Publications Project 10 -
Nonlinear Phenomena in Complex Photonic Structures

Project Leader: Stefan Rotter

Optimal control of non-Markovian dynamics in a single-mode cavity strongly coupled to an inhomogeneously broadened spin ensemble

D. O. Krimer, B. Hartl, F. Mintert and S. Rotter

  Ensembles of quantum-mechanical spins offer a promising platform for quantum memories, but proper functionality requires accurate control of unavoidable system imperfections. We present an efficient control scheme for a spin ensemble strongly coupled to a single-mode cavity based on a set of Volterra equations relying solely on weak classical control pulses. The viability of our approach is demonstrated in terms of explicit storage and readout sequences that will serve as a starting point towards the realization of more demanding full quantum-mechanical optimal control schemes.

Published: 2017-10-16
Nature 549, 163-164 (2017)
DOI: 10.1103/PhysRevA.96.043837

Optical physics: A laser model for cosmology

S. Rotter

  Experiments reveal that the laws governing the immediate aftermath of the Big Bang also apply to the behaviour of coupled lasers. The findings could be used to solve complex computational problems.

Published: 2017-09-13
Nature 549, 163-164 (2017)
DOI: 10.1038/549163a

Wave propagation through disordered media without backscattering and intensity variations

K. G Makris, A. Brandstötter, P. Ambichl, Z. H. Musslimani and S. Rotter

  A fundamental manifestation of wave scattering in a disordered medium is the highly complex intensity pattern the waves acquire due to multi-path interference. Here we show that these intensity variations can be entirely suppressed by adding disorder-specific gain and loss components to the medium. The resulting constant-intensity waves in such non-Hermitian scattering landscapes are free of any backscattering and feature perfect transmission through the disorder. An experimental demonstration of these unique wave states is envisioned based on spatially modulated pump beams that can flexibly control the gain and loss components in an active medium.

Published: 2017-09-08
Light: Science & Applications (2017) 6, e17035
DOI: 10.1038/lsa.2017.35

Press release TU Wien, 2017-09-13 [55/2017]

Focusing inside Disordered Media with the Generalized Wigner-Smith Operator

P. Ambichl, A. Brandstötter, J. Böhm, M. Kühmayer, U. Kuhl, and S. Rotter

  We introduce a wave front shaping protocol for focusing inside disordered media based on a generalization of the established Wigner-Smith time-delay operator. The key ingredient for our approach is the scattering (or transmission) matrix of the medium and its derivative with respect to the position of the target one aims to focus on. A specific experimental realization in the microwave regime is presented showing that the eigenstates of a corresponding operator are sorted by their focusing strength—ranging from strongly focusing on the designated target to completely bypassing it. Our protocol works without optimization or phase conjugation and we expect it to be particularly attractive for optical imaging in disordered media.

Published: 2017-07-18
American Physical Society PRL 119, 033903 (2017)
DOI: 10.1103/PhysRevLett.119.033903

Symmetry, stability, and computation of degenerate lasing modes

D. Liu, B. Zhen, L. Ge, F. Hernandez, A. Pick, S. Burkhardt, M. Liertzer, S. Rotter and S. G. Johnson

  We present a general method to obtain the stable lasing solutions for the steady-state ab initio lasing theory (SALT) for the case of a degenerate symmetric laser in two dimensions (2D). We find that under most regimes (with one pathological exception), the stable solutions are clockwise and counterclockwise circulating modes, generalizing previously known results of ring lasers to all 2D rotational symmetry groups. Our method uses a combination of semianalytical solutions close to lasing threshold and numerical solvers to track the lasing modes far above threshold. Near threshold, we find closed-form expressions for both circulating modes and other types of lasing solutions as well as for their linearized Maxwell-Bloch eigenvalues, providing a simple way to determine their stability without having to do a full nonlinear numerical calculation. Above threshold, we show that a key feature of the circulating mode is its “chiral” intensity pattern, which arises from spontaneous symmetry breaking of mirror symmetry, and whose symmetry group requires that the degeneracy persists even when nonlinear effects become important. Finally, we introduce a numerical technique to solve the degenerate SALT equations far above threshold even when spatial discretization artificially breaks the degeneracy.

Published: 2017-02-23
Phys. Rev. A 95, 023835 (2017)
DOI: 10.1103/PhysRevA.95.023835

Principal modes in multimode fibers: exploring the crossover from weak to strong mode coupling

W. Xiong, P. Ambichl, Y. Bromberg, B. Redding, S. Rotter, and H. Cao

  We present experimental and numerical studies on principal modes in a multimode fiber with mode coupling. By applying external stress to the fiber and gradually adjusting the stress, we have realized a transition from weak to strong mode coupling, which corresponds to the transition from single scattering to multiple scattering in mode space. Our experiments show that principal modes have distinct spatial and spectral characteristic in the weak and strong mode coupling regimes. We also investigate the bandwidth of the principal modes, in particular, the dependence of the bandwidth on the delay time, and the effects of the mode-dependent loss. By analyzing the path-length distributions, we discover two distinct mechanisms that are responsible for the bandwidth of principal modes in weak and strong mode coupling regimes. Their interplay leads to a non-monotonic transition of the average principal mode bandwidth from weak to strong mode coupling. Taking into account the mode-dependent loss in the fiber, our numerical results are in qualitative agreement with our experimental observations. Our study paves the way for exploring potential applications of principal modes in communication, imaging and spectroscopy.

