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 26-Jul-2022 12:24:35 (NZT):

Full SQL Query: "select * from FissionAll where E = 'Tb' and E1 = 'C' order by MeV desc limit 1000"

One row was found.

Results Table:

id	neutrino	E	A	nBorF	Z	aBorF	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	MeV
1070	right	Tb	159	f	65	b	C	13	f	6	f	Nd	146	b	60	b	8.295884

All Nuclides Appearing in Results Table: (3)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
16	13	6	f	f	C	13.00335483521	97.10512005305	7.46962461947	SPN	50.0000	null	0.0000	1.1100	2.22	37	1/2-	0.7023690000	null	1.0000	100.589	6.72828600
220	146	60	b	b	Nd	145.91312250300	1212.36458796720	8.30386704087	SPN	50.0000	null	0.0000	17.2200	7.1463	null	null	null	null	null	null	null
240	159	65	f	b	Tb	158.92535393300	1301.98354368210	8.18857574643	SPN	50.0000	null	0.0000	100.0000	1.2	null	3/2+	2.0090000000	1.4320000000	330.0000	90.714	6.43100000

All Elements Appearing in Results Table: (3)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
6	C	Carbon	2	14	12.01114	67	5.31466	3823	4300	2.55	153.9	4	6	47277	2260	0.1	140	710	200	4600	Diamagnetic	null	-0.00001400000
60	Nd	Neodymium	6	6	144.24076	206	20.57643	1294	3373	1.14	50	3	4	3900	7010	1.6	17	190	41.5	null	Paramagnetic	null	0.00336480000
65	Tb	Terbium	6	11	158.92495	225	19.33629	1629	3503	null	50	4	4	3839	8219	0.83	11	182	1.2	null	Paramagnetic	222	0.11177840000