| Literature DB >> 31766268 |
Alexander Basov1,2, Liliya Fedulova3, Ekaterina Vasilevskaya3, Stepan Dzhimak2,3,4.
Abstract
This article presents the original descriptions of some recent physics mechanisms (based on the thermodynamic, kinetic, and quantum tunnel effects) providing stable 2H/1H isotope fractionation, leading to the accumulation of particular isotopic forms in intra- or intercellular space, including the molecular effects of deuterium interaction with 18O/17O/16O, 15N/14N, 13C/12C, and other stable biogenic isotopes. These effects were observed mainly at the organelle (mitochondria) and cell levels. A new hypothesis for heavy nonradioactive isotope fractionation in living systems via neutron effect realization is discussed. The comparative analysis of some experimental studies results revealed the following observation: "Isotopic shock" is highly probable and is observed mostly when chemical bonds form between atoms with a summary odd number of neutrons (i.e., bonds with a non-compensated neutron, which correspond to the following equation: Nn - Np = 2k + 1, where k ϵ Z, k is the integer, Z is the set of non-negative integers, Nn is number of neutrons, and Np is number of protons of each individual atom, or in pair of isotopes with a chemical bond). Data on the efficacy and metabolic pathways of the therapy also considered 2H-modified drinking and diet for some diseases, such as Alzheimer's disease, Friedreich's ataxia, mitochondrial disorders, diabetes, cerebral hypoxia, Parkinson's disease, and brain cancer.Entities:
Keywords: deuterium; electron density delocalization; isotopic discrimination; isotopic resonance; living systems; mitochondrial disorders; neurodegenerative diseases; neutron; nonradioactive isotopes
Mesh:
Substances:
Year: 2019 PMID: 31766268 PMCID: PMC6891295 DOI: 10.3390/molecules24224101
Source DB: PubMed Journal: Molecules ISSN: 1420-3049 Impact factor: 4.411
Figure 1Reaction 1: Fractionation of isotopes (atomic mass n+mX > atomic mass nX) is observed at k1 ≈ k2; k3 >> k4; k3 >> k1. Note: S—(bio-)chemical substrate; P—product of (bio-)chemical reaction; E—enzyme (catalyst).
Figure 2Reaction 2: Fractionation of deuterium is observed when k1 ≈ k2; k3 >> k4; k3 >> k1. Note: S—(bio-)chemical substrate; P—product of (bio-)chemical reaction; E—enzyme (catalyst).
Figure 3Reaction 3: Fractionation of oxygen isotope 18O is observed when k1 ≈ k2; k3 >> k4; k3 >> k1. Note: S—(bio-)chemical substrate; P—product of (bio-)chemical reaction; E—enzyme (catalyst).
Isotopic resonance regularity in biological and natural systems occurring because of the neutron Basov–Dzhimak hypothesis in individual chemical bonds and some individual isotopes.
| I | II | III | IV | V | VI | VII | VIII | IX | X |
|---|---|---|---|---|---|---|---|---|---|
| 12C-1H | 12C-2H | ||||||||
| 6n − 7p | −1 | 7n − 7p | 0 | ||||||
| R-spin | 0+ & ½+ is ½+ + | R-spin | 0+ & 1+ is 1+ + | ||||||
| 13C-1H [ | 13C-2H [ | ||||||||
| 7n − 7p | 0 | 8n − 7p | 1 | ||||||
| R-spin | ½− & ½+ is 1− + | R-spin | ½− & 1+ is 1½− + | ||||||
| 14N–1H | 14N-2H | ||||||||
| 7n − 8p | −1 | 8n − 8p | 0 | ||||||
| R-spin | 1+ & ½+ is 1½+ + | R-spin | 1+ & 1+ is 2+ + | ||||||
| 15N-1H [ | 15N-2H | ||||||||
| 8n − 8p | 0 | 9n − 8p | 1 | ||||||
| R-spin | ½− & ½+ is 1− + | R-spin | ½− & 1+ is 1½− + | ||||||
| 16O-1H | 17O-1H | 18O-1H [ | |||||||
| 8n − 9p | −1 | 9n − 9p | 0 | 10n − 9p | 1 | ||||
