Fission 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 ("Fission.php") enables SQL commands to query the Fission tables 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, TwoToTwo 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 the Fission tables, A1 is never greater than A2 in any row, i.e. A1 <= A2. This also applies implicitly, in that, if the ouput side of the Core Query only involves E1 and E2, only rows for which their associated mass numbers obey the rule that A1 <= A2 will be included in the results

Input used for this run on 23-Aug-2020 13:15:17 (NZT):

Full SQL Query: "select * from FissionAllNew where E = 'Fe' and E2 in ('S') order by MeV desc"

6 rows were found.

Results Table:

id	neutrino	E	A	nBorF	Z	aBorF	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	MeV
909	none	Fe	54	b	26	b	Ne	20	b	10	b	S	34	b	16	b	-19.280247
976	right	Fe	57	f	26	f	Na	23	f	11	b	S	34	b	16	b	-20.719644
911	none	Fe	54	b	26	b	Ne	22	b	10	b	S	32	b	16	b	-22.213623
937	none	Fe	56	b	26	b	Ne	22	b	10	b	S	34	b	16	b	-22.650019
910	none	Fe	54	b	26	b	Ne	21	f	10	f	S	33	f	16	f	-23.936242
946	right	Fe	56	b	26	b	Na	23	f	11	b	S	33	f	16	f	-24.490720

All Nuclides Appearing in Results Table:

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz
22	20	10	b	b	Ne	19.99244017620	160.64033816500	8.03201690825	SPN	50.0000	null	0.0000	90.9200	null	1548	null	null	null	null	null
23	21	10	f	f	Ne	20.99384668500	167.40127014932	7.97148905473	SPN	50.0000	null	0.0000	0.2570	null	null	3/2+	-0.6617000000	0.1020000000	null	null
24	22	10	b	b	Ne	21.99138511400	177.76529654911	8.08024075223	SPN	50.0000	null	0.0000	8.8200	null	208	null	null	null	null	null
25	23	11	f	b	Na	22.98976928200	186.55918845272	8.11126906316	SPN	50.0000	null	0.0000	100.0000	23600	33	3/2+	2.2175000000	0.1040000000	525.0000	105.808
34	32	16	b	b	S	31.97207117440	271.77299100150	8.49290596880	SPN	50.0000	null	0.0000	95.0000	332.5	396	null	null	null	null	null
35	33	16	f	f	S	32.97145890980	280.41439896867	8.49740602935	SPN	50.0000	null	0.0000	0.7600	2.66	null	3/2+	0.6432500000	-0.0678000000	null	null
36	34	16	b	b	S	33.96786700400	291.83132582967	8.58327428911	SPN	50.0000	null	0.0000	4.2200	14.77	null	null	null	null	null	null
64	54	26	b	b	Fe	53.93960899000	471.75191088088	8.73614649779	SPN	50.0000	null	0.0000	5.8200	3276.66	72	null	null	null	null	null
65	56	26	b	b	Fe	55.93493633000	492.24664111678	8.79011859137	SPN	50.0000	null	0.0000	91.6600	51604.58	1169	null	null	null	null	null
66	57	26	f	f	Fe	56.93539284000	499.89249160021	8.77004371228	SPN	50.0000	null	0.0000	2.1900	1232.97	28	1/2-	0.0906400000	null	null	null