Published: 2017-02-06
Optics Express Vol. 25, Issue 3, pp. 2709-2724 (2017)
DOI: 10.1364/OE.25.002709

Spectral hole burning and its application in microwave photonics

S. Putz, A.s Angerer, D. O. Krimer, R. Glattauer, W. J. Munro, S. Rotter, J. Schmiedmayer & J. Majer

  Spectral hole burning, used in inhomogeneously broadened emitters, is a well-established optical technique, with applications from spectroscopy to slow light and frequency combs. In microwave photonics, electron spin ensembles are candidates for use as quantum memories with potentially long storage times. Here, we demonstrate long-lived collective dark states by spectral hole burning in the microwave regime. The coherence time in our hybrid quantum system (nitrogen–vacancy centres strongly coupled to a superconducting microwave cavity) becomes longer than both the ensemble's free-induction decay and the bare cavity dissipation rate. The hybrid quantum system thus performs better than its individual subcomponents. This opens the way for long-lived quantum multimode memories, solid-state microwave frequency combs, spin squeezed states, optical-to-microwave quantum transducers and novel metamaterials. Beyond these, new cavity quantum electrodynamics experiments will be possible where spin–spin interactions and many-body phenomena are directly accessible.

Published: 2016-11-21
Nature Photonics 11, 36–39 (2017)
DOI: 10.1038/nphoton.2016.225

Sustained photon pulse revivals from inhomogeneously broadened spin ensembles

D. O. Krimer, M. Zens, S. Putz and S. Rotter

  A very promising recent trend in applied quantum physics is to combine the advantageous features of different quantum systems into what is called “hybrid quantum technology”. One of the key elements in this new field will have to be a quantum memory enabling to store quanta over extended periods of time. Systems that may fulfill the demands of such applications are comb-shaped spin ensembles coupled to a cavity. Due to the decoherence induced by the inhomogeneous ensemble broadening, the storage time of these quantum memories is, however, still rather limited. Here we demonstrate how to overcome this problem by burning well-placed holes into the spectral spin density leading to spectacular performance in the multimode regime. Specifically, we show how an initial excitation of the ensemble leads to the emission of more than a hundred well-separated photon pulses with a decay rate significantly below the fundamental limit of the recently proposed “cavity protection effect”.

Published: 2016-11-22
Laser & Photonics Reviews Volume 10, Issue 6, pages 1023–1030 (2016)
DOI: 10.1002/lpor.201600189

Constant Intensity Supermodes in Non-Hermitian Lattices

K.G. Makris, Z.H. Musslimani, D.N. Christodoulides, S. Rotter

  We study the existence of a novel class of waves, with constant intensity (CI) in coupled non-Hermitian photonic systems. These generalized plane waves exist only in optical structures that are composed of gain and loss (in both linear and nonlinear domains). In the framework of coupled mode theory, we examine the properties of such supermodes in finite waveguide lattices. In particular, CI-supermodes with periodic, localized, and disordered phases in finite chains of optical elements are considered in detail. Extensions to the nonlinear regime and the connection to the continuum limit are also studied.

Published: 2016-09
IEEE Volume: 22, Issue: 5, Sept.-Oct. 2016
DOI: 10.1109/JSTQE.2016.2593866

Random lasers for broadband directional emission

S. Schönhuber, M. Brandstetter, T. Hisch, C. Deutsch, M. Krall, H. Detz, A. M. Andrews, G. Strasser, S. Rotter, and K. Unterrainer

  Broadband coherent light sources are becoming increasingly important for sensing and spectroscopic applications, especially in the mid-infrared and terahertz (THz) spectral regions, where the unique absorption characteristics of a whole host of molecules are located. The desire to miniaturize such light emitters has recently led to spectacular advances, with compact on-chip lasers that cover both of these spectral regions. The long wavelength and small size of the sources result in a strongly diverging laser beam that is difficult to focus on the target that one aims to perform spectroscopy with. Here, we introduce an unconventional solution to this vexing problem, relying on a random laser to produce coherent broadband THz radiation as well as an almost diffraction-limited far-field emission profile. Our random lasers do not require any fine tuning and thus constitute a promising example of practical device applications for random lasing.

