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    Giant Invisible Space Ribbon
    By Alex "Sandy" Antunes | January 15th 2010 12:49 PM | 10 comments | Print | E-mail | Track Comments
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    Where are we?  Cosmically, I mean.  We have barely made steps to get to the edge of our solar system, via Voyager 1 and 2.  It's ironic that we can see back 13 billion years using telescopes, but we have little idea of what 'stuff' is out there-- matter, dark matter, energy.  Or even what is just outside our local solar system.

    The Voyager probes sensed strong magnetic fields near the edge of our solar system, and earlier Interstellar Boundary Explorer (IBEX) results supported that.  IBEX is in a high-altitude highly elliptical Earth orbit that helps it get above the Earth's magnetic field.  Now, the picture is clear.  There's a giant invisible space ribbon, made of energetic hydrogen atoms pumped up in energy by a galactic magnetic field.

    giant space ribbon

    Space is, paradoxically, both extremely empty and very full.  In interstellar space (the space between stars, aka the galaxy medium), our sun's solar wind and extended magnetic field interacts with traveling cosmic rays and random interstellar clouds of mostly cold hydrogen gas.  The ambient galactic magnetic field in our area is weak-- perhaps 5 milliGauss, or a fractional five one-thousands of a Gauss, versus the 50 Gauss of a refrigerator magnet or the half Gauss field of the Earth -- but potentially pervasive.  A little field over a big area can have a strong effect.

    So we have outward streaming particles from our sun, hitting a galactic magnetic field.  What we get is the ribbon.  The first reports of the invisible space ribbon were covered in Science by Richard Kerr, under the title "Tying Up the Solar System with a Ribbon of Charged Particles."
    IBEX "revealed a sky-spanning "ribbon" of unexpectedly intense emissions of energetic neutral atoms (ENAs). No one knows what is creating the ENA ribbon, but everyone agrees that it means the textbook picture of the heliosphere—in which the solar system's enveloping pocket filled with the solar wind's charged particles is plowing through the onrushing "galactic wind" of the interstellar medium in the shape of a comet—is wrong."

    Now further IBEX work reveals a possible cause for the ribbon. From this week's NASA press release, "We  believe the ribbon is a reflection," says Jacob Heerikhuisen,.. "It is where solar wind particles  heading out into interstellar space are reflected back into  the solar system by a galactic magnetic field."

    Since no good astronomy article neglects catastrophe, here's NASA's spiffy line, well worth me stealing here.  "And  upon this field, the future may hinge.".

    Our solar system is in a bubble, the heliosphere.  The ribbon (and the Voyager probes) are near its edge, and outside are the aforementioned high energy cosmic rays zinging around, and the occasional interstellar cloud of 'stuff'.  The heliosphere keeps most of that outside of our solar system, and we end up with a stable environment consisting of mostly just what the sun puts out.  Baring a local supernova, we're safe.  But a "strong magnetic field just outside the  solar system could press against the heliosphere and interact  with it in unknown ways. Will this strengthen our natural  shielding—or weaken it?"

    model vs reality

    And just to be clear, we mean IBEX the satellite, not Ibex the mountain goat.
     IbexIBEX

    Alex, the Daytime Astronomer

    Tues and Fri here, via RSS feed, and twitter @skyday
    Read about my own private space venture in The Satellite Diaries

    Comments

    An interesting revelation from the good people at NASA. This is the first I've heard of the ENA ribbon. Thanks for writing about it and for the links. : )

    Clear skies,
    Eric
    Hfarmer
    Very interesting article.  I especially liked how you described the effects of the solar magnetic field in keeping out interstellar radiations.   As for our field interacting with another, to borrow a line from StarTrek I don't know of our shields will hold captain.
    Science advances as much by mistakes as by plans.
    This solar wind inflates a giant bubble in interstellar space called the heliosphere — the region of space dominated by the Sun's influence in which the Earth and other planets reside.The nanotube sheets combine high transparency with high electronic conductivity, are highly flexible and provide giant gravimetric surface areas, which has enabled the team to demonstrate their use as electrodes for bright organic light emitting diodes for displays and as .... One of the things that concerns me is huge almost invisible ribbons or sails of this stuff floating around in our oceans or in our atmosphere trapping and killing fish, whales, birds

