Two To Two Reactions - data provided by Dr. Alexander Parkhomov

Facilitated by the Martin Fleischmann Memorial Project

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:

Full SQL Query: "select * from TwoToTwoAll where E1 = 'S' and E2 = 'S' order by MeV desc limit 100"

23 rows were found.

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
224969	left	33267	S	33	f	16	f	S	34	b	16	b	He	4	b	2	b	Cu	63	f	29	b	6.639692
213888	left	33261	S	32	b	16	b	S	33	f	16	f	H	1	f	1	b	Zn	64	b	30	b	6.115261
224968	left	33268	S	33	f	16	f	S	34	b	16	b	H	1	f	1	b	Zn	66	b	30	b	5.079439
236108	none	78707	S	34	b	16	b	S	34	b	16	b	He	4	b	2	b	Zn	64	b	30	b	3.709200
224960	none	78698	S	33	f	16	f	S	33	f	16	f	C	12	b	6	b	Fe	54	b	26	b	3.074900
224963	none	78700	S	33	f	16	f	S	33	f	16	f	Si	28	b	14	b	Ar	38	b	18	b	3.046000
224967	none	78703	S	33	f	16	f	S	33	f	16	f	S	32	b	16	b	S	34	b	16	b	2.778600
224962	none	78699	S	33	f	16	f	S	33	f	16	f	O	16	b	8	b	Cr	50	b	24	b	1.822000
213891	left	33262	S	32	b	16	b	S	33	f	16	f	P	31	f	15	b	S	34	b	16	b	1.776361
224965	none	78701	S	33	f	16	f	S	33	f	16	f	Si	30	b	14	b	Ar	36	b	18	b	1.502500
224970	left	33269	S	33	f	16	f	S	34	b	16	b	C	12	b	6	b	Mn	55	f	25	b	1.184862
213890	left	33263	S	32	b	16	b	S	33	f	16	f	Si	30	b	14	b	Cl	35	f	17	b	0.856045
224961	left	33265	S	33	f	16	f	S	33	f	16	f	O	16	b	8	b	V	50	b	23	f	0.784320
236109	none	78708	S	34	b	16	b	S	34	b	16	b	C	12	b	6	b	Fe	56	b	26	b	0.743300
236107	left	33271	S	34	b	16	b	S	34	b	16	b	H	1	f	1	b	Zn	67	f	30	f	0.704212
213889	left	33264	S	32	b	16	b	S	33	f	16	f	Si	28	b	14	b	Cl	37	f	17	b	0.663226
224964	left	33266	S	33	f	16	f	S	33	f	16	f	Si	29	f	14	f	Cl	37	f	17	b	0.498351
224971	left	33270	S	33	f	16	f	S	34	b	16	b	O	16	b	8	b	V	51	f	23	b	0.403339
213892	none	78704	S	32	b	16	b	S	34	b	16	b	C	12	b	6	b	Fe	54	b	26	b	0.296200
224966	none	78702	S	33	f	16	f	S	33	f	16	f	P	31	f	15	b	Cl	35	f	17	b	0.283200
236110	none	78709	S	34	b	16	b	S	34	b	16	b	O	16	b	8	b	Cr	52	b	24	b	0.280400
213893	none	78705	S	32	b	16	b	S	34	b	16	b	Si	28	b	14	b	Ar	38	b	18	b	0.267300
224972	none	78706	S	33	f	16	f	S	34	b	16	b	Si	29	f	14	f	Ar	38	b	18	b	0.102500