ライフサイエンスコーパス: optical lattice

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

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

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

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

5 ynamically reconfigurable, three-dimensional optical lattice.

6 ic atoms in a multiorbital three-dimensional optical lattice.

7 alize a FQH state with ultracold atoms in an optical lattice.

8 7)Rb molecules confined in a two-dimensional optical lattice.

9 (13,14) in a two-dimensional, tunnel-coupled optical lattice.

10 n polaritons (MPPs) to form a sub-wavelength optical lattice.

11 superfluidity of spin-polarized fermions in optical lattice.

12 s in a gas of ultracold rubidium atoms in an optical lattice.

13 erates entirely within the Bloch bands of an optical lattice.

14 les confined to two-dimensional planes in an optical lattice.

15 the scalable, homogeneous environment of an optical lattice.

16 Einstein condensate held in a time-modulated optical lattice.

17 strongly correlated ultracold fermions in an optical lattice.

18 cting ultracold bosonic gas confined in a 2D optical lattice.

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

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

21 5 by 5 three-dimensional array created by an optical lattice.

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

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

24 two-dimensional square array of atoms in an optical lattice.

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

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

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

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

29 rring ultracold atoms between orbitals in an optical lattice.

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

31 stein condensates loaded into spin-dependent optical lattices.

32 x dynamics with fermionic ultracold atoms in optical lattices.

33 in the quantum material cobalt niobate or in optical lattices.

34 h ultracold molecules both in bulk gases and optical lattices.

35 nded edge modes of topologically non-trivial optical lattices.

36 in ultracold atoms with highly controllable optical lattices.

37 nipulated using the surface-wave analogue of optical lattices.

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

39 Einstein condensate into periodically driven optical lattices.

40 ngly correlated Bloch oscillations in tilted optical lattices.

41 uperfluid with staggered orbital currents in optical lattices.

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

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

44 ystal phases(15) and dipolar spin liquids in optical lattices(16).

45 ctional quantum Hall liquids(1), to atoms in optical lattices(2) and twisted bilayer graphene(3).

46 0(-18) or better using ensembles of atoms in optical lattices(2,3) or individual ions in radio-freque

47 in an eight-fold symmetric quasicrystalline optical lattice(5).

48 trongly interacting fermions in a triangular optical lattice(5,6).

49 including photonics(2-5), ultracold atoms in optical lattices(6-8) and others(9-12).

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

51 em: ultracold lithium-6 in a two-dimensional optical lattice, a testing ground for strong interaction

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

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

54 chromium atoms pinned in a three dimensional optical lattice and prepared in a pure coherent spin sta

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

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

57 pin the molecules in a deep two-dimensional optical lattice and, following dissociation, collect flu

58 ale architectures such as photonic cavities, optical lattices and qubits, and provide perspectives fo

59 orming quantum simulation and computation in optical lattices and tweezers.

60 nd examples have been found more recently in optical lattices and two-dimensional materials(4-9).

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

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

63 Polar molecules confined in an optical lattice are a versatile platform to explore spin

64 potentials: unlike real solids, traditional optical lattices are silent because they are infinitely

65 tanglement of pairs of fermionic atoms in an optical lattice array.

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

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

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

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

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

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

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

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

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

75 An optical lattice clock based on partially delocalized Wan

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

77 the groundwork for using a three-dimensional optical lattice clock to probe quantum magnetism and spi

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

79 r realizing a compact, robust, transportable optical lattice clock with systematic uncertainty at the

80 we implement a 'multiplexed' one-dimensional optical lattice clock, in which spatially resolved stron

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

82 y on its intended application as a strontium optical lattice clock.

83 Optical lattice clocks are at the forefront of precision

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

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

86 Strontium optical lattice clocks have the potential to simultaneou

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

88 Optical lattice clocks with extremely stable frequency a

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

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

91 of highly coherent and precisely controlled optical lattice clocks.

92 The stability of optical-lattice clocks (OLCs) is limited both by the int

93 we use an external electric field along with optical lattice confinement to create a two-dimensional

94 ing, using ultracold fermions in anisotropic optical lattices continuously tunable from a square to a

95 Our approach utilizes a series of two optical lattice conveyor belts to transport atom reservo

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

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

98 ow-entropy states with controlled filling in optical-lattice experiments.

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

100 The power of optical lattices for quantum simulation and computation

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

102 Ultracold atoms in optical lattices have been used to indirectly characteri

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

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

105 na consistent with bad-metal behaviour in an optical-lattice Hubbard model by measuring the transport

106 We demonstrate how different optical lattice illumination patterns can be tuned to pr

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

108 Light sheets based on dithered optical lattices improve axial resolution and beam unifo

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

110 ntium atom ensembles are trapped in the same optical lattice, interrogated simultaneously by a shared

111 Ultracold atoms are delivered from a moving optical lattice into the PCW.

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

113 g resolution of many-body quantum systems in optical lattices is routinely achieved with quantum-gas

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

115 Two-photon- and adaptive optical lattice light-sheet microscope-based time-lapse

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

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

118 s(4-6), the accessible temperatures in these optical lattice material analogues are still too high to

119 rometers with atoms suspended for 70 s in an optical-lattice mode filtered by an optical cavity have

120 However, the optical lattice must balance Earth's gravity by applying

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

122 e system, or interference techniques such as optical lattices of cold atoms.

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

124 Quantum gases in optical lattices offer an opportunity to experimentally

125 Ultracold fermionic atoms in optical lattices offer pristine realizations of Hubbard

126 zed using long-range dipolar interactions in optical lattices, opening the door to quantum simulation

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

128 na in periodically modulated atomic gases in optical lattices or light-driven materials.

129 is created by simultaneous modulations of an optical lattice potential and interatomic interactions,

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

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

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

133 Optical-lattice realizations of crystals therefore lack

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

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

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

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

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

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

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

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

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

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

144 te Fermi gas loaded into a three-dimensional optical lattice to study the effect of a tunable Fermi-H

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

146 th that of leading atomic systems, which use optical lattices to interrogate many thousands of atoms

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

148 of cold atoms into cavity-enhanced 1D and 2D optical lattice traps, all within a single compact assem

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

150 e discuss the feasibility of measurements in optical lattices using current techniques.

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

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

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

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

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

156 hange statistics using ultracold atoms in an optical lattice, where we engineer the statistical phase

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

158 etry breaking in the second Bloch band of an optical lattice with hexagonal boron nitride geometry.

159 Here, we create an optical lattice with phonon modes using a Bose-Einstein

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

161 for ultracold fermions in spin-orbit-coupled optical lattices with tunable dissipation, which exhibit

162 10(4) spin-polarized atoms of (87)Sr in the optical lattice within 500 ms; we observe a vacuum-limit

163 an optical conveyor belt formed by a moving optical lattice within a tweezer potential, we show that