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Diabatization: a simple way to get to high-lying excited states
  • A.T. Le  and  C.D. Lin
  • Dept. of Physics, KSU
  • April 14, 2004
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Outline
  • Introduction
  • Diabatization procedure: what’s new?
  • Doubly excited states of helium
  • Antihydrogen formation in antiproton colliding with excited positronium


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Introduction
  • Difficulties with adiabatic basis:
  • Avoided crossings
  • Many channels need to be included
  • Difficult to do calculations with high excited states


  • Diabatic basis has long been proposed.


  • Our goal:
  • Simplified picture with less channels involved
  • Practical calculations.
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Table 3: Comparison for 4(3,0)+n of He(1Se)
   Resonance positions are given as -E (a.u.).

  •      HSCC   HSCC   HSCC Complex
  •  n   1-channel 2-channel 14-channel rotation


  •  4 0.2012 0.2017 0.2017 0.2010
  •  5 0.1651 0.1664 0.1665 0.1657
  •  6 0.1491 0.1514 0.1515 0.1508
  •  7 0.1411 0.1428 0.1429 0.1426
  •  8 0.1366 0.1377 0.1378 0.1377
  •  9 0.1337 0.1345 0.1346 0.1246
  • 10 0.1318 0.1323 0.1324 0.1325
  • 11 0.1304 0.1308 0.1309 0.1310
  • 12 0.1294 0.1298 0.1298 0.1299
  • 13 0.1287 0.1289 0.1290 0.1293


  • Complex rotation: Burgers et al, JPB 28, 3161 (1995)


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Antihydrogen formation
  • Progress in production of cold antihydrogen


  • Charge exchange:


  • Two-stage mechanism


  •     Other important mechanisms: Three-body recombination, spontaneous (laser stimulated) radiative recombination.
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Note: all the channel are adiabatic with many avoided crossing
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The channels are diabatic!
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Summary

  • Diabatization seems to work well;
  • Less channels, simpler for understanding;
  • “Quantum chaos” signature were found for 3D He;
  • Antihydrogen formation from high-excited Ps can be calculated;