Abstracts of Monday Posters
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Monday Posters Atom interferometry Mo-001 57 $GLJLWDODWRPLQWHUIHURPHWHUZLWKVLQJOHSDUWLFOHFRQWURO Andrea Alberti 1, *, Andreas Steffen 1, Wolfgang Alt 1, Noomen Belmechri 1, Sebastian Hild 1, 0LFKDá.DUVNL 1, Artur Widera 2,1 and Dieter Meschede 1 ,QVWLWXWIU$QJHZDQGWH3K\VLN8QLYHUVLWlW%RQQ*HUPDQ\ 2. Fachbereich Physik und Forschungszentrum OPTIMAS, Universität Kaiserslautern, Germany *[email protected] Coherent control and delocalization of single trapped atoms constitute powerful new resources for quantum technologies. We will report on a single-atom interferometer that uses spin-dependent periodic potentials to co- herently split and recombine particles with spatial separations of up to 24 lattice sites, equivalent to more than 10 ȝm. The interferometer geometry can be reprogrammed in a digital manner by freely assembling basic coherent operations at discrete time intervals; this allowed us to contrast different geometries and to develop a geometrical- analogue of the well-known spin-echo refocusing. We tested the interferometer by probing external potential gra- dients, achieving with single atoms 5 × 10 –4 precision in units of gravitational acceleration g. Furthermore, a novel scheme for spin-dependent optical lattices is presently underway, with which we expect to reach splitting distances of 1 mm. This coherent control of single-atom wave packets gives us a new way to investigate and exploit interaction effects between atoms; for instance, molecular bound states of two atoms are predicted to occur in quantum walk experiments as a result of matter-wave interference [1]. Reference [1] A. Ahlbrecht, A. Alberti, D. Meschede, V. B. Scholz, A. H. Werner, R. F. Werner, Bound Molecules in an Interacting Quantum :DONDU;LYY Atom interferometry Mo-002 ,QWHUIHURPHWU\ZLWKFKLSEDVHGDWRPODVHUV E. M. Rasel*, for the QUANTUS cooperation QUEST, Institut fr Quantenoptik - Leibniz Universitt, Hannover, Germany *[email protected] We report on the implementation of a Bragg-type interferometer operated with a chip-based atom laser for Rubidium 87 Rb. With the chip based atom laser we can generate thermal ensemble as well as Bose-Einstein conden- sates (BEC) [1]. With the help of delta kick cooling [2], implemented via the atom chip, we can further slow down the expansion of thermal and condensed atoms. In addition, the chip allows to transfer atoms in the individual Zee- PDQVWDWHVRIWKHWZRK\SHU¿QHJURXQGVWDWHVLQSDUWLFXODULQWRWKHQRQPDJQHWLFVWDWH:LWKWKLVWRROER[ZHFRXOG extend the observation of a BEC of only 10000 atoms to macroscopic time scales approaching two seconds. Ben- H¿WLQJIRUPWKHH[WHQGHGIUHHIDOOLQPLFURJUDYLW\ZHFRXOGFRPELQHWKLVZLWKDQDV\PPHWULF0DFK=HKQGHUW\SH interferometer over hundreds of milliseconds to study the coherence and to analyze the delta kick cooling with the help of the observed interference fringes. This experiment can be considered as a double slit experiment in micro- JUDYLW\1%7KH48$1786FRRSHUDWLRQFRPSULVHVWKHJURXSRI&/lPPHU]DKO 8QLY%UHPHQ $:LFKW )%+ $3HWHUV +XPEROGW8QLY%HUOLQ 7+lQVFK-5HLFKHO 034(16 .6HQJVWRFN 8QLY+DPEXUJ 5:DOVHU (TU Darmstadt), and W. P. Schleich (Univ. Ulm). References [1] van Zoest et al. , %RVH(LQVWHLQFRQGHQVDWLRQLQPLFURJUDYLW\ , Science 328, 1540 (2010). [2] H. Amman and N. Christensen, 'HOWD.LFN&RROLQJ$1HZ0HWKRGIRU&RROLQJ$WRPV , Phys. Rev. Lett., 78 , 2088 (1997). 