Fetching the paper…
Reading the bibliography…
Artificial gauge fields open new possibilities to realize quantum many-body systems with ultracold atoms, by engineering Hamiltonians usually associated with electronic systems.
D. R. Hofstadter, Phys. Rev. B 14
1976
Earlier work this paper cites.
M. V. Berry, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences 392
1984
Earlier work this paper cites.
Y. B. Ovchinnikov et al. , Phys. Rev. Lett. 83
1999
Earlier work this paper cites.
R. Grimm, M. Weidemüller, and Y. B. Ovchinnikov, Adv. At. Mol. Opt. Phys. 42
2000
Earlier work this paper cites.
M. Cristiani et al. , Opt. Express 12
2004
Earlier work this paper cites.
M. Machholm, A. Nicolin, C. J. Pethick, and H. Smith, Phys. Rev. A 69
2004
Earlier work this paper cites.
A. Sørensen, E. Demler, and M. Lukin, Phys. Rev. Lett. 94
2005
Cited alongside, same era.
T. Fukui, Y. Hatsugai, and H. Suzuki, J. Phys. Soc. Jpn. 84
2005
Cited alongside, same era.
M. Hafezi, A. Sørensen, E. Demler, and M. Lukin, Phys. Rev. A 76
2007
Cited alongside, same era.
R. A. Williams, S. Al-Assam, and C. J. Foot, Phys. Rev. Lett. 104
2010
Cited alongside, same era.
F. Gerbier and J. Dalibard, N. J. Phys. 12
2010
Cited alongside, same era.
J. Dalibard, F. Gerbier, G. Juzeliūnas, and P. Öhberg, Rev. Mod. Phys. 83
2011
Cited alongside, same era.
Y.-J. Lin et al. , Nature 462
Cited in the paper.
D. Ciampini, O. Morsch, and E. Arimondo, Int. J. of Quant. Inf. 9
2011
Later among the works it cites.
M. Aidelsburger et al. , Phys. Rev. Lett. 107
2011
Later among the works it cites.
Y.-J. Lin et al. , Nature Physics 7
2011
Later among the works it cites.
N. R. Cooper, Phys. Rev. Lett. 106
2011
Later among the works it cites.
S. Chen et al. , arXiv: 1201.6018v1
2012
Closest in time.
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…
In some experiments, both the trap frequencies and λ \lambda were slightly different: ( f x , f y , f z ) = ( 17.3 , 41.4 , 90 ) (f_{x},f_{y},f_{z})=(17.3,41.4,90) Hz, and λ = 790.14 \lambda=790.14 nm
Cited in the paper.
Y.-J. Lin et al. , Phys. Rev. Lett. 102
Cited in the paper.
See Supplementary Material
Cited in the paper.
The general relation between effective mass and tunneling amplitude is m / m ∗ ( k x ) = π 2 c o s ( π k x / k L − ϕ ) t / E L m/m^{*}(k_{x})=\pi^{2}\mathop{cos}\nolimits(\pi k_{x}/k_{L}-\phi)t/E_{L} . For small sloshing amplitudes Δ k x \Delta k_{x} around the minimum k x = ( ϕ / π ) k L k_{x}=(\phi/\pi)k_{L} , the effective mass is almost uniform
Cited in the paper.
We use Ω rf = Ω rf 0 + Δ Ω rf c o s ( 2 π f rf Ω z ) \Omega_{\rm rf}=\Omega_{\rm rf_{0}}+\Delta\Omega_{\rm rf}\mathop{cos}\nolimits(2\pi f_{\rm rf}\Omega_{z}) , where ℏ Ω rf 0 = 0.75 E L \hbar\Omega_{\rm rf_{0}}=0.75E_{L} , ℏ Δ Ω rf = 0.23 E L \hbar\Delta\Omega_{\rm rf}=0.23E_{L} and f rf / ℏ = 0.4 E L − 1 f_{\rm rf}/\hbar=0.4E_{L}^{-1}
Cited in the paper.