Published: 2016-09-21
Optica 1035, Vol. 3, No. 10 (2016)
DOI: 10.1364/OPTICA.3.001035
(--> also listed in Project 02 & 09)

PT-symmetry breaking in the steady state of microscopic gain–loss systems

K. V. Kepesidis, T. J. Milburn, J. Huber, K. G. Makris, S. Rotter and P. Rabl

  The phenomenon of PT (parity- and time-reversal) symmetry breaking is conventionally associated with a change in the complex mode spectrum of a non-Hermitian system that marks a transition from a purely oscillatory to an exponentially amplified dynamical regime. In this work we describe a new type of PT-symmetry breaking, which occurs in the steady-state energy distribution of open systems with balanced gain and loss. In particular, we show that the combination of nonlinear saturation effects and the presence of thermal or quantum noise in actual experiments results in unexpected behavior that differs significantly from the usual dynamical picture. We observe additional phases with preserved or 'weakly' broken PT-symmetry, and an unconventional transition from a high-noise thermal state to a low-amplitude lasing state with broken symmetry and strongly reduced fluctuations. We illustrate these effects here for the specific example of coupled mechanical resonators with optically induced loss and gain, but the described mechanisms will be essential for a general understanding of the steady-state properties of actual PT-symmetric systems operated at low amplitudes or close to the quantum regime.

Published: 2016-09-07
New J. Phys. 18, 095003 (2016)
DOI: 10.1088/1367-2630/18/9/095003

Diffusive to quasi-ballistic random laser: incoherent and coherent models

W. Guerin, Y. D. Chong, Q. Baudouin, M. Liertzer, S. Rotter, and R. Kaiser

  We study the crossover between the diffusive and quasi-ballistic regimes of random lasers. In particular, we compare incoherent models based on the diffusion equation and the radiative transfer equation (RTE), which neglect all wave effects, with a coherent wave model for the random laser threshold. We show that both the incoherent and the coherent models predict qualitatively similar thresholds, with a smooth transition from a diffuse to a quasi-ballistic regime. The shape of the intensity distribution in the sample as predicted by the RTE model at threshold is also in good agreement with the coherent model. The approximate incoherent models thus provide useful analytical predictions for the threshold of random lasers as well as the shape of the random laser modes at threshold.

Published: 2016-08-12
Journal of the Optical Society of America B Vol. 33, Issue 9, pp. 1888-1896 (2016)
DOI: 10.1364/JOSAB.33.001888

Effective PT-symmetric metasurfaces for subwavelength amplified sensing

S. Xiao, J. Gear, S. Rotter and J. Li

  We propose a novel design principle for ultrathin metasurfaces to realize optically amplified sensing with a performance that exceeds those of passive coherent perfect absorbers by several orders of magnitude. Our strategy is based on a generalized condition of lasing, coherent perfect absorption and their coexistence in metamaterials that feature an effective PT-symmetry. The devices we introduce here can be operated in configurations that involve both a one-sided or a two-sided wave incidence, where the latter case allows us to tune the degree of amplified absorption through the coherent phase between the two input beams. We also discuss how the conditions on the material parameters can be relaxed, away from the ideal case, such that a substantial amplification of the sensing performance can easily be reached in practical applications.

Published: 2016-08-08
New Journal of Physics, Volume 18, August 2016
DOI: 10.1088/1367-2630/18/8/085004

Spatiotemporal Control of Light Transmission through a Multimode Fiber with Strong Mode Coupling

W. Xiong, P. Ambichl, Y. Bromberg, B. Redding, S. Rotter, and H. Cao

  We experimentally generate and characterize eigenstates of the Wigner-Smith time-delay matrix, called principal modes, in a multimode fiber with strong mode coupling. The unique spectral and temporal properties of principal modes enable global control of temporal dynamics of optical pulses transmitted through the fiber, despite random mode mixing. Our analysis reveals that well-defined delay times of the eigenstates are formed by multipath interference, which can be effectively manipulated by spatial degrees of freedom of input wave fronts. This study is essential to controlling dynamics of wave scattering, paving the way for coherent control of pulse propagation through complex media.

Published: 2016-07-25
Phys. Rev. Lett. 117, 053901 (2016)
DOI: 10.1103/PhysRevLett.117.053901

Particlelike wave packets in complex scattering systems

B. Gérardin, J. Laurent, P. Ambichl, C. Prada, S. Rotter, and A. Aubry

  A wave packet undergoes a strong spatial and temporal dispersion while propagating through a complex medium. This wave scattering is often seen as a nightmare in wave physics whether it be for focusing, imaging, or communication purposes. Controlling wave propagation through complex systems is thus of fundamental interest in many areas, ranging from optics or acoustics to medical imaging or telecommunications. Here, we study the propagation of elastic waves in a cavity and a disordered waveguide by means of laser interferometry. From the direct experimental access to the time-delay matrix of these systems, we demonstrate the existence of particlelike wave packets that remain focused in time and space throughout their complex trajectory. Due to their limited dispersion, their selective excitation will be crucially relevant for all applications involving selective wave focusing and efficient information transfer through complex media.

