# Tilman Enss | Ruprecht-Karls-Universität Heidelberg

## Priv.-Doz. Dr. Tilman Enss

Institut für Theoretische PhysikUniversität Heidelberg

Philosophenweg 19

69120 Heidelberg

Germany

Room 006

Phone: +49 6221 54 9337

Fax: +49 6221 54 9331

Email: enss (at) thphys.uni-heidelberg.de

getting there (Google maps)

my entry in the university directory (LSF)

curriculum vitæ

## Teaching

Summer term 2016: Condensed Matter TheoryWinter term 2015/2016: Many-body physics with ultracold atoms

Summer term 2015: Condensed Matter Theory

Winter term 2014/2015: Theory of Ultracold Atoms

Summer term 2014: Condensed Matter Theory

Winter term 2013/2014: Special topics in quantum mechanics

Summer term 2013: Quantum mechanics

Winter term 2012/2013: Many-body methods in solid state physics

more on teaching

## Team members

Martin Braß (Master student)

Sergej Trenkenschu (Master student)

**Former students and team members**

Dominik Lorenz (Bachelor student, Heidelberg 2016: Quench dynamics in the
Hubbard model)

Daniel Issing (Bachelor student, Heidelberg 2015: Bethe ansatz and
quench dynamics for 1D integrable quantum systems)

Bruno Faigle-Cedzich (Bachelor student, Heidelberg 2015: Shear
viscosity of two-component Fermi gas)

## Research interests

My research focuses on many-body theory, mainly dynamics and transport in strongly correlated quantum systems, ranging from ultracold atomic gases to superconductors and quantum wires.I work on the development of several modern and advanced theoretical tools including the functional renormalization group (fRG), Hamiltonian flows, Luttinger-Ward calculations, transfer-matrix DMRG and the newly developed Lightcone RG.

- Quench dynamics in 1d chains and Many-body localization (MBL), using the Lightcone renormalization group
- Many-body dynamics and transport in interacting ultracold atomic gases
- Quantum critical behavior in disordered correlated electron systems
- Nonequilibrium dynamics and transport in quantum dots and Luttinger liquids
- Raman and optical spectroscopy in cuprates
- Functional renormalization group method (fRG)
- Aging behavior in stochastic systems without detailed balance

my articles on Google Scholar

## Funding

SFB 1225 ISOQUANT (DFG)Isolated quantum systems and universality under extreme conditions, 07/2016—06/2020

## Recent work

### Evidence for ferromagnetic instability in a repulsive Fermi gas of ultracold atoms

Ferromagnetism is among the most spectacular manifestations of interactions within many-body fermion systems. In contrast to weak-coupling phenomena, it requires strong repulsion to develop, making a quantitative description of ferromagnetic materials notoriously difficult. This is especially true for itinerant ferromagnets, where magnetic moments are not localized into a crystal lattice. In particular, it is still debated whether the simplest case envisioned by Stoner of a homogeneous Fermi gas with short-range repulsive interactions can exhibit ferromagnetism at all. In this work, we positively answer this question by studying a clean model system consisting of a binary spin-mixture of ultracold Li6 atoms, whose repulsive interaction is tuned via a Feshbach resonance...G. Valtolina, F. Scazza, A. Amico, A. Burchianti, A. Recati, T. Enss, M. Inguscio, M. Zaccanti, and G. Roati,

arXiv:1605.07850.

### Equation of state of ultracold fermions in
the 2D BEC-BCS crossover region

*PRL Editors' suggestion*

*Viewpoint in Physics:
Journey from Classical to Quantum in Two Dimensions, by Meera
M. Parish*

We report the experimental measurement of the equation of state of a two-dimensional Fermi gas with attractive s-wave interactions throughout the crossover from a weakly coupled Fermi gas to a Bose gas of tightly bound dimers as the interaction strength is varied. We demonstrate that interactions lead to a renormalization of the density of the Fermi gas by several orders of magnitude. We compare our data near the ground state and at finite temperature with predictions for both fermions and bosons from quantum Monte Carlo simulations and Luttinger-Ward theory. Our results serve as input for investigations of close-to-equilibrium dynamics and transport in the two-dimensional system.Boettcher, L. Bayha, D. Kedar, P. A. Murthy, M. Neidig, M. G. Ries, A. N. Wenz, G. Zürn, S. Jochim, and T. Enss,

Phys. Rev. Lett.

**116**, 045303 (2016).

Viewpoint in Physics: Journey from Classical to Quantum in Two Dimensions, by Meera M. Parish.

*Ultrakalte Atome in zwei Dimensionen*(popular article in German, Phys. Unserer Zeit

**47**, 113 (2016)).

slides of talk in Budapest, 2015.

### Nonlinear spin diffusion and spin rotation in a trapped Fermi gas

Transverse spin diffusion in a polarized, interacting Fermi gas leads to the Leggett-Rice effect, where the spin current precesses around the local magnetization. With a spin-echo sequence both the transverse diffusivity and the spin-rotation parameter γ are obtained; the sign of γ reveals the repulsive or attractive character of the effective interaction. In a trapped Fermi gas the spin diffusion equations become nonlinear, and their numerical solution exhibits an inhomogeneous spin state even at the spin echo time. While the microscopic diffusivity and γ increase at weak coupling, their apparent values inferred from the trap-averaged magnetization saturate in agreement with a recent experiment for a dilute ultracold Fermi gas.Tilman Enss, Phys. Rev. A

**91**, 023614 (2015).

### Observation of the Leggett-Rice effect in a unitary Fermi
gas

*PRL Editors' suggestion*

We observe that the diffusive spin current in a strongly interacting degenerate Fermi gas of 40K precesses about the local magnetization. As predicted by Leggett and Rice, precession is observed both in the Ramsey phase of a spin-echo sequence, and in the nonlinearity of the magnetization decay. At unitarity, we measure a Leggett-Rice parameter γ=1.08(9) and a bare transverse spin diffusivity D_{0}

^{⊥}=2.3(4)ℏ/m for a normal-state gas initialized with full polarization and at one fifth of the Fermi temperature, where m is the atomic mass. For a unitary gas, γ→0 as temperature is increased to the Fermi temperature. Tuning the scattering length a, we find that a sign change in γ occurs in the range 0<(kFa)

^{-1}≤1.3, where kF is the Fermi momentum. We discuss how γ reveals the effective interaction strength of the gas, such that a change in γ indicates a switching of branch, between a repulsive and an attractive Fermi gas.

S. Trotzky, S. Beattie, C. Luciuk, S. Smale, A. B. Bardon, T. Enss, E. Taylor, S. Zhang, and J. H. Thywissen,

Phys. Rev. Lett.

**114**, 015301 (2015).

### Purification and many-body localization in cold atomic gases

We propose to observe many-body localization in cold atomic gases by realizing a Bose-Hubbard chain with binary disorder and studying its non-equilibrium dynamics. In particular, we show that measuring the difference in occupation between even and odd sites, starting from a prepared density-wave state, provides clear signatures of localization. As hallmarks of the many-body localized phase we confirm, furthermore, a logarithmic increase of the entanglement entropy in time and Poissonian level statistics. Our numerical density-matrix renormalization group calculations for infinite system size are based on a purification approach which allows to perform the disorder average exactly, thus producing data without any statistical noise, and with maximal simulation times of up to a factor 10 longer than in the clean case.Felix Andraschko, Tilman Enss, and Jesko Sirker, Phys. Rev. Lett.

