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Experimental results are shown for three energies in a coplanar symmetric geometry, and for three energies in an asymmetric geometry. Ionization of atomic and molecular targets is one of the most complex and fundamental collision processes that can be studied in detail. To fully characterize these interactions, it is necessary to perform sophisticated measurements where an incident electron of well controlled momentum scatters and ionizes the target. In these (e,2e) experiments, information about the collision is obtained by measuring the outgoing momenta of the collision products.
For molecular targets, it is difficult to know the orientation and alignment of the molecule prior to the interaction occurring, unless this can be defined prior to the collision or can be measured following the collision. The interaction of low to intermediate energy electrons with molecular targets has been much less studied compared with high energy electron collisions.
Experiments on molecular targets often employ effusive beams produced at room temperature, and so the targets may have internal rotational and vibrational energy. Results are presented here for an H2O target at significantly lower energies than has been studied before.
Figure 1.1 Representation of the 1b1 state of H2O, showing an incident electron ionizing the molecule. The experiments described here were carried out in the fully computer controlled and computer optimized (e,2e) spectrometer that operates in Manchester.
For the coplanar symmetric experiments described here, the electron detectors were moved so that their angles with respect to the incident beam direction were equal to each other throughout measurement (see figure 1.2). For coplanar asymmetric experiments, analyzer 1 was fixed at a scattering angle thetaa = 22A°, while analyzer 2 was swept around the scattering plane. The fixed scattering angle thetaa = 22A° was chosen as this was the smallest angle that could be used without the incident electron beam from the gun striking the side of the analyzer (and so producing unacceptable levels of noise on the coincidence signal). The energy resolution of the spectrometer is set by the resolution of the electron gun and the pass energy of the analyzers. Production of a high quality molecular beam of H2O required careful monitoring of the experiment as it progressed.
The de-gassed water was then transferred to a 150mm long tubular stainless steel flask which was connected to the main vacuum system using a swagelok fitting. An AD590 sensor was secured to the aluminium block surrounding the flask, so that the temperature of the insulated assembly could be monitored and controlled. To monitor the molecular beam inside the vacuum chamber produced from the water, a quadrupole mass spectrometer was installed onto the spectrometer.
Figure 1.3 shows a typical coincidence energy spectrum obtained from the experiment during operation.
The experiments were carried out over a period of several months, using electron beam currents ~200nA for all data runs. As the incident energy increases, the ratio of forward to backward scattering cross section increases, as has been seen for most atomic targets in this geometry.
The measured coplanar asymmetric data is shown in figure 4, again normalized to unity at thetab = 45A°.
As the incident energy is increased to 55eV above threshold, the forward lobe splits into two clear peaks of approximately equal magnitude, as seen in figure 1.5(b). Results from the 1b1 state of water have been presented for coplanar symmetric and asymmetric energies.
These results have been compared to a DWBA theory in the paper J Phys B, however the averaging used in this theory was not a good approximation, and so is not expected to yield accurate results for this state. Experimental results are presented for electron impact ionization of water in the energy regime from near threshold to intermediate energies. Results of a sophisticated model which approximates the random orientation of the target using a spherical averaging of the wave-function prior to the collision, using sophisticated distorted wave Born calculations that include post-collisional interactions in first order and to all orders of perturbation theory are also shown for comparison (see J. The calculations predict the data most accurately at the lowest energy studied (4eV above threshold) in a coplanar symmetric geometry, whereas the comparison between theory and experiment is generally poor for higher energies and for non-coplanar geometries. Energy deposition and angular distributions resulting from electron collisions with water are used in charged particle track structure analyses to model radiation damage in biological samples. These low energy electrons have an effect over a much wider volume than the targeted cancer site.
At incident energies less than ~200eV, the collision dynamics are strongly influenced by effects including post-collision interactions, target polarization, distortions in the wave-functions for the participating electrons and multiple collisions. Current models now yield reasonable agreement with experimental data for a range of atoms, implying a good understanding of the collision dynamics under the conditions used in the experiments, and these models are now being extended to low energy (e,2e) collisions from molecules.
Recent experiments studying simple diatomic targets including H2 and N2 have provided benchmark data. The apparatus at Manchester can also access non-coplanar geometries, and so has provided additional data to further test these models. In a previous study the groups at Manchester and Missouri investigated the 1b1 (HOMO) state of H2O in coplanar kinematics. By contrast, the 3a1 orbital of interest here is involved in the O-H bonding and has a charge density distribution distorted from that of a symmetric atomic like orbital. The experimental triple differential cross sections (TDCS) presented here were measured in the (e,2e) apparatus at the University of Manchester.
The spectrometer can be operated in a standard coplanar geometry where the momenta of all three electrons (the incident and two outgoing electrons) are within the same detection plane (psi = 0A°, figure 2.1). The power supplies for the electrostatic lenses in the electron gun and the electron analyzers are fully computer controlled and computer optimized, allowing for automated tuning at regular intervals, with the analyzers being re-optimized each time they move to a new angle. The energy of the spectrometer was re-calibrated at the start of each new kinematic arrangement, by measuring the coincidence binding energy spectrum. Over the course of this study the binding energy spectra were recorded for various energies and geometries, and it is estimated that contamination from neighbouring orbitals was always less than 10%, and is more typically in the range of 0.5%. The distilled water sample used to provide the molecular target beam was contained within a 50mm diameter 100mm long stainless steel vessel sealed by a CF-70 flange to a 6.35mm swagelok fitting. The sample vessel and gas handling line were held at a constant temperature of 50A?C throughout data collection, so as to create sufficient driving pressure for the target beam. The purity of the target beam was verified with a Spectra VacScan mass spectrometer fitted to the scattering chamber. The background pressure within the scattering chamber was set to 1.1 x 10-5 torr during operation, and was found to remain constant throughout all data runs. During these experiments we observed an unusual behaviour of the tungsten hairpin filament used as the incident electron source. To facilitate this, the current measured by the Faraday cup located on the opposite side of the interaction region to the electron gun was monitored by the computer control software, and the current through the filament adjusted to maintain a beam current of 300nA throughout data collection. In the present study we also measured the coincidence energy resolution from ionization of helium, and found this did not change, indicating that the temperature of emission remained approximately constant. The data presented in figures 3-5 were then averaged over these angular sweeps, and the uncertainties in the measurements determined from the complete set of data for each scattering angle. The experimental data are not measured on an absolute scale and so experiment and theory are normalized to a maximum of unity at each energy, as shown in figure 2.2. As the energy of the outgoing electrons is lowered, it would be expected that the Coulomb repulsion between the outgoing electrons should play an increasingly important role, driving the electrons apart. The best agreement between experimental data and theory is at the lowest energy, where the experimental data and MDW model are in excellent agreement for the binary peak.
A key advantage of the spectrometer in Manchester is the ability to measure data for kinematics in non-coplanar geometries. Non-coplanar measurements were hence taken here with both outgoing electrons having an energy of 10eV. As shown in figure 1, the geometry adopted in this spectrometer provides a common normalization point (xi1 = xi2 = 90A°) for all gun angles psi, which allows ALL data at a given energy to be referenced to a common point. For the current measurements, the coplanar data have been normalized to a maximum of unity, as before. The data in figure 2.3 show a clear trend indicating the binary and recoil peaks diminish in magnitude as the angle of the electron gun angle increases.
The data contrasts strongly with the theoretical models for the larger gun angles y, where the theories predict significantly more structure than is seen in the data. The final kinematic configuration used symmetric geometries and 20eV excess energy as above, however in this case the data are for unequal energy sharing between the outgoing electrons. The data were only taken for coplanar and perpendicular plane geometries, so as to contrast differences in these two extremes.
The key differences that can be seen in these data for the coplanar geometry are that the binary peak moves to a smaller angle as the energy asymmetry increases, as might be expected from post collisional interactions. Agreement is mixed, and rather surprisingly gives best results at low energies, where it might be expected that the approximations are least accurate. The experimental results for both equal and non-equal energy sharing in the perpendicular plane show almost no structure, whereas the theoretical calculations predict that three clearly defined lobes should be seen. This work was supported by the University of Manchester and the US National Science Foundation under Grant. 12.A A  Naja A, Staicu-Casagrande E M, Lahmam-Bennani A, Nekkab M, Mezdari F, Joulakian B, Chuluunbaatar O and Madison D H 2007 J.
In 1912, Langmuir [39] immersed a hot tungsten wire in a hydrogen atmosphere, and found that above 3000 K, heat was carried away from the wire at a rate much higher than would be expected by convection alone. This analysis shows that in dilute gases, dissociation and ionization are two separate events.
If a plasma phase transition existed, it could lead to the revision of astrophysical models [42] -- for example, giant planets like Jupiter have dense hydrogen near their core, and an abrupt phase change would change the way helium partitioned itself between molecular and metallic phases of hydrogen. In our simulations, we placed hydrogen molecules (64 nuclei) in a cubic periodic box, set atom velocities randomly from a Boltzmann distribution, then integrated the dynamics equations of motion with fixed volume and energy and a time step of 0.01 fs.
However, since our system includes Pauli exclusion forces as well, such a calculation gives the wrong result, whereas ours agrees with numerical differentiation of . By looking at the distribution of electron sizes over the course of the simulation, we can estimate how many electrons become ionized. The eFF Hugoniot curve matches the curves obtained by the gas gun and Z machine, but not the ones obtained by the Nova laser. Another group has performed a WPMD simulation of hydrogen plasma, but used the earlier described Klakow potential, with an additional term added to capture electrostatic energy changes upon antisymmetrization. Reproduction of the experimental shock Hugoniot curve obtained by gas gun and Z machine; Nova laser remains an outlier. To summarize, the electron force field shows that at bohr, dissociation from molecular to atomic fluid is gradual, and the equation of state and proton-proton pair distribution functions are consistent with path-integral Monte Carlo calculations. We have examined ionization as well, but only by measuring the concentration of free (large) electrons; we find that at low densities, the temperature required to create large electrons in free space increases with increasing density, as we would expect from a Saha model. In this web page we provide detailed (e,2e) studies of electron impact ionization of noble gases including helium, neon, argon, krypton and xenon from near threshold to intermediate energies, where the outgoing electrons carry equal energy from the interaction. The experiments were conducted in the perpendicular plane, where the outgoing electrons are detected orthogonal to the incident electron beam.
The data show the cross sections undergo complex variations as a function of incident energy, and in particular ionization of the heaviest target is at variance to all others that have been studied here.
The (e,2e) process provides the most precise experimental data for the study of the ionization of atomic and molecular targets by electron impact. By determining the momenta of the scattered and ejected electrons in a time correlated coincidence measurement, the differential ionization cross section (DCS) is derived for comparison with theoretical models. Since the scattered and ejected electrons may emerge over a wide range of different angles, experiments usually define a specific scattering geometry in which to carry out the measurements. In the present work, we have constrained the spectrometer to measure the DCS only in the perpendicular geometry, where psi = 90A°. For both electrons to emerge in this geometry it is necessary for an interaction with the target nucleus to occur, and this provides a stringent test of current ionization models.
We have taken measurements with the incident electron energy E0 ranging from near the ionization threshold of the selected target, through to energies up to 80eV above the ionization potential (IP). Understanding these processes is hence important in areas ranging from the production of plasmas in stellar and planetary atmospheres, through to electron impact ionization in lasers and in nuclear reactors. In all cases results are presented for the outgoing electrons having equal energies at the analysers.
The apparatus can measure the DCS from the coplanar to the perpendicular plane geometry by moving the electron gun, gas jet and Faraday cup together around the interaction region (figure 2). The electron analysers consist of a 3-element electrostatic lens that focuses electrons from the interaction region into a hemispherical energy selector.
The data were taken over a period of several months, and the electron gun current was varied for each of the data sets so as to ensure linearity of the detection system.
The energy of the incident electron beam was determined by observing the negative ion elastic scattering resonance in helium at ~19eV, so as to determine the offset in the gun due to contact potentials.
The energies of the outgoing electrons were determined by observing inelastic scattering from the excited targets, and by considering the location of Fano resonances in the ionization continuum.
The experimental data for helium are taken from previous work carried out in Manchester re-presented here normalised to unity at the peak of the DCS to allow comparison with other noble gases. The ground state of helium is 1S0, with an electronic configuration 1s2, and so both bound electrons occupy s-shell orbitals prior to the interaction.
For helium, neon and argon targets, the bound electrons occupy either s-orbitals or p-orbitals in their ground state. It was not possible to resolve these individual channels in our experiment (due to the limited energy resolution of the spectrometer) apart from for xenon, where results were taken for production of the different ion states at incident electron energies from 10eV to 30eV above the IP. Figure 3 presents results for ionization of helium in the perpendicular plane for ten different incident energies ranging from 3eV to 80eV above the IP. As the incident electron energy increases, additional peaks are seen at angles around 90A° & 270A°.
By 20eV above the IP three distinct peaks are clearly visible, the relative strength of the central peak to outer lobes decreasing monotonically as the energy increases.
The physical reasons behind these structures has been described by several models, ranging from DWBA calculations through to TDCC models. There is only one process that can produce a peak at 180A? in the perpendicular plane without interaction with the target nucleus. The peaks at around 90A° & 270A° are found to result from elastic scattering of the incident electron from the core, followed by a single binary collision between the incident electron and a bound electron. It should be noted that although agreement between theory and experiment in the perpendicular plane has proven to be very good, the results in a coplanar geometry are not as satisfactory, particularly for non-equal outgoing electron energies. The results at the lowest energy are similar in shape to that for helium, with a single broad peak observed centred around 180A°. As the incident energy increases, the DCS for neon shows a very different character to that for helium. The mechanisms that produce these structures in neon must be quite different to that proposed for helium, apart from at the lowest energy where PCI is expected to dominate for all targets.
Al-Hagan and co-workers recently considered the low energy regime for both He and H2 from threshold to ~10eV above threshold, and concluded that for these targets PCI dominates at energies <2eV, which is also consistent with the observations for neon presented here. The results in figure 4 indicate that the interaction is clearly more complex, and may be due to the momentum distribution of the ionized p-electron and polarizability of the atom (which is 1.9 times greater for neon than for helium).
A similar study was carried out for argon, whose outer electronic structure ([Ne]3s23p6) is similar to neon ([He]2s22p6). In the frozen-core approximation as used in many theories, the inner electrons are considered as spectators during the interaction, and so in this approximation the structure of the DCS should be similar for neon and argon.
For argon, nine separate energies were chosen for study, so as to reveal the complex variation in the DCS as a function of energy. Once again the results for argon are not consistent with the simple models found successful for helium. Figure 6 shows the results for krypton, which unlike helium, argon and neon also has bound electrons occupying the 3d-shell. Once again results were taken for a lowest energy 2eV above the IP, with the data having much better statistical significance compared to those for argon at the same energy.
As the energy increases, the results for krypton show a similar trend to that for argon, with the central minimum deepening until around 10eV above the IP where a central peak starts to emerge. The similarity between argon and krypton data tends to indicate that the d-shell electrons in the heavier target are not playing a significant role in the ionization process.
