Byuon theory and a new anisotropic interation in

natureYu.A.BaurovYu.A.Baurov

Research Institute of Cosmic Physics, Closed Joint-Stock Research Institute of Cosmic Physics, Closed Joint-Stock Company, 141070, Korolev, Moscow Region, Pionerskaya Company, 141070, Korolev, Moscow Region, Pionerskaya

4, Russia.4, Russia.

Byuon Theory

Basic axioms and hypothesesBasic axioms and hypotheses Maim hypotheses and forming of RMaim hypotheses and forming of R33 space space

Probability of interactionProbability of interaction Potential energy of byuon’s interactionPotential energy of byuon’s interaction Initial conditions and assumptionsInitial conditions and assumptions Scales of RScales of R33 space space

Basic results of byuon theoryBasic results of byuon theory Fundamental experimentsFundamental experiments

Basic axioms and hypotheses

It is assumed unobservable object (the byuon (i))

x(i) is “length” of the byuon, a real (positive or negative) valuethe index i = 0,1,2,…k,… is a quantum number for (i); Ag 1.951011 Gscm – cosmological vector-potential

Statics. In the set {(i)}, no static states with time t > 0 are meant. That is, the byuon is always in state of continuous changing.

Kinematics. A free byuon state (that is, not interacting with another state) can correspond only to one of four so called vacuum states II+, I+, I, II

o - a quantum of time

Introduce the following definitionsIntroduce the following definitions of of vacuum statesvacuum states II II++, I, I++, I, I, II, II(VSs)(VSs)

1. A free byuon is in vacuum state II+ if its positive length discretely increases of a quantum of distance ~х0 in a quantum of time o. At that the speed of byuon

propagation (increasing in length) сх

с

~

0

00

0

(c0 is speed of light).

2. A free byuon is in VS I+ if its lenght discretely decreases of a quantum of distance ~х0

in a quantum of time 0. In this case сх

с

0 0

00

~

.

3. A free byuon is in VS II if the modulus of its negative length discretely increases of

~х0 in a time о. Therewith сх

с

~

0

00

0

.

4. A free byuon is in VS I if the modulus of its negative length discretely decreases of

~х0 in a time о. In this case сх

с

0 0

00

( ~ )

.

The known fundamental constant, light speed, appears in the byuon theory as a result of byuon changes. 0.910-43s, ~х0 2.810-33cm

Advance main hypothesis

Let the observable three-dimensional space RLet the observable three-dimensional space R33 be be

formed as a result of minimization of potential formed as a result of minimization of potential energy of byuon energy of byuon VSsVSs interaction in the one- interaction in the one-dimensional space Rdimensional space R

11 formed by them. formed by them.

More precisely, the space RMore precisely, the space R33 is fixed by us in is fixed by us in

consequence of dynamics of objects generated by consequence of dynamics of objects generated by interaction of interaction of VSsVSs of the byuon. of the byuon.

That is, dynamic processes arise in the space RThat is, dynamic processes arise in the space R33 for for

objects with residual (after minimization) positive objects with residual (after minimization) positive potential energy of interaction of byuon potential energy of interaction of byuon VSsVSs, and, as , and, as a result, wave properties of appearing elementary a result, wave properties of appearing elementary particles come into existence.particles come into existence.

Forming of RForming of R33 space space

Fig. 1.1Interaction of byuons in vacuum states

(the smallest loop).

Fig. 1.2Completion of vacuum states II + and II –

by vacuum states I + and I –.(“points” D, “points” A).

Probability of interaction of byuons

Introduce functions of index Introduce functions of index ii,, characterizing the characterizing the

origin of such or another VS by byuons:origin of such or another VS by byuons:

The physical sense of the introduced functions The physical sense of the introduced functions consists in that their product determines the consists in that their product determines the probability of two-contact interaction of byuonsprobability of two-contact interaction of byuons

The product of four functions determines the The product of four functions determines the probability of four-contact interaction etc.probability of four-contact interaction etc.

ikII

iII

ΨΨ ,2 , determining the processes of byuon length magnitude origin and increase

at positive and negative X(i), respectively; 2ik

IiI,Ψ

, determining the processes of byuon length magnitude cancellation and

decrease at positive and negative X(i), respectively

kiII

iIIΨΨ 22 determines the probability of interaction of byuons k2i

II2iII

XAXA ][][ и

Probability of interaction of byuons

Normalize the introduced functions for the Normalize the introduced functions for the case case 0 0 i < k i < k in the following manner in the following manner

Pij

0j

k2jNkP

IIjNkP

II

1NP

1

2

NPij

0j

22jNkPII

jI

2/)kNkP(

0

2

NPij

0j

22jNkPI

22jNkPII

jI

2jII

2/)kNkP(

0

2

NPij

0j

22jNkPI

2jII

2/)kNkP(

0

When normalizing, it was taken into account that within a period in i = k, one four-contact interaction occurs with probability 1.

