ultracold-atoms

Layer 1 — Physics24 concepts in this subtree

Physics of dilute neutral-atom gases in the nK-μK temperature regime. Laser-cooling (Hansch-Schawlow 1975 proposal, Chu-Cohen-Tannoudji-Phillips 1997 Nobel) down to the Doppler limit T_D = ℏΓ/(2 k_B); sub-Doppler (Sisyphus,…

BEC order parameter Ψ(r,t): macroscopic occupation of the ground state
Doppler cooling limit: T_D = ℏΓ/(2 k_B) (Hansch-Schawlow 1975)
Forced evaporative cooling: truncate the Boltzmann tail to cool the remainder
BEC critical temperature: k_B T_c = (2πℏ²/m) · (n/ζ(3/2))^(2/3)
GP healing length: ξ = 1/√(8π n a_s) (kinetic ≡ interaction)
Feshbach resonance: a(B) = a_bg(1 − Δ/(B − B_0)) — tunable interactions
Thomas–Fermi approximation for trapped BEC: kinetic term dropped, μ = V(r) + g·n(r)
Polylog / Riemann-zeta Bose–Einstein integrals: g_ν(z) = Li_ν(z); g_ν(1) = ζ(ν)
Bose-Hubbard in optical lattice: H = -J·Σ b†b + (U/2)·Σ n(n-1) in tensor-product site basis
Thomas–Fermi radius for trapped BEC: R_TF = sqrt(2μ/(m·ω²))
BEC condensate fraction: N₀/N = 1 − (T/Tc)^(3/2); k_B·Tc = 2π·ℏ²·n^(2/3)/(m·ζ(3/2)^(2/3))
Bose-Hubbard MI-SF critical ratio (strong-coupling): (U/J)_c = 2·√(2·n·(n+1)) at integer filling n
Cohen-Tannoudji sub-Doppler cooling
BEC (Anderson 1995)
Optical lattice (Jaksch 1998)
Feshbach tunable
Rydberg arrays (Saffman 2010)
Dipolar droplets (Kadau 2016)
BEC (Cornell-Wieman-Ketterle 1995)
Doppler cooling (Hänsch-Schawlow 1975)
MOT trap (Phillips-Chu Nobel 1997)
Hubbard lattice (Jaksch-Zoller 1998)
Feshbach (Inouye 1998)
Synthetic gauge (Lin 2009)
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