As the heaviest isotopically stable noble gas target, xenon has the largest calculated size (108 pm) due to full occupation of the 4d, 5s and 5p shells.
The ionic ground states of Xe+ are sufficiently separated that it was possible to resolve ionization to individual states during the experiments, for energies up to 30eV above the IP. The data are particularly surprising since they do not follow the general trend seen for all other noble gas targets at higher energies.
The minimum at 180A° is significantly deeper than for krypton under the same outgoing energy conditions, and unlike krypton this minimum then becomes shallower as the incident energy increases.
These results show that the mechanism for ionization of xenon must once again be different to all other targets that have been studied. As far as we are aware this phenomenon has never been observed for any other target, and it remains to be seen why this should occur for xenon.
Only three energies were selected for these experiments, due to the difficulty of obtaining good statistical data.
The set of data presented here for isotopically stable noble gases shows there is a large variation in the probability of ionization in the perpendicular plane. The perpendicular plane is particularly poignant for testing the most sophisticated electron impact ionization models, since multiple scattering must occur for electrons to emerge in this plane. The perpendicular plane has proven to be a fertile ground to test recent theoretical models, which have found success for simple targets such as helium and molecular hydrogen. It appears that PCI plays a role at the lowest measured energy for each target, although the significance of this process reduces as the target weight increases. The most surprising result is for the heaviest target xenon, since the relative magnitude of the central peak continues to increase as the incident energy increases, and the side lobes reduce to insignificance. It is worth noting that the resolved data for ionization to the different Xe+ states indicate there is little variation to the measured cross section due to fine structure effects.
KLN thanks the Royal Society for an International Newton Research Fellowship held at the University of Manchester.
If you look out your window but cana€™t see the masts because they are obstructed by other buildings then the power density will be mainly absorbed by those buildings and too low to worry about. If the substation is immediately next to your home there is little in a practical sense you can do to reduce the magnetic fields. Unless the substation is immediately adjacent to your house the EMFa€™s from these small street substations fall to background levels within about 3 meters. WI-FI and DECT phones are overwhelmingly the main contributors to household electro pollution with power densities far above any nearby mobile phone mast.
If your internet connection is by telephone you will need the Netgear DG834 model opposite. If your internet connection is via a cable connection you would need the Linksys wired modem opposite. These alarms use the same technology as DECT cordless phones and will continuously pulsate microwave energy throughout the babya€™s room and beyond.
Best to change your old cathode-ray monitors (the ones with the deep backs) to any type of flat screen monitor as these give of far less Electromagnetic fields than the old type which thankfully you cana€™t buy any more. In order to get your body back to its proper earth bound resonance you need to be sleeping earthed.A  Explanation of what is sleeping earthed and how you can do it is found on my website. Geobiology explores the relationship between life and the Eartha€™s physical and chemical environment. The history of geobiology in this respect dates back to 1929 when a German aristocrat Baron Gustov Von Pohl, an eminent dowser, made the extraordinary claim that cancer was caused by a€?energy linesa€™ that ran under the beds of the people that had died from the disease.
Underground Streams: a€?Water will flow through any underground passage, fracture of fissure. The dark square with flashing white lines is a photographic print of microwaves radiating in the space above an underground watercourse taken in total darkness.
Diagram depicts the flow of underground water and consequential chemical reactions within certain geological features that could be the origin of geopathic stress issues.
The dipolar nature of water molecules can also be part of the origin of electromagnetic fields originating from ground contained water. The electromagnetic spectrum refers to the range of different types of Electromagnetic Radiation.a€?These are usually sorted by the frequency. For visual explanation, NASA have a simple but useful diagram, and there is a far more detailed diagram available from thinkgeek (purchase required). We believe that one of the main reasons that EMFs (particularly microwave frequencies) are potentially bioactive is due to the nature of the signal itself.
We have evolved with the natural levels of EMFs produced by both the sun and world around us.
Power frequency (50Hz in the UK) is given off by any appliance or transmission of AC (alternating current) electrity.
Childhood leukaemia has been internationally accepted as linked to powerfrequency exposure magnetic fields, with a wealth of literature finding increases in risk to this and other illnesses.
It is well documented and generally accepted that over-exposure to ultraviolet rays can cause burning and skin cancer.
There are internationally accepted guidelines by the International Commission for Non-Ionising Radiation Protection (ICNIRP) that have been designed to limit both residential and occupational exposure to levels that are safely below those that can heat up tissue. However, recently there has been a number of studies showing very specific biological effects far lower than these levels (see our Studies list), and as yet there is no international guidance that has taken any of these studies into effect.
Powerfrequency electromagnetic fields are generated by any appliance running off AC (alternating current) power - anything plugged into a main power socket will generate them to some degree. At the moment, health effects primarily associated with powerfrequency EMFs are due to the magnetic component - these include, but are not limited to, Childhood Leukaemia, Adult Leukaemia, Amyotrophic Lateral Sclerosis, Miscarriage, and Clinical Depression. There is a fairly brief overview of health risks and evidence in the health concerns section of the electric power transmission article on Wikipedia. The last type of geopathic disturbance that I want to talk about before we have a look at man-made electromagnetic energies concerns the earth's natural geomagnetic field (the one that makes a compass needles pointA  north).


The first geomagnetogram (G1) typically represents the values of the Earths normal geomagnetic field taken by me in a farmer's field near Poynings village not far from where I live.
The second geomagnetogram (G2) was taken above a sprung mattress from a lady suffering from chronic fatigue syndrome and severe depression, and has a magnetic anomaly of 22,435.4 nT. The Cliff of Tears a€?It is important not to underestimate the value of the earth's natural geomagnetic field (DC Field) which interacts with our bodies in many positive waysA  This DC field rarely shows an anomaly above or below 2% of its normal strength which differs according to the latitude in which you live. Unnatural Alterations in the Earth's Geomagnetic Field a€?A second and equally important influence on the sequence of mitosis is the role in which the normal earth's geomagnetic field (DC field) influences the formation and production of a healthy pregnancy. Health risks due to exposure to electromagnetic fields EMFa€™s in the home were first suggested in America by Wertheimer and Leeper, when they estimated the levels people were exposed to, using a€?wire codesa€™, and the local incidence of childhood leukaemia. Stress sensitive hormones such as prolactin and thyroxide have been found to be elevated in people at work in high electromagnetic environments.A  Prolactin plays a key role in moderating parts of the neuro-immune system and may also be an important precipitator of auto immune diseases. It has been scientifically proven for the first time, with a double blind study by means of an electrocardiogram, that the detrimental effects of a€?water veinsa€? and other geopathically disturbing phenomena can cause serious health problems to persons exposed to them. This presentation took place in March 2003 in the large auditorium of the Saint Johanns-hospital Landesklinjken SalzburgA  Germany. At locations where Geopathic stress zones are present, subsurface water plays a predominantrole, either as lakes, slowly moving underground water, or as water streams. Technical electromagnetic fields can also drastically affect the human body, as soon as certain field strengths are reached. The electromagnetic spectrum refers to the range of different types of Electromagnetic Radiation.These are usually sorted by the frequency.
The Cliff of Tears It is important not to underestimate the value of the earth's natural geomagnetic field (DC Field) which interacts with our bodies in many positive waysA  This DC field rarely shows an anomaly above or below 2% of its normal strength which differs according to the latitude in which you live.
Coplanar symmetric and asymmetric electron impact ionization studies from the 1b1 state of H2O at low to intermediate impact energies. The experimental data show a wide variation in the cross section over this range of energies.
These ionizing collisions are important in a wide range of different areas, ranging from plasma physics, astrophysics, atmospheric physics, medical and biological processes involving low energy electrons through to the study of high voltage discharges.
