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 19-Nov-2023 13:13:19 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('H') and E2 in ('Pb', 'Bi' ) 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
288	left	270	H	1	f	1	b	Pb	207	f	82	f	Pb	208	b	82	b	6.594049
287	left	268	H	1	f	1	b	Pb	206	b	82	b	Pb	207	f	82	f	5.936414
289	none	866	H	1	f	1	b	Pb	208	b	82	b	Bi	209	f	83	b	3.774400

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
4	1	1	f	b	H	1.00782503224	0.00000000000	0.00000000000	SPN	50.0000	null	0.0000	99.9850	1399.79	705700	1/2+	2.7928473510	null	5700.0000	400.000	26.75222080
307	206	82	b	b	Pb	205.97446512400	1622.27816677790	7.87513673193	SPN	50.0000	null	0.0000	23.6000	3.304	null	null	null	null	null	null	null
308	207	82	f	f	Pb	206.97589673500	1629.01571620510	7.86964114109	SPN	50.0000	null	0.0000	22.6000	3.164	null	1/2-	0.5906000000	null	11.8000	83.432	5.57670000
309	208	82	b	b	Pb	207.97665191800	1636.38335448150	7.86722766578	SPN	50.0000	null	0.0000	52.3000	7.322	null	null	null	null	null	null	null
310	209	83	f	b	Bi	208.98039851900	1640.18217043150	7.84776158101	UPN	19.2788	A	3.1370	100.0000	0.0085	null	9/2-	4.0920000000	-0.5160000000	777.0000	64.277	4.37470000

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
1	H	Hydrogen	1	1	1.00798	53	11212.19021	14.01	20.28	2.2	72.8	1	1	1312	0.0899	null	0.1805	14300	1400	739000	Diamagnetic	null	-0.00000000223
82	Pb	Lead	6	14	207.17711	154	18.26959	600.61	2022	2.33	35.1	4	5	6640	11340	4.8	35	127	14	null	Diamagnetic	null	-0.00001700000
83	Bi	Bismuth	6	15	208.98042	143	21.36814	544.4	1837	2.02	91.2	5	6	8520	9780	0.77	8	122	0.0085	null	Diamagnetic	null	-0.00017000000