Experiments have been and are being conducted in the field of entanglement of particles.
Two articles have been published in X archives in November 2004, one was published in March 2005, and one in November 2006. Xarchives can be reached on the Net at: www.arxiv.org .
Paper # 1 (November 2004)
" Induced Quantum Entanglement of Nuclear Metastable States of 115In "
Abstract:
Experiments conducted in our laboratory
conclusively demonstrated that at least 20% of 115In metastable states
become quantum entangled (QE) during gamma photo-excitation processes where
a significant fraction of the photo-excitation gamma (E > 1.02 MeV) are
QE. In addition, it was found that the half-life of 115mIn populations
in identical photo-excited indium foils varied as much as 70% depending
on whether the 99.999% purity indium foils were photo-excited with a High
Intensity 60Co Source (HICS) or a Varian CLINAC (Compact Linear Accelerator)
with average energy 2 MeV and maximum energy 6 MeV Bremsstrahlung photo-excitation
quanta. Decay kinetics of 115mIn populations in indium foils demonstrate
that these metastable states are primarily QE in pairs when photo-excited
in the HICS apparatus and at higher orders of entanglement of triplets
and possibly quadruplets when photo-excited with the CLINAC. It appears
that QE gamma photons can transfer quantum entangled properties to radioactive
metastable states.
Conclusion:
The data from this experiment strongly
indicates that high energy gamma and Bremsstrahlung photons are entangled
to various degrees. The rationale for shorter half-lives of entangled
metastable states is quite straight forward since one would expect that
when two metastable states are entangled, the decay probability should
double from 0.002586/min to 0.005172/min and so on for triplets, quadruplets,
etc. These different probabilities are easily deconvoluted from compound
exponential data with QE metastable state decay.
This photon quantum entanglement can be
transferred to metastable nuclei of photo-excitable elemental metals. The
data reported here demonstrate that there are multiorders of metastable
state entanglement possible, depending upon the maximum photon energy available.
Since the HICS source yields gamma photons at approximately 1100 and 1300
keV, only doublets can be formed in that case. On the other hand, the CLINAC
yields a maximum energy of 6 MeV photons which could theoretically
create up to quintuplet QE nuclei. During the analyses of the experimental
data via numerical modeling, doublets and triplets were easily observable
and necessary for the constraints of the model.
Acknowledgement:
I thank Professor Robert Desbrandes (LSU
emeritus from Petroleum Engineering) for his help in the experiments and
their interpretation. I also thank the Veterinary School of LSU for the
use of its CLINAC accelerator and the Nuclear Science Center of LSU for
using its HICS Cobalt 60 source and Germanium gamma counter
The full paper can be seen at www.arxiv.org/abs/nucl-ex/0411047 by clicking on "PDF".
Paper # 2 (November 2004)
" Remote Stimulated Triggering of Quantum Entangled Nuclear Metastable States of 115mIn "
Abstract:
We report experiments in which two indium
foils were quantum entangled via photoexcitation of stable 115In to radioactive
115mIn by utilizing Bremsstrahlung gamma photons produced by a Varian Compact
Linear Accelerator (CLINAC). After photo-excitation, remote triggering
of the “master” foil with low energy gamma photons, yielded stimulated
emissions of 336 keV gamma photons from quantum entangled 115mIn in the
“slave” foil located up to 1600 m away from the “master” foil. These experiments
strongly demonstrate that useful quantum information can be transferred
through quantum channels via modulation of quantum noise (accelerated radioactive
decay of 115mIn metastable nuclei). Thus, this modality of QE transmission
is fundamentally different from optical QE information transfer via quantum
entangled space “q-bits” as developed by information theorists for quantum
channel information transfer. Additionally, there is no obvious potential
for signal degradation with increasing distance nor the problems associated
with misalignment of optical information transfer systems.
Conclusion:
This experiment strongly demonstrates
that useful quantum information can be transferred through quantum channels
via modulation of quantum noise (accelerated radioactive decay of 115mIn).
Thus, this modality of QE transmission is fundamentally different from
optical QE information transfer via quantum entangled space “q-bits” as
developed by information theorists for quantum channel information transfer.
Additionally, there is no obvious potential for signal degradation with
increasing distance nor the problem of misalignment of optical information
transfer systems Although 115mIn metastable states have a spontaneous decay
half-life of 4.68 hours, other much longer-lived metastable states such
as 178m2Hf with a half-life of 31 years could potentially be utilized for
viable global communications.
Even though only two foils were quantum
entangled per irradiation during this experiment, there is no foreseeable
reason why multiple numbers of foils could not be utilized as well. If
this is possible, one “master” foil could be utilized to remotely trigger
multiple QE “slave” foils.
Acknowledgement:
I thank Professor Robert Desbrandes (LSU
emeritus from Petroleum Engineering) for his help in the experiments and
their interpretation. I also thank the Veterinary School of LSU for the
use of its CLINAC accelerator and the Nuclear Science Center of LSU for
using its HICS Cobalt 60 source and Germanium gamma counter.
The full paper can be seen at www.arxiv.org/abs/nucl-ex/0411050 by clicking on "PDF".
Paper # 3 (March 2005)
"Remote Stimulated Triggering of Quantum Entangled Photoluminescent Molecules of Strontium Aluminate".
Abstract:
We report experiments in which two photoluminescent
samples of Strontium Aluminate pigments and Zinc Sulfide pebbles were quantum
entangled via photoexcitation with entangled photons from a mercury lamp
and a CRT screen. After photo-excitation, remote triggering of one
of the sample with infrared (IR) photons yielded stimulated light variation
from the quantum entangled other sample located 4 m away. The initial half-life
of Strontium Aluminate is approximately one minute. However, molecules
with a longer half-life may be found in the future. These experiments demonstrate
that useful quantum information could be transferred through quantum channels
via de-excitation of one sample of photoluminescent material quantum entangled
with another.
Conclusion:
Although relatively crude, these experiments
seem to demonstrate that useful quantum information could be transferred
through quantum channels via photoluminescent pigments. Thus, this
modality of QE transmission would be fundamentally different from optical
QE information transfer via quantum entangled space “q-bits” as developed
by information theorists for quantum channel information transfer.
Although SrAl pigments have a rather short lifetime, of the order of days,
molecules with a much longer lifetime may be found in the future.
The reported experiments were performed at a distance of 4 m, but there
is no obvious potential reason for signal degradation with increasing distance
according to Quantum Mechanics, nor the problem of misalignment of optical
transfer systems. Even though only two samples were quantum entangled
with illumination during these experiments, there is no foreseeable reason
why a multiple number of samples could not be utilized as well. If
this is possible, one “master” sample could be utilized to remotely trigger
multiple QE “slave” samples.
Acknowlegement
The authors thank the E-Quantic Communications
Company for sponsoring this work and for the use of the equipment in its
laboratory. They also thank LumiNova Co, subsidiary of Nemoto &
Co LTD, and Metal Safe Sign International for providing samples of photoluminescent
pigments.
The full paper can be seen at www.arxiv.org/abs/physics/0503052 by clicking on "PDF".
Paper # 4 (November2006)
"Intercontinental quantum liaisons between entangled electrons in ion traps of thermoluminescent crystals".
Abstract:
The experiments reported in this paper
were carried out with space-separated entangled thermoluminescent dosimetry
(TLD) crystals in Baton Rouge, Louisiana (USA) and Givarlais (France)
at 8,182 km between entangled samples. Samples consisted of doped lithium
fluoride TLD's that were simultaneously irradiated in pairs together at
one location by Bremsstrahlung radiation generated by a Varian CLINAC unit.
One of the paired TLD crystals was then mailed to Baton Rouge and its entangled
counterpart remained in Givarlais. The crystal in Baton Rouge (master)
was then subjected to thermal stimulation which elicited a measurable light
emission response in the counterpart (slave) under a photomultiplier in
Givarlais. Highly correlated passive light emissions were observed in the
nonheated slave TLD while the master TLD was ramped up in temperature and
then allowed to cool to ambient temperature. Maximum correlations in the
slave TLD light emissions were observed at the turn around temperature
which is the point where the master TLD temperature is allowed to decrease.
The experimenter in Girvalais was thus able to determine with high accuracy
the point in time at which the master TLD heating oven was turned off (turn
around point) without any communication between the experimenters during
the heating-cooling phase of the experiment. The implications of these
observed results are of great significance for quantum communication technology.