| R-spin | 0+ & ½+ is ½+ + | R-spin | 5/2+ & ½+ is 3+ + | R-spin | 0+ & ½+ is ½+ + | ||||
| 16O-2H | 17O-2H | 18O-2H | |||||||
| 9n − 9p | 0 | 10n − 9p | 1 | 11n − 9p | 2 | ||||
| R-spin | 0+ & 1+ is 1+ + | R-spin | 5/2+ & 1+ is 3½+ + | R-spin | 0+ & 1+ is 1+ + | ||||
| 32S-1H | 32S-2H | 34S-1H | 34S-2H | ||||||
| 16n − 17p | −1 | 17n − 17p | 0 | 18n − 17p | 1 | 19n − 17p | 2 | ||
| R-spin | 0+ & ½+ is ½+ + | R-spin | 0+ & 1+ is 1+ + | R-spin | 0+ & ½+ is ½+ + | R-spin | 0+ & 1+ is 1+ + | ||
| 12C-12C | 12C-13C | ||||||||
| 12n − 12p | 0 | 13n − 12p | 1 | ||||||
| R-spin | 0+ & 0+ is 0+ + | R-spin | 0+ & ½− is ½+ − | ||||||
| 12C-14N | 12C-15N | ||||||||
| 13n − 13p | 0 | 14n − 13p | 1 | ||||||
| R-spin | 0+ & 1+ is 1+ + | R-spin | 0+ & ½− is ½ + − | ||||||
| 13C-14N | 13C-15N [ | ||||||||
| 14n − 13p | 1 | 15n − 13p | 2 | ||||||
| R-spin | ½− & 1+ is 1½ + − | R-spin | ½− & ½− is 1 − − | ||||||
| 12C-16О | 12C-17О | 12C-18О | |||||||
| 14n − 14p | 0 | 15n − 14p | 1 | 16n − 14p | 2 | ||||
| R-spin | 0+ & 0+ is 0+ + | R-spin | 0+ & 5/2+ is 5/2+ + | R-spin | 0+ & 0+ is 0+ + | ||||
| 13C-16О | 13C-17О | 13C-18О [ | |||||||
| 15n − 14p | 1 | 16n − 14p | 2 | 17n − 14p | 3 | ||||
| R-spin | ½− & 0+ is ½− + | R-spin | ½− & 5/2+ is 3− + | R-spin | ½− & 0+ is ½− + | ||||
| 14N-16O | 14N-17O | 14N-18O | |||||||
| 15n − 15p | 0 | 16n − 15p | 1 | 17n − 15p | 2 | ||||
| R-spin | 1+ & 0+ is 1+ + | R-spin | 1+ & 5/2+ is 3½+ + | R-spin | 1+ & 0+ is 1+ + | ||||
| 15N-16O [ | 15N-17O | 15N-18O [ | |||||||
| 16n − 15p | 1 | 17n − 15p | 2 | 18n − 15p | 3 | ||||
| R-spin | ½− & 0+ is ½ − + | R-spin | ½− & 5/2+ is 3 − + | R-spin | ½− & 0+ is ½− + | ||||
| 40Ca [ | 43Ca [ | ||||||||
| 20n − 20p | 0 | 23n − 20p | 3 | ||||||
| R-spin | 0+ | R-spin | 7/2− | ||||||
| 24Mg [ | 25Mg [ | 26Mg [ | |||||||
| 12n − 12p | 0 | 13n − 12p | 1 | 14n − 12p | 2 | ||||
| R-spin | 0+ | R-spin | 5/2+ | R-spin | 0+ | ||||
| 63Cu-18O | |||||||||
| 44n − 37p | 7 | ||||||||
| R-spin | 3/2− & 0+ is 3/2− + | ||||||||
| 63Cu | |||||||||
| 34n − 29p | 5 | ||||||||
| R-spin | 3/2− | ||||||||
| 65Cu | |||||||||
| 36n − 29p | 7 | ||||||||
| R-spin | 3/2− | ||||||||
| 28Si [ | 29Si [ | 30Si [ | |||||||
| 14n − 14p | 0 | 15n − 14p | 1 | 16n − 14p | 2 | ||||
| R-spin | 0+ | R-spin | 1/2+ | R-spin | 0+ | ||||
| 64Zn [ | 67Zn [ | ||||||||
| 34n − 30p | 4 | 37n − 30p | 7 | ||||||
| R-spin | 0+ | R-spin | 5/2− | ||||||
| 66Zn [ | |||||||||
| 36n − 30p | 6 | ||||||||
| R-spin | 0+ | ||||||||
| 238U [ | 235U [ | ||||||||
| 146n − 92p | 54 | 143n − 92p | 51 | ||||||
| R-spin | 0+ | R-spin | 7/2− |
Note: n—neutron; p—proton; D—deuterium; R-spin—resultant spin of individual isotopes or pair of isotopes with chemical bonds (as a sum of individual spins); k—integer. In the table, all references [27,29,41,84,85,86,87,88,89,90,91,92,93] confirm the new hypothesis and arising resonance in living and natural systems only under certain isotopes. Note: I, III, and VII—pairs of isotopes with chemical bonds and individual isotopes that must have no isotopic resonance; II—there is no isotopic resonance for: Nn − Np = −1; IV—there is no isotopic resonance for: Nn − Np = 0; V and IX—pairs of isotopes with chemical bonds and individual isotopes that have some isotopic resonance; VI—there is some isotopic resonance for: Nn − Np = 1; VIII—there is no isotopic resonance for: Nn − Np = 2, and Nn − Np = 2k; X—there is some isotopic resonance for: Nn − Np = 2k + 1; N—number.