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 20-Apr-2020 09:14:34 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H', 'D') and E2 in ('Pd' ) and A3 = 12 order by MeV desc"

15 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
5653	left	368	D	2	b	1	f	Pd	102	b	46	b	C	12	b	6	b	Zr	92	b	40	b	13.461955
5768	right	4279	D	2	b	1	f	Pd	105	f	46	f	C	12	b	6	b	Mo	95	f	42	f	12.129910
5716	right	4276	D	2	b	1	f	Pd	104	b	46	b	C	12	b	6	b	Mo	94	b	42	b	12.036761
5654	right	4271	D	2	b	1	f	Pd	102	b	46	b	C	12	b	6	b	Mo	92	b	42	b	11.878407
5806	right	4283	D	2	b	1	f	Pd	106	b	46	b	C	12	b	6	b	Mo	96	b	42	b	11.878407
5840	right	4288	D	2	b	1	f	Pd	108	b	46	b	C	12	b	6	b	Mo	98	b	42	b	11.654848
5715	left	397	D	2	b	1	f	Pd	104	b	46	b	C	12	b	6	b	Zr	94	b	40	b	10.732677
5856	right	4292	D	2	b	1	f	Pd	110	b	46	b	C	12	b	6	b	Mo	100	b	42	b	10.276237
5805	left	420	D	2	b	1	f	Pd	106	b	46	b	C	12	b	6	b	Zr	96	b	40	b	8.478461
903	right	4277	H	1	f	1	b	Pd	105	f	46	f	C	12	b	6	b	Mo	94	b	42	b	7.195786
809	left	350	H	1	f	1	b	Pd	102	b	46	b	C	12	b	6	b	Zr	91	f	40	f	7.000180
902	left	407	H	1	f	1	b	Pd	105	f	46	f	C	12	b	6	b	Zr	94	b	40	b	5.891702
984	right	4286	H	1	f	1	b	Pd	108	b	46	b	C	12	b	6	b	Mo	97	f	42	f	5.584301
855	none	596	H	1	f	1	b	Pd	104	b	46	b	C	12	b	6	b	Nb	93	f	41	b	4.997500
950	right	4281	H	1	f	1	b	Pd	106	b	46	b	C	12	b	6	b	Mo	95	f	42	f	4.941570

All Nuclides Appearing in Results Table (21):

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
4	2	1	b	f	D	2.0141020	1.5034	SPN	50.0000	null	0.0000	0.0150	0.21	23
13	12	6	b	b	C	12.0000000	8.0714	SPN	50.0000	null	0.0000	98.8900	197.78	3032
113	91	40	f	f	Zr	90.9052500	9.0413	SPN	50.0000	null	0.0000	11.2300	18.5295	null
114	92	40	b	b	Zr	91.9045900	9.0374	SPN	50.0000	null	0.0000	17.1100	28.2315	null
115	94	40	b	b	Zr	93.9061400	9.0015	SPN	50.0000	null	0.0000	17.4000	28.71	null
116	96	40	b	b	Zr	95.9082000	8.9621	UPN	19.3010	2 b-	3.4000	2.8000	4.62	null
117	93	41	f	b	Nb	92.9060200	9.0127	SPN	50.0000	null	0.0000	100.0000	20	null
118	92	42	b	b	Mo	91.9062900	9.0202	SPN	50.0000	null	0.0000	15.8400	0.19008	null
119	94	42	b	b	Mo	93.9047400	9.0154	SPN	50.0000	null	0.0000	9.0600	0.10872	null
120	95	42	f	f	Mo	94.9057200	8.9958	SPN	50.0000	null	0.0000	15.7200	0.18864	null
121	96	42	b	b	Mo	95.9045500	8.9975	SPN	50.0000	null	0.0000	16.3300	0.19596	null
122	97	42	f	f	Mo	96.9057500	8.9765	SPN	50.0000	null	0.0000	9.4600	0.11352	null
123	98	42	b	b	Mo	97.9055100	8.9695	SPN	50.0000	null	0.0000	23.7800	0.28536	null
124	100	42	b	b	Mo	99.9075700	8.9324	UPN	18.8923	2 b-	3.0350	9.1300	0.10956	null
133	102	46	b	b	Pd	101.9049400	8.9395	SPN	50.0000	null	0.0000	0.9600	0.000144	null
134	104	46	b	b	Pd	103.9035600	8.9352	SPN	50.0000	null	0.0000	10.9700	0.0016455	null
135	105	46	f	f	Pd	104.9046400	8.9174	SPN	50.0000	null	0.0000	22.2300	0.0033345	null
136	106	46	b	b	Pd	105.9032000	8.9220	SPN	50.0000	null	0.0000	27.3300	0.0040995	null
137	108	46	b	b	Pd	107.9039200	8.9001	SPN	50.0000	null	0.0000	26.7100	0.0040065	null
138	110	46	b	b	Pd	109.9045000	8.8801	SPN	50.0000	null	0.0000	11.8100	0.0017715	null