Conclusion:
The reported experiments are a practical
implementation of the entanglement phenomenon of Quantum Mechanics. Two
particles are said to be entangled when they are emitted simultaneously
by the same atomic wave function, for example; photons emitted by a nucleus,
or an electron, and the photons temporarily form an interactive interference
pattern with one another. Such particles are quantum-connected to each
other and interaction with a measurement system by one of them is “sensed”
immediately by the entangled counterpart. Entanglement can be swapped between
two particles and two other particles. Entangled particles, such as electrons,
can be “stored” in ion traps or impurities within thermoluminescent crystal
lattices and remain isolated from environmental decoherence effects in
the traps for considerable amounts of time. Electrons can be forced to
leave these traps and then drop down to their respective ground state energies
in the crystal lattice by thermal heating or by stimulated luminescence.
An entangled electron dropping out of its ion trap will go through spin
transitions which affect its entangled counterpart electron by reason of
spin conservation laws such that it becomes favorable for the counterpart
electron to exit its trap as a result, emitting some light while dropping
to ground state, at whatever distances the traps are located from
one another. Since traps can be entangled even though present in separate
crystal lattices, such samples can be separated by a large distance and
the entangled electrons still be connected until perturbed by thermal heating
of the crystal lattice containing one of the trapped entangled electron
pairs. It appears that the trapped entangled electrons escape only at discrete
and unique temperature values, thus allowing the same glow curve response
(although much less intense than the heated crystal) to be recorded for
each non-heated thermoluminescent crystal when the temperature of the heated
crystal lattice is increased and decreased. These experiments amply demonstrate
that:
- Bremsstrahlung gamma ray or X photons
are entangled,
- The entangled photons can transfer their
entanglement to particles (electrons)
- swapping entanglement between particles
is possible and does occur,
- entangled particles can be “stored”
as wave functions in ion traps that behave as QED cavities within thermoluminescent
materials,
- environmental decoherence appears extremely
feeble within ion traps containing entangled electrons since the heating
and measurement experiments were conducted over one month after co-irradiation
of separate TLD chips,
- entangled electrons appear to exit the
traps only at very discrete and characteristic temperatures during temperature
increase and not in accord with the Arrhenius equation which dictates that
ordinary electron traps empty as a function of a continuum of release temperatures.
This is a significant finding of this experiment which should provide quantitative
clues for the interaction mechanisms involved in entangled electrons within
ion traps
- slave chip (non-heated entangled counterpart
crystal) glow curves correlate for the crystal lattice temperature increasing
and then decreasing via cooling (temperature turn around point) in a very
symmetrical and systematic way,
- quantum liaisons can be established
between locations situated 8,182 km apart.
Remarks:
Due to the significance of these results,
we would like to encourage other serious investigators to repeat these
experiments. Please contact either or both of the authors via email or
otherwise if you would like to replicate these experiments in order to
obtain CLINAC irradiated TLDs, etc.
Acknowledgment:
The authors thank E-Quantic Communications
SARL-ACV for funding this research. Many thanks to the Centre de Radiothérapie
Joseph Belot of the Saint François clinic of Montluçon for
irradiating the chips.
Note:
Colored pictures of the curves Figures
8 and 9 of the article can be seen as well as the photographs of the
various steps of the experiments by clicking HERE
. Many new successful tests have been run since the publication. Two of
them are presented.
Abstract can be seen by clincking
http://www.arxiv.org/abs/quant-ph/0611109 .
Complete text can be seen in English on
http://www.arxiv.org/ftp/quant-ph/papers/0611/0611109.pdf
A French text corrected by the author
can be seen by clicking HERE.
A German text corrected by a native
German can be seen by clicking HERE
Machine translations are available in
Spanish,
Italian,
Japanese,
Dutch,
Portuguese,
Russian,
and Chinese by clicking on the corresponding
link.
Note:
The machine translations have not been
corrected by native speakers of these languages.
If anyone feels like correcting some of
the translations, he or she is welcome. Just send your e-mail address to:
rdesbrandes(alice)@(bob)e-quantic.com
, delete alice, bob, and parenthesis.
I will e-mail a Word version of the paper
in the chosen language.
Thanks in advance.