    MarshallBarnes
    Inadvertently, you've just given the intelligent design crowd another piece of ammunition. And so it goes...
    Solar magnetic field by its cross middle frequency cross polarized oscillation initiate Rogue waves in sea during June-July along surface plasmons polaritons.
    Abstract: We propose and experimentally demonstrate the generation of cross-polarized photon pairs via four-wave mixing with cross-polarized frequency-conjugate laser equivalent pulse of solar magnetic field pulses of frequency-conjugate laser dynamics at 45 degree grace angle This method can be used for astrogenetic applications and various quantum information applications such as the preparation of Bell states of Toa cross polarization integrated over stoke and antistoke split stages that lead the stoke by cos 45 degrees.
    Solar magnetic field ejecting surface plasmons that oscillate along middle frequency resonance oscillation seems to be an important investigation on super string wave theory of helium fluid calls of optic lattices of Equi potential for wz of rotating dynamics of ds squeezed for cross polariton resonance of Bosenova oscillation from air affine to water affined affine the sea water.
    It has been demonstrated that by injecting a laser beam into a single mode optical lattice (SMF) or a MF, correlated Stokes (ωs) and anti-Stokes (ωas) photon pairs at conjugate frequencies are generated via degenerate four-wave mixing process (FWM) at the phase matching condition, ωs+ωas=2ω0 [16-19]. In a reverse process, it was also shown that by recombining these pairs of parallel-polarized conjugate photons in a second layer, photon pairscan be generated at the middle frequency with good efficiency, ω0=ωs+ωas [20].It is known that in an ideal single mode fiber (SMF), a mode excited with its polarization. This effect has been used to generate polarization-entangled photon pairs by synchronizing two orthogonal but degenerate FWM processes in a dispersion-shifted fiber(DSF) [22, 23]. Two same wavelength laser pulses with polarizations perpendicular to eachother coupled into a DSF, each create a correlated photon pair in the polarization state ofHsHi> or |VsVi>. |H> and |V> are two orthogonally polarized photon states and “s” and “i”stand for signal (anti-Stokes) and idler (Stokes) photons at different wavelengths. |HsHi> and
    |VsVi> are interferometrically combined.
    We overlap a Stokes (Es(t,z)) laser pulse polarized along principal axis x with an anti-Stokes (Eas(t,z)) laser pulse polarized along principal axis y in a MF, in thephoton pairs by FWM at the iddle frequency generating correlated state of |x> |y> when phase matching condition is satisfied.(1) At delay t1, overlap only occurs between Easx and Esy. In this case we launch the anti-Stokes pulse ahead of the Stokes pulse into MF2. Cross-polarized photon pairs in the state|x>|y> are generated by FWM at the middle frequency. This is similar to a collineardegenerate type-II PDC process [24].(2) At delay t3, overlap only occurs between Easy and Esx, generating cross-polarizedphoton pairs in the state |x>|y> at the middle frequency through FWM. In this case, we launchthe Stokes pulse ahead of the anti-Stokes pulse into MF2.With polarization oriented at 45o with respect to axes x and y, the Stokes (anti-Stokes)pulse is split into two pulses with equal power in MF2 polarized along axes x and y,respectively, resulting in a four-pulse co-propagation configuration in MF2. The electric fieldof the four-pulse is,
    Es(t,z)=Esx(t,z)x+Esy(t,z)y, (1a)
    Eas(t,z)=Easx(t,z)x+Easy(t,z)
    Rotational vector frequency of cross polariton resonance amplifying the sea during June-july by space polaritons of 69 dynamics of solar magnetic field at cancer-reg [Incident: 100729-000144 news@nature.com
    Some interesting simulation on fliud mechanics that could be derived using the velocity potential of -1 as as dy/dx -1at Wz =1/2(dv/dx-du/dy) that simulate violent surface palsmons by incearsed rotational frequencies due to circularly polarised polariton collection on water surface from linearity to partitionned polarity and collapsible resonance amplify the force by the cross polarisaing stoke and antistoke forces. They’re the stuff of sea captains' nightmares—giant waves barreling in seemingly from out of nowhere to capsize or swamp even the largest vessels or offshore drilling platforms. What creates these elusive monsters? In a new paper to be published in Physical Review Letters, researchers use a computer model to simulate a rogue wave's birth and propagation. Two or more small waves, driven forward by strong currents, and at the same time resisted by powerful headwinds, suddenly combine and amplify their height into a single, giant wave. Once formed, the wave structure stabilizes itself and concentrates its energy in one direction. That enables it to travel many kilometers before breaking up, typically when either the driving currents or headwinds subside. Along the way, anyone unfortunate enough to be sitting in the wave's path is bound to remember the experience. The same experience occurred to Lord Kitchner nval commander of England who had Einstein’s spooky hologram plane in his palm print of cross polarization graphics at the end of travel line confirmed the astro genetic theory along the plane of cross polarized surface polaritons of solar magnetic field acted as a timer in his case.. Sankara Velayudhan Nandakumar along with Hon. Sir J.Pendry F.R.S of imperial college uk special officer on combustion nano technology along with Dr.GANESAN ,IIT professor ,combustion dept Cape Institute of Technology,Nagercoil formerly with ,KNSK Engineering college ,Nagercoil as research scholar,Anna University with Hubble space research committee of Hon.Roger Davies,Hon.Collin Webbs FRS of Laser dn of Oxford uk,Hon.Marteen Rees ,Emeritus Professor of cosmology Cambridge ,former president of Royal society London

