Science, Volume 333, Issues 6039-6044John Michels (Journalist) American Association for the Advancement of Science, 2011 |
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Page 158
... atom - by - atom by subsequently adding Fe atoms with an interatomic distance d = 0.923 nm , where the interatomic exchange coupling is antiferromagnetic ( 0.1 meV ) ( Fig . 2 , A to E ) for spin leads with lengths of up to six atoms ...
... atom - by - atom by subsequently adding Fe atoms with an interatomic distance d = 0.923 nm , where the interatomic exchange coupling is antiferromagnetic ( 0.1 meV ) ( Fig . 2 , A to E ) for spin leads with lengths of up to six atoms ...
Page 197
... atoms , optically pumped to my = +1 , are then transferred to an Ioffe - Pritchard- type magnetic trap . * He * atoms are evaporative- ly cooled toward Bose - Einstein condensation by stimulating radio - frequency ( RF ) transitions to ...
... atoms , optically pumped to my = +1 , are then transferred to an Ioffe - Pritchard- type magnetic trap . * He * atoms are evaporative- ly cooled toward Bose - Einstein condensation by stimulating radio - frequency ( RF ) transitions to ...
Page 691
... atom spinning either up or down and deflecting it accordingly . The inten- sities of the two beams then reveal the per amounts of up and down in the atoms ' Squantum state . Such a " strong " measurement oblit- erates the original up ...
... atom spinning either up or down and deflecting it accordingly . The inten- sities of the two beams then reveal the per amounts of up and down in the atoms ' Squantum state . Such a " strong " measurement oblit- erates the original up ...
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