Published: 2016-07-25
Physical Review B 94, 014209 (2016)
DOI: 10.1103/PhysRevB.94.014209

Modulational instability in a PT-symmetric vector nonlinear Schrödinger system

J.T. Cole, K.G. Makris, Z.H. Musslimani, D.N. Christodoulides, S. Rotter

  A class of exact multi-component constant intensity solutions to a vector nonlinear Schrödinger (NLS) system in the presence of an external PTPT-symmetric complex potential is constructed. This type of uniform wave pattern displays a non-trivial phase whose spatial dependence is induced by the lattice structure. In this regard, light can propagate without scattering while retaining its original form despite the presence of inhomogeneous gain and loss. These constant-intensity continuous waves are then used to perform a modulational instability analysis in the presence of both non-hermitian media and cubic nonlinearity. A linear stability eigenvalue problem is formulated that governs the dynamical evolution of the periodic perturbation and its spectrum is numerically determined using Fourier–Floquet–Bloch theory. In the self-focusing case, we identify an intensity threshold above which the constant-intensity modes are modulationally unstable for any Floquet–Bloch momentum belonging to the first Brillouin zone. The picture in the self-defocusing case is different. Contrary to the bulk vector case, where instability develops only when the waves are strongly coupled, here an instability occurs in the strong and weak coupling regimes. The linear stability results are supplemented with direct (nonlinear) numerical simulations.

Published: 2016-07-25
Physica D (2016)
DOI: 10.1016/j.physd.2016.07.001

Dynamically encircling an exceptional points for asymmetric mode switching

J. Doppler, A.A. Mailybaev, J. Böhm, U. Kuhl, A. Girschik, F. Libisch, T.J. Milburn, P. Rabl, N. Moiseyev, S. Rotter

  Physical systems with loss or gain have resonant modes that decay or grow exponentially with time. Whenever two such modes coalesce both in their resonant frequency and their rate of decay or growth, an ‘exceptional point’ occurs, giving rise to fascinating phenomena that defy our physical intuition. Particularly intriguing behaviour is predicted to appear when an exceptional point is encircled sufficiently slowly, such as a state-flip or the accumulation of a geometric phase. The topological structure of exceptional points has been experimentally explored, but a full dynamical encircling of such a point and the associated breakdown of adiabaticity have remained out of reach of measurement. Here we demonstrate that a dynamical encircling of an exceptional point is analogous to the scattering through a two-mode waveguide with suitably designed boundaries and losses. We present experimental results from a corresponding waveguide structure that steers incoming waves around an exceptional point during the transmission process. In this way, mode transitions are induced that transform this device into a robust and asymmetric switch between different waveguide modes. This work will enable the exploration of exceptional point physics in system control and state transfer schemes at the crossroads between fundamental research and practical applications.

Published: 2016-07-25
Nature Letter (2016)
DOI: 10.1038/nature18605

Press release TU Wien, 2016-07-26 [46/2016]


Chiral modes and directional lasing at exceptional points

B. Peng, S.K. Özdemir, M. Liertzer, W. Chen, J. Kramer, H. Yilmaz, J. Wiersig, S. Rotter, L. Yang

  Controlling the emission and the flow of light in micro- and nanostructures is crucial for on-chip information processing. Here we show how to impose a strong chirality and a switchable direction of light propagation in an optical system by steering it to an exceptional point (EP)—a degeneracy universally occurring in all open physical systems when two eigenvalues and the corresponding eigenstates coalesce. In our experiments with a fiber-coupled whispering-gallery-mode (WGM) resonator, we dynamically control the chirality of resonator modes and the emission direction of a WGM microlaser in the vicinity of an EP: Away from the EPs, the resonator modes are nonchiral and laser emission is bidirectional. As the system approaches an EP, the modes become chiral and allow unidirectional emission such that by transiting from one EP to another one the direction of emission can be completely reversed. Our results exemplify a very counterintuitive feature of non-Hermitian physics that paves the way to chiral photonics on a chip.  

Published: 2016-06-21
Proc. Natl. Acad. Sci. U.S.A. (2016)
DOI: 10.1073/pnas.1603318113


Twofold PT symmetry in doubly exponential optical lattices

J.T. Cole, K.G. Makris, Z.H. Musslimani, D.N. Christodoulides, S. Rotter

  We introduce a family of non-Hermitian optical potentials that are given in terms of double-exponential periodic functions. The center of ΡΤ symmetry is not around zero and the potential satisfies a shifted ΡΤ-symmetry relation at two distinct locations. Motivated by wave transmission through thin phase screens and gratings, we examine these refractive index modulations from the perspective of optical lattices that are homogeneous along the propagation direction. The diffraction dynamics, abrupt phase transitions in the eigenvalue spectrum, and exceptional points in the band structure are examined in detail. In addition, the nonlinear properties of wave propagation in Kerr nonlinearity media are studied. In particular, coherent structures such as lattice solitons are numerically identified by applying the spectral renormalization method. The spatial symmetries of such lattice solitons follow the shifted ΡΤ-symmetric relations. Furthermore, such lattice solitons have a power threshold and their linear and nonlinear stabilities are critically dependent on their spatial symmetry point.