    Main reference: Generation of cross-polarized photon pairs in a microstructure fiber with frequency-conjugatemicrostructure fiber with frequency-conjugate laser pump pulsesJ. Fan and A.MigdallOptical Technology DivisionNational Institute of Standards and Technology
    100 Bureau Drive, Mail Stop 8441, Gaithersburg. MD 20899-8441Jfan@nist.gov
    References and links
    1. C. Kurtsiefer, P. Aarda, M. Halder, H. Weinfurter, P. M. Gorman, P. R. Tapster, “Quantum cryptography:
    A step towards global key distribution,” Nature 419, 450 (2002).
    2. M. Aspelmeyer, H. R. Böhm, T. Gyatso, T. Jennewein, R. Kaltenbaek, M. Lindenthal, G. Molina Terriza,
    A. Poppe, K. Resch, M. Taraba, R. Ursin, P. Walther, and A. Zeilinger, “Long-distance free-Space
    distribution of quantum entanglement,” Science 301, 621 (2003).
    3. I. Marcikic, H. de Riedmatten,W. Tittel, H. Zbinden, M. Legre, and N. Gisin, “Distribution of time-bin
    entangled qubits over 50 km of optical fiber,” Phys. Rev. Lett. 93, 180502 (2004).
    4. D. C. Burnham, D. L. Weinberg, “Observation of simultaneity in parametric production of optical photon
    pairs,” Phys. Rev. Lett. 25, 84 (1970).
    5. S. Friberg, C. K. Hong, and L. Mandel, “Measurement of time delays in the parametric production of
    photon pairs,” Phys. Rev. Lett. 54, 2011 (1985).
    6. S. Friberg and L. Mandel, “Production of squeezed states by combination of parametric down-conversion
    and harmonic generation,” Opt. Commun. 48, 439 (1984).
    7. P. G. Kwiat, E. Waks, A. G. White, I. Appelbaum, and P. H. Eberhard, “Ultrabright source of polarizationentangled
    photons,” Phys. Rev. A60, R773 (1999).
    8. C. Kurtsiefer, M. Oberparleiter, and H. Weinfurter, “High-efficiency entangled photon pair collection in
    type-II parametric fluorescence,” Phys. Rev. A 64, 023802 (2001)
    9. E. Brannen, F. R. Hunt, R. H. Adlington, R. W., Hicholls, “Application of nuclear coincidence methods to
    atomic transitions in the wavelength range 2000-6000A,” Nature 175, 810 (1955).
    10. A. Kuzmich, W. P. Bowen, A. D. Boozer, A. Boca, C. W. Chou, L.-M. Duan, and H.J. Kimble,
    “Generation of nonclassical photon pairs for scalable quantum communication with atomic ensembles,”
    Nature 423, 731 (2003).
    11. C. Santori, D. Fattal, J. Vu, G. S. Solomon, Y. Yamamoto, “Indistinguishable photons from a single-photon
    device,” Nature 419, 594 (2002).
    12. S. Tanzilli, F. D. Riedmatten, W. Tittle, H. Zbinden, P. Baldi, M. D., Micheli, D. B. Ostrowsky, N. Gisin,
    “Highly efficient photon-pair source using periodically poled lithium niobate waveguide,” Electron. Lett.
    37, 26 (2001).
    13. S. J. Mason, M. A. Albota, F. Konig, and F. N. C. Wong, “Efficient generation of tunable photon pairs at
    m,” Opt. Lett.0.8 and 1.6 27, 2115 (2002).
    14. F. Konig, E. J. Mason, F. N. C. Wong, and M. A. Albota, “Efficient spectrally bright source of polarizationentangled
    photons,” Phys. Rev. A 71, 033805 (2005).
    15. T. A. Birks, J. C. Knight, and P. St. J. Russell, “Endlessly single-mode photonic crystal fibers,” Opt. Lett.
    22, 961 (1997).
    16. M. Fiorentino, P. L. Voss, J. E. Sharping, and P. Kumar, “All-fiber photon-pair source for quantum
    communication,” IEEE Photonics Tech. Lett. 14, 983 (2002).
    17) Your call CNSHD789849 regarding With polarization oriented at 45 degrees with respect to axes x and y, the Stokes (anti-Stokes) may shifted for anti laser-reg has been received Outreach@stsci.edu
    18) #TAG# With polarization oriented at 45 degrees with respect to axes x and y, the Stokes (anti-Stokes) may shifted for anti laser-reg [Incident: 100802-000314 news@nature.com"