The scattered electron is then detected in time correlated coincidence with either the electron ejected during ionization, or with the resulting ion. This is usually accomplished by determining a cross section that is five fold differential in angle and energy. In most cases, this means that an averaging over the orientation of the target must be included for theory to compare with experimental results. This energy region (from threshold to ~200eV) is important as it is here that the cross section for ionization is largest.
The ionization potential from these ground ro-vibrational states is usually less defined than for atomic targets, due to the associated Franck-Condon overlap between the potential energy curves of the neutral molecules and the resulting ions. This apparatus is described in detail on other web pages on this fileserver, and has been designed to operate in the energy regime from ~10eV to ~300eV. In this configuration, the energies selected for the scattered and ejected electrons were equal.
The inner diameter of this flask was 9mm, and the outside diameter was 12.7mm, so that a standard swaged fitting could be used. This was accomplished using a Newport model 325 temperature controller, which supplied drive current to the TEC. This proved invaluable, as it was then possible to continuously monitor the background gases in the chamber during operation. In this example, the analyzers were set to pass electrons of energy 20eV, and a symmetric geometry was chosen with thetaa = thetab = 45A°. Over this period of time, the filament current driving the cathode had to be steadily decreased, probably since the water vapour within the vacuum chamber slowly reduced the diameter of the filament. The data is normalized to unity at thetaa = thetab = theta = 45A°, since the results have not been placed on an absolute scale.
Results were taken in symmetric coplanar and non-coplanar geometries, with both equal and non-equal outgoing electron energies. The human body, and other biological material comprise of ~80% water, which makes it an ideal test case to investigate processes occurring in the body. These models are an active area of research since the observation that high energy radiation that is used to treat cancers also liberates many low energy electrons, causing additional damage to cell DNA. Knowledge of the collision dynamics of low energy electrons with biological systems is hence needed, so as to develop robust models of these processes. In such experiments the energy and momenta of the outgoing electrons are measured, giving a five fold differential cross section. In this regime these processes must be considered on an equal basis, and so the complexity of the interactions means that theoretical studies have mainly been limited to atomic targets. This contrasts to atoms which have a single nuclear scattering centre, and which can hence be described using a spherical basis. A further challenge arises since the experiments cannot, at present, align the molecules prior to the collision, so the models must consider the random orientation of the targets for accurate comparison.
The majority of data is recorded in a coplanar geometry, where the incident and two outgoing electrons are in the same plane, and were conducted at a higher incident energy than the studies presented here.
The symmetry of the 2py oxygen atomic orbital, representing the lone pair of electrons on the oxygen atoms, prevents it from hybridizing with the H atomic orbital, leaving the molecular 1b1 HOMO orbital essentially atomic like, and therefore symmetric. However, the orientation averaged molecular orbital used in the theoretical calculation is a bad approximation for that state given the cancellations due to the orbital symmetry. The molecular orbital used in the model therefore should not suffer from the same cancellation problem during the orientational averaging procedure.
This apparatus is fully computer controlled and computer optimized, allowing it to operate continuously without user intervention. A coplanar geometry (psi = 0A?) is defined when all three electrons are in the detection plane.
The angular resolution of the apparatus is estimated as A±3A°, based on geometric considerations of the electrostatic lenses at those energies.
Several freeze-pump-thaw cycles were performed using a salted ice slurry bath, to remove dissolved gas impurities from the water prior to admission into the scattering chamber. Over time the emission current from the filament dramatically increased, when a constant current was delivered to the filament. The data were normalized to a collection time of 1000sec for each measurement, and up to 30 sweeps of the detection plane were used to produce statistically significant results. The overall shape of the TDCS measured at corresponding energies in a previous study of the 1b1 state are qualitatively similar, however the 1b1 state shows a second peak in the binary region emerging at higher energies that is not observed in the 3a1 state. PCI would also be expected to shift the recoil peak towards xi = 90A°, although this cannot be confirmed in the data. This agreement diminishes as the energy increases, which is unexpected since the MDW model is usually more accurate at higher energies. The TDCS measured in the perpendicular plane is almost constant over all analyzer angles, which is very different to what is observed for atomic targets.
The progression in both models shows a decrease in cross section from psi = 0A° to 45A°, after which the intensity once again increases. There also appears to be a narrowing in the main binary peak as the asymmetry increases, with a new shoulder appearing around xi = 60A°.
This contrasts markedly with the calculations, which predict triple peaks in the perpendicular plane that change magnitude only marginally with the asymmetry. This discrepancy is seen both for equal energy and for non-equal energy data, which have been taken in coplanar and perpendicular geometries.
Their results agreed well with eFF at low temperatures, but deviated significantly at higher temperatures, with a higher compressibility (6.4 times) that better matches the Nova laser data. For electrons to emerge in this geometry they must undergo multiple scattering including scattering from the nucleus of the target, and so this provides a highly sensitive test for scattering theories. In these experiments a single electron of well defined momentum impacts with a target in the interaction region, resulting in target ionization and a scattered and ejected electron which emerge after the interaction has taken place. Our (e,2e) apparatus can access a wide range of geometries from a coplanar geometry, where the incident, scattered and ejected electrons all occupy the same plane, through to the perpendicular geometry, where the scattered and ejected electrons emerge in a plane orthogonal to the incident electron trajectory (figure 1). In this regime the probability of single ionization is a maximum, and so it is here that most ionizing collisions with electrons occur in nature.
Low energy electron ionization has also been attributed to the production of DNA damage in biological tissue, and so it is important to understand these collisions at a fundamental level to describe the physics of these processes. The helium results are reproduced from previous studies carried out in Manchester, re-presented here for completeness. By choosing the analyser residual energy to pass electrons around the selector, a channel electron multiplier detects electrons of the specified energy for subsequent amplification and counting. In the perpendicular plane, only the mutual angle phi = xi1 + xi2 is relevant, where xi1, xi2 are as shown in figure 1. The orbital angular momentum of each electron is hence zero, with a momentum distribution that peaks around zero a.u. The configuration of the 10 electrons in neon is 1s22s22p6, whereas argon has 18 electrons occupying a configuration [Ne]3s23p6. The data files for these results can be downloaded as a TAB deliminated text file Helium.txt. Experimental results for the ionization of helium in the perpendicular plane, with incident energies ranging from 3eV to 80eV above the ionization potential for this target. This is considered to be due to the dominance of post-collisional interactions (PCI) between the outgoing electrons, which drives electrons emerging with equal energies from the interaction region asymptotically towards opposite directions.
At ~50eV excess energy the three lobes have equal amplitudes, whereas at higher energies the outer lobes dominate. The DWBA theory most easily allows the different processes involved in the interaction to be switched on and off, and this has explained the origin of these lobes. This process requires the momentum of the incident electron to be exactly matched by the momentum of the bound electron, with both electrons moving in opposite directions prior to the interaction. In this case, since the particles have equal mass and energy, they emerge from the interaction region at a mutual angle of 90A° & 270A° as observed. It is therefore clear that further work is needed to fully describe the ionization reaction, even for a simple target like helium. The lowest energy studied was 5eV above the IP, with six measurements being taken up to 50eV above the IP as shown.
Experimental results for the ionization of neon in the perpendicular plane, with incident energies ranging from 5eV to 50eV above the ionization potential for this target. The width for this peak in neon is ~120A°, which is broader than ~80A° for the same outgoing electron energy in helium. As the energy is raised to 10eV above the IP, the broad single peak seen at the lowest energy increases in width, and develops a flat structure at the peak. However, at higher energies the mechanisms proposed for helium ionization described above would be expected to produce similar structures in all targets that have a central ionic core.
