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 09-Apr-2020 21:08:45 (NZT):

Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and E1 in ('Al') and E2 in ('Al', 'Cr' ) order by MeV desc limit 100"

17 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
166725	none	59778	Al	27	f	13	b	Al	27	f	13	b	He	4	b	2	b	Cr	50	b	24	b	13.428400
166727	none	59780	Al	27	f	13	b	Al	27	f	13	b	O	16	b	8	b	Ar	38	b	18	b	5.058000
166726	none	59779	Al	27	f	13	b	Al	27	f	13	b	C	12	b	6	b	Ca	42	b	20	b	4.137700
166729	none	59782	Al	27	f	13	b	Al	27	f	13	b	Mg	24	b	12	b	Si	30	b	14	b	3.971900
166731	none	59784	Al	27	f	13	b	Al	27	f	13	b	Mg	26	b	12	b	Si	28	b	14	b	3.308700
166728	none	59781	Al	27	f	13	b	Al	27	f	13	b	Ne	20	b	10	b	S	34	b	16	b	2.573700
167139	none	59942	Al	27	f	13	b	Cr	54	b	24	b	Si	30	b	14	b	V	51	f	23	b	2.491700
167140	none	59943	Al	27	f	13	b	Cr	54	b	24	b	P	31	f	15	b	Ti	50	b	22	b	1.733500
167128	none	59939	Al	27	f	13	b	Cr	53	f	24	f	Si	29	f	14	f	V	51	f	23	b	1.599400
167130	none	59940	Al	27	f	13	b	Cr	53	f	24	f	Si	30	b	14	b	V	50	b	23	f	1.173700
167115	none	59925	Al	27	f	13	b	Cr	50	b	24	b	P	31	f	15	b	Ti	46	b	22	b	1.108500
167119	none	59927	Al	27	f	13	b	Cr	50	b	24	b	Ar	38	b	18	b	K	39	f	19	b	1.068400
167120	none	59937	Al	27	f	13	b	Cr	52	b	24	b	Si	28	b	14	b	V	51	f	23	b	1.065600
166730	none	59783	Al	27	f	13	b	Al	27	f	13	b	Mg	25	f	12	f	Si	29	f	14	f	0.688400
167132	none	59941	Al	27	f	13	b	Cr	53	f	24	f	P	31	f	15	b	Ti	49	f	22	f	0.517900
167123	none	59938	Al	27	f	13	b	Cr	52	b	24	b	P	31	f	15	b	Ti	48	b	22	b	0.314800
167118	none	59926	Al	27	f	13	b	Cr	50	b	24	b	Cl	35	f	17	b	Ca	42	b	20	b	0.095900

All Nuclides Appearing in Results Table (27):

id	A	Z	nBorF	aBorF	E	AMU	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar
7	4	2	b	b	He	4.0026030	7.4652	SPN	50.0000	null	0.0000	99.9999	null	275200
13	12	6	b	b	C	12.0000000	8.0714	SPN	50.0000	null	0.0000	98.8900	197.78	3032
18	16	8	b	b	O	15.9949150	8.3674	SPN	50.0000	null	0.0000	99.7590	459888.99	9592
22	20	10	b	b	Ne	19.9924420	8.4234	SPN	50.0000	null	0.0000	90.9200	null	1548
26	24	12	b	b	Mg	23.9850450	8.6518	SPN	50.0000	null	0.0000	78.7000	18337.1	513
27	25	12	f	f	Mg	24.9858400	8.5990	SPN	50.0000	null	0.0000	10.1300	2360.29	69
28	26	12	b	b	Mg	25.9825910	8.6951	SPN	50.0000	null	0.0000	11.1700	2602.61	79
29	27	13	f	b	Al	26.9815350	8.7084	SPN	50.0000	null	0.0000	100.0000	82300	58
30	28	14	b	b	Si	27.9769270	8.8390	SPN	50.0000	null	0.0000	92.2100	260032.2	653
31	29	14	f	f	Si	28.9764910	8.8265	SPN	50.0000	null	0.0000	4.7000	13254	34
32	30	14	b	b	Si	29.9737610	8.8861	SPN	50.0000	null	0.0000	3.0900	8713.8	23
33	31	15	f	b	P	30.9737630	8.8598	SPN	50.0000	null	0.0000	100.0000	1050	null
36	34	16	b	b	S	33.9678650	8.9518	SPN	50.0000	null	0.0000	4.2200	14.77	null
37	35	17	f	b	Cl	34.9688550	8.9003	SPN	50.0000	null	0.0000	75.5300	109.5185	null
40	38	18	b	b	Ar	37.9627250	8.9851	SPN	50.0000	null	0.0000	0.0630	null	null
42	39	19	f	b	K	38.9637140	8.9381	SPN	50.0000	null	0.0000	93.1000	19457.9	null
46	42	20	b	b	Ca	41.9586280	8.9890	SPN	50.0000	null	0.0000	0.6400	265.6	null
52	46	22	b	b	Ti	45.9526330	9.0306	SPN	50.0000	null	0.0000	7.9300	444.08	null
54	48	22	b	b	Ti	47.9479480	9.0815	SPN	50.0000	null	0.0000	73.9400	4140.64	null
55	49	22	f	f	Ti	48.9478670	9.0624	SPN	50.0000	null	0.0000	5.5100	308.56	null
56	50	22	b	b	Ti	49.9447900	9.0999	SPN	50.0000	null	0.0000	5.3400	299.04	null
57	50	23	b	f	V	49.9471650	9.0557	UPN	17.1461	b+ or b-	2.2050	0.2400	0.288	null
58	51	23	f	b	V	50.9439780	9.0946	SPN	50.0000	null	0.0000	99.7600	119.712	null
59	50	24	b	b	Cr	49.9460510	9.0764	SPN	50.0000	null	0.0000	4.3100	4.3962	null
60	52	24	b	b	Cr	51.9405140	9.1370	SPN	50.0000	null	0.0000	83.7600	85.4352	null
61	53	24	f	f	Cr	52.9406510	9.1145	SPN	50.0000	null	0.0000	9.5500	9.741	null
62	54	24	b	b	Cr	53.9388790	9.1257	SPN	50.0000	null	0.0000	2.3800	2.4276	null