Departament de Fìsica i Enginyeria Nuclear, Campus Nord B4-B5, Universitat Politècnica de Catalunya, Barcelona, Spain Dipolar and Coulomb one-dimensional gases G.E. Astrakharchik Summer school, Trier, August 16 (2012) CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations OVERVIEW: SHORT-RANGE INTERACTION IN 1D • Short-range interaction can be modeled by a δ-function interaction potential (Lieb-Liniger model) • high density (small γ) – mean-field regime, properties are described by Gross-Pitaevskii equation • low density (large γ) – Tonks-Girardeau regime, diagonal properties and energy same as in ideal Fermi gas • low density (large and negative γ) – super-Tonks-Girardeau regime, properties of in the gas-like metastable state are similar to that of a gas of hard-rods • is it possible to realize a stable gas in super-Tonks-Girardeau regime with long-range potentials? CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations DIPOLE-DIPOLE INTERACTION MODEL HAMILTONIAN CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations ARE DIPOLAR INTERACTIONS LONG RANGE? DESCRIBE DIPOLAR INTERACTIONS AS δ-POTENTIAL MONTE CARLO METHODS CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations E/N GROUND STATE ENERGY 10 6 10 5 10 4 10 3 10 2 10 1 10 0 10 -1 10 -2 10 -3 dipoles Tonks-Girardeau gas crystal -4 10 0.01 0.1 1 10 n1D r0 100 Energy per particle as a function of n1D r0 (red solid line), energy of the TonksGirardeau gas ETG (dashed line), energy of a classical crystal Ecr (dot-dashed line). A. S. Arkhipov, G. E. A., A. V. Belikov, and Yu. E. Lozovik , JETP Letters, 82, 39 (2005) CLASSICAL CRYSTAL LIMIT • In the limit of large density (n1Dr0 1) the potential energy dominates, in 2D geometry a crystal gets formed • Phonons in one-dimensional geometry destroy crystalline order • Still the energy can be calculated assuming a crystalline order ECC 2 (3) 2 ( nr0 )3 N mr0 i.e. energy of corresponding classical crystal - is cubic in the density. E/N Energy per particle 10 6 10 5 10 4 10 3 10 2 10 1 10 0 10 -1 10 -2 10 -3 dipoles Tonks-Girardeau gas crystal -4 10 0.01 0.1 1 10 n1D r0 100 GENERIC BOSE-FERMI MAPPING Following quantities are known exactly: 1) Energy per particle: ETG 2 2n 2 N 6m i.e. energy of corresponding fermi gas - is quadratic in the density. E/N TONKS-GIRARDEAU LIMIT 10 6 10 5 10 4 10 3 10 2 10 1 10 0 10 -1 10 -2 10 -3 dipoles Tonks-Girardeau gas crystal -4 10 0.01 0.1 1 10 n1D r0 100 TONKS-GIRARDEAU LIMIT II 2) Pair distribution function (gives the possibility to find a particle at a distance x from another particle) In the Tonks-Girardeau regime is the same as in the corresponding Fermi system and experience Friedel-like oscillations: 3) Static structure factor (correlation function of the momentum distribution between elements –k and k) In the Tonks-Girardeau regime is the same | k | /(2n ), | k | 2n as in the corresponding fermi system, is S ( k ) | k | 2n 1, linear up to 2kf, with kf = π n being the fermi momentum. CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations PAIR DISTRIBUTION FUNCTION 2 n1Dr0 = 0.01 n1Dr0 = 0.1 n1Dr0 = 1 g2(x) n1Dr0 = 10 1 0 0 1 2 n1D x 3 Pair distribution function g2 (z) obtained from a DMC calculation for densities n r0 =10-2; 0.1; 1; 10 (larger amplitude of oscillations correspond to higher peaks) PAIR DISTRIBUTION FUNCTION 2 n1Dr0 = 0.01 n1Dr0 = 1 n1Dr0 = 0.1 n1Dr0 = 10 g2(x) 1 0 0 1 2 3 4 5 6 7 8 9 10 n1D x Pair distribution function g2 (z) obtained from a DMC calculation for densities n r0 =10-2; 0.1; 1; 10 (larger amplitude of oscillations correspond to higher peaks) CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations LUTTINGER LIQUID LUTTINGER PARAMETER STATIC STRUCTURE FACTOR 3 2 n1Dr0 = 0 (TG gas) Sk 2 n1Dr0 = 0.1 2 2 n1Dr0 = 1 1 0 0 5 10 k / n1D 15 Static structure factor S(k) obtained from a DMC. A higher peak corresponds to a higher density. The red line corresponds to the static structure factor S(k) in the Tonks-Girardeau regime. LUTTINGER PARAMETER IN 1D DIPOLAR GAS Luttinger exponent K. Classical crystal and Tonks-Girardeau limits are shown with dashed lines. Inset: small-momentum part of the static structure factor. Fig. from R. Citro, E. Orignac, S. De Palo, M.-L. Chiofalo PRA 75, 051602 (2007) LUTTINGER PARAMETER IN LIEB-LINIGER GAS Luttinger exponent K versus γ. The dashed lines are the small γ approximations obtained from Bogoliubov theory whereas the dotted-dashed lines correspond to the asymptotic expressions for large γ. Fig. from M. A. Cazalilla J. Phys. B 37, S1 (2004) STATIC STRUCTURE FACTOR Static structure factor S(k) for obtained in Reptation Quantum Monte Carlo calculation with N=40 particles and different values of n1D r0 =0.01; 50; 100; 1000 . Decreasing slopes for small momentum and the emergence of additional peaks correspond increasing n1D r0. Fig. from R. Citro, et al. PRA 75, 051602 (2007) FREQUENCIES OF COLLECTIVE OSCILLATIONS Square of the breathing mode frequency ω2 (in units of trap frequency) as a function of characteristic parameter N r02/ az2. The external potential is taken to be harmonic: Vext 1m z2 zi2 COMPARISON WITH SHORT-RANGE POTENTIAL We make comparison of the properties of a long-range dipole potential with the properties of a short-range potential Vint (z) = g1Dδ(z) , where the coupling constant is related to 1D scattering length g1D = -22 /(m a1D2). Properties of the system are governed by a one-dimensional gas parameter na1D. Two situations should be considered separately: 1) Repulsive interaction (Lieb-Liniger gas): - coupling constant g1D>0 - s-wave scattering length a1D<0 The gas state is always stable. 2) Attractive interaction - coupling constant g1D - - s-wave scattering length a1D +0 The ground state has large negative energy and corresponds to solitonlike solution. The gas like state is stable in the regime of small densities n a1D <0.3 (Super-Tonks gas) and has analogies with a gas of hard-rods GROUND STATE ENERGY: COMPARISON Energy in units of ћ2/mr02 (or ћ2/ma1D2). Solid lines- green: system of dipoles, blue: Lieb-Liniger gas, red:Super-Tonks gas. Dashed lines- green ~n1,dark green: ~n2, blue: ~n3.At small n LL and ST energy correction to TG gas has same absolute value CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations 6 4 0 MF -GP a1D 2 resonance TG, g1D /(aoscosc); a1D / aosc 8 g1D + sTG GAS OF DIPOLES: IDEA g1D -2 sTG, ne collapse / solito g 1D - -4 -6 -3 -2 -1 0 1 2 3 a3D / aosc 0.4 (x) Repulsion, g1D > 0 Attraction, g1D < 0 0.3 0.2 0.1 0.0 -0.1 -10 x, [a.u.] a1D < 0 a1D > 0 -5 0 5 10 sTG GAS OF DIPOLES: WAVE FUNCTION 3 Repulsion, +1/|x| 