kf mit colloquium 2019 - cold fusion · track cce a = 621.1 ±7.3 μm n = 5.0 a.) ellipse fitted...
TRANSCRIPT
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elliptical tracksevidence for superluminal electrons?
quantized elliptical tracks
sizes expected of bound monopoles
yet requiring v > c
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ICCF 11: Urutskoev, Ivoilov, Lochak, Strange radiation
ICCF 18: replication of tracks with simplified technique
Do these particles respond to electric or magnetic fields?
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n = 5.0track cce a = 621.1 ±7.3 μm
a.) Ellipse fitted to trackb.) After processing and background eradication.c.) Photo using Leitz PL 40x objective.
y (μm)c.b.a.
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track lee2
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n = 2.75track lee2 a = 56.9 ±13.0 μm
a.) Ellipse fitted to trackb.) After processing and background eradication.c.) Photo using Leitz PL 100x objective.
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n = 8track be a = 4078.6 ±14.6 μm
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n = 2.75track rse2 a = 56.7 ±9.5 μm
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a (μm)
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No observed curvature effects due to applied electric or magnetic fields
Elliptical tracks are 1372n2 bigger than Bohr-Sommerfeld hydrogen
Decay events
the ellipses must be bound states caused by an inverse square (1/r2) central force
breakthrough
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larger than Bohr-Sommerfeld hydrogen
1372n2 = n2
α2 , g = 2gD
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g = ecα
Schwinger quantization condition g = 2gD
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using analogy with the electron, the coupling constant for the magnetic monopole is
αm = α−1 = kmg 2
ℏc
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Semi-major axes of the fitted ellipses, , differ fromthe semi-major axes, , of corresponding Bohr-Sommerfeld ellipses for hydrogen by .
am = aen2
α2
≃ 1372n2
amae
Using g = 2gD ,
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a0e = ℏ/mecα,a0m = ℏα/mmc
Substituting the Bohr radius,monopole Bohr radius, (αm = 1/α),
a0m
a0e= 1
α2
For n = 1,
and the
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mm = meα4
= 1.45 × 10−3
monopole mass:
eV/c2
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interesting aside…
1.45 × 10−3
∼ 1.33 × 10−3
eV/c2
eV/c2
John Wallace’s exceedingly small effective mass
= 2 × (1.3 × 10−9me)
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Bohr radius
a0e = ℏmecα
a0m = ℏαmmc
v0e = kee2
ℏ = cα < c
v0m = kmg 2
ℏ = cα
> c
gso velocity
!
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c
a0m
λcm
r0m
a0e
λce
r0e
c/α
cα
lengthvelocity
α
α
α
α
α
α
α
α
L > d
L < d
v > c
v < c 2.82x10-15
3.86x10-13
9.93x10-07
1.36x10-04
1.86x10-02
7.25x10-09
4.11x1010
2.99x108
2.19x106
v0m
v0e 5.29x10-11
d
d/α
dα
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there is a relativistic scale transformationand framesv > c v < c
( n2
α2 )2
( x2
a(n)2m
+ y2
b(n)2m ) = 1 ,
here contracting the monopole ellipse into the electron ellipse
between
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the Coulomb flip
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the superluminal electron, equivalent to a magnetic charge, together with the subluminal electron, creates the condition for charge quantization
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next
thick nuclear track emulsions
replicate quantized elliptical tracks
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best evidence yet for magnetic charge?
repeatable experiment
consistent with the idea of magnetic charge
funding for 1 physicist
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Q: How can you be sure that the applied magnetic fields are not responsible for the tracks?
A: The magnetic source creating the central force for the ellipse has to be a spherically symmetric point source. The applied magnetic fields were not spherically symmetric point sources.
Q: Under quantum mechanics, how can these tracks even occur? Any sharply defined track, including all those routinely observed in bubble chambers or in photographic films, is produced by a sufficiently small, fast moving wave packet. And the latter is generally formed only by a superposition of many stationary states, even though each such state alone is spatially extended. This is universally true in relativistic and non-relativistic domain. One cannot in principle attribute a single definite quantum number n to a semi-classical track observed.
A: This apparent contradiction points to new physics. The classicaltracks occur and are quantized making them semi-classical in the spirit of Bohr-Sommerfeld.
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1.) initial particle, P1, trajectory.
2.) at point a. particle decays into P1′, continuing on initial trajectory and P2, which is captured into an elliptical orbit.3.) at point b. particle escapes from the elliptical orbit.
Capture into and escape from an elliptical orbit
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Urutskoev
Ivoilov
Lochak
Priem, Daviau, etc
Fredericksdischarges in water
discharges in water
discharges in water
light leptonic monopoleuniform photon exposure
Othersglow discharge,laser irradiation,electron beams
theoryexperiment
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Periodicity
Penetration
Random motion
Correlation of tracks
Central force
Tracks in various materials
Large angles of curvature
White tracks
emulsions, metals, semiconductors
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elliptical tracks
Disk Magnet
white track
black trackshadow
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E(n)m = − km
g 2
2a(n)m
E(n)e = − ke
e2
2a(n)e
v(n)m = n
cα
v(n)e = c
αn
p(n)m = nℏ
a(n)m
p(n)e = nℏ
a(n)e
m(n)m = n4ℏα
a(n)m c
m(n)e = n2ℏ
a(n)e cα
superluminal dualof electron electron
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Low Energy Generation of the “Strange” Radiation, N. G. Ivoilov (2006).
Transmutations et traces de monopôles obtenues lors de décharges électriques, D. Priem et al. (2009).
Unusual structures on the material surfaces irradiated by low energy ions, B. Rodionov and I. Savvatimova, (2005)
Low-energy nuclear reactions and the leptonic monopole, G. Lochak and L. Urutskoev, (2004)
Tracks of magnetic monopoles, C. Daviau, D. Fargue, D. Priem, and G. Racineux (2013).
Observation of transformation of chemical elements during electric discharge Urutskoev, L. I.; Liksonov, V. I.; Tsinoev, V. G. (2000)
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• K. A. Fredericks. Possible detection of tachyon monopoles in photographic emulsions. Eng. Phys., 6, 2013.
• K. A. Fredericks. Possibility of tachyon monopoles detected in photographic emulsions. J. Condensed Matter Nucl. Sci., 15:203–230, 2015.
• K. A. Fredericks, Monopole mass from fundamental lengths, Phys. Essays 30, 269 (2017).