**113**, 217201 (2014).

### Universal equation of state and pseudogap in the two-dimensional Fermi gas

We determine the thermodynamic properties and the spectral function for a homogeneous two- dimensional Fermi gas in the normal state using the Luttinger-Ward, or self-consistent T-matrix, approach. The density equation of state deviates strongly from that of the ideal Fermi gas even for moderate interactions, and our calculations suggest that temperature has a pronounced effect on the pressure in the crossover from weak to strong coupling, consistent with recent experiments. We also compute the superfluid transition temperature for a finite system in the crossover region. There is a pronounced pseudogap regime above the transition temperature: the spectral function shows a Bogoliubov-like dispersion with backbending, and the density of states is significantly suppressed near the chemical potential. The contact density at low temperatures increases with interaction and compares well with both experiment and zero-temperature Monte Carlo results.Marianne Bauer, Meera M. Parish, and Tilman Enss, Phys. Rev. Lett.

**112**, 135302 (2014).

### Viewpoint: Crossing a Quantum Fluid Divide

Ultracold atoms provide a platform for studying the transition between bosonic and fermionic superfluidity in 2D quantum fluids.Tilman Enss, Physics

**7**, 9 (2014).

### Damping of the quadrupole mode in a two-dimensional Fermi gas

In a recent experiment [E. Vogt et al., Phys. Rev. Lett. 108, 070404 (2012)], quadrupole and breathing modes of a two-dimensional Fermi gas were studied. We model these collective modes by solving the Boltzmann equation via the method of phase-space moments up to fourth order, including in-medium effects on the scattering cross section. In our analysis, we use a realistic Gaussian potential deformed by the presence of gravity and magnetic field gradients. We conclude that the origin of the experimentally observed damping of the quadrupole mode, especially in the weakly interacting (or even non-interacting) case, cannot be explained by these mechanisms.Silvia Chiacchiera, Dany Davesne, Tilman Enss, and Michael Urban, Phys. Rev. A

**88**, 053616 (2013).

M. Urban, S. Chiacchiera, D. Davesne, T. Enss, and P.-A. Pantel, J. Phys.: Conf. Ser.

**497**, 012028 (2014).

### Transverse spin diffusion in strongly interacting Fermi gases

We compute spin diffusion in a dilute Fermi gas at arbitrary temperature, polarization and strong interaction in the normal phase. While the longitudinal spin diffusivity depends weakly on polarization and diverges for small temperatures, the transverse spin diffusivity D_{⊥}has a strong polarization dependence and approaches a finite value for T→0 in the Fermi liquid phase. For a 3D unitary Fermi gas at infinite scattering length the diffusivities reach a minimum near the quantum limit of diffusion ℏ/m in the quantum degenerate regime and are strongly suppressed by medium scattering, and we discuss the importance of the spin-rotation effect. In two dimensions, D

_{⊥}attains a minimum at strong coupling -1 ≤ ln(k

_{F}a

_{2D}) ≤ 1 and reaches D

_{⊥}~ 0.2...0.3 ℏ/m at large polarization. These values are consistent with recent measurements of two-dimensional ultracold atomic gases in the strong coupling regime...

Tilman Enss, Phys. Rev. A

**88**, 033630 (2013).

slides of talk at conference "Cold Atoms and beyond", Aarhus 2014

slides of talk at conference "Recent Progress in Many-Body Theories", Rostock 2013

### Quantum mechanical limitations to spin diffusion in the unitary Fermi gas

We compute spin transport in the unitary Fermi gas using the strong-coupling Luttinger-Ward theory. In the quantum degenerate regime the spin diffusivity attains a minimum value of*D*approaching the quantum limit of diffusion for a particle of mass

_{s}~ 1.3 ℏ/m*m*. Conversely, the spin drag rate reaches a maximum value of

*Γ*in terms of the Fermi temperature

_{sd}~ 1.2 k_{B}T_{F}/ℏ*T*...

_{F}Tilman Enss and Rudolf Haussmann, Phys. Rev. Lett.

