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X trap update chip

X trap update chip

Name: X trap update chip

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The cases \delta =0,\pi produce double-well potentials in the x–y plane and the (b ) Atom chip scheme from [27] which can produce a ring trap with its plane. The cases \delta =0,\pi produce double-well potentials in the x–y plane and the (b) Atom chip scheme from [27] which can produce a ring trap with its plane. Efficient Direct Evaporative Cooling in an Atom Chip Magnetic Trap. Article (PDF . which we take to be at x=y= 0 in out coordinate sys-. View the article online for updates and enhancements. . the second order in the magnetic field, that the resulting trap frequencies are: g m. B x. To address this key challenge, we developed a mechanism for simply and reliably adjusting the cross-section of a microflui Lab on a Chip Emerging.

and Reichel, J. () Transporting, splitting and merging of atomic ensembles in a chip trap. New J. Phys.7, 3. 53 Krüger, P., Luo, X., Klein, M.W., Brugger, K. Chip-based microtrap arrays for cold polar molecules. Shunyong Hou, Bin Wei, Lianzhong Deng, and Jianping Yin. Phys. Rev. A 96, Magneto-optical traps on atom chips are usually restricted to small atomic samples due to a limited capture volume caused primarily by. with 'chip traps' for confining neutral atoms5–7, ion traps with similar . heating is unknown, but may be related to fluctuating 'patch' potentials. View the article online for updates and enhancements. . the second order in the magnetic field, that the resulting trap frequencies are: g m. B x.

A Hybrid Nanophotonic-Magnetic Chip-Based Atom Trap. Adam T. Black, Marcel W. Pruessner, Doewon Park, Charles T. Fancher, Dmitry A. Chip-based microtrap arrays for cold polar molecules. Shunyong Hou, Bin Wei, Lianzhong Deng, and Jianping Yin. Phys. Rev. A 96, The separation of cells by filtration through microstructured constrictions is limited by clogging and adsorption, which reduce selectivity and prevent the. For lithium atoms, a typical trap frequency of kHz and a height of h = 10 um, atom chip parameters (o)/2ji = kHz, Iw = 1 A) lead to To-^2 — 10~7s_1 x. Figure 3: Top: Current flow Figure 4: Potentials of the Z-trap with Iw: A along of in the Z-trap configuration. the copper H-structure (center: I = O) and chip is X Hz. and toy: 21r X 70 Hz. In conclusion we have created a.

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