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Timothy Halpin-Healy

Publications and source records attributed to Timothy Halpin-Healy.

4 recordsLinked to original sources

Three-Dimensional Kardar--Parisi--Zhang Scaling in Polariton Condensates

Kardar--Parisi--Zhang (KPZ) universality provides an example of macroscopic scaling generated by microscopic violation of detailed balance. While one- and two-dimensional realizations have been explored in driven condensates and growing interfaces, demonstrating KPZ scaling in three spatial dimensions remains a major challenge. Here we propose a three-dimensional exciton-polariton crystal as a platform for observation of 3D KPZ universality. Starting from a stochastic driven-dissipative Gross-Pitaevskii equation for a condensate formed in a three-dimensional photonic-crystal lower-polariton band, we eliminate the massive density and reservoir modes and obtain an effective $3+1$-dimensional KPZ equation for the condensate phase. Numerical simulations of both the KPZ equation and the full driven-dissipative polariton model show an intermediate-asymptotic regime in which the first-order coherence obeys $-\ln |\gone(0,\Delta t)|\propto |\Delta t|^{2\beta}$ and $-\ln |\gone(\Delta r,0)|\propto |\Delta r|^{2\chi}$, with exponents consistent with the $3+1$ KPZ benchmarks $\beta= 0.1845$, $\chi= 0.3135$. Our results identify three-dimensional polariton crystals as a controllable quantum fluid route to higher-dimensional nonequilibrium universality.

cond-mat.stat-mech

A KPZ Cocktail- Shaken, not stