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 04-Oct-2021 12:29:10 (NZT):

Full SQL Query: "select * from FissionAll where neutrino = 'none' and (E = 'Tl' ) 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
1709	none	Tl	203	f	81	b	B	11	f	5	b	Os	192	b	76	b	1.505300

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
14	11	5	f	b	B	11.00930516600	76.20258012611	6.92750728419	SPN	50.0000	null	0.0000	80.4000	8.04	null	3/2-	2.6883780000	0.0405900000	754.0000	128.286	8.58470700
287	192	76	b	b	Os	191.96147888100	1526.07356154380	7.94829979971	SPN	50.0000	null	0.0000	41.0000	0.000615	null	null	null	null	null	null	null
304	203	81	f	b	Tl	202.97234402200	1600.82303379690	7.88582775269	SPN	50.0000	null	0.0000	29.5000	0.25075	null	1/2+	1.6160000000	null	null	null	15.53933900

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	MagVolSus
5	B	Boron	2	13	10.81402	87	4.39594	2348	4273	2.04	26.7	3	5	32826.7	2460	0	27	1030	10	null	Diamagnetic	-0.00002140000
76	Os	Osmium	6	8	190.32953	185	8.41794	3306	5285	2.2	106.1	8	2	1600	22610	12	88	130	0.0015	null	Paramagnetic	0.00001400000
81	Tl	Thallium	6	13	204.38383	156	17.24758	577	1746	1.62	19.2	3	3	2878	11850	6.7	46	129	0.85	null	Diamagnetic	-0.00003560000