Probability of interaction of byuons

Obtain an equation in terms of Obtain an equation in terms of --functions, describing the functions, describing the

propagation of four-contact interaction of byuonspropagation of four-contact interaction of byuons

Assuming only linear dependences and equiprobability of Assuming only linear dependences and equiprobability of VSsVSs of byuons neighbouring in of byuons neighbouring in ii, we obtain the following , we obtain the following equations for equations for --functions of four-contact interactions of functions of four-contact interactions of byuonsbyuons

.,,,f

,,,,f

,,,,f

,,,,f

iI

2iII

2iNkPII

1iNkPII

2iNkPI

iI

2iII

1iNkPI

1iNkPIIII

iNkPII

2iNkPI

iNkPII

iII

1iII

iI

2iNkPI

iNkPII

2iI

1iIIII

2iII

][

][

][

][

IIi

IIi

Ii

IINkP i

INkP i

Ii

Ii

IIi

IINkP i

INkP i

IINkP i

IINkP i

INkP i

IIi

Ii

INkP i

INkP i

IINkP i

IIi

Ii

2 1 2 2

1 2

1 1 2

2 1 2 2

,

,

,

.

Probability of interaction of byuons

From the first and second pairs of Eqs. it is From the first and second pairs of Eqs. it is easy to obtain the following equationseasy to obtain the following equations

It is seen that the process in It is seen that the process in ii is of is of oscillatory character for the functionsoscillatory character for the functions

01iI

1iII

1iI

1iII

][

01iNkPI

1iNkPII

1iNkPI

1iNkPII

][

)( 1iI

1iII

)( 1iNkP

I1iNkP

II

andand

denote the second finite differences in index i

Potential energy of byuon’s interactionPotential energy of byuon’s interaction For the case For the case ii k k, write an equation for an increment in potential , write an equation for an increment in potential

energy of byuon interaction energy of byuon interaction E(i)E(i), corresponding to the occurrence of , corresponding to the occurrence of VSs and Minimization of VSs and Minimization of E(i)E(i) is assumed to be going at each step in is assumed to be going at each step in ii

Potential energy of byuon’s interactionPotential energy of byuon’s interaction

The expressions determining the maximum The expressions determining the maximum energy of byuon interactionenergy of byuon interaction

The minimization of The minimization of E(i)E(i) is achieved in is achieved in the functional space of the following the functional space of the following variables:variables:

Initial conditions and assumptionInitial conditions and assumptionss 1.1. The conditions of symmetry during the “closure of the The conditions of symmetry during the “closure of the

loop” in loop” in ii are fulfilled as well as symmetry of the world are fulfilled as well as symmetry of the world and antiworld, which conditions can be represented asand antiworld, which conditions can be represented as

2.2. Initial conditions for Initial conditions for - function- function

3.3. Using the solutions of the probability equationsUsing the solutions of the probability equations

contract the space of contract the space of variables down to four: variables down to four:

The result of minimization of potential energy

Seek for Seek for min min E(i)E(i) by the steepest descent by the steepest descent method, retaining only method, retaining only 1414 terms of the series terms of the series min min E(iE(i) will correspond to the following ) will correspond to the following values of variables:values of variables:

5,52,

42

420

6015

1020013.1cos,1001887.1cos

,10100043.1),8(999.0

,1000136.1),6(999.0

,103,102.6

iNkpkiNkP

IIII

ii

III

NkP

I

NkP

II

III

NkPk

Scales of RScales of R33 space space

Fig. 1.3Characteristic hierarchy of scales in our world.

Fig. 1.4The filled loop with characteristic dimension x0

has VS I+ at the outlet and does not let out any information connected with the process of extension of byuon VS II+ with velocity c0.

