2005
DOI: 10.1103/physreva.71.063619
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Combined chips for atom optics

Abstract: We present experiments with Bose-Einstein condensates on a combined atom chip. The combined structure consists of a large-scale "carrier chip" and smaller "atom-optics chips", containing micron-sized elements. This allows us to work with condensates very close to chip surfaces without suffering from fragmentation or losses due to thermally driven spin flips. Precise three-dimensional positioning and transport with constant trap frequencies are described. Bose-Einstein condensates were manipulated with submicro… Show more

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Cited by 66 publications
(63 citation statements)
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“…Since the advent of microchip traps for cold atoms [1][2][3][4][5][6][7][8][9][10][11][12], interest in developing quantum hybrid systems, which exploit the long coherence times of Bose-Einstein condensates with the flexibility of modern micro-and nanoelectronics, continues to grow. There is potential to use such systems as quantum memory devices [13][14][15], precision measurement devices [16][17][18][19] and even rewritable electronic systems [20].…”
Section: Introductionmentioning
confidence: 99%
“…Since the advent of microchip traps for cold atoms [1][2][3][4][5][6][7][8][9][10][11][12], interest in developing quantum hybrid systems, which exploit the long coherence times of Bose-Einstein condensates with the flexibility of modern micro-and nanoelectronics, continues to grow. There is potential to use such systems as quantum memory devices [13][14][15], precision measurement devices [16][17][18][19] and even rewritable electronic systems [20].…”
Section: Introductionmentioning
confidence: 99%
“…So far, experiments have dealt with atoms prepared in the electronic ground state, due to their intrinsic stability. Despite their weak interactions, ground-state atoms on atom chips have been used to sensitively probe the intrinsic thermal noise near surfaces [3][4][5], map magnetic and electric field distributions [6][7][8][9][10][11], and investigate the Casimir-Polder potential in the micrometer range [12][13][14]. Comparatively, atoms excited to high-lying Rydberg states have extremely large transition dipole moments (scaling with n 2 ) resulting in long-range interactions and have large electric polarizabilities (∝ n 7 ) which can greatly enhance both atomatom and atom-surface interactions.…”
Section: Introductionmentioning
confidence: 99%
“…Typically, 3 · 10 8 Rubidium atoms from a magnetooptical trap are transferred into a standard magnetic trap and precooled by forced evaporation to a temperature of 5µK. Next, the atoms are adiabatically shifted into a micro trap transport system that allows to generate a harmonic trapping potential at an arbitrary position within a volume of 1.5 x 0.3 x 20 mm 3 (x, y, zdirection) [13]. The transport system consists of an assembly of 100µm wide gold conductors electroplated on both sides of a 250µm thick substrate ("carrier chip").…”
mentioning
confidence: 99%
“…A Bose-Einstein condensate consisting of 1.2 · 10 5 87 Rb atoms in the F=2, m F =2 hyperfine state is trapped in an elongated magnetic trap close to the surface of a chip that carries a magnetic lattice [13]. It consists of a set of 372 parallel conductors perpendicular to the long axes of the trap, each 1µm wide and separated by 1µm gaps [14].…”
mentioning
confidence: 99%