Published: 2016-01-04
Physical Review A 93, 013803 (2016)
DOI: 10.1103/PhysRevA.93.013803


Interaction-induced mode switching in steady-state microlasers

L. Ge, D. Liu, A. Cerjan, S. Rotter, H. Cao, S.G. Johnson, H.E. Türeci, A.D. Stone

  We demonstrate that due to strong modal interactions through cross-gain saturation, the onset of a new lasing mode can switch off an existing mode via a negative power slope. In this process of interaction-induced mode switching (IMS) the two involved modes maintain their identities, i.e. they do not change their spatial field patterns or lasing frequencies. For a fixed pump profile, a simple analytic criterion for the occurrence of IMS is given in terms of their self- and cross-interaction coefficients and non-interacting thresholds, which is verified for the example of a two-dimensional microdisk laser. When the spatial pump profile is varied as the pump power is increased, IMS can be induced even when it would not occur with a fixed pump profile, as we show for two coupled laser cavities. Our findings apply to steady-state lasing and are hence different from dynamical mode switching or hopping. IMS may have potential applications in robust and flexible all-optical switching.

Published: 2016-01-04
Optics Express 41, Vol. 24, No. 1 (2016)
DOI: 10.1364/OE.24.000041


General description of quasiadiabatic dynamical phenomena near exceptional points

T.J. Milburn, J. Doppler, C.A. Holmes, S. Portolan, S. Rotter, P. Rabl

  The appearance of so-called exceptional points in the complex spectra of non-Hermitian systems is often associated with phenomena that contradict our physical intuition. One example of particular interest is the state-exchange process predicted for an adiabatic encircling of an exceptional point. In this work we analyze this and related processes for the generic system of two coupled oscillator modes with loss or gain. We identify a characteristic system evolution consisting of periods of quasistationarity interrupted by abrupt nonadiabatic transitions and we present a qualitative and quantitative description of this switching behavior by connecting the problem to the phenomenon of stability loss delay. This approach makes accurate predictions for the breakdown of the adiabatic theorem as well as the occurrence of chiral behavior observed previously in this context and provides a general framework to model and understand quasiadiabatic dynamical effects in non-Hermitian systems.

Published: 2015-11-30
Physical Review A 92, 052124 (2015)
DOI: 10.1103/PhysRevA.92.052124


Smooth Optimal Quantum Control for Robust Solid-State Spin Magnetometry

T. Nöbauer, A. Angerer, B. Bartels, M. Trupke, S. Rotter, J. Schmiedmayer, F. Minert, J. Majer

  We experimentally demonstrate a simple yet versatile optimal quantum control technique that achieves tailored robustness against qubit inhomogeneities and control errors while requiring minimal bandwidth. We apply the technique to nitrogen-vacancy (NV) centers in diamond and verify its performance using quantum process tomography. In a wide-field NV center magnetometry scenario, we achieve a homogeneous sensitivity across a 33% drop in control amplitude, and we improve the sensitivity by up to 2 orders of magnitude for a normalized detuning as large as 40%, achieving a value of 20 nT Hz-1/2 μm3/2 in sensitivity times square root volume.

Published: 2015-11-06
Physical Review Letter 115, 190801 (2015)
DOI: 10.1103/PhysRevLett.115.190801
Press release TU Wien, 2015-11-12 [105/2015]


Analytical study of quantum-feedback-enhanced Rabi oscillations

J. Kabuss, D.O. Krimer, S. Rotter, K. Stannigel, A. Knorr, A. Carmele

  We present an analytical solution of the single-photon quantum feedback in a cavity quantum electrodynamics system based on a half-cavity setup coupled to a structured continuum. Our exact analytical expression constitutes an important benchmark for quantum-feedback models and allows us to unravel the necessary conditions for the previously reported numerical result that a single-emitter-cavity system, which is initially in the weakcoupling regime, can be driven into the strong-coupling regime via the proposed quantum-feedback mechanism [A. Carmele et al., Phys. Rev. Lett. 110, 013601 (2013)]. We specify the phase relations between the cavity mode and the delay time and state explicitly the theoretical limit for a feedback effect in the single-photon regime. Via the photon-path representation, we prove that the stabilization phenomenon relies on a destructive interference effect and we discuss the stabilization time in the weak- and strong-coupling limits.

Published: 2015-11-02
Physical Review A92, 053801 (2015)
DOI: 10.1103/PhysRevA.92.053801


Steady-state ab initio laser theory for fully or nearly degenerate cavity modes

S. Burkhardt, M. Liertzer, D.O. Krimer, S. Rotter

  We investigate the range of validity of the recently developed steady-state ab initio laser theory (SALT). While very efficient in describing various microlasers, SALT is conventionally believed not to be applicable to lasers featuring fully or nearly degenerate pairs of resonator modes above the lasing threshold. Here we demonstrate how SALT can indeed be extended to describe such cases as well, with the effect that we significantly broaden the theory’s scope. In particular, we show how to use SALT in conjunction with a linear stability analysis to obtain stable single-mode lasing solutions that involve a degenerate mode pair. Our flexible and efficient approach is tested on one-dimensional ring lasers as well as on two-dimensional microdisk lasers with broken symmetry.

