| BERKELEY, CA —  For
      over half a century, theorists have tried and failed to provide a complete
      solution to scattering in a quantum system of three charged particles, one
      of the most fundamental phenomena in atomic physics. Such interactions are
      everywhere; ionization by electron impact, for example, is responsible for
      the glow of fluorescent lights and for the ion beams that engrave silicon
      chips.
       Now, collaborators at the Department of Energy's Lawrence Berkeley
      National Laboratory, Lawrence Livermore National Laboratory, and the
      University of California at Davis have used supercomputers to obtain a
      complete solution of the ionization of a hydrogen atom by collision with
      an electron, the simplest nontrivial example of the problem's last
      unsolved component. They report their findings in the 24 December, 1999,
      issue of Science magazine. 
      
        
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            A REPRESENTATIVE RADIAL WAVE FUNCTION OF TWO ELECTRONS SCATTERED
            IN THE COLLISION OF AN ELECTRON WITH A HYDROGEN ATOM
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      Their breakthrough employs a mathematical transformation of the
      Schrödinger wave equation that makes it possible to treat the outgoing
      particles not as if their wave functions extend to infinity -- as they
      must be treated conventionally -- but instead as if they simply vanish at
      large distances from the nucleus. 
      "Using this transformation we compute accurate solutions of the
      quantum-mechanical wave function of the outgoing particles, and from these
      solutions we extract all the dynamical information of the
      interaction," says Bill McCurdy, Berkeley Lab's Associate Laboratory
      Director for Computing Sciences and a principal author of the Science
      article. 
      McCurdy and his longtime collaborator Thomas Rescigno, a staff
      physicist at Livermore Lab, and their co-authors, doctoral candidate Mark
      Baertschy of UC Davis and postdoctoral fellow William Isaacs at Berkeley
      Lab, used the SGI/Cray T3E at the National Energy Research Scientific
      Computing Center (NERSC) at Berkeley Lab and the IBM Blue Pacific computer
      at Livermore Lab for their solution of the three-charged-body scattering
      problem. 
      "An exact first-principles solution of the wave function for the
      hydrogen atom was vital to establishing the new quantum theory in the
      1920s," says Rescigno. "But even today, for systems with three
      or more charged particles, no analytic solutions exist" -- that is,
      there are no explicit solutions to the Schrödinger equation for such
      systems. 
      Rescigno points out that "it wasn't until the late 1950s, using
      early computers, that accurate solutions were obtained even for the bound
      states of helium," an atom with two electrons closely orbiting the
      nucleus. "Scattering problems are a lot more difficult." 
      As with all scattering problems, the electron-ionization of a hydrogen
      atom begins with a particle incoming at a certain velocity. This electron
      interacts with the atom, and two electrons fly out at an angle to each
      other, leaving the proton behind. The likelihood that a specific incoming
      state will result in an outgoing state with the particles at specific
      angles and energies is the "cross section" for that result. 
      Cross sections of quantum-mechanical processes are derived from the
      system's wave function, solutions of the Schrödinger equation which yield
      probabilities of finding the entities involved in a certain state. In
      scattering problems, wave functions are not localized but extend over all
      space. 
      Moreover, says McCurdy of the electromagnetic forces between charged
      particles, "Coulomb interactions are forever." These infinities
      make it impossible to define the final state of scattering exactly.
      "The form of the wave function where all three particles are widely
      separated is so intractable that no computer-aided numerical approach has
      been able to incorporate it explicitly." 
      But, Rescigno notes, "this obviously hasn't stopped people from
      working with plasmas and other ionization phenomena. Mathematically,
      they've come up with incredibly artful dodges, and some of them even seem
      to work." 
      Earlier this year, however, in the Proceedings of the Royal Society,
      Colm T. Whelan of Cambridge University and his colleagues published their
      conclusion that all such approximations perform inconsistently and that
      those few cases which appear to yield good agreement with experiment
      "are largely fortuitous." 
      By contrast, the method developed by McCurdy and Rescigno and their
      co-authors allows the calculation of a highly accurate wave function for
      the outgoing state that can be interrogated for details of the incoming
      state and interaction in the same way an experimenter would interrogate a
      physical system. 
      They begin with a transformation of the Schrödinger equation called
      "exterior complex scaling," invented by Caltech's Barry Simon in
      1979 to prove formal theorems in scattering theory. The transformation
      leaves the solution unchanged in regions which correspond to physical
      reality, producing the correct outgoing waveform based upon the angular
      separation and distances of two electrons far from the nucleus. 
      Once the wave function has been calculated, it must be analyzed by
      computing the "quantum mechanical flux," a means of finding the
      distribution of probability densities that dates from the 1920s. This
      computationally intensive process can yield the probability of producing
      electrons at specific energies and directions from the ionized atom.
      (Because electrons are identical, there is no way to distinguish between
      the initially bound and initially free electron). 
      The researchers acknowledge important advances made earlier by others
      such as Igor Bray and Andres Stelbovics, whose methods could give the
      total cross section for ionization of a scattering reaction but could not
      give specifics such as the directions or energies of outgoing electrons.
      By contrast, says Rescigno, "Our work produces absolute answers at
      the ultimate level of detail." 
      
        
            
             
            PREDICTED CROSS SECTIONS OF SCATTERED ELECTRONS (SOLID CURVES)
            AND EXPERIMENTAL MEASUREMENTS (DOTS) MATCH ALMOST EXACTLY
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      Comparison with real scattering experiments, such as those recently
      published by J. Röder et al, who scattered incoming 17.6 electron-volt
      electrons from hydrogen atoms and measured the angles and energies of the
      outgoing electrons, prove the accuracy of the new method. The experimental
      data points match the graph of the cross sections calculated by Rescigno,
      Baertschy, Isaacs, and McCurdy with astonishing exactitude. 
      "Even if the specific methods have changed, quantum chemistry was
      founded when the helium atom with two bound electrons was solved -- it
      showed that these problems were in principle solvable," McCurdy says.
      "What we have done is analogous. The details of our method probably
      won't survive, but we've taken a big step toward treating ionizing
      collisions of electrons with more complicated atoms and molecules." 
      "Collisional breakup in a quantum system of three charged
      particles," by T.N. Rescigno, M. Baertschy, W.A. Isaacs, and C.W.
      McCurdy appears in Science magazine, 24 December 1999. The authors
      conclude by noting that the same computing power and tools necessary for
      investigating the complexity of increasingly larger systems are also
      needed "to answer a basic physics question for one of the simplest
      systems imaginable in physics and chemistry." 
      The Berkeley Lab is a U.S. Department of Energy national laboratory
      located in Berkeley, California. It conducts unclassified scientific
      research and is managed by the University of California. 
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