The calculated atomic radius of argon (71pm) is however significantly larger than that for helium (31pm) or neon (38pm) due to the n=3 shell being occupied. Experimental results for the ionization of argon in the perpendicular plane, with incident energies ranging from 2eV to 50eV above the ionization potential for this target. The lowest energy studied was 2eV above the IP, the data at this energy having poor statistics due to experimental difficulties working with argon at this energy. This minimum flattens at 10eV above the IP and rapidly evolves into a clear peak 15eV above the IP. The results further indicate that the use of a A”frozen-coreA• approximation is unlikely to be accurate in any theory attempting to emulate these data.
The physical size of krypton (88pm) is slightly larger than argon due to occupation of this shell, and due to closed occupation of the 4s and 4p shells.
Experimental results for the ionization of krypton in the perpendicular plane, with incident energies ranging from 2eV to 50eV above the ionization potential for this target. Ionization of krypton no longer shows the dominance of PCI as predicted by Wannier, since there is now a central minimum at 180A°. This central peak is not as significant in krypton compared to the side lobes, and by 30eV above the IP is once again diminishing. It also appears that the variation in cross section as a function of energy follows a similar pattern for each of these targets.
A coincidence energy loss spectrum is shown in figure 7 to illustrate this separation at an incident electron energy 10eV above the IP for this target. The results were taken from 2eV above the IP to 70eV above the IP for this target, so as to establish the variation in the cross section that is observed. At the lowest energy 2eV above the IP, a clear two-peak structure is observed which is similar to that observed from krypton. The results at higher energies are surprising, as the mechanism that produces the central peak with the electrons moving opposite each other is clearly dominating all other scattering processes.
The data files for these results can be downloaded as a TAB deliminated text file Xenon2.txt. These data indicate that fine structure in the final ion state does not play a significant role in the ionization process, since the comparison between this data and that reproduced from figure 8 shows that the shapes of the cross section for each energy are very similar. This contrasts to the coplanar geometry most often adopted, where the dominant scattering mechanism is usually a single binary scattering between electrons, resulting in a high probability that forward scattering occurs. The results presented here will hence further test these models for heavier targets, so as to elucidate the scattering mechanisms that result in the observations.
Argon, krypton and xenon also all evolve a central peak as the incident electron energy increases from near threshold, which cannot be due to PCI. The side lobes observed previously in the perpendicular plane have been attributed to a binary collision between the incident electron elastically scattered into this plane and a bound electron. It is hence likely that the results for neon, argon and krypton are also not significantly altered by these effects, even though the spectrometer was not capable of resolving their individual ion states. CK would like to thank the University of Manchester for providing a PhD scholarship while carrying out this work. Or if you are addicted to cordless phones by the low energy Eco + friendly types that only emit a signal when you are using them.A  Google Siemens Gigaset Low Radiation Phones. An example of this is a digital bedside alarm clock that only need 6 volts to operate but plugged into your 240 volt ring circuit. Click first on my a€?Studenta€™s Notesa€™ button and scroll to the end for pictures and explanation. The term was adopted many years ago by some German dowsers, a€?geobiologistsa€™ who specialised in surveying houses for both geopathic and electromagnetic stress using both dowsing and scientific instruments. To test his theory he persuaded the Mayor of the Bavarian town of Vilsbiburg to allow him to survey the town for such energies with his dowsing rod. As it does so it produces its own electromagnetic field often high into microwave frequency.
It has been known for a long time that when there is flowing water under a dwelling the inhabitants always feel more tired, are prone to premature aging and have a loss of vitality than those who sleep above neutral ground. As an extremely dialectic medium, water favours the formation of potential vortices, which immediately after their formation contract swiftly.
Background levels of EMFs vary hugely depending on which part of the spectrum being looked for - natural light is an obvious example. Electrical wiring creates electric and magnetic powerfrequency fields throughout houses and other wired buildings, but these levels are usually very low unless there is a wiring fault. Most areas of science can only deal in probabilities, and that becomes clearer as more scientific studies investigating health effects are produced. There is more disagreement about ill health effects from radiofrequency radiation, which is newer for most of the population, though a well-established 'microwave sickness' has been described. As a result fortunes are spent on protective sun cream and information services as to prudent avoidance of such exposures. Molecules in the food are vibrated by high levels of microwave frequency Electromagnetic energy, causing it to heat up and subsequently cook. This, coupled with misleading statements designed to imply that there is currently no published evidence showing a link from organisations such as WHO, are the primary reasons why this topic remains in such hotly-disputed contention. ICNIRP have set guidelines for residential and occupational exposure to powerfrequency magnetic fields, based primarily on electric shock responses and induced currents, currently set at 100 microtesla (AµT) - equivalent to 1 Gauss. The evidence on these is mixed, but the link with Childhood Leukaemia is now considered to be pretty solid, with a doubling in risk at magnetic fields above 0.4 AµT (again far below the guidelines set by ICNIRP). The bottom line is that nature neverA  intended us to sleep on such a disturbed site as shown in figure G2 which has been artificially produced by the bed being placed near to a radiator ( causing the high spike to the right of the graph)A  and the springs causing the rest of the disturbed site. As you can see the magnetic contours of this bed size area (6a€™x4a€™) are very gentle and slightly undulating showing an overall geomagnetic anomaly of 582 nT (nano Tesla). The sprung mattresses I have measured so far over the past two years have had magnetic anomalies between 4,000 and 61,000 nT.
However there are instances in nature where abnormal magnetic anomalies exist usually due to a sudden change in mineralogy or geological structure over a short distance. It appears that the exposure of a dividing cell to an inhomogeneous DC magnetic field causes a physical force to be exerted on the chromosomes or on one of the other microscopic structures associated with mitosis, resulting in structural abnormalities in the chromosomes. Since that time, international research has increased year by year, and the potential health risks have been identified as cancer (especially childhood leukaemia, probably the most studied illness because of the original findings), depression, suicide, miscarriage, some forms of dementia, respiratory and immune system problems. Research by scientists such as Ross Adey in the USA and Dr Cyril Smith here in Britain is moving the frontier of our understanding. Hubank of Vienna: a€?Speaking at a conference in England paid tribute to a group of Austrian researches composed of medical doctors, physicists and biochemists. There is clear indication that a combination of technical fields and Geopathic stress zones can multiply the effect and therefore become extremely harmful to all living beings.
Theoretical approximations accurate at high impact energies can no longer be applied, and so there are stringent demands on theory which must be satisfied for accurate comparison with data. The (e,2e) coincidence signal for molecules may then have a correspondingly lower yield compared to an atomic target where the ionization potential is well defined. A pictorial representation of the water molecule in the 1b1 state is given in figure 1.1 below.
The spectrometer allows measurements to be conducted from a coplanar geometry through to the perpendicular plane, although in the present measurements only a coplanar geometry was used.
The analyzer pass energy was then set to measure electrons so that the overall resolution of the coincidence signal (as measured using a helium atomic target) was 600meV. The pump removed background gas from the flask, and extracted dissolved gases held in the water.
The flask was secured to the cold side of a 50mm x 50mm thermo-electric cooler (TEC) using a large aluminium block, and the assembly (flask + block) was insulated from the air using Styrofoam. The 1b1, 3a1 and 1b2 states are clearly resolved in this spectrum, which is fitted to three Gaussian peaks to ascertain the widths of the spectral profiles. These data were measured in a coplanar geometry with outgoing electron energies of 20eV detected at theta1 = theta2 = 55A°.
Figure 1.5(a) shows the lowest energy results, with an incident energy 15eV above the ionization threshold.
