Fusion 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 ("Fusion.php") enables SQL commands to query the Fusion tables originally 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 Fission 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 all Fusion tables, A1 is never greater than A2 in any row, i.e. A1 <= A2. This also applies implicitly in that, if the input side of the Core Query only involves E1 and E2, only rows whose associated mass numbers obey A1 <= A2 will appear in the results

Input used for this run on 20-Dec-2021 05:21:04 (NZT):

Full SQL Query: "select * from FusionAll where neutrino = 'none' and (E1= 'Si' and E2 = 'Si' ) order by MeV desc limit 100"

3 rows were found.

Results Table:

id	neutrino	id_sub	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	E	A	nBorF	Z	aBorF	MeV
3593	none	1079	Si	29	f	14	f	Si	29	f	14	f	Ni	58	b	28	b	16.431600
3609	none	1081	Si	30	b	14	b	Si	30	b	14	b	Ni	60	b	28	b	15.592300
3588	none	1080	Si	28	b	14	b	Si	30	b	14	b	Ni	58	b	28	b	14.294700

All Nuclides Appearing in Results Table: (5)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
33	28	14	b	b	Si	27.97692653499	236.53056909801	8.44752032493	SPN	50.0000	null	0.0000	92.2100	260032.2	653	null	null	null	null	null	null
34	29	14	f	f	Si	28.97649466525	245.00394027528	8.44841173363	SPN	50.0000	null	0.0000	4.7000	13254	34	1/2+	-0.5550520000	null	2.0900	79.468	-5.31903000
35	30	14	b	b	Si	29.97377013600	255.61291079491	8.52043035983	SPN	50.0000	null	0.0000	3.0900	8713.8	23	null	null	null	null	null	null
77	58	28	b	b	Ni	57.93534178000	506.44647384250	8.73183575591	SPN	50.0000	null	0.0000	67.8800	57.0192	49	null	null	null	null	null	null
79	60	28	b	b	Ni	59.93078525600	526.83302405250	8.78055040087	SPN	50.0000	null	0.0000	26.2300	22.0332	null	null	null	null	null	null	null

All Elements Appearing in Results Table: (2)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
14	Si	Silicon	3	14	28.08561	111	12.05391	1687	3173	1.9	133.6	4	14	257923	2330	0.001	150	710	282000	650	Diamagnetic	null	-0.00000373000
28	Ni	Nickel	4	10	58.72843	149	6.59277	1728	3186	1.91	112	4	28	1039668	8908	14	91	445	84	null	Ferromagnetic	631	null