| 2010 Summary in Physics Today | ATRAP Antihydrogen Collaboration |
Long Term Goal: Precise laser or microwave spectroscopy of trapped antihydrogen |
``When antihydrogen is formed in an ion trap, the neutral atoms will no longer be confined and will thus quickly strike the trap electrodes. Resulting annihilations of the positron and antiproton could be monitored. ..." |
|
"... it is clear that the very low [antihydrogen production rate] will make ... experiments with antihydrogen to be very ... difficult. For me, the most attractive way ... would be to capture the antihydrogen in a neutral particle trap ... The objective would be to then study the properties of a small number of [antihydrogen] atoms confined in the neutral trap for a long time." |
|
ATRAP Simultaneously Loads Positrons and Antiprotons During a 100 Second Cycle |
tick marks: 1 meter |
||
| Cold positrons and | ||
accumulates positrons |
cold antiprotons are accumulated | |
from a 22Na source |
in Penning traps located | |
| within a 1-3 Tesla solenoid | ||
| (below left) | ||
| Antiprotons come from | ||
| the CERN Antiproton | ||
time axis |
Decelerator (AD) | |
| storage ring | ||
0 seconds antiprotons load |
30 seconds positrons load |
70 seconds more positrons load |
100 seconds cycle starts over |
![]() |
![]() |
Anihydrogen is produced |
Solenoid and vacuum container for the traps |
Inside view of Penning traps and Ioffe trap |
Note: everyone at ATRAP helps out as needed on whatever part of the project needs help, so these divisions are often blurred |