Published: 2015-07-27
Physical Review A 92, 013847 (2015)
DOI: 10.1103/PhysRevA.92.013847


Hybrid Quantum Systems with Collectively Coupled Spin States: Suppression of Decoherence through Spectral Hole Burning

D.O. Krimer, B. Hartl, S. Rotter

  Spin ensemble based hybrid quantum systems suffer from a significant degree of decoherence resulting from the inhomogeneous broadening of the spin transition frequencies in the ensemble. We demonstrate that this strongly restrictive drawback can be overcome simply by burning two narrow spectral holes in the spin spectral density at judiciously chosen frequencies. Using this procedure we find an increase of the coherence time by more than an order of magnitude as compared to the case without hole burning. Our findings pave the way for the practical use of these hybrid quantum systems for the processing of quantum information.

Published: 2015-07-14
Physical Review Letters 115, 033601 (2015)
DOI: 10.1103/PhysRevLett.115.033601


Constant-intensity waves and their modulation instability in non-Hermitian potentials

K.G. Makris, Z.H. Musslimani, D.N. Christodoulides, S. Rotter

  In all of the diverse areas of science where waves play an important role, one of the most fundamental solutions of the corresponding wave equation is a stationary wave with constant intensity. The most familiar example is that of a plane wave propagating in free space. In the presence of any Hermitian potential, a wave’s constant intensity is, however, immediately destroyed due to scattering. Here we show that this fundamental restriction is conveniently lifted when working with non-Hermitian potentials. In particular, we present a whole class of waves that have constant intensity in the presence of linear as well as of nonlinear inhomogeneous media with gain and loss. These solutions allow us to study the fundamental phenomenon of modulation instability in an inhomogeneous environment. Our results pose a new challenge for the experiments on non-Hermitian scattering that have recently been put forward.

Published: 2015-07-08
Nature Communications 6, 7257 (2015)
DOI: 10.1038/ncomms8257

Press release TU Wien, 2015-08-10 [80/2015]


Parity-time symmetry from stacking purely dielectric and magnetic slabs

J. Gear, F. Liu, S.T. Chu, S. Rotter, J. Li

  We show that parity-time symmetry in matching electric permittivity to magnetic permeability can be established by considering an effective parity operator involving both mirror symmetry and coupling between electric and magnetic fields. This approach extends the discussion of parity-time symmetry to the situation with more than one material potential. We show that the band structure of a one-dimensional photonic crystal with alternating purely dielectric and purelymagnetic slabs can undergo a phase transition between propagation modes and evanescent modes when the balanced gain or loss parameter is varied. The cross matching between different material potentials also allows exceptional points of the constitutive matrix to appear in the long-wavelength limit where they can be used to construct ultrathin metamaterials with unidirectional reflection.

Published: 2015-03-20
Physical Review A 91, 033825 (2015)
DOI: 10.1103/PhysRevA.91.033825


Invariance property of wave scattering through disordered media

R. Pierrat, P. Ambichl, S. Gigan, A. Haber, R. Carminati, S. Rotter

  A fundamental insight in the theory of diffusive random walks is that the mean length of trajectories traversing a finite open system is independent of the details of the diffusion process. Instead, the mean trajectory length depends only on the system’s boundary geometry and is thus unaffected by the value of the mean free path. Here we show that this result is rooted on a much deeper level than that of a random walk, which allows us to extend the reach of this universal invariance property beyond the diffusion approximation. Specifically, we demonstrate that an equivalent invariance relation also holds for the scattering of waves in resonant structures as well as in ballistic, chaotic or in Anderson localized systems. Our work unifies a number of specific observations made in quite diverse fields of science ranging from the movement of ants to nuclear scattering theory. Potential experimental realizations using light fields in disordered media are discussed.

Published: 2014-11-28
PNAS (2014)
DOI: 10.1073/pnas.1417725111

Press release TU Wien, 2014-11-26 [117/2014]


Non-Markovian dynamics of a single-mode cavity strongly coupled to an inhomogeneously broadened spin ensemble

D.O. Krimer, S. Putz, J. Majer, S. Rotter

  We study the dynamics of a spin ensemble strongly coupled to a single-mode resonator driven by external pulses. When themean frequency of the spin ensemble is in resonance with the cavity mode, damped Rabi oscillations are found between the spin ensemble and the cavity mode which we describe very accurately, including the dephasing effect of the inhomogeneous spin broadening. We demonstrate that a precise knowledge of this broadening is crucial both for a qualitative and a quantitative understanding of the temporal spin-cavity dynamics. On this basis we show that coherent oscillations between the spin ensemble and the cavity can be enhanced by a few orders of magnitude, when driving the system with pulses that match special resonance conditions. Our theoretical approach is tested successfully with an experiment based on an ensemble of negatively charged nitrogen-vacancy centers in diamond strongly coupled to a superconducting coplanar single-mode waveguide resonator.

