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Trapped Antihydrogen Mike Charlton, Physics, Swansea University UK Trapped Antihydrogen Birmingham December 7 th 2011 Summary of the Talk Motivation for Antihydrogen Experiments Processes and Some Insights from Simulations Positron and


  1. Trapped Antihydrogen Mike Charlton, Physics, Swansea University UK Trapped Antihydrogen Birmingham December 7 th 2011

  2. Summary of the Talk Motivation for Antihydrogen Experiments Processes and Some Insights from Simulations Positron and Antiproton Clouds - Collection and Manipulation Antihydrogen Production The ALPHA Antihydrogen Trapping Experiment Trapped Antihydrogen Birmingham December 7 th 2011

  3. Motivation for Antihydrogen Experiments | Antihydrogen | = | Hydrogen | ? CPT Theorem. (Based upon Lorentz Invariance, spin-statistics and locality ) Some of the most precise tests of CPT Relative precision Trapped Antihydrogen Birmingham December 7 th 2011

  4. Motivation for Antihydrogen Experiments An outside view …? Quote from John Ellis (CERN Theory Division) writing in his article “Antimatter matters” a “news and views feature” from Nature 424 (2003) 631-4 “ But CERN has recently embarked on an experimental programme … to look for any differences between the structure (…) of hydrogen and antihydrogen down to one part in 10 12 or 10 15 . Admittedly we theorists do not really expect that CPT violation will show up in these experiments ….. – but we have been wrong before.” Trapped Antihydrogen Birmingham December 7 th 2011

  5. Motivation for Antihydrogen Experiments 1S-2S transition in H; Niering et al. PRL 84 (2000) 5496 2 466 061 413 187 103(46) Hz, or 1.8 parts in 10 14 Ground State Hyperfine transition in H; Essen et al. Nature 229 (1971) 110 1 420 405 751.7667(9) Hz, or 6.4 parts in 10 13 Trapped Antihydrogen Birmingham December 7 th 2011

  6. Motivation for Antihydrogen Experiments | Antihydrogen | = | Hydrogen | ? Gravity Trapped Antihydrogen Birmingham December 7 th 2011

  7. Antihydrogen Production: Formation Processes Trapped Antihydrogen Birmingham December 7 th 2011

  8. Antihydrogen Production: Formation Processes The TBR is a quasi-elastic encounter of 2 positrons in the vicinity of an antiproton. Energy exchange ~ k B T e , which will be the same order of the binding energies. Thus, these are very weakly bound states which are strongly influenced by the ambient fields Electric and magnetic fields of the Penning trap AND   ( ) / 2 E r n er The plasma self electric field 0 r e The combination of E r and B z results in a tangential drift speed, which to 2 nd order is given by: 2 /    3 ( ) / ( ) v d E r B mE r eB r Trapped Antihydrogen Birmingham December 7 th 2011

  9. Antihydrogen Production: Insights from Simulations        e e p H e Work of Jonsell et al ., J.Phys.B 42 (2009) 215002 Total antiproton loss T e = 15 K Detected antihydrogen B = 0 Lines are for different values of the applied B = ∞ magnetic field, B B = 3 T n e Trapped Antihydrogen Birmingham December 7 th 2011

  10. Antihydrogen Production: Insights from Simulations T e = 15 K Antihydrogen binding energies as the Antihydrogen binding energies on detection atoms leave the positron plasma n e = 10 15 m -3 (+); 5 ( ○ ), 2 ( Δ ) and 1 ( □ ) x 10 14 m -3 n e = 10 15 m -3 (x); n e = 5 x 10 13 m -3 (+) and 5 x 10 13 m -3 (x) Trapped Antihydrogen Birmingham December 7 th 2011

  11. Antihydrogen Production: Insights from Simulations Radial distribution of antihydrogen formation positions at different time intervals n e = 10 15 m -3 n e = 5 x10 13 m -3 short (x), medium ( Δ ) and long ( □ ) times NB at 10 15 m -3 a “long” time is > 1ms Trapped Antihydrogen Birmingham December 7 th 2011

  12. Positron Accumulation Segmented electrode for Rotating Wall 300 Gauss guiding fields Coldhead T = 6 K Beam strength: 50 mCi 22 Na 6 million e+ per second Solid neon moderator Trap electrode voltages Energy loss through collisions Based upon the industry standard … e+ {Solid-Ne moderator -plus - UCSD Penning Malmberg buffer gas trap: Surko and co- workers} e+      * ( ) ( ) e E N e E N Distance along the trap 2 2 i f Trapped Antihydrogen Birmingham December 7 th 2011

  13. Positron Accumulation 200 Open circles: Accumulated positrons / millions no rotating electric field 150 Closed circles: 100 rotating field applied 50 Plasma formed after 0 about 10-15 s 0 200 400 600 Accumulation time / sec. Trapped Antihydrogen Birmingham December 7 th 2011

  14. Positron Accumulator – 3 rd stage Trapped Antihydrogen Birmingham December 7 th 2011

  15. Positron Plasma Rotating Wall Compression Rotating electric field in same sense as ExB drift B Positron plasma radial distributions r.w. r.w with added No r.w. with N 2 cooling gas Trapped Antihydrogen Birmingham December 7 th 2011

  16. Antiprotons: CERN’s “Accelerators” The AD, or Antiproton Decelerator Trapped Antihydrogen Birmingham December 7 th 2011

  17. Antiprotons: the AD, Antiproton Decelerator From PS: 1.5x1013 protons/bunch, 26 GeV/c 2 Injection at 3.5 GeV/c Antiproton 1 Production 4 Extraction ( 2x107 in 200 ns) ATRAP Stochastic Cooling Deceleration and 3 Cooling (3.5 - 0.1 GeV/c) ASACUSA ATHENA ALPHA Kinetic energy about 5.3 MeV Electron Cooling 0 20 m 10 Trapped Antihydrogen Birmingham December 7 th 2011

  18. Antiprotons: Capture and Cooling Method devised by Gabrielse and co-workers: PRL, The trap walls are cooled to 15 K 57, 2504 (1986) and PRL ,63, 1360 (1989) ATHENA Antiproton Capture Trap Similar apparatus used currently in ALPHA ALPHA will routinely stack up to 8 shots from the AD to To (or close to) the provide ~ 2 x 10 5 antiprotons into mixing trap temperature Trapped Antihydrogen Birmingham December 7 th 2011

  19. Antiprotons: ALPHA-Sympathetic Compression using Electrons Sympathetic compression of an antiproton cloud by electrons G. Andresen et al, PRL, 101 (2008) Typically use a fixed frequency 203401 rotating wall technique at 10 MHz Trapped Antihydrogen Birmingham December 7 th 2011

  20. Antiprotons: ALPHA – Evaporative Cooling Andresen et al . PRL (2010) 105 013003 23 K 9 K 19 K 325 K 1040 K 57 K Typically (9 ± 4) K is lowest achievable at the lowest well available at which (6 ± 1) % of the initial antiprotons remain Trapped Antihydrogen Birmingham December 7 th 2011

  21. Antiprotons: So far … Antiprotons into the AD at ~ 3.5 GeV (~3x10 7 from 1.5x10 13 protons at 26 GeV) ~ 100 s of cooling in the AD to 5.3 MeV; ejection in a 100 ns burst Capture and electron cooling in a Penning Malmberg trap for ~ 20 s ( ε ~ 10 -3 ) Stacking of up to 8 AD shots. Takes ~ 1000 s for ~ 2 x10 5 cold antiprotons Shuffle to 1 T region. Recool and sympathetic radial compression for about 60 s Evaporative cooling if desired to very low temperatures. Takes ~ 10 s … Now ready for mixing with positrons … Trapped Antihydrogen Birmingham December 7 th 2011

  22. Antihydrogen Production: ATHENA Fill positron well in mixing region with 75·10 6 positrons; 1. allow them to cool to ambient temperature (15 K) Launch 10 4 antiprotons into mixing region 2. 3. Mixing time 190 sec - continuous monitoring by detector 4. Repeat cycle every 5 minutes For comparison: “hot” mixing = continuous -125 antiprotons RF heating of positron cloud -100 (suppression of formation of -75 antihydrogen) -50 0 2 6 8 10 12 4 Length (cm) Trapped Antihydrogen Birmingham December 7 th 2011

  23. Antihydrogen Detection: ATHENA • Charged tracks to reconstruct antiproton annihilation vertex. • Identify 511 keV photons from e + -e - annihilations. • Identify space and time coincidence of the two. 511 keV   Two annihilation events from antihydrogen which strikes the wall of the Silicon micro strips  charged particle traps • Compact (3 cm thick) CsI • Solid angle > 70% crystals • High granularity  • Operation at 140K, 3 T 511 keV  Trapped Antihydrogen Birmingham December 7 th 2011

  24. Antihydrogen Production: ATHENA • Reconstruct annihilation vertex • Search for ‘clean’ 511 keV -photons: exclude crystals hit by charged particles + its 8 nearest neighbours • ‘511 keV’ candidate = 400… 620 keV no hits in any adjacent crystals • Select events with two ‘511 keV’ photons • Reconstruction efficiency ≤ 0.25 % Trapped Antihydrogen Birmingham December 7 th 2011

  25. Antihydrogen Production: ATHENA 200 Cold Mixing : Cold mixing 103270 vertices, 180 Hot mixing 7125 2x511keV events 131± 22 events 160 (or about 50,000 antihydrogen atoms made) 140 120 Antihydrogen suppressed 100 80 No peak Hot Mixing : 60 Scaled (x1.6) to 165 mixing 40 cycles. 20 0 -1 -0.5 0 0.5 1 cos(   ) Amoretti et al., Nature 419 456 (2002) Trapped Antihydrogen Birmingham December 7 th 2011

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