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 12:59:27 (NZT):

Full SQL Query: "select * from FissionAllNew where E = 'Ni' and E1 in ('C') order by MeV desc"

15 rows were found.

Results Table:

id	neutrino	E	A	nBorF	Z	aBorF	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	MeV
1165	none	Ni	62	b	28	b	C	12	b	6	b	Ti	50	b	22	b	-15.315183
1135	none	Ni	61	f	28	f	C	12	b	6	b	Ti	49	f	22	f	-15.658522
1099	none	Ni	60	b	28	b	C	12	b	6	b	Ti	48	b	22	b	-15.980810
1072	none	Ni	58	b	28	b	C	12	b	6	b	Ti	46	b	22	b	-16.101168
1176	right	Ni	62	b	28	b	C	12	b	6	b	V	50	b	23	f	-17.522005
1196	right	Ni	64	b	28	b	C	13	f	6	f	V	51	f	23	b	-18.019809
1184	none	Ni	64	b	28	b	C	14	b	6	b	Ti	50	b	22	b	-18.687694
1136	none	Ni	61	f	28	f	C	13	f	6	f	Ti	48	b	22	b	-18.854605
1197	right	Ni	64	b	28	b	C	14	b	6	b	V	50	b	23	f	-20.894516
1167	none	Ni	62	b	28	b	C	14	b	6	b	Ti	48	b	22	b	-21.274025
1166	none	Ni	62	b	28	b	C	13	f	6	f	Ti	49	f	22	f	-21.308068
1065	left	Ni	58	b	28	b	C	13	f	6	f	Sc	45	f	21	b	-22.282001
1137	none	Ni	61	f	28	f	C	14	b	6	b	Ti	47	f	22	f	-22.304826
1100	none	Ni	60	b	28	b	C	13	f	6	f	Ti	47	f	22	f	-22.661157
1101	none	Ni	60	b	28	b	C	14	b	6	b	Ti	46	b	22	b	-23.365444

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
13	12	6	b	b	C	12.00000000000	92.15904307956	7.67992025663	SPN	50.0000	null	0.0000	98.8900	197.78	3032	null	null	null	null	null
14	13	6	f	f	C	13.00335483507	97.10512018346	7.46962462950	SPN	50.0000	null	0.0000	1.1100	2.22	37	1/2-	0.7023690000	null	1.0000	100.589
15	14	6	b	b	C	14.00324198840	105.28132317876	7.52009451277	UPN	3.7581	b-	0.1565	0.0000	0	null	3-	0.8200000000	null	null	null
51	45	21	f	b	Sc	44.95590828000	387.84109900019	8.61869108889	SPN	50.0000	null	0.0000	100.0000	22	null	7/2-	4.7540000000	-0.2200000000	1710.0000	97.167
52	46	22	b	b	Ti	45.95262772000	398.18567560272	8.65621033919	SPN	50.0000	null	0.0000	7.9300	444.08	null	null	null	null	null	null
53	47	22	f	f	Ti	46.95175879000	407.06616593561	8.66098225395	SPN	50.0000	null	0.0000	7.2800	407.68	null	5/2-	-0.7881400000	0.3020000000	null	null
54	48	22	b	b	Ti	47.94794198000	418.69258978450	8.72276228718	SPN	50.0000	null	0.0000	73.9400	4140.64	null	null	null	null	null	null
55	49	22	f	f	Ti	48.94786568000	426.83474976378	8.71091326049	SPN	50.0000	null	0.0000	5.5100	308.56	null	7/2-	-1.1037000000	0.2470000000	null	null
56	50	22	b	b	Ti	49.94478689000	437.77371216463	8.75547424329	SPN	50.0000	null	0.0000	5.3400	299.04	null	null	null	null	null	null
57	50	23	b	f	V	49.94715601000	434.78455689911	8.69569113798	UPN	17.1461	b+ or b-	2.2050	0.2400	0.288	null	6+	3.3442000000	0.2100000000	null	null
58	51	23	f	b	V	50.94395704000	445.83546628896	8.74187188802	SPN	50.0000	null	0.0000	99.7600	119.712	null	7/2-	5.1464000000	-0.0430000000	2160.0000	101.212
70	58	28	b	b	Ni	57.93534241000	506.44588700108	8.73182563795	SPN	50.0000	null	0.0000	67.8800	57.0192	49	null	null	null	null	null
71	60	28	b	b	Ni	59.93078588000	526.83244280003	8.78054071333	SPN	50.0000	null	0.0000	26.2300	22.0332	null	null	null	null	null	null
72	61	28	f	f	Ni	60.93105557000	534.65231505485	8.76479205008	SPN	50.0000	null	0.0000	1.1900	0.9996	null	3/2-	-0.7496500000	0.1620000000	null	null
73	62	28	b	b	Ni	61.92834537000	545.24793795928	8.79432157999	SPN	50.0000	null	0.0000	3.6600	3.0744	null	null	null	null	null	null
74	64	28	b	b	Ni	63.92796682000	561.74272906251	8.77723014160	SPN	50.0000	null	0.0000	1.0800	0.9072	null	null	null	null	null	null