Published: 2014-10-24
APS Physics - Physical Review A 90, 043852 (2014)
DOI: 10.1103/PhysRevA.90.043852


Loss-induced suppression and revival of lasing

B. Peng, S.K. Özdemir, S. Rotter, H. Yilmaz, M. Liertzer, F. Monifi, C.M. Bender, F. Nori, L. Yang

  Controlling and reversing the effects of loss are major challenges in optical systems. For lasers, losses need to be overcome by a sufficient amount of gain to reach the lasing threshold. In this work, we show how to turn losses into gain by steering the parameters of a system to the vicinity of an exceptional point (EP), which occurs when the eigenvalues and the corresponding eigenstates of a system coalesce. In our system of coupled microresonators, EPs are manifested as the loss-induced suppression and revival of lasing. Below a critical value, adding loss annihilates an existing Raman laser. Beyond this critical threshold, lasing recovers despite the increasing loss, in stark contrast to what would be expected from conventional laser theory. Our results exemplify the counterintuitive features of EPs and present an innovative method for reversing the effect of loss.

Published: 2014-10-17
DOI: 10.1126/science.1258004

Press release TU Wien, 2014-10-17 [103/2014]


Protecting a spin ensemble against decoherence in the strong-coupling regime of cavity QED

S. Putz, D.O. Krimer, R. Amsüss, A. Valookaran, T. Nöbauer, J. Schmiedmayer, S. Rotter, J. Majer

  Hybrid quantum systems based on spin ensembles coupled to superconducting microwave cavities are promising candidates for robust experiments in cavity quantum electrodynamics (QED) and for future technologies employing quantum mechanical effects. At present, the main source of decoherence in these systems is inhomogeneous spin broadening, which limits their performance for the coherent transfer and storage of quantum information. Here we study the dynamics of a superconducting cavity strongly coupled to an ensemble of nitrogen–vacancy centres in diamond. We experimentally observe how decoherence induced by inhomogeneous broadening can be suppressed in the strong-coupling regime - a phenomenon known as ‘cavity protection’. To demonstrate the potential of this effect for coherent-control schemes, we show how appropriately chosen microwave pulses can increase the amplitude of coherent oscillations between the cavity and spin ensemble by two orders of magnitude.

Published: 2014-08-17
Nature Physics Letter
DOI: 10.1038/NPHYS3050

Press release TU Wien, 2014-08-18 [87/2014]


Reversing the pump dependence of a laser at an exceptional point

M. Brandstetter, M. Liertzer, C. Deutsch, P. Klang, J. Schöberl, H.E. Türeci, G. Strasser, K. Unterrainer, S. Rotter

  When two resonant modes in a system with gain or loss coalesce in both their resonance position and their width, a so-called exceptional point occurs, which acts as a source of nontrivial physics in a diverse range of systems. Lasers provide a natural setting to study such non-Hermitian degeneracies, as they feature resonant modes and a gain material as their basic constituents. Here we show that exceptional points can be conveniently induced in a photonic molecule laser by a suitable variation of the applied pump. Using a pair of coupled microdisk quantum cascade lasers, we demonstrate that in the vicinity of these exceptional points the coupled laser shows a characteristic reversal of its pump dependence, including a strongly decreasing intensity of the emitted laser light for increasing pump power.

Published: 2014-06-03
Nature Communications 5, Article number: 4034
DOI: 10.1038/ncomms5034
(--> also listed in Project 02 and 09)

Press release TU Wien, 2014-06-17 [63/2014]


Reflection resonances in surface-disordered waveguides: strong higher-order effects of the disorder

J. Doppler, J.A. Méndez-Bermúdez, J. Feist, O. Dietz, D.O. Krimer, N.M. Makarov, F.M. Izrailev, S. Rotter

  We study coherent wave scattering through waveguides with a step-like surface disorder and find distinct enhancements in the reflection coefficients at welldefined resonance values. Based on detailed numerical and analytical calculations, we can unambiguously identify the origin of these reflection resonances to be higher-order correlations in the surface disorder profile which are typically neglected in similar studies of the same system. A remarkable feature of this new effect is that it relies on the longitudinal correlations in the step profile, although individual step heights are random and thus completely uncorrelated. The corresponding resonances are very pronounced and robust with respect to ensemble averaging, and lead to an enhancement of wave reflection by more than one order of magnitude.

Published: 2014-05-09
New Journal of Physics 16, 053026
DOI: 10.1088/1367-2630/16/5/053026


Random lasers: Playing pinball with light

S. Rotter

  Without a well-defined cavity, there is no obvious way to control the resonant modes in a random laser. Experiments now show that shaping the optical pump allows for controlled single-mode operation at predetermined lasing wavelengths.

Published: 2014-04-20
Nature Physics 10, 412–413
DOI: 10.1038/nphys2960


The single-channel regime of transport through random media

A. Pena, A. Girschik, F. Libisch, S. Rotter, A.A. Chabanov

  The propagation of light through samples with random inhomogeneities can be described by way of transmission eigenchannels, which connect incoming and outgoing external propagating modes. Although the detailed structure of a disordered sample can generally not be fully specified, these transmission eigenchannels can nonetheless be successfully controlled and used for focusing and imaging light through random media. Here we demonstrate that in deeply localized quasi-1D systems, the single dominant transmission eigenchannel is formed by an individual Anderson-localized mode or by a ‘necklace state’. In this single-channel regime, the disordered sample can be treated as an effective 1D system with a renormalized localization length, coupled through all the external modes to its surroundings. Using statistical criteria of the single-channel regime and pulsed excitations of the disordered samples allows us to identify long-lived localized modes and short-lived necklace states at long and short time delays, respectively.

Published: 2014-03-24
Nature Communications 5, Article number: 3488
DOI: 10.1038/ncomms4488


Route from spontaneous decay to complex multimode dynamics in cavity QED

D.O. Krimer, M. Liertzer, S. Rotter, H.E. Türeci

  We study the non-Markovian quantum dynamics of an emitter inside an open multimode cavity, focusing on the case where the emitter is resonant with high-frequency cavity modes. Based on a Green’s-function technique suited for open photonic structures, we study the crossovers between three distinct regimes as the coupling strength is gradually increased: (i) overdamped decay with a time scale given by the Purcell modified decay rate, (ii) underdamped oscillations with a time scale given by the effective vacuum Rabi frequency, and (iii) pulsed revivals. The final multimode strong-coupling regime (iii) gives rise to quantum revivals of the atomic inversion on a time scale associated with the cavity round-trip time. We show that the crucial parameter to capture the crossovers between these regimes is the nonlinear Lamb shift, accounted for exactly in our formalism.

Published: 2014-03-11
APS Physics - Physical Review A 89, 033820
DOI: 10.1103/PhysRevA.89.033820


Breaking of ΡΤ Symmetry in Bounded and Unbounded Scattering Systems

P. Ambichl, K.G. Makris, L. Ge, Y. Chong, A.D. Stone, S. Rotter

  PT-symmetric scattering systems with balanced gain and loss can undergo a symmetry-breaking transition in which the eigenvalues of the nonunitary scattering matrix change their phase shifts from real to complex values. We relate the PT-symmetry-breaking points of such an unbounded scattering system to those of the underlying bounded systems. In particular, we show how the PT thresholds in the scattering matrix of the unbounded system translate into analogous transitions in the Robin boundary conditions of the corresponding bounded systems. Based on this relation, we argue and then confirm that the PT transitions in the scattering matrix are, under very general conditions, entirely insensitive to a variable coupling strength between the bounded region and the unbounded asymptotic region, a result that can be tested experimentally and visualized using the concept of Smith charts.

Published: 2013-12-18
APS Physics - Physical Review X 3, 041030
DOI: 10.1103/PhysRevX.3.041030


Double-layered nanoparticle stacks for surface enhanced infrared absorption spectroscopy

J. Srajer, A. Schwaighofer, G. Ramer, S. Rotter, B. Guenay, A. Kriegner, W. Knoll, B. Lendl, C. Nowak

  We demonstrate that double-layered stacks of gold and insulator nanoparticles arranged on a flat gold surface dramatically enhance the sensitivity in absorption infrared microscopy. Through morphological variations of the nanoparticles, the frequency of the plasmon resonances can be tuned to match the frequency of the molecular vibration in the mid-infrared region. The results show that the nanostructures enhance the absorption signal of the molecules by a factor of up to ∼2.2 x 106, while preserving their characteristic lineshape remarkably well.

Published: 2013-10-22
Nanoscale 6, 127-131
DOI: 10.1039/c3nr04726a


Domesticating random lasers

M. Liertzer, S. Rotter

  When pumped with a spatially modulated light beam, random lasers can be tuned to emit into specific, predetermined directions.

Published: 2013-09-20
SPIE Newsroom
DOI: 10.1117/2.1201309.005132


Pump-Controlled Directional Light Emission from Random Lasers

T. Hisch, M. Liertzer, D. Pogany, F. Mintert, S. Rotter

  The angular emission pattern of a random laser is typically very irregular and difficult to tune. Here we show by detailed numerical calculations that one can overcome the lack of control over this emission pattern by actively shaping the spatial pump distribution. We demonstrate, in particular, how to obtain customized pump profiles to achieve highly directional emission. Going beyond the regime of strongly scattering media where localized modes with a given directionality can simply be selected by the pump, we present an optimization-based approach which shapes extended lasing modes in the weakly scattering regime according to any predetermined emission pattern.

Published: 2013-07-12
APS Physics - Physical Review Letters 111, 023902
DOI: 10.1103/PhysRevLett.111.023902






Share This

Follow Us