    A Cross polarized oscillation in solar magnetic field calls for genetic catastrophe of air-water affined genes on the palm print of W.T.Stead as well as on Lord Kitchner-reg
    Very very important finding at last solving the enigmatic crossgraphics of palm print of W.T.Stead
    This matter is very very important as this will reveal an intersting cross polarised rsonance observed as a cross at the end of travel line as per the palm prinyt of W.T.Stead who was drowned into sea in Titanic who was born between JUn-July confirming a cross polarised oscillation of genes recorded as a cross along the plane of holgram ,the palm print.This could demonstarate a typical cross polarised oscillation of solar magnetic field along the air -water affined bosenova resonances
    With polarization oriented at 45o with respect to axes x and y, the Stokes (anti-Stokes) pulse is split into two pulses with equal power in MF2 polarized along axes x and y,respectively, resulting in a four-pulse co-propagation configuration in MF2. The electric fieldof the four-pulse is,Es(t,z)=Esx(t,z)x+Esy(t,z)y, (1a)
    Eas(t,z)=Easx(t,z)x+Easy(t,z)y . (1b)For this short fiber, group velocity dispersion (GVD) is negligible [17]. Pulses polarizedalong axis x walk off from pulses polarized along axis y in MF2 due to PMD. By adjusting therelative delay of the anti-Stokes pulse with respect to the Stokes pulse in MF2, we canarrange to overlap either Esx(t,z)x with Easy(t,z)y or Esy(t,z)x with Easx(t,z)y. These delay configurations acted as genetic timer in case of W.T.Stead ,journalist of Review of Reviewers..
    At delay t1, overlap only occurs between Easx and Esy. In this case we launch the anti-Stokes pulse ahead of the Stokes pulse into MF2. Cross-polarized photon pairs in the state|x>|y> are generated by FWM at the middle frequency. This is similar to a collinear degenerate type-II PDC process
    (2) At delay t3, overlap only occurs between Easy and Esx, generating cross-polarized photon pairs in the state |x>|y> at the middle frequency through FWM. In this case, we launch the Stokes pulse ahead of the anti-Stokes pulse into MF2.(3) At a delay t2 between t1 and t3, both Stokes and anti-Stokes pulses enter MF2 at the same time. Before the PMD walk-off, FWM can occur in both parallel- and cross-polarization schemes. For FWM with parallel-polarized pump pulses, Easx overlaps with Esx to generate photon pairs in the polarization state |x>|x> along axis x, Easy overlaps with Esy to generate photon pairs in the polarization state |y>|y> along axis y. These two processes are coherent forming a superposed state.
    This only has occured in solar magnetic field resonance that initiated a holographic cross at the end of travel line from T cell ejections of W.T.Stead as well as that of Lord Kitchner former naval commander of England.
    Sankara Velayudhan Nandakumar along with Hon. Sir J.Pendry F.R.S of imperial college uk special officer on combustion nano technology along with Dr.GANESAN ,IIT professor ,combustion dept Cape Institute of Technology,Nagercoil formerly with ,KNSK Engineering college ,Nagercoil as research scholar,Anna University with Hubble space research committee of Hon.Roger Davies,Hon.Collin Webbs FRS of Laser dn of Oxford uk,Hon.Marteen Rees ,Emeritus Professor of cosmology Cambridge ,former president of Royal society London.
    Sankara Velayudhan Nandakumar member PNAS ,American ,JILA Group member on behalf of Loyola college of Engineering and technology ,Member American committee for the Weizman institute of science ,Energy renovation committee cape Institute of Technology,Nagercoil ,former Guest lecturer ,KNSK Enginering college ,Anna University have surprisingly found out genetic mirror
    1. C. Kurtsiefer, P. Aarda, M. Halder, H. Weinfurter, P. M. Gorman, P. R. Tapster, “Quantum cryptography:
    A step towards global key distribution,” Nature 419, 450 (2002).
    2. M. Aspelmeyer, H. R. Böhm, T. Gyatso, T. Jennewein, R. Kaltenbaek, M. Lindenthal, G. Molina Terriza,
    A. Poppe, K. Resch, M. Taraba, R. Ursin, P. Walther, and A. Zeilinger, “Long-distance free-Space
    distribution of quantum entanglement,” Science 301, 621 (2003).
    3. I. Marcikic, H. de Riedmatten,W. Tittel, H. Zbinden, M. Legre, and N. Gisin, “Distribution of time-bin
    entangled qubits over 50 km of optical fiber,” Phys. Rev. Lett. 93, 180502 (2004).
    4. D. C. Burnham, D. L. Weinberg, “Observation of simultaneity in parametric production of optical photon
    pairs,” Phys. Rev. Lett. 25, 84 (1970).
    5. S. Friberg, C. K. Hong, and L. Mandel, “Measurement of time delays in the parametric production of
    photon pairs,” Phys. Rev. Lett. 54, 2011 (1985).
    6. S. Friberg and L. Mandel, “Production of squeezed states by combination of parametric down-conversion
    and harmonic generation,” Opt. Commun. 48, 439 (1984).
    7. P. G. Kwiat, E. Waks, A. G. White, I. Appelbaum, and P. H. Eberhard, “Ultrabright source of polarizationentangled
    photons,” Phys. Rev. A60, R773 (1999).
    8. C. Kurtsiefer, M. Oberparleiter, and H. Weinfurter, “High-efficiency entangled photon pair collection in
    type-II parametric fluorescence,” Phys. Rev. A 64, 023802 (2001)
    9. E. Brannen, F. R. Hunt, R. H. Adlington, R. W., Hicholls, “Application of nuclear coincidence methods to
    atomic transitions in the wavelength range 2000-6000A,” Nature 175, 810 (1955).
    10. A. Kuzmich, W. P. Bowen, A. D. Boozer, A. Boca, C. W. Chou, L.-M. Duan, and H.J. Kimble,
    “Generation of nonclassical photon pairs for scalable quantum communication with atomic ensembles,”
    Nature 423, 731 (2003).
    11. C. Santori, D. Fattal, J. Vu, G. S. Solomon, Y. Yamamoto, “Indistinguishable photons from a single-photon
    device,” Nature 419, 594 (2002).
    12. S. Tanzilli, F. D. Riedmatten, W. Tittle, H. Zbinden, P. Baldi, M. D., Micheli, D. B. Ostrowsky, N. Gisin,
    “Highly efficient photon-pair source using periodically poled lithium niobate waveguide,” Electron. Lett.
    37, 26 (2001).
    13. S. J. Mason, M. A. Albota, F. Konig, and F. N. C. Wong, “Efficient generation of tunable photon pairs at
    0.8 and 1.6 m,” Opt. Lett. 27, 2115 (2002).
    14. F. Konig, E. J. Mason, F. N. C. Wong, and M. A. Albota, “Efficient spectrally bright source of polarizationentangled
    photons,” Phys. Rev. A 71, 033805 (2005).
    15. T. A. Birks, J. C. Knight, and P. St. J. Russell, “Endlessly single-mode photonic crystal fibers,” Opt. Lett.
    22, 961 (1997).
    16. M. Fiorentino, P. L. Voss, J. E. Sharping, and P. Kumar, “All-fiber photon-pair source for quantum
    communication,” IEEE Photonics Tech. Lett. 14, 983 (2002).
    #7815 - $15.00 US Received 14 June 2005; revised 15 July 2005
    Ref:Generation of cross-polarized photon pairs in a
    microstructure fiber with frequency-conjugate
    laser pump pulses
    J. Fan and A. Migdall
    Optical Technology Division
    National Institute of Standards and Technology
    100 Bureau Drive, Mail Stop 8441, Gaithersburg. MD 20899-8441
    Jfan@nist.gov