Basic results of byuon theoryBasic results of byuon theory Created:Created:

The physical model of creation of the observed physical space The physical model of creation of the observed physical space from byuons;from byuons;

The physical model of time and physical vacuum;The physical model of time and physical vacuum; The unified way of understanding of existing interactions and The unified way of understanding of existing interactions and

a new principle of relativity;a new principle of relativity; The physical models of galactic, intergalactic magnetic fields The physical models of galactic, intergalactic magnetic fields

and relic radiation.and relic radiation. Predicted:Predicted:

The global space anisotropy associated with cosmological The global space anisotropy associated with cosmological vector potential vector potential AgAg and a new interaction connected with and a new interaction connected with vector-potential Ag;vector-potential Ag;

The existence of a new quantum information channel and The existence of a new quantum information channel and Universal mind.Universal mind.

Basic results of byuon theoryBasic results of byuon theory

Literature BooksBooks

Baurov Yu.A., Baurov Yu.A., ««On the structure of physical On the structure of physical vacuum and a new interaction in Nature vacuum and a new interaction in Nature (Theory, Experiment and Applications)(Theory, Experiment and Applications)»,», Nova Nova Science, NY, 2000.Science, NY, 2000.

Baurov Yu.ABaurov Yu.A.., , ««Global Anisotropy of Physical Global Anisotropy of Physical Space. Experimental and Theoretical BasisSpace. Experimental and Theoretical Basis»». . Nova Science, NY, 2004Nova Science, NY, 2004

Fundamental experimental investigations of new anisotropic interaction

First experiments (1987-1994, IOFAN)First experiments (1987-1994, IOFAN) Expression for anisotropic forceExpression for anisotropic force ExperimentsExperiments with gravimeter “Sodin” with gravimeter “Sodin” Experimental investigations of new Experimental investigations of new

force by measuring fluctuations in force by measuring fluctuations in intensity of intensity of -decay of radioactive -decay of radioactive elementselements

Masses of all leptons from byuon theory

||342

3

20

2 Ae

hc

k

hccme

||342 2

0

2 Ae

hc

k

hccm

e

||34

32

5.520412 A

hc

ehccm

||34

2963

5.520412 A

hc

ehccm

||34

3

5.320412 A

hc

ehccm

||34

2123

5.320412 A

hc

ehccm

Experiments at IOFAN with a water-cooled solenoid

Water-cooled solenoid having Water-cooled solenoid having an aperture of an aperture of 60mm60mm in diameter in diameter

Magnetic flux up to Magnetic flux up to 15Т15Т, , Body weight Body weight 30g30g in mass was made in mass was made

from from -tin manifesting a weak -tin manifesting a weak paramagnetism at a room paramagnetism at a room temperature.temperature.

The deflection The deflection xx of the weight of the weight depending on magnetic flux density depending on magnetic flux density BB in the regions in the regions 1 1  4  4 of the solenoid of the solenoid apertureaperture

13h 45m (1), 13h 00m (2), 13h 45m (1), 13h 00m (2), 14h 15m (3), 15h 00m (4)14h 15m (3), 15h 00m (4);;

The straight line is a linear The straight line is a linear approximation (theory)approximation (theory) 1

1

8

2

2

10

3

3

12

4

4

B, T

5

6

8

7

X

12

3

4

5

6

7

89

X

0 2 4 6

S

N

1234

Expression for a new force

1

20

)()(||2||

X

A

A

AAcANmF

G

Expression for (A) based on the specific experimental results

k

k

k

k Ax

ct

y

r

A

AA

1

2/3

0

*

exp)(G

N is the number of stable elementary particles in the body

x

AANF

*~23*

0 )( ctx

which can be acted upon by the electromagnetic field potentials

200

20 c|A|m2cm2

e G

is part of the energy

Experimental investigations with quartz gravimeter “Sodin”

The sensing system of Canadian The sensing system of Canadian high- accuracy quartz gravimeter high- accuracy quartz gravimeter

““Sodin”Sodin”1 -1 - rod, rod,

2 - horizontal system of suspending on quartz 2 - horizontal system of suspending on quartz torsion filaments, torsion filaments,

3 - main string, 3 - main string, 4 - lamp, 5 - lens, 6 - rod,4 - lamp, 5 - lens, 6 - rod,7 - piezosensitive rule, 8 - prism, 7 - piezosensitive rule, 8 - prism, 9, 10 - temperature compensator, 9, 10 - temperature compensator, 11, 12, 13, 14 -micrometric compensative 11, 12, 13, 14 -micrometric compensative

mechanism, mechanism, 15 - permanent magnet15 - permanent magnet

Events on gravimeter “Sodin”

Readings of the gravimeter The event on March 18, 1996.

