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 12:02:03 (NZT):

Full SQL Query: "select * from TwoToTwoAllNewPlus where e1 in ('n') and a2 in (184) and e2 <> 'Os' and a4 >= 100 and MeV > 115 order by MeV desc limit 202"

5 rows were 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
169479	right	N	14	b	7	f	W	184	b	74	b	1577.54818473	Se	82	b	34	b	Cd	116	b	48	b	1701.01263306	123.464448
169478	right	N	14	b	7	f	W	184	b	74	b	1577.54818473	Ge	76	b	32	b	Sn	122	b	50	b	1697.86049350	120.312309
169477	right	N	14	b	7	f	W	184	b	74	b	1577.54818473	Ge	74	b	32	b	Sn	124	b	50	b	1696.36290491	118.814720
169476	right	N	14	b	7	f	W	184	b	74	b	1577.54818473	Ge	72	b	32	b	Sn	126	b	50	b	1693.30740974	115.759225
169475	right	N	14	b	7	f	W	184	b	74	b	1577.54818473	Zn	70	b	30	b	Te	128	b	52	b	1693.26471936	115.716535

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
18	14	7	b	f	N	14.00307400446	104.65546585700	7.47539041836	SPN	50.0000	null	0.0000	99.6300	18.9297	1105	1+	0.4035730000	0.0204400000	null	null	1.93377980
89	70	30	b	b	Zn	69.92531918100	611.07084473809	8.72958349626	SPN	50.0000	null	0.0000	0.6200	0.434	null	null	null	null	null	null	null
93	72	32	b	b	Ge	71.92207582600	628.66951864558	8.73152109230	SPN	50.0000	null	0.0000	27.4300	0.41145	null	null	null	null	null	null	null
95	74	32	b	b	Ge	73.92117776200	645.64823409601	8.72497613643	SPN	50.0000	null	0.0000	36.5400	0.5481	null	null	null	null	null	null	null
96	76	32	b	b	Ge	75.92140272600	661.58085532802	8.70501125432	UPN	21.2553	2 B-	2.0390	7.6700	0.11505	null	null	null	null	null	null	null
104	82	34	b	b	Se	81.91669953700	712.82370418095	8.69297200221	UPN	20.0414	2 B-	2.9950	8.8200	0.00441	null	null	null	null	null	null	null
163	116	48	b	b	Cd	115.90476323000	987.40659547047	8.51212582302	UPN	19.4916	2 B-	2.8090	7.5800	0.01137	null	null	null	null	null	null	null
174	122	50	b	b	Sn	121.90344400100	1035.49730475840	8.48768282589	SPN	50.0000	null	0.0000	4.9200	0.11316	null	null	null	null	null	null	null
175	124	50	b	b	Sn	123.90527669200	1049.93233740000	8.46719626936	SPN	50.0000	null	0.0000	5.9400	0.13662	null	null	null	null	null	null	null
176	126	50	b	b	Sn	125.90765883600	1063.85555768560	8.44329807687	UPN	5.0000	B-	0.0700	null	null	null	null	null	null	null	null	null
185	128	52	b	b	Te	127.90446131100	1081.41154120770	8.44852766569	UPN	24.3424	2 B-	2.5300	31.7900	0.0003179	null	null	null	null	null	null	null
276	184	74	b	b	W	183.95093326000	1472.89271887610	8.00485173302	SPN	50.0000	null	0.0000	30.6400	0.383	null	null	null	null	null	null	null

All Elements Appearing in Results Table: (8)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
7	N	Nitrogen	2	15	14.00693	56	11196.58705	63.05	77.36	3.04	7	3	7	64360	1.251	null	0.026583	1040	19	960	Diamagnetic	null	-0.00000000680
30	Zn	Zinc	4	12	65.38688	142	9.15783	692.68	1180	1.65	0	2	21	179100	7140	17	120	388	70	null	Diamagnetic	null	-0.00001580000
32	Ge	Germanium	4	14	72.56952	125	13.63320	1211.4	3093	2.01	119	4	5	9020	5323	0.002	60	321.4	1.5	null	Diamagnetic	null	-0.00000798000
34	Se	Selenium	4	16	86.37918	103	17.92471	494	958	2.55	195	6	7	14990	4819	null	0.52	321.2	0.05	null	Diamagnetic	null	-0.00001930000
48	Cd	Cadmium	5	12	112.43420	161	12.99817	594.22	1040	1.69	0	2	3	3616	8650	14	97	230	0.15	null	Diamagnetic	null	-0.00001990000
50	Sn	Tin	5	14	118.97773	145	16.27602	505.08	2875	1.96	107.3	4	5	7456	7310	9.1	67	217	2.3	null	Diamagnetic	null	-0.00002270000
52	Te	Tellurium	5	16	128.58720	123	20.60692	722.66	1261	2.1	190.2	6	7	13200	6240	0.01	3	201	0.001	null	Diamagnetic	null	-0.00002430000
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