    TAG# A Cross polarized oscillation in solar magnetic field calls for genetic catastrophe of air-water affined genes on the palm print of W.T.Stead-reg [Incident: 100802-000279 news@nature.com"
    Your call CNSHD789847 regarding Cross polarised genetic air-water affined catastrophe solved at last -reg has been received Outreach@stsci.edu"

    Quantum teleportation though neutron beam may be possible in future
    The magnetic field is used to tune the chains of spins to a quantum critical state. The resonant modes (“notes”) are detected by scattering neutrons. These scatter with the characteristic frequencies of the spin chains. (Credit: Image courtesy of Helmholtz Association of German Research Centres
    On the atomic scale particles do not behave as we know it in the macro-atomic world. New properties emerge which are the result of an effect known as the Heisenberg's Uncertainty Principle. In order to study these nanoscale quantum effects the researchers have focused on the magnetic material cobalt niobate. It consists of linked magnetic atoms, which form chains just like a very thin bar magnet, but only one atom wide and are a useful model for describing ferromagnetism on the nanoscale in solid state matter.
    When applying a magnetic field at right angles to an aligned spin the magnetic chain will transform into a new state called quantum critical, which can be thought of as a quantum version of a fractal pattern. Prof. Alan Tennant, the leader of the Berlin group, explains "The system reaches a quantum uncertain -- or a Schrödinger cat state. This is what we did in our experiments with cobalt niobate. We have tuned the system exactly in order to turn it quantum critical. By tuning the system and artificially introducing more quantum uncertainty the researchers observed that the chain of atoms acts like a nanoscale guitar string.
    Dr. Radu Coldea from Oxford University, who is the principal author of the paper and drove the international project from its inception a decade ago until the present, explains: "Here the tension comes from the interaction between spins causing them to magnetically resonate. For these interactions we found a series (scale) of resonant notes: The first two notes show a perfect relationship with each other. Their frequencies (pitch) are in the ratio of 1.618…, which is the golden ratio famous from art and architecture." Radu Coldea is convinced that this is no coincidence. "It reflects a beautiful property of the quantum system -- a hidden symmetry. Actually quite a special one called E8 by mathematicians, and this is its first observation in a material," he explains. The observed resonant states in cobalt niobate are a dramatic laboratory illustration of the way in which mathematical theories developed for particle physics may find application in nanoscale science and ultimately in future technology.
    Prof. Tennant remarks on the perfect harmony found in quantum uncertainty instead of disorder. "Such discoveries are leading physicists to speculate that the quantum, atomic scale world may have its own underlying order. Similar surprises may await researchers in other materials in the quantum critical state."
    The researchers achieved these results by using a special probe -- neutron scattering. It allows physicists to see the actual atomic scale vibrations of a system. Dr. Elisa Wheeler, who has worked at both Oxford University and Berlin on the project, explains "using neutron scattering gives us unrivalled insight into how different the quantum world can be from the every day
    However, "the conflicting difficulties of a highly complex neutron experiment integrated with low temperature equipment and precision high field apparatus make this a very challenging undertaking indeed." In order to achieve success "in such challenging experiments under extreme conditions" the HZB in Berlin has brought together world leaders in this field. By combining the special expertise in Berlin whilst taking advantage of the pulsed neutrons at ISIS, near Oxford, permitted a perfect combination of measurements to be made.
    'You might expect to see random fluctuations of the spins at this critical point but what we uncovered was a remarkable structure in the resonances of the magnetic spins indicating a perfectly harmonious state,' said Radu Coldea from Oxford University's Department of Physics wholed the team.
    Some information requiring 45 degree tangential cross polarization on middle frequency resonance and oscillation on symmetry breaking dynamics to be evolved says Sankaravelayudhan Nandakumar on behalf of Oxford astro genetic team headed by Hon.Roger Davies and his colleagues.

    Contrary to Cooper theory of paired electrons this commonly held theory, Lebed said, "We show that superconducting electron pairs are not unchanged elementary particles but rather complex objects with characteristics that depend on the strength of a magnetic field." When the spins of the two electrons are in opposite directions, one spinning up and the other spinning down, they are called singlets, or non-rotating Cooper pairs. When the spins are in same direction, they are called triplets, or rotating Cooper pairs.
    Super-strong magnetic fields create exotic Cooper pairs that behave according to the weird, non-intuitive laws of quantum mechanics: the electron pairs are both rotating and non-rotating at the same time. They behave kind of like microscopic "quantum mechanical hurricanes, applied along corcinova rotation at middle frequency cross polarized criticality says Sankara velayudhan Nandakumar as observed by the Astro genetic team. Cross Polarizations of these two pulses are parallel to each other and oriented at 45 degree with respect to axes x and y.With polarization oriented at 450 with respect to axes x and y, the Stokes (anti-Stokes).
    In this case we launch the anti-Stokes pulse ahead of the Stokes pulse into MF2. Cross-polarized photon pairs in the state|x>|y> are generated by FWM at the middle frequency. This is similar to a collinear degenerate type-II PDC process [24].(2) At delay t3, overlap only occurs between Easy and Esx, generating cross-polarized pulse is split into two pulses with equal power.
    correlated Stokes (ωs) and anti-Stokes (ωas) photon pairs at conjugate frequencies are generated via degenerate four-wave mixing process (FWM) at the phase matching condition, ωs+ωas=2ω0 [16-19]. In a reverse process, it was also shown that by recombining these pairs of parallel-polarized conjugate photons in a second fiber, photon pairs can be generated at the middle frequency with good efficiency, 2ω0=ωs+ωas.Cross polarized photon plasmons are of great importance in astro genetic field. They demonstrate the generation of cross-polarized photon pairs via four-wave mixing with cross-polarized frequency-conjugate.

