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 created from Dr Parkhomov's two spreadsheets the latest of which includes the effects of neutrinos

To make full use of this and the other database tables, a good grasp of SQL is essential.

It replaces its orginal (and rather misnamed) version "FissionFusion.php".

But note that it and Fission and Fusion is each dedicated to querying only one table ("TwoToTwo", "Fission" and "Fusion" respectively).

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.

New Feature (1): In the checkbox, you may indicate which of the three tables you want effectively included. The resulting query is only on TwoToTwoAll but it uses the new field "neutrino" (setable to "left" and/or "none" and/or "right") to effectively select "TwoToTwoEoL" and/or "TwoToTwo" and/or "TwoToTwoEoR".

New Feature (2): 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 if its A number is even; if odd a Fermion (thus nBorF = 'b' or 'f'). The atom itself is considered a Boson if its number of neutrons (A - Z) is even; if odd a Fermion (thus aBorF = 'b' or 'f').

The above extra parameters can be used either passively by observing the distributions of 'b' and 'f' in inputs and/or outputs, and/or actively by the New Feature (3) of selecting 'b only', 'f only' or 'either' in the boxes below.

Input used for this run on 11-Mar-2020 23:47:40 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H') and E2 in ('W' ) and neutrino='left' order by MeV desc limit 100"

12 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
3685	left	1239	H	1	f	1	b	W	183	f	74	f	Ca	48	b	20	b	Xe	136	b	54	b	91.781047
3614	left	1218	H	1	f	1	b	W	180	b	74	b	Ne	21	f	10	f	Gd	160	b	64	b	31.518036
3611	left	1219	H	1	f	1	b	W	180	b	74	b	O	18	b	8	b	Dy	163	f	66	f	25.406504
3609	left	1220	H	1	f	1	b	W	180	b	74	b	O	17	f	8	f	Dy	164	b	66	b	25.002235
3605	left	1221	H	1	f	1	b	W	180	b	74	b	C	13	f	6	f	Er	168	b	68	b	17.764526
3642	left	1234	H	1	f	1	b	W	182	b	74	b	C	13	f	6	f	Er	170	b	68	b	16.050577
3600	left	1222	H	1	f	1	b	W	180	b	74	b	He	4	b	2	b	Hf	177	f	72	f	8.124494
3663	left	1240	H	1	f	1	b	W	183	f	74	f	He	4	b	2	b	Hf	180	b	72	b	8.105864
3636	left	1235	H	1	f	1	b	W	182	b	74	b	He	4	b	2	b	Hf	179	f	72	f	6.960126
3601	left	1223	H	1	f	1	b	W	180	b	74	b	Be	9	f	4	f	Yb	172	b	70	b	5.643925
3637	left	1236	H	1	f	1	b	W	182	b	74	b	Be	9	f	4	f	Yb	174	b	70	b	4.554077
3691	left	1242	H	1	f	1	b	W	184	b	74	b	Be	9	f	4	f	Yb	176	b	70	b	3.622583

All Nuclides Appearing in Results Table (24):

id	A	Z	nBorF	aBorF	E	AMU	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar
3	1	1	f	b	H	1.0078250	0.7824	SPN	50.0000	null	0.0000	99.9850	1399.79	705700
7	4	2	b	b	He	4.0026030	7.4652	SPN	50.0000	null	0.0000	99.9999	null	275200
10	9	4	f	f	Be	9.0121860	6.8101	SPN	50.0000	null	0.0000	100.0000	2.8	null
14	13	6	f	f	C	13.0033540	7.8311	SPN	50.0000	null	0.0000	1.1100	2.22	37
19	17	8	f	f	O	16.9991340	8.1188	SPN	50.0000	null	0.0000	0.0370	170.57	null
20	18	8	b	b	O	17.9991600	8.1149	SPN	50.0000	null	0.0000	0.2040	940.44	null
23	21	10	f	f	Ne	20.9938490	8.3442	SPN	50.0000	null	0.0000	0.2570	null	null
50	48	20	b	b	Ca	47.9523630	8.9958	UPN	19.3619	2 b-	4.2740	0.1800	74.7	null
180	136	54	b	b	Xe	135.9072210	8.7068	UPN	21.3354	2 b-	2.4620	8.8700	null	null
219	160	64	b	b	Gd	159.9271200	8.4957	SPN	50.0000	null	0.0000	21.9000	1.3578	null
226	163	66	f	f	Dy	162.9283700	8.4807	SPN	50.0000	null	0.0000	24.9700	1.29844	null
227	164	66	b	b	Dy	163.9288300	8.4756	SPN	50.0000	null	0.0000	28.1800	1.46536	null
233	168	68	b	b	Er	167.9323800	8.4463	SPN	50.0000	null	0.0000	27.0700	0.94745	null
234	170	68	b	b	Er	169.9355100	8.4248	SPN	50.0000	null	0.0000	14.8800	0.5208	null
238	172	70	b	b	Yb	171.9365600	8.4150	SPN	50.0000	null	0.0000	21.8100	0.69792	null
240	174	70	b	b	Yb	173.9390200	8.3978	SPN	50.0000	null	0.0000	31.8400	1.01888	null
241	176	70	b	b	Yb	175.9427400	8.3744	SPN	50.0000	null	0.0000	12.7300	0.40736	null
246	177	72	f	f	Hf	176.9434800	8.3688	SPN	50.0000	null	0.0000	18.5000	0.555	null
248	179	72	f	f	Hf	178.9460200	8.3523	SPN	50.0000	null	0.0000	13.7500	0.4125	null
249	180	72	b	b	Hf	179.9468100	8.3466	SPN	50.0000	null	0.0000	35.2400	1.0572	null
252	180	74	b	b	W	179.9469800	8.3458	UPN	18.2555	a	2.5090	0.1400	0.00175	null
253	182	74	b	b	W	181.9482700	8.3361	SPN	50.0000	null	0.0000	26.4100	0.330125	null
254	183	74	f	f	W	182.9502900	8.3244	SPN	50.0000	null	0.0000	14.4000	0.18	null
255	184	74	b	b	W	183.9509900	8.3195	SPN	50.0000	null	0.0000	30.6400	0.383	null