58 Mo-003 Atom interferometry 3UHFLVLRQLQWHUIHURPHWU\ZLWK%RVH(LQVWHLQFRQGHQVDWHV WRZDUGDQHZPHDVXUHPHQWRIWKH¿QHVWUXFWXUHFRQVWDQW Alan O. Jamison 1, *, Ben Plotkin-Swing 1, Anders Hansen 1, Alexander Khramov 1, William Dowd 1, J. Nathan Kutz 1,2, and Subhadeep Gupta 1 'HSWRI3K\VLFV8QLYHUVLW\RI:DVKLQJWRQ6HDWWOH86$ 'HSWRI$SSOLHG0DWKHPDWLFV8QLYHUVLW\RI:DVKLQJWRQ6HDWWOH86$ MDPLVRQD#XZHGX We report progress, both theoretical and experimental, toward an atom interferometric measurement of ƫMYb , IURPZKLFKDYDOXHIRUWKH¿QHVWUXFWXUHFRQVWDQWPD\EHGHWHUPLQHG%\XVLQJDV\PPHWULFWKUHHDUPFRQWUDVW interferometer in free space many potential sources of systematic error cancel. For part per billion precision, such an interferometer requires two of the arms to be coherently accelerated. Experimental progress includes improved DWRPFRROLQJHI¿FLHQF\DOORZLQJSURGXFWLRQRIODUJH aî 5 atom), nearly pure condensates of 174Yb and faster cycle times for a low-momentum prototype interferometer. Theoretical progress includes new techniques for SUHGLFWLQJPHDQ¿HOGHIIHFWVIRUDOOLQWHUDFWLRQVWUHQJWKVLQFOXGLQJWKHLQWHUPHGLDWHVWUHQJWKUHJLPHZKLFKLVNH\ to precision BEC interferometry [1]. These techniques are also valid for waveguide interferometers. A comparison of various coherent acceleration schemes will also be presented. Reference [1] A. O. Jamison, et al. , $WRPLF,QWHUDFWLRQVLQ3UHFLVLRQ,QWHUIHURPHWU\8VLQJ%RVH(LQVWHLQ&RQGHQVDWHV , Phys. Rev. A, 84 , pp. 043643 (2011). Mo-004 Atom interferometry Quantum feedback control of atomic coherent states Ralf Kohlhaas 1, Thomas Vanderbruggen 1, Andrea Bertoldi 1, Simon Bernon 1, Alain Aspect 1, Arnaud Landragin 2, and Philippe Bouyer1,3,* 1. Laboratoire Charles Fabry, Institut d’Optique, CNRS, Université Paris-Sud, Campus Polytechnique, RD 128, 91127 Palaiseau cedex, France 2. LNE-SYRTE, Observatoire de Paris, CNRS and UPMC, 61 avenue de l’Observatoire, F-75014 Paris, France /DERUDWRLUH3KRWRQLTXH1XPpULTXHHW1DQRVFLHQFHV/318QLYHUVLWp%RUGHDX[,2*6&156 805%kW$FRXUVGHODOLEHUDWLRQ7DOHQFH)UDQFH *[email protected] Quantum superposition states are under constant threat to decohere by the interaction with their environment. Active feedback control can protect quantum systems against decoherence, but faces the problem that the measure- ment process itself can change thequantum system. The adaptation of the measurement strategy to a given stabili- zation goal is therefore an essential step to implement quantum feedback control. Here, we present the protection of a collective internal state of an atomic ensemble against a simple decoherence model. A coherent spin state is prepared and exposed to a noise which randomly rotates the state on the Bloch sphere. We use weak nondestruc- WLYHPHDVXUHPHQWVZLWKQHJOLJLEOHSURMHFWLRQRIWKHDWRPLFVWDWHZKLFKVWLOOJLYHVXI¿FLHQWLQIRUPDWLRQWRDSSO\ feedback. This method is used to increase the coherence lifetime of the initial superposition state by about one order of magnitude. Atom interferometry Mo-005 59 $QRYHOFDYLW\EDVHGDWRPLQWHUIHURPHWHU Justin M. Brown1, *, Brian Estey 1, and Holger Müller 1,2 'HSDUWPHQWRI3K\LVFV8QLYHUVLW\RI&DOLIRUQLD%HUNHOH\%HUNHOH\&$86$ /DZUHQFH%HUNHOH\1DWLRQDO/DERUDWRU\2QH&\FORWURQ5RDG%HUNHOH\&$86$ MPEURZQ#EHUNHOH\HGX The world’s leading atom interferometers are housed in bulky atomic fountains. They employ a variety of tech- niques to increase the spatial separation between atomic clouds including high order Bragg diffraction. The largest momentum transfer in a single Bragg beamsplitter has been limited to 24 ƫN by laser power and beam quality [1]. We present an atom interferometer in a 40 cm optical cavity to enhance the available laser power, minimize wave- front distortions, and control other systematic effects symptomatic to atomic fountains. We expect to achieve spatial separations between atomic trajectories comparable to larger scale fountains within a more compact device. We report on progress in developing this new interferometer using cold Cs atoms and discuss its prospects for exploring large momentum transfer up to 100 ƫNLQDVLQJOH%UDJJGLIIUDFWLRQSURFHVV7KHFRPSDFWGHVLJQZLOOHQDEOHWKH¿UVW demonstration of the gravitostatic Aharonov-Bohm effect [2]. References [1] Holger Müller, Sheng-wey Chiow, Quan Long, Sven Herman, and Steven Chu. “Atom Interferometry with up to 24-Photon- Momentum-Transfer Beam Splitters”. Phys. Rev. Lett. 100(18), 180405, (2008). >@0LFKDHO$+RKHQVHH%ULDQ(VWH\3DXO+DPLOWRQ$QWRQ=HLOLQJHUDQG+ROJHU0OOHU³)RUFHIUHHJUDYLWDWLRQDOUHGVKLIWD JUDYLWRVWDWLF$KDUQRQY%RKPH[SHULPHQW´HSULQWDU;LYY Atom interferometry Mo-006 Coherent population transfer of cold 87 5EDWRPVE\ FRXQWHULQWXLWLYHOLJKWSXOVHV Hoon Yu, Mi Hyun Choi, Seung Jin Kim, and Jung Bog Kim 3K\VLFV(GXFDWLRQ.RUHD1DWLRQDO8QLYHUVLW\RI(GXFDWLRQ&KXQJ%XN.RUHDUHSXEOLF We consider counter-intuitive light pulses to transfer atoms coherently from the ground state to another ground VWDWHWKURXJKWKHFRPPRQH[FLWHGVWDWHODPEGDW\SHFRQ¿JXUDWLRQ>@:HLQLWLDOO\SUHSDUHG¿HOGIUHHFROG 87 Rb at- oms in the ground state of 5S ) $QGZHGHWHFWHGWKHÀXRUHVFHQFHE\DWRPVLQDQRWKHUJURXQGVWDWH6 (F=2), to measure amount of transferred atoms. We optimized experimental parameters - width of pulses, power of each pulse, delay time between two pulses, and the two photon detuning- until the effective Rabi frequency of over- ODSSHGDUHDRIWZRSXOVHVFRUUHVSRQGVWRʌZKLFKPHDQVWRWDOWUDQVIHU Reference [1] J. B. Kim, J. Lee, A. S. Choe, and Y. Rhee, “Geometrical representation of coherent-excitation methods using delayed and detuned lasers”, Phys. Rev. A 55, pp. 3819-3825 (1997). 60 Mo-007 Atom interferometry 4XDQWXP5DPVH\LQWHUIHURPHWU\ U. Dorner 1,2 1. Centre for Quantum Technologies, National University of Singapore, 3 Science Drive 2, Singapore 117543 2. Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, UK [email protected] The measurement of atomic transition frequencies with Ramsey interferometry has been established as an im- portant tool, not only for general spectroscopic purposes but also to determine frequency standards on which atomic clocks are based on. Improvements of Ramsey interferometry via quantum effects are therefore highly desirable. Here we present methods for quantum enhanced Ramsey-type interferometry