270	2630	7.7	35	300	370	null	Paramagnetic	null	0.00000347000
39	Y	Yttrium	5	3	88.90543	212	19.88046	1799	3618	1.22	29.6	3	12	36090	4472	1.8	17	298	33	null	Paramagnetic	null	0.00029780000
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
41	Nb	Niobium	5	5	92.90602	198	10.84084	2750	5017	1.6	86.1	5	7	12100	8570	6.7	54	265	20	null	Paramagnetic	null	0.00023700000