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 17-Apr-2022 09:54:34 (NZT):

Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and (A2 in (208 ) and E4 in ('Sn') ) order by MeV desc limit 100"

6 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
224844	none	92395	S	32	b	16	b	Pb	208	b	82	b	Cd	116	b	48	b	Sn	124	b	50	b	128.982000
276466	none	113775	Ar	36	b	18	b	Pb	208	b	82	b	Sn	122	b	50	b	Sn	122	b	50	b	127.961000
276465	none	113774	Ar	36	b	18	b	Pb	208	b	82	b	Sn	120	b	50	b	Sn	124	b	50	b	127.449000
305177	none	123981	K	39	f	19	b	Pb	208	b	82	b	Sb	123	f	51	b	Sn	124	b	50	b	121.996000
285849	none	113791	Ar	38	b	18	b	Pb	208	b	82	b	Sn	122	b	50	b	Sn	124	b	50	b	121.764000
292937	none	113796	Ar	40	b	18	b	Pb	208	b	82	b	Sn	124	b	50	b	Sn	124	b	50	b	119.742000

All Nuclides Appearing in Results Table: (11)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
37	32	16	b	b	S	31.97207117443	271.77299097355	8.49290596792	SPN	50.0000	null	0.0000	95.0000	332.5	396	null	null	null	null	null	null
43	36	18	b	b	Ar	35.96754510500	306.70868002741	8.51968555632	SPN	50.0000	null	0.0000	0.3370	null	77	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
45	40	18	b	b	Ar	39.96238312378	343.80138413029	8.59503460326	SPN	50.0000	null	0.0000	99.6000	null	null	null	null	null	null	null	null
46	39	19	f	b	K	38.96370648661	333.71525878127	8.55680150721	SPN	50.0000	null	0.0000	93.1000	19457.9	null	3/2+	0.3914700000	0.0585000000	null	null	1.25006120
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
173	120	50	b	b	Sn	119.90220187300	1020.51216602870	8.50426805024	SPN	50.0000	null	0.0000	32.8500	0.75555	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
178	123	51	f	b	Sb	122.90421401600	1042.06879370080	8.47210401383	SPN	50.0000	null	0.0000	42.7500	0.0855	null	7/2+	2.5457000000	-0.6920000000	111.0000	51.836	3.48920000
309	208	82	b	b	Pb	207.97665191800	1636.38335448150	7.86722766578	SPN	50.0000	null	0.0000	52.3000	7.322	null	null	null	null	null	null	null

All Elements Appearing in Results Table: (7)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
16	S	Sulfur	3	16	32.05750	88	16.35587	388.36	717.87	2.58	200	6	16	337138	1960	0	0.205	705	350	440	Diamagnetic	null	-0.00001220000
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
19	K	Potassium	4	1	39.09811	243	45.67536	336.53	1032	0.82	48.4	1	19	476063	856	14	100	757	20900	null	Paramagnetic	null	0.00000574000
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
51	Sb	Antimony	5	15	121.75892	133	18.18111	903.78	1860	2.05	103.2	5	6	10400	6697	2.5	24	207	0.2	null	Diamagnetic	null	-0.00007300000
82	Pb	Lead	6	14	207.17711	154	18.26959	600.61	2022	2.33	35.1	4	5	6640	11340	4.8	35	127	14	null	Diamagnetic	null	-0.00001700000