Molecular wave-functions are generally not spherical, the nuclei within the molecule providing multiple scattering centres. This becomes a computationally intensive problem, and so approximations are usually made to allow these calculations to become tractable.
In this study the analyzers were always kept in a symmetric configuration with xi1 = xi2 = xi.
A needle valve at the entrance to the scattering chamber controlled the flow of target H2O vapour into the interaction region. This indicates that an H2O target molecular beam of high purity was created, as confirmed from binding energy spectral studies.
This increase in emission current was often more than a factor of 2 within a 24 hour period. The solid line shows results from the Molecular Distorted Wave Born Approximation (MDW) while the dashed line was generated from the Molecular 3-body Distorted Wave Approximation (M3DW).
This trend is much clearer in the present data compared to that from the 1b1 state measured at higher energies.
For the theoretical model, the coplanar TDCS has also been normalized to unity for both MDW and M3DW models. These measurements were taken in a series of symmetric non-coplanar geometries with outgoing electron energies of 10eV. The M3DW model follows a trend that is closer to the experimental data, although neither model accurately predicts the results that have been obtained. The theoretical calculations are also shown, where once again the data and theory have been normalized to unity at the peak in the coplanar geometry.
The minimum around 90A° in this geometry does not change substantially as the energy sharing changes. Hence it is possible to accumulate a full range of DCS measurements over all scattering angles using this spectrometer. The incident electron can move from the coplanar geometry (psi = 0A°) to the perpendicular plane (psi = 90A°), the outgoing electrons being measured in the detection plane. The shape of the DCS for a given energy and target is then of importance, for comparison with theory.
This contrasts with the other noble gas targets whose levels are 1S0, but whose valence electrons occupy closed p-orbitals.
By contrast, the bound electrons in both of the heavier targets also occupy d-orbitals, with a correspondingly more complex momentum distribution. As the outgoing electron energy is lowered, the post collisional interaction time increases, resulting in an increased flux in the 180A° direction. At excess energies over 80eV above the IP the central lobe has virtually disappeared, leaving only the two outer lobes in the DCS. In this case, momentum conservation requires the outgoing electrons to move in opposite directions (180A°) in the perpendicular plane. The data files for these results can be downloaded as a TAB deliminated text file Neon.txt.


At 15eV above the IP this flat structure has evolved into two peaks with 180A° now being a local minimum. The static polarization of argon is eight times larger than for helium, so scattering effects due to polarization of the target are expected to be significantly larger than for neon or helium. The data files for these results can be downloaded as a TAB deliminated text file Argon.txt.
This central peak is visible for incident energies up to 40eV above the IP, until at the highest energy (50eV above the IP) this has once again disappeared, the side peaks having also moved outwards compared to at the lower energies. The relative magnitude of this minimum compared to the peaks around 110A° & 250A° is however larger than for higher incident energies, so there is probably a contribution to the cross section at this angle due to PCI.
This central peak has virtually disappeared 40eV above the IP and there is no evidence of a peak 50eV above the IP. It might hence be expected that the cross section for the heaviest target (xenon) would follow a similar trend to that of argon and krypton. The data are fitted to two Gaussians, showing that contamination from each ionic state is <10% when the spectrometer is set to each peak in the cross section. The data files for these results can be downloaded as a TAB deliminated text file Xenon1.txt. This indicates that PCI is once again not the dominant mechanism producing the cross section at this energy.
The relative magnitude of this peak compared to the lobes at 110A° and 250A° then increases in magnitude as the energy increases, as with krypton and argon. This result indicates that fine structure does not appear to play a significant role in electron collision processes at these energies. The marked contrast between results for helium and all other noble gas targets demand that these models carefully consider the intricacies of the interaction, since a simple extension of the basic physical ideas presented for helium cannot explain the experimental data. For argon and krypton the relative magnitude of this peak increases with respect to the side lobes until it reaches a maximum, then decreases to become insignificant at the highest energies measured. This process has always been considered as the dominant mechanism at higher incident energies, yet the new results presented here indicate these ideas need to be revisited for this heavy target. The Mayor agreed and in January that year Baron Von Pohl accompanied by the Mayor and other officials measured numerous energy lines that ran through the streets and houses of the town. This field will fluctuate depending on what is dissolved in it, how fast it is flowing or whether it is interacting with any other type of earth energy. While water running beneath a domestic dwelling should be avoided, a stream situated nearby and open to the sky will favourably discharge its negative energies harmlessly into the atmosphere.
Taking its electric charge distribution in to account, turning a water molecule will result in a changed field composition.
The electric field is produced by stationary charges, and the magnetic field by moving charges (currents). The earth's magnetic fields are static fields, unlike man-made alternating current (AC), which has no natural counterpart.
Unfortunately the studies are not always well done, and the flaws in any given study (showing an effect or otherwise) are often not reported. Precautionary levels which will protect us from illness have not been agreed on, as some countries wish the levels to be lower than others. If you stood in front of an operational microwave with no door your insides would slowly be cooked. The reason for these abnormally high magnetic abnormalities is a result of the bed springs intensifying the magnetic flux of these fields, made worse by the interaction of high magnetic fields around the bed and house from numerous electrical appliances, extension cables running under the bed and transformers placed near to the bed. One instance of this is in the USA, at a place called Gyngywamp, near Croton, Connecticut knownA  as 'The Cliff of Tears' where visitors to this site very frequently become depressed, gums start to bleed and nose bleeds occur. Messages pass between the brain, nerves and organs and even from cell to cell by electro- magnetic signalling. In the course of several years research using classical medical methods they investigated about 1000 people for the effects of these geopathic interference zones.
There were about 400 people present including numerous renowned specialists; physicians, physicists and geologists, in the all-German audience. Also, metal ions moved by water can induce small intensity broadband electromagnetic fields (EMF). The angles that could be accessed in this configuration ranged from thetaa = thetab = 25A° through to thetaa = thetab = 135A°.
The acceptance angle of the analyzer lenses was A±3A°, as set by input apertures at the entrance to the electrostatic lenses. This de-gassing procedure was carried out for ~2 hours before the water sample was used in the experiment, to ensure that the proportion of dissolved gases in the water was minimized. The hot side of the TEC was attached using thermal conducting paste to an aluminium heatsink to which a 12VDC boxer fan was secured, so that heat from the TEC could be dissipated efficiently. If this ratio reduced, the experiment was halted and the water changed to a newly de-gassed sample. In this case, the 1b1 state was found to have a width of 620meV, which is comparable to that for an atomic target. The contrast between the maximum and minimum in the cross section increases as the energy increases. As the energy increases further to 95eV above threshold (figure 1.5(c)), the double peak in the forward direction is still visible but the magnitudes of the peaks are now different. The purity of this beam was monitored regularly using the mass spectrometer throughout this study. To ensure constant incident electron beam current throughout the measurements as required, the filament current was hence also placed under computer control.
The experimental and theoretical data has been independently normalised to unity at each energy.
Dr Kate Nixon thanks the British Council for funding under the research exchange programme, and the Royal Society for a Newton International Fellowship. For the data presented here, the perpendicular plane was chosen, so only the mutual angle phi = xi1 + xi2 is relevant. The combined coincidence energy resolution of the unselected energy electron gun and the two analysers is ~1eV.
Krypton has 36 electrons and has a ground state configuration [Ar]3d104s24p6, while xenon has 54 electrons with a ground state configuration [Kr]4d105s25p6. This type of threshold behaviour was first predicted by Wannier and was later considered by Peterkop, Rau and others to explain results in this regime.