**109**, 195303 (2012).

slides of talk at TU Darmstadt

slides of talk at Delta 2013 workshop

### Shear viscosity and spin diffusion in a two-dimensional Fermi gas

We investigate the temperature dependence of the shear viscosity and spin diffusion in a two-dimensional Fermi gas with contact interactions, as realized in ultra-cold atomic gases. We describe the transport coefficients in terms of a Boltzmann equation and present a full numerical solution for the degenerate gas. In contrast to previous works we take the medium effects due to finite density fully into account. This effect reduces the viscosity to entropy ratio, η/s, by a factor of three, and similarly for spin diffusion.Tilman Enss, Carolin Küppersbusch, and Lars Fritz, Phys. Rev. A

**86**, 013617 (2012).

### Quantum critical transport in the unitary Fermi gas

The thermodynamic and transport properties of the unitary Fermi gas at finite temperature T are governed by a quantum critical point at T=0 and zero density. We compute the universal shear viscosity to entropy ratio η/s in the high-temperature quantum critical regime T≫|μ| and find that this strongly coupled quantum fluid comes close to perfect fluidity η/s=ℏ/4π*k*

_{B}. Using a controlled large-N expansion we show that already at the first non-trivial order the equation of state and the Tan contact density C agree well with the most recent experimental measurements and theoretical Luttinger-Ward and Bold Diagrammatic Monte Carlo calculations.

Tilman Enss, Phys. Rev. A

**86**, 013616 (2012).

slides of talk at ERG 2012 conference

### Fermi polarons in two dimensions

We theoretically analyze inverse radiofrequency (rf) spectroscopy experiments in two-component Fermi gases. We consider a small number of impurity atoms interacting strongly with a bath of majority atoms. In two-dimensional geometries we find that the main features of the rf spectrum correspond to an attractive polaron and a metastable repulsive polaron. Our results suggest that the attractive polaron has been observed in a recent experiment [Phys. Rev. Lett. 106, 105301 (2011)].Richard Schmidt, Tilman Enss, Ville Pietilä, and Eugene Demler, Phys. Rev. A

**85**, 021602(R) (2012).

### Lightcone renormalization and quantum quenches in one-dimensional Hubbard models

The Lieb-Robinson bound implies that the unitary time evolution of an operator can be restricted to an effective light cone for any Hamiltonian with short-range interactions. Here we present a very efficient renormalization group algorithm based on this light cone structure to study the time evolution of prepared initial states in the thermodynamic limit in one-dimensional quantum systems...Tilman Enss and Jesko Sirker, New J. Phys.

**14**, 023008 (2012).

Light cone renormalization group (LCRG) source code

Movie of impurity dynamics

### Excitation spectra and rf-response near the polaron-to-molecule transition from the functional renormalization group

A light impurity in a Fermi sea undergoes a transition from a polaron to a molecule for increasing interaction. We develop a new method to compute the spectral functions of the polaron and molecule in a unified framework based on the functional renormalization group with full self-energy feedback. We discuss the energy spectra and decay widths of the attractive and repulsive polaron branches as well as the molecular bound state and confirm the scaling of the excited state decay rate near the transition. The quasi-particle weight of the polaron shifts from the attractive to the repulsive branch across the transition, while the molecular bound state has a very small residue characteristic for a composite particle. We propose an experimental procedure to measure the repulsive branch in a Li6 Fermi gas using rf-spectroscopy and calculate the corresponding spectra.Richard Schmidt and Tilman Enss, Phys. Rev. A

**83**, 063620 (2011).

slides of talk at ERG 2014 conference

### Viscosity and Scale Invariance of the Unitary Fermi Gas

The unitary Fermi gas, a scale invariant quantum fluid, appears to be the most perfect non-relativistic fluid that exists in nature: the ratio between its shear viscosity and the entropy density exhibits a minimum near the superfluid transition temperature, whose value is larger than the string theory bound ℏ/4π*k*

_{B}by a factor of about seven.

Tilman Enss, Rudolf Haussmann, and Wilhelm Zwerger, Annals of Physics

**326**, 770–796 (2011).

slides of viscosity talk in Nancy