ライフサイエンスコーパス: optical lattice

1 mmetry based on Bose condensates in a shaken optical lattice.

2 5 by 5 three-dimensional array created by an optical lattice.

3 s for bosons in a two-dimensional disordered optical lattice.

4 idium molecules (KRb) in a three-dimensional optical lattice.

5 in condensate in a shallow three-dimensional optical lattice.

6 an s-wave interacting atomic Fermi gas in an optical lattice.

7 ors in a system with cold atomic gases in an optical lattice.

8 berg states of an ultracold atomic gas in an optical lattice.

9 rring ultracold atoms between orbitals in an optical lattice.

10 lity on individual sites of a Hubbard-regime optical lattice.

11 e transport of ultracold atoms trapped in an optical lattice.

12 ry of a binary bosonic mixture trapped in an optical lattice.

13 nt among an ensemble of atoms confined in an optical lattice.

14 uilt on a tunable robust system, a cold atom optical lattice.

15 e-Einstein condensate in a three-dimensional optical lattice.

16 ynamically reconfigurable, three-dimensional optical lattice.

17 g the complex dynamics of atomic mixtures in optical lattices.

18 Einstein condensate into periodically driven optical lattices.

19 ngly correlated Bloch oscillations in tilted optical lattices.

20 uperfluid with staggered orbital currents in optical lattices.

21 ip design offers a simple way to form stable optical lattices.

22 iticality with two-dimensional Bose gases in optical lattices.

23 We simultaneously load into the optical lattice a Mott insulator of bosonic Rb atoms and

24 lations in a two-dimensional, Hubbard-regime optical lattice and demonstrate the ability to measure t

25 ng fermions in a one-dimensional quasirandom optical lattice and identified the MBL transition throug

26 erences, even for molecules pinned in a deep optical lattice and should be observable in current expe

27 ective spin-1/2 bosons into a spin-dependent optical lattice and use the lattice to separately contro

28 e Majorana modes at edge dislocations in the optical lattice, and we provide an experimentally feasib

29 ed for photons in waveguide arrays, atoms in optical lattices, and through accidental degeneracy.

30 Here, we show that optical-lattice-based experiments can be tailored to dir

31 g ladder derived from the above experimental optical lattice by dimension reduction.

32 onic and fermionic atoms in a Hubbard-regime optical lattice can be used for quantum simulations of s

33 Such strongly interacting fermions in an optical lattice can be used to study a new class of hami

34 g and demonstrate that the DM interaction in optical lattices can be made extremely strong with reali

35 Spin-orbit coupling in optical lattices can give rise to the Dzyaloshinskii-Mor

36 demonstrate that microscopy of cold atoms in optical lattices can help us to understand the low-tempe

37 Unlike a simple 1D optical lattice case, T c in the mixed dimensions has a

38 evaluate the uncertainty of a strontium (Sr) optical lattice clock at the 1 x 10(-16) fractional leve

39 Our (87)Sr optical lattice clock now achieves fractional stability

40 we report on an atom source for a strontium optical lattice clock which circumvents these limitation

41 ered to occur naturally in a one-dimensional optical lattice clock.

42 tion environment, we improve the accuracy of optical lattice clocks by a factor of 22.

43 The increasing performance of optical lattice clocks has made them attractive for scie

44 Strontium optical lattice clocks have the potential to simultaneou

45 sults lay the groundwork for using fermionic optical lattice clocks to probe new phases of matter.

46 Optical lattice clocks with extremely stable frequency a

47 escribe the development and operation of two optical lattice clocks, both using spin-polarized, ultra

48 stability and accuracy is currently held by optical lattice clocks.

49 of highly coherent and precisely controlled optical lattice clocks.

50 Weakly repulsive fermions in an optical lattice could undergo d-wave pairing at low temp

51 antum simulation using ultracold fermions in optical lattices could help to answer open questions abo

52 Optical lattices filled with a two-spin-component Fermi

53 The power of optical lattices for quantum simulation and computation

54 nts with fermions and bosonic bound pairs in optical lattices have been reported but have not yet add

55 Ultracold atoms in optical lattices have great potential to contribute to a

56 Recent experiments on ultracold atoms in optical lattices have synthesized a variety of tunable b

57 of fermionic atom pairs is released from an optical lattice, implying long-range order (a property o

58 trip geometry, consisting of the sites of an optical lattice in the long direction and of three inter

59 th Rubidium and Caesium atoms in a bipartite optical lattice involving laser-dressed Rydberg-Rydberg

60 s including ultracold atoms and molecules in optical lattices, Josephson junction arrays, and certain

61 interferometer for a graphene-type hexagonal optical lattice loaded with bosonic atoms.

62 antum matter, such as the recent double-well optical lattices loaded with s and p orbital ultracold a

63 Here we use an optical lattice of double-well potentials to isolate and

64 Ultracold atoms in optical lattices offer a unique platform for investigati

65 Quantum gases in optical lattices offer an opportunity to experimentally

66 using ions in a linear rf-trap, atoms in an optical lattice or quantum dots in a cavity.

67 robing anisotropic systems, such as atoms in optical lattice potentials.

68 essed atomic fermions in a three-dimensional optical lattice predicting the existence of hitherto unh

69 Polar molecules in an optical lattice provide a versatile platform to study qu

70 d the difficulty of applying stable rotating optical lattices, rotational approaches are not able to

71 quantum-degenerate Fermi gases and ultracold optical lattice simulations of condensed-matter phenomen

72 h these low temperatures using a compensated optical lattice technique, in which the confinement of e

73 The atoms are trapped in a two-dimensional optical lattice that enables cycles of compression to in

74 ultrathin light sheets from two-dimensional optical lattices that allowed us to image three-dimensio

75 nstrating a route to quantum magnetism in an optical lattice, this work should facilitate further inv

76 nerate Fermi gas in a three-dimensional (3D) optical lattice to guard against on-site interaction shi

77 rystal fibre are transversely confined by an optical lattice to prevent atoms from interacting with t

78 olar molecules pinned in a three-dimensional optical lattice to realize a lattice spin model.

79 te Bose gas of rubidium atoms confined in an optical lattice to simulate a chain of interacting quant

80 derable interest in using atomic fermions in optical lattices to emulate the mathematical models that

81 onstrate ponderomotive spectroscopy by using optical-lattice-trapped Rydberg atoms, pulsating the lat

82 In analogy with optical lattices used in ultra-cold atom physics, such m

83 lator phase transition of ultracold atoms in optical lattices was an enabling discovery in experiment

84 Using interacting bosonic atoms in an optical lattice, we directly observed fundamental effect

85 tion measurements of cold trapped ions in an optical lattice, we observed a finite version of the Aub

86 gas of rubidium atoms loaded in a honeycomb optical lattice, we realize strong-force dynamics in Blo

87 solved control of ultracold bosonic atoms in optical lattices, we prepare two identical copies of a m

88 ponent is confined on a one-dimensional (1D) optical lattice whereas the other is in a homogeneous 3D

89 astly higher temperatures than achievable in optical lattices with cold atoms.