A millimeter-scale Ioffe-Pritchard trap is used to achieve quantum degeneracy in $^{7}\mathrm{Li}$ . The trap employs freestanding copper coils integrated onto a direct-bond copper surface-electrode structure. The trap achieves a radial magnetic gradient of $420\phantom{\rule{0.3em}{0ex}}\mathrm{G}∕\mathrm{cm}$ , an axial oscillation frequency of $50\phantom{\rule{0.3em}{0ex}}\mathrm{Hz}$ , and a trap depth of $66\phantom{\rule{0.3em}{0ex}}\mathrm{G}$ with a $100\phantom{\rule{0.3em}{0ex}}\mathrm{A}$ drive current and $7\phantom{\rule{0.3em}{0ex}}\mathrm{W}$ total power dissipation.A millimeter-scale Ioffe-Pritchard trap is used to achieve quantum degeneracy in $^{7}\mathrm{Li}$. The trap employs freestanding copper coils integrated onto a direct-bond copper surface-electrode structure. The trap achieves a radial magnetic gradient of $420\phantom{\rule{0.3em}{0ex}}\mathrm{G}∕\mathrm{cm}$, an axial oscillation frequency of $50\phantom{\rule{0.3em}{0ex}}\mathrm{Hz}$, and a trap depth of $66\phantom{\rule{0.3em}{0ex}}\mathrm{G}$ with a $100\phantom{\rule{0.3em}{0ex}}\mathrm{A}$ drive current and $7\phantom{\rule{0.3em}{0ex}}\mathrm{W}$ total power dissipation.

Physical Review AJan 10, 200724 citations

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^{7}

Li BEC in a millimeter-scale Ioffe-Pritchard trap

A millimeter-scale Ioffe-Pritchard trap is used to achieve quantum degeneracy in

^{7}\mathrm{Li}

. The trap employs freestanding copper coils integrated onto a direct-bond copper surface-electrode structure. The trap achieves a radial magnetic gradient of

420\phantom{\rule{0.3em}{0ex}}\mathrm{G}∕\mathrm{cm}

, an axial oscillation frequency of

50\phantom{\rule{0.3em}{0ex}}\mathrm{Hz}

, and a trap depth of

66\phantom{\rule{0.3em}{0ex}}\mathrm{G}

with a

100\phantom{\rule{0.3em}{0ex}}\mathrm{A}

drive current and

7\phantom{\rule{0.3em}{0ex}}\mathrm{W}

total power dissipation.

Creation and Characterization of a BEC of

^{7}

Formation of a Matter-Wave Breather in a

^7 \mathrm{Li}

BEC