0.003 (x) 0.002 0.001 x, [a.u.] 0.000 0.0 0.1 0.2 3 Attraction, -2/|x| 0.10 (x) 0.05 0.00 -0.05 x, [a.u.] -0.10 0.0 0.1 0.2 STABILITY OF DIPOLAR sTG GAS 0.05 E/N 0.04 Tonks-Girardeau gas repulsive dipoles attractive dipoles fit 0.03 0.02 0.01 0.00 0.0 0.1 0.2 n1D r0 0.3 CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations COULOMB INTERACTION POTENTIAL CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations FERMIONS: SIGN PROBLEM MODEL HAMILTONIAN ONE COMPONENT SYSTEM:IDEAL FERMI GAS CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations GROUND STATE ENERGY 4 10 E/N 3 10 DMC IFG / TG E/N = n /6m Wigner cr. E/N = e n ln N 2 2 2 2 2 10 N = 1000 N = 100 N = 10 1 10 0 10 -1 10 -2 10 -3 10 -3 10 -2 10 -1 10 0 10 1 10 2 n a0 10 ONE COMPONENT SYSTEM:WIGNER CRYSTAL CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations PLASMON DISPERSION RELATION STATIC STRUCTURE FACTOR 2 10 Monte Carlo phonons, ~ |k| 1/2 plasmons, ~ (3-2 ln |k|) |k| harmonic theory (upper bound) S(k) 1 10 0 10 -1 10 -2 10 -3 10 0.1 1 10 k/n LUTTINGER LIQUID PAIR DISTRIBUTION FUNCTION g2(z) DMC bosonization 1/2 amplitude: 1 A1exp{-4 c2 ln z} 2 1 0 0 5 10 z / ao 15 CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations MOMENTUM DISTRIBUTION 10 na=1 fermions bosons n(k) 5 -6 -3 0 3 k/n 6 MOMENTUM DISTRIBUTION 1.5 n a = 0.1 fermions bosons IFG n(k) 1.0 0.5 0.0 -6 -3 0 3 k/n 6 CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations TRAPPED SYSTEM TRAPPED IDEAL FERMI / TONKS-GIRARDEAU GAS 1.5 n(x) 1.0 0.5 0.0 -5 -4 -3 -2 -1 0 1 2 3 4 x / aho 5 CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations LOCAL DENSITY APPROXIMATION LDA: POLYTROPIC EoS LDA vs EXACT PROFILE or GPE 1.5 n(x) 1.0 0.5 0.0 -6 -5 -4 -3 -2 -1 0 1 2 3 4 5 x / aho 6 LDA: IFG / TG GAS / LIMIT OF SMALL CHARGE LDA: LIMIT OF LARGE CHARGE ENERGY OF A TRAPPED COULOMB GAS 4 10 Wigner crystal, 2 2/3 E/N = 3/10 (3q N ln N) E/N 3 10 IFG / TG, E/N = N/2 2 10 N=5 N = 10 N = 100 1 10 0 10 -2 10 -1 10 0 10 1 10 2 q 10 DENSITY PROFILE: q=0.1 0.15 n(r) charge q = 0.1 LDA, IFG/TG LDA, Wigner cr. 0.10 0.05 0.00 -10 -5 0 5 r / aho 10 DENSITY PROFILE: q=0.316 0.15 n(r) charge q = 0.316 LDA, IFG/TG LDA, Wigner cr. 0.10 0.05 0.00 -10 -5 0 5 r / aho 10 DENSITY PROFILE: q=1 0.15 n(r) charge q = 1 LDA, IFG/TG LDA, Wigner cr. 0.10 0.05 0.00 -10 -5 0 5 r / aho 10 DENSITY PROFILE: q=3.16 0.15 n(r) charge q = 3.16 LDA, IFG/TG LDA, Wigner cr. 0.10 0.05 0.00 -10 -5 0 5 r / aho 10 DENSITY PROFILE: q=10 0.15 n(r) charge q = 10 LDA, IFG/TG LDA, Wigner cr. 0.10 0.05 0.00 -20 -15 -10 -5 0 5 10 15 r / aho 20 CONTENTS: • Dipole-dipole interactions • Are dipolar interactions long-range? • Ground-state energy: crystal, Tonks-Girardeau regimes • Correlation functions • Luttinger liquid • Attractive dipoles: dipolar analog of sTG gas • Coulomb gas • Fermionic sign problem • Energy • Excitation spectrum: plasmons • Momentum distribution: bosons vs fermions • Trapped gases • Local density approximation • Frequency of collective oscillations FREQUENCIES OF COLLECTIVE OSCILLATIONS Square of the breathing mode frequency ω2 (in units of trap frequency) as a function of characteristic parameter N r02/ az2 (or N a1D2/ az2). CONCLUSIONS 1/4 CONCLUSIONS 2/4 CONCLUSIONS 3/4 CONCLUSIONS 4/4 DANKE SCHÖN FÜR IHRE AUFMERKSAMKEIT!