    Another unexpected and unique magnetic field-dependent property is mirror reflection.
    Because Cooper pairs are quantum objects, they behave both as particles and as standing waves. One standing wave property is mirror reflection, or "parity." Physicists earlier found that wave symmetry in conventional, or singlet, superconductors is even. It is mathematically termed as +1. They also discovered that unconventional, or triplet, superconductor parity is odd, or - 1.
    When singlets or triplets are reflected in a mirror, the reflected waves always have the same (+1) or opposite (-1) parity of the original waves. as observed in NRI materials of Hon.Sir Pendry FRS.
    "Because these Cooper pair electrons behave so differently than conventional singlet and unconventional triplet Cooper pairs, we call them 'exotic' Cooper pairs at cos 45 ,sin 45 degree cross polarized oscillation which may act along breaking symmetry dynamics of Eric Bosoneva.calls for Nambu’s symmetry breaking.(Kindly refer symmetry breaking surface solar magnetic plasmons at Capricorn as the sun moves through) Time reversal symmetry is the idea that most fundamental physical laws would not change if time ran backwards instead of forward
    Sankara Velayudhan Nandakumar along with Hon. Sir J.Pendry F.R.S of imperial college uk special officer on combustion nano technology along with Dr.GANESAN ,IIT professor ,combustion dept Cape Institute of Technology,Nagercoil formerly with ,KNSK Engineering college ,Nagercoil as research scholar,Anna University with Hubble space research committee of Hon.Roger Davies,Hon.Collin Webbs FRS of Laser dn of Oxford uk,Hon.Marteen Rees ,Emeritus Professor of cosmology Cambridge ,former president of Royal society, London.
    Sankara Velayudhan Nandakumar member PNAS ,American ,JILA,NIST ,Hubble Group member on behalf of Loyola college of Engineering and technology ,Member American committee for the Weizman institute of science ,Energy renovation committee cape Institute of Technology,Nagercoil ,former Guest lecturer ,KNSK Enginering college ,Anna University have surprisingly found out genetic mirror
    1. C. Kurtsiefer, P. Aarda, M. Halder, H. Weinfurter, P. M. Gorman, P. R. Tapster, “Quantum cryptography:
    A step towards global key distribution,” Nature 419, 450 (2002).
    2. M. Aspelmeyer, H. R. Böhm, T. Gyatso, T. Jennewein, R. Kaltenbaek, M. Lindenthal, G. Molina Terriza,
    A. Poppe, K. Resch, M. Taraba, R. Ursin, P. Walther, and A. Zeilinger, “Long-distance free-Space
    distribution of quantum entanglement,” Science 301, 621 (2003).
    3. I. Marcikic, H. de Riedmatten,W. Tittel, H. Zbinden, M. Legre, and N. Gisin, “Distribution of time-bin
    entangled qubits over 50 km of optical fiber,” Phys. Rev. Lett. 93, 180502 (2004).
    4. D. C. Burnham, D. L. Weinberg, “Observation of simultaneity in parametric production of optical photon
    pairs,” Phys. Rev. Lett. 25, 84 (1970).
    5. S. Friberg, C. K. Hong, and L. Mandel, “Measurement of time delays in the parametric production of
    photon pairs,” Phys. Rev. Lett. 54, 2011 (1985).
    6. S. Friberg and L. Mandel, “Production of squeezed states by combination of parametric down-conversion
    and harmonic generation,” Opt. Commun. 48, 439 (1984).
    7. P. G. Kwiat, E. Waks, A. G. White, I. Appelbaum, and P. H. Eberhard, “Ultrabright source of polarizationentangled
    photons,” Phys. Rev. A60, R773 (1999).
    8. C. Kurtsiefer, M. Oberparleiter, and H. Weinfurter, “High-efficiency entangled photon pair collection in
    type-II parametric fluorescence,” Phys. Rev. A 64, 023802 (2001)
    9. E. Brannen, F. R. Hunt, R. H. Adlington, R. W., Hicholls, “Application of nuclear coincidence methods to
    atomic transitions in the wavelength range 2000-6000A,” Nature 175, 810 (1955).
    10. A. Kuzmich, W. P. Bowen, A. D. Boozer, A. Boca, C. W. Chou, L.-M. Duan, and H.J. Kimble,
    “Generation of nonclassical photon pairs for scalable quantum communication with atomic ensembles,”
    Nature 423, 731 (2003).
    11. C. Santori, D. Fattal, J. Vu, G. S. Solomon, Y. Yamamoto, “Indistinguishable photons from a single-photon
    device,” Nature 419, 594 (2002).
    12. S. Tanzilli, F. D. Riedmatten, W. Tittle, H. Zbinden, P. Baldi, M. D., Micheli, D. B. Ostrowsky, N. Gisin,
    “Highly efficient photon-pair source using periodically poled lithium niobate waveguide,” Electron. Lett.
    37, 26 (2001).
    13. S. J. Mason, M. A. Albota, F. Konig, and F. N. C. Wong, “Efficient generation of tunable photon pairs at
    m,” Opt. Lett.0.8 and 1.6 27, 2115 (2002).
    14. F. Konig, E. J. Mason, F. N. C. Wong, and M. A. Albota, “Efficient spectrally bright source of polarizationentangled
    photons,” Phys. Rev. A 71, 033805 (2005).
    15. T. A. Birks, J. C. Knight, and P. St. J. Russell, “Endlessly single-mode photonic crystal fibers,” Opt. Lett.
    22, 961 (1997).
    16. M. Fiorentino, P. L. Voss, J. E. Sharping, and P. Kumar, “All-fiber photon-pair source for quantum
    communication,” IEEE Photonics Tech. Lett. 14, 983 (2002).
    17) Your call CNSHD789849 regarding With polarization oriented at 45 degrees with respect to axes x and y, the Stokes (anti-Stokes) may shifted for anti laser-reg has been received Outreach@stsci.edu
    18) #TAG# With polarization oriented at 45 degrees with respect to axes x and y, the Stokes (anti-Stokes) may shifted for anti laser-reg [Incident: 100802-000314 news@nature.com"
    19)Quantumm teleportation by neutron beam may be posssible by breaking 45 degree cross polarised resonance-reg [Incident: 100805-000130
    20)Your call CNSHD790230 regarding Quantum teleportation by neutron beam may be posssible by breaking 45 degree cross polarised resonance-reg has been received) news@nature.com