This mechanism was considered as being the main reason for the peak at 180A° until the work of Madison and co-workers in 2009 showed the probability of this occurring was low. As the energy increases further, the peaks separate in angle, and the minimum at 180A° deepens. This angular shift of the side lobes is consistent with PCI playing a continuing role in the interaction, since as the energy increases the effects of PCI diminish, and the electrons move away from 180A° as is observed. The data files for these results can be downloaded as a TAB deliminated text file Krypton.txt. However, unlike krypton and argon whose central peak reaches a maximum and then decreases, the central peak in xenon continues to dominate the cross section as the energy rises.
Further, the frozen core approximation often adopted in these models which treat all non-ionized electrons as spectators does not appear valid for the heavier targets when compared to neon, even thought the outer valence electrons have the same p-type character. Baron Von Pohla€™s energy lines were then compared with the towna€™s record of houses where people had died from cancer during the last ten years, which showed a remarkable coincidence. Dr WA?rst conducted experiments in several German towns, in the rooms of cancer patients and found unusual amounts of gamma radiation in the houses he surveyed using a Geiger a€“counter. Interference with the earths natural energy field is particularly marked by the flow of these underground streams especially where two watercourses or other types of energy line cross. If thus in a pipe a hydronamic flow vortex is produced, an electric and magnetic vortex and eddy current, are the result.
Microwave frequency exposure is a relatively new phenomenon: 100 years ago the background radiation was millions of times lower than it is now, and it is as recent as the mobile phone boom (~1990's) that the modern, digitally pulsed signals have become ubiquitous in the Western world.
Because of this, microwave ovens are stringently designed against leaks, and opening the door operates a safety mechanism which disables the oven, thus removing the risk to the operator. Within our evolutionary history our bodies own magnetic field has integrated with this magnetic field which is responsible for controlling amongst other things, circadian rhythms, mood changes and certain hormone production such as melatonin and serotonin. Our forefathers sleeping on straw or feathered mattresses in houses devoid of any electrical fields or microwave energy would not have experienced such geomagnetic disturbances. Much of the research in the past 35 years into EMF health effects has concentrated on magnetic fields because they are easier to measure and it was thought they were more likely to interact with our bodiesa€™ cells.
When this is interfered with by outside EMFa€™s problems begin to emerge, as the systems that control and regulate our bodies are impaired. They found that the altered electrical and magnetic field above a geographical distressed zone changed the electrical impulses passing along the nerves of the body. For asymmetric geometries, thetaa is fixed at 22A° while analyzer 2 is swept around the scattering plane. A glass flask was used for this procedure as this allowed the process to be visually monitored.
This indicates that the energetic effects of ro-vibrational transitions from the ground state to the ion state are negligible for this state.
Further checks were made regularly on the energy of the incident electron beam by monitoring the coincidence energy spectrum (figure 1.3), and regular monitoring of the partial pressures of the gases in the vacuum chamber. A second peak occurs in the backscatter region, however the maximum of this peak appears to occur at thetab < 225A°. For non-coplanar geometries the electron gun is lifted out of the plane, and is defined by the angle psi. Heavier atoms ionize at even higher temperatures, and Saha [40] proposed in 1920 that one could infer the temperature of stars from their relative concentration of ions. They proposed a triple scattering mechanism to describe this peak, where the incident electron first scatters elastically from the nucleus so as to enter the detection plane, followed by a binary inelastic collision with a bound electron, followed by elastic scattering of one of the electrons back from the nucleus.
This trend continues up to the highest energy which was possible to measure (70eV above the IP), where the central peak is seen to be broad with a width ~100A°. It is hence likely that these assumptions will need to be relaxed to accurately model the data. Well this surprised the establishment at the time, and knowing Vilsbiburg to have a high degree on cancer victims anywayA  he was asked to repeat the exercise in the City of Stetten which had a far lower incidence of cancer thus ironing out any chance factors. StA¤ngle, who had a very good reputation of locating water bearing fissures in crystalline rock with his dowsing rod developed a stintilisation counter more sensitive and accurate than a Geiger counter and carried out a scientific survey in the French town of Moulins where a local physician, Dr, J Prichard claimed that cancer victims in the town dwelt above geological faults. In a league table of radiation associated with biological damage, the outside line of a subterranean water course would be at the very top since it is found in association with many terminal and debilitating diseases. You can't see, feel or hear electromagnetic fields, apart from visible light, which is a part of the electromagnetic spectrum.
Each static magnetic field bump or sink on geomagnetogram (G2) may speed up or slow down body fluids (blood and lymphatic) in exposed areas such as the brain, heart, lung, liver, legs etc. Most scientists believe that, although EMFa€™s do not directly cause the illness in most cases, at least, living in fields above 200 nT (nano Tesla) may make a person develop the cancer or other illness, when if they didn't live in this field level, their bodies would be able to repair themselves, or cope with the daily damage from other causes in a healthier way. This wrong or confused information resulted in the dysfunction of individual organs and also explained the high number of diseases.
There is an offset of 1eV in the position of the peaks which is due to contact potentials in the spectrometer.
The full line represents a three-Gaussian fit, whereas the dotted lines show the individual Gaussians from this fit, illustrating the degree of separation measured with the current energy resolution. The results in the backward direction also have structure, with a minimum occurring when thetab ~ 250A°.
This complex mechanism was found to emulate the cross section more closely compared to the single scattering process originally envisaged. As for all measurements in this study, the DCS must be zero for the electrons emerging at the same angle (0A°, 360A°), due to post collisional interactions between outgoing electrons of equal energy.
At all energies greater than 40eV above the IP, the outer peaks seen in all other targets have disappeared. Whilst WA?rst and StA¤ngle thought that gamma radiation from fissures could be a significant cause of cancer, more recent studies suggest that this is unlikely as gamma radiation tends to whiz straight through the body rather than causing direct hits on DNA.
Sleep time exposure to the same sharp variations of magnetic fields for years may induce some chronic health effect. Indeed, in the town nearby, doctors and nurses are familiar with this sudden onset of illness in visitors to this old Indian sacred site. They proved a weakening in the immune system, which interacts with the wrongly programmed nervous system in persons who had been exposed. Using a randomized double blinded trial*, it has been scientifically shown that Geopathic stress zones do cause chronic stress and therefore can weaken the body's defence systems.
Finally, this stress, in combination with a possible suppression of certain functions of the immune system.
Very little contamination is expected from neighbouring orbitals in the measured TDCS for the 3a1 state. Harger, chairman of the city's medical scientific association, declared that all such a€?deadly earth currentsa€™ ran beneath the beds of all the 5,348 people who had died from cancer during the last 21 years. The culprit is thought to be the more pernicious alpha radiation from Radon which is found with high levels of gamma radiation.
The World Health Organization in a health criteria report recognizes interactions between variations in static magnetic fields in cellular tissues to include an induction of electrical potentials and magneto hydrodynamic effects in the circulatory systems and by direct stimulation of nerve and muscle cells even under extremely weak thresholds.
The causation seems to be that within a few meters the geomagnetic DC field varies from 330 milligauss at an 80 degree dip to 700 milligauss at a 59 degree dip. Confirmation of these experiments continue to appear and links have been, formed with the onset of cancer, Alzheimer's Disease, Chronic Fatigue Syndrome, Miscarriages, Multiple Sclerosis (MS) and other diseases of the central nervous system. Research in this field continues with an increasing number of sophisticated environmental measuring instruments coming on the market to aid the geobiologist in identifying causative factors to illness and disease. The very high electric fields associated with high voltage overhead power lines also cause air ionization, charging toxic aerosols so that they become even more dangerous. To varying degrees the health consequences of staying above one of these geopathically stressed locations can be replicatedA  in our own homes by the choice of mattresses we use.A  The bottom line is, if you suspect your sleeping site is being disturbed by an unusually high magnetic anomaly then buy a bed that has a wooden base and place there upon a mattress that has no springs and make sure it is not placed near a radiator or other heavy metal object. In the 1930a€™s a French engineer Pierie Cody who lived in the sea-port of Le HavreA knew of local a€?cancer housesa€™ in the port where many people had died from cancer over the years. This equipment known as the Genitron Felix - 3 detects ultra short and radio microwave frequencies with the ability to print them out on a [UKW- Spektrometer und Linienschreiber] This equipment is used in German universities and research institutes that confirms dowsable energy above subterranean water lines. Effects central nervous system and the brain in the ways which effect powerful hormonal mechanisms. After checking large numbers of these dwellings, Cody concluded that the air in these a€?Cancer Housesa€™ were ionized to an unusual degree. Important areas to be aware of are bedrooms, especially where pillows are on beds, because EMFa€™s affect an area of the brain, called the pineal gland, which works to protect the body against illness overnight.
From various other tests Cody concluded that the ionization radiation consisted of positively charged Alpha Particles. It is also a good idea to look at places like a favourite armchair, or in front of a computer or TV.
The only known source of alpha particle emission in dwellings was from a radioactive gas called Radon.
It is important that places like these where you are sitting or lying still for a longish period of time should have low EMFa€™s; cells tend to cope better with external fields if the person is moving around.
Without first reading the introductory overview, it's difficult to understand the later informaiton that is being presented here. When you are sitting still and particular cells keep being interfered with by EMFa€™s, there is an increased risk that the damage may become unrepairable.
They are shocked to realize that what they had been reading about (and studying photographs of) is also taking place right over their heads. It is worthwhile taking particular precautionary action with regard to childrena€™s living environments. What some people had dismissed as mere "jet plane exhaust" (because there are now scores of internet propaganda web sites trying to convince you that 'everything is well' and 'there's nothing to be alarmed about' and that unaccountable 'jet plane exhaust'A  plumes are magically being converted into horizon-to-horizon overcasts of "cirrus clouds"A !) are dismayed to realize that chemtrails are indeed the toxin-laden aerosols that have been described here and at other web sites since 1998 and they are not being sprayed for any benign or national security reason as the disinformation peddlers would have you believe. I had taken my 35 mm camera with me to the monthly meeting of the Orange County Chapter of the American Society of Dowsers and after the meeting, I had stopped off at a supermarket. After getting out of the car, I photographed for the very first time, the strange looking "contrails" that William Thomas had been describing on the Art Bell radio program a couple of weeks earlier.
Thomas had dubbed them "chemtrails" on the Bell show to distinguish them from genuine (and rarely seen) short-lived ice crystal trailings properly identified as contrails. Although I had a number of articles about the NWO and their dark Machiavellian agendas posted at my web site, I was now witnessing (and breathing in) the stark reality of those depopulation plans. A  Chemtrail spraying seems to be heaviest and most constant over North America and most countries ofA  western Europe.
Some countries in Asia are being sprayed (Japan and Korea), but the greatest exception to any chemtrail activity whatsover is China. The Chinese are being spared completely because China is being groomed by the NWO to replace the United States as the leading nation of the world, both economically and militarily. If you want to hasten the demise of the chemtrail spraying program, please take the time to read about orgone generators, chembusters, and the use of your mind-with focused intent- to rid the sky of these poisons. People are now reporting the ability to clear the skies of chemtrails by use of the mind alone to obtain assistance from unseen helpers (Sylphs and others) and do the job for you based on your focused intention. I first posted an article in 2002 by Rich Work about using the mind and the the power of prayer to disperse chemtrails, and now we see this ability coming into reality with many people. Read these articles to understand what Sylphs are, what orgone generators are, and the difference between a DOR atmosphere and an OR atmosphere. We are talking about nothing less than the demise of the chemtrail spraying operations!
Chemtrails cannot exist in the presence of these giant air elementals and are they being destroyed as rapidly as they are being sprayed out of spew planes. All of the information posted below is interesting and informative, but it is now HISTORY.
We are winning the battle against chemtrails and defeating the satanic traitors at their own game.
Spread the word: DEPLOY ORGONE GENERATORS IN YOUR NEIGHBORHOOD and you too will be free of chemtrail laden skies!
I have seen the evidence here in southern California and have read of similar reports from different regions of America.
Read the articles below for an historical overview of chemtrails and the reasons for their deployment, but don't dwell on the negative aspects of this story because things are beginning to look up and we have good reason for optimism! Get involved with making or obtaining orgone generators in your immediate environment and be part of the 'hit team' bringing down this Luciferian inspired genocide operation. The fourth article describes a metaphysical method to destroy chemtrails that could work better than the physical method if employed by enough people and practiced correctly.
Len Horowitz's latest book (Death in the Air) on the chemtrail spraying program describing its sinister goals, It's a valuable resource to have in your library.
Deploying orgone generators in your immediate environment is an easy, safe, and highly effective way to mitigate chemtrails in your area. However, note that the person who is posting this information does not recognize that many of the photos show Sylphs neutralizing chemtrails, rather than government technology directed at harming the public. With the exception of the EDB petroleum aerosol rings seen around the sun, the majority of photos which reveal a "rainbow" effect are in fact demonstrating the presence of Sylphs who are transmuting the chemtrails into less harmful substances. Other Sylph photos show a large heart-shaped "hole" in the cloud cover which the web master assumes is government technology, but it is not negative technology. Joe Burton has been aggressively investigating and reporting on this story from early on.
Apparently he had been too aggressive, because his house had been targeted for direct spraying by low flying, unmarked aircraft.A  In a story postedA  Feb. 15, 1999, Joe reports the physical symptoms that his family and his pet have been experiencing from the sprayings. Joe believes that many of these military tankers responsible for the sprayings are remote controlled aircraft, but Al Cuppet (6 years with the US Joint Chiefs of Staff) has told radio talk show hostA  Jeff Rense during interviews on June 1, 1999, May 16, 1999, and May 7, 1999 felt that many of these tanker planes were more likely being flown by foreign pilots, possibly Chinese or Russian.
His reports are titled Contrail Spraying of Cities is RealA  Part 1 , Part II, and Part IIIA  These articles chronicle Ken's apprehension and dismay at the discovery that the United States government was brazenly spraying the skies of southern Texas on April 9, 1999 with Chemtrails. In June, a report from Florida said that sprayings had been going on for weeks over the Ft Lauderdale andA  Jacksonville areas, including military bases. Some people have gotten very ill and the symptoms seem to keep returning after a short period of improvement.
It's possible that some of these sprayings might contain special bioengineered pathogens designed to affect only certain racial groups. In other words, a secondA  substance might be required (aerial spraying or substances added to the water supplyA  for example) to bring out the virulent phase of the pathogen, but of course this is only speculation.
Rick Malinowski's long and detailed article also suggest the notion of a 2 or 3 part piggy back element to the chemtrail sprayings. He has been interviewed many times on the Art Bell Radio show to discuss the chemtrails story and has many excellent articles and Photos posted at his own web site as well as other locations including-Jeff Rense's Sightings on the Radio .
Thomas has concluded that these sprayings are genocidal in nature and are intended to reduce or weaken the general population. In a November '99 interview with Art Bell, Thomas also voiced the idea that there might be a mind control element to the most recent spraying, since many people are reporting mental confusion and depression following recent sprayings. Thomas has reminded radio listeners that the government has had a long history of exposing the public to biological pathogens without their knowledge or consent.
Most people would like to believe that, but the evidence is too strong in the opposite direction.




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