Y  - is displacement of platinum weight. One division is 0.1 m, or 0.2 gal, x  - is time in minutes.

2 4 0 0 0 .0 0

2 8 0 0 0 .0 0

3 2 0 0 0 .0 0

2 0 0 0 0 .0 0

4 0 .0 0 8 0 .0 0 1 2 0 .0 0 1 6 0 .0 0 2 0 0 .0 00 .0 0

Experiment with two gravimeters S209 & S211

Readings of the gravimeters at Jun.6.2000.

y – the displacement of platinum weight(one division is equal to 0.1 μ and

corresponds to 0.2 μGal);x – time (in minutes);

Event (peak 2) at 12h01m UTC.

Experimental investigations of new force by measuring fluctuations in intensity of -decay of radioactive elements 60Co & 137Cs

Baurov Yu.A., Konradov A.A., Kuznetsov E.A., Kushniruk V.F.,Baurov Yu.A., Konradov A.A., Kuznetsov E.A., Kushniruk V.F.,Ryabov Y.B., Senkevich A.P., Sobolev Yu.G., Zadorozsny S.Ryabov Y.B., Senkevich A.P., Sobolev Yu.G., Zadorozsny S.““Experimental Investigations of Changes in Experimental Investigations of Changes in -Decay rate of -Decay rate of 6060Co and Co and 137137Cs” Mod. Phys.Lett A. v.16, N 32 (2001), p.2089Cs” Mod. Phys.Lett A. v.16, N 32 (2001), p.2089

Results of our experiment performed at the Results of our experiment performed at the same time at INR of RAS (Troitsk, Moscow same time at INR of RAS (Troitsk, Moscow region) and region) and JINR (Dubna, Moscow region) with the use of JINR (Dubna, Moscow region) with the use of germanium-lithium detectorsgermanium-lithium detectors

The variation of theThe variation of the flow of flow of -quanta accompanying -quanta accompanying the the -decay of -decay of 137137Cs, with the time (JINR, Dubna)Cs, with the time (JINR, Dubna)

The variation of the flow of -quanta accompanying the -decay of 60Co, with the time (INR, Troitsk)

The spatial positions of sites where the clearly expressed extrema in the magnitude of the flow of -quanta in the experiment with the -decay of 60Co

- the site of the maximum flow of - the site of the maximum flow of -quanta -quanta with the indication of the direction of with the indication of the direction of action of the new force drawn along the action of the new force drawn along the tangent line to the parallel of latitude; tangent line to the parallel of latitude;

a – the trajectory of motion of the radioactive a – the trajectory of motion of the radioactive source rotating together with the Earth source rotating together with the Earth

b – the trajectory of motion of the Earth and b – the trajectory of motion of the Earth and the radioactive source around the Sun;the radioactive source around the Sun;

21.03 etc. – the point of the vernal equinox 21.03 etc. – the point of the vernal equinox and other characteristic points of the and other characteristic points of the trajectory “b”; trajectory “b”;

AAEE – the direction of the vectorial potential of – the direction of the vectorial potential of the magnetic field of the Earth’s dipole;the magnetic field of the Earth’s dipole;

AAgg – the direction of the cosmological vectorial potential – the direction of the cosmological vectorial potential

The spatial positions of sites where the clearly expressed extrema in the magnitude of the flow of -quanta in the experiment with the -decay of 137Cs

- the site of the maximum flow of - the site of the maximum flow of -quanta -quanta with the indication of the direction of with the indication of the direction of action of the new force drawn along the action of the new force drawn along the tangent line to the parallel of latitude; tangent line to the parallel of latitude;

a – the trajectory of motion of the radioactive a – the trajectory of motion of the radioactive source rotating together with the Earth source rotating together with the Earth

b – the trajectory of motion of the Earth and b – the trajectory of motion of the Earth and the radioactive source around the Sun;the radioactive source around the Sun;

21.03 etc. – the point of the vernal equinox 21.03 etc. – the point of the vernal equinox and other characteristic points of the and other characteristic points of the trajectory “b”; trajectory “b”;

AAEE – the direction of the vectorial potential of – the direction of the vectorial potential of the magnetic field of the Earth’s dipole;the magnetic field of the Earth’s dipole;

AAgg – the direction of the cosmological vectorial potential – the direction of the cosmological vectorial potential