    19 Your call CNSHD790230 regarding Quantum teleportation by neutron beam may be posssible by breaking 45 degree cross polarised resonance-reg has been received)

    Solar magnetic field emitting air-water during June-july affined polritons in space crossing our erath as Twisters for tappiing the energy:
    Solar rays could be converged to produce cross polarized Bossonova resonance between Air affined and water affined middle frequency resonance as Monster twisters in ferromagnetic cloud chambers for tapping energy –Electricity
    Solar rays could be converged to produce cross polarized Bossonova resonance between Air affined and water affined middle frequency resonance as Monster twisters in ferromagnetic cloud chambers for tapping energy –Electricity:
    “crossover physics”, which reflects the anomalously short coherence length. Both schools are currentlyvery interested in explaining the origin of the mysterious pseudogap phase. In this Review we have presenteda case for its origin in crossover physics. The pseudogap in the normal state can be associated withmeta-stable pairs of fermions; a (pseudogap) energy must be supplied to break these pairs apart into theirseparate components. The pseudogap also persists below Tc in the sense that there are noncondensed fermion pair excitations of the condensate. These concepts have a natural analogue in self consistent theories of superconducting fluctuations, but for the crossover problem the width of the “critical region” is extremely large. This reflects the much stronger-than-BCS attractive interaction. It was not our intent to shortchange the role of Mott physics which will obviously be of importance in our ultimate understanding of the superconducting cuprates. There is, however, much in this regard which is still uncertain associated with establishing the simultaneous relevance and existence of spin-charge
    separation (Anderson, 1997), stripes (Kivelson et al., 2003), and hidden order parameters (Chak
    et al., 2001). What we do have in hand, though, is a very clear experimental picture of an extremely unusual superconductor in which superconductivity seems to evolve gradually from above Tc to below.We have in this Review tried to emphasize the common ground between high Tc superconductors and ultracold superfluids.
    These Mott issues may nevertheless, set the agenda for future cold atom studies of
    fermions in optical lattices (Hofstetter et al., 2002).The recent discovery of superfluidity in cold fermion gases opens the door to a new set of fascinating problems in condensed matter physics. Unlike the bosonic system, there is no ready-made counterpart of Gross Pitaevskii theory. A new mean field theory which goes beyond BCS and encompasses BEC in some form or another will have to be developed in concert with experiment.
    An interesting Cross Polarized Bossoneva Twisters(CPBT) convergence in laser cooling dynamics that oscillate between air affined surface polaritons forming cross polarized as they oscillate along middle frequencies in fferro magnetic vaporized cloud chambers of MOT requires further research in NIST,and Jila ,MIT University.
    Astro physics related information in solar magnetic field shifting of half spins fermions to full spin Boson shift is possible of solar ray emissions .Infact quasinatured full spin boson converted as half spin fermions on Taurus mageneto optic quantum sector is observed.(refer graphical codes of half circle over full circle)
    The Boson natured Bossonnova retrograde resonance between Gemini and cancer call for similat crocc polarized Bossonova resonance at polariton cross overs requires an investigation.
    Conclusion: Ferromagnetic vaporized injection in solar rays could be utilized in laser colling bosennova resonance polariton cross over dynamics to produce Monster Twisers that could drive Turbine blades to produce electricity in generators or directly as jet propulsion systems.
    Sankara Velayudhan Nandakumar of Energy renovation coordinator along with Hon. Sir J.Pendry F.R.S of imperial college uk special officer on combustion nano technology along with Dr.GANESAN ,IIT professor ,combustion dept Cape Institute of Technology,Nagercoil formerly with ,KNSK Engineering college ,Nagercoil as research scholar,Anna University with Hubble space research committee of Hon.Roger Davies,Hon.Collin Webbs FRS of Laser dn of Oxford uk,Hon.Marteen Rees ,Emeritus Professor of cosmology Cambridge ,former president of Royal society London
    List of references:
    Bossonova resoannce reserch works carried out at NIST and JILA
    1. C. Kurtsiefer, P. Aarda, M. Halder, H. Weinfurter, P. M. Gorman, P. R. Tapster, “Quantum cryptography:
    A step towards global key distribution,” Nature 419, 450 (2002).
    2. M. Aspelmeyer, H. R. Böhm, T. Gyatso, T. Jennewein, R. Kaltenbaek, M. Lindenthal, G. Molina Terriza,
    A. Poppe, K. Resch, M. Taraba, R. Ursin, P. Walther, and A. Zeilinger, “Long-distance free-Space
    distribution of quantum entanglement,” Science 301, 621 (2003).
    3. I. Marcikic, H. de Riedmatten,W. Tittel, H. Zbinden, M. Legre, and N. Gisin, “Distribution of time-bin
    entangled qubits over 50 km of optical fiber,” Phys. Rev. Lett. 93, 180502 (2004).
    4. D. C. Burnham, D. L. Weinberg, “Observation of simultaneity in parametric production of optical photon
    pairs,” Phys. Rev. Lett. 25, 84 (1970).
    5. S. Friberg, C. K. Hong, and L. Mandel, “Measurement of time delays in the parametric production of
    photon pairs,” Phys. Rev. Lett. 54, 2011 (1985).
    6. S. Friberg and L. Mandel, “Production of squeezed states by combination of parametric down-conversion
    and harmonic generation,” Opt. Commun. 48, 439 (1984).
    7. P. G. Kwiat, E. Waks, A. G. White, I. Appelbaum, and P. H. Eberhard, “Ultrabright source of polarizationentangled
    photons,” Phys. Rev. A60, R773 (1999).
    8. C. Kurtsiefer, M. Oberparleiter, and H. Weinfurter, “High-efficiency entangled photon pair collection in
    type-II parametric fluorescence,” Phys. Rev. A 64, 023802 (2001)
    9. E. Brannen, F. R. Hunt, R. H. Adlington, R. W., Hicholls, “Application of nuclear coincidence methods to
    atomic transitions in the wavelength range 2000-6000A,” Nature 175, 810 (1955).
    10. A. Kuzmich, W. P. Bowen, A. D. Boozer, A. Boca, C. W. Chou, L.-M. Duan, and H.J. Kimble,
    “Generation of nonclassical photon pairs for scalable quantum communication with atomic ensembles,”
    Nature 423, 731 (2003).
    11. C. Santori, D. Fattal, J. Vu, G. S. Solomon, Y. Yamamoto, “Indistinguishable photons from a single-photon
    device,” Nature 419, 594 (2002).
    12. S. Tanzilli, F. D. Riedmatten, W. Tittle, H. Zbinden, P. Baldi, M. D., Micheli, D. B. Ostrowsky, N. Gisin,
    “Highly efficient photon-pair source using periodically poled lithium niobate waveguide,” Electron. Lett.
    37, 26 (2001).
    13. S. J. Mason, M. A. Albota, F. Konig, and F. N. C. Wong, “Efficient generation of tunable photon pairs at
    0.8 and 1.6 m,” Opt. Lett. 27, 2115 (2002).
    14. F. Konig, E. J. Mason, F. N. C. Wong, and M. A. Albota, “Efficient spectrally bright source of polarizationentangled
    photons,” Phys. Rev. A 71, 033805 (2005).
    15. T. A. Birks, J. C. Knight, and P. St. J. Russell, “Endlessly single-mode photonic crystal fibers,” Opt. Lett.
    22, 961 (1997).
    16. M. Fiorentino, P. L. Voss, J. E. Sharping, and P. Kumar, “All-fiber photon-pair source for quantum
    communication,” IEEE Photonics Tech. Lett. 14, 983 (2002).
    #7815 - $15.00 US Received 14 June 2005; revised 15 July 2005
    Ref:Generation of cross-polarized photon pairs in a
    microstructure fiber with frequency-conjugate
    laser pump pulses
    J. Fan and A. Migdall
    Optical Technology Division
    National Institute of Standards and Technology
    100 Bureau Drive, Mail Stop 8441, Gaithersburg. MD 20899-8441
    Jfan@nist.gov

    TAG# A Cross polarized oscillation in solar magnetic field calls for genetic catastrophe of air-water affined genes on the palm print of W.T.Stead-reg [Incident: 100802-000279 news@nature.com"
    Your call CNSHD789847 regarding Cross polarised genetic air-water affined catastrophe solved at last -reg has been received Outreach@stsci.edu"

    New Reference
    1) Solar rays could be converged to produce cross polar ized Bossonova resonance between Air affined and water affin ed middle frequency resonance as Monster twisters in ferroma gnetic cloud chambers for tapping e [Incident: 100807-000356] news@nature.com"
    2) Your call CNSHD790505 regarding A HubbleSite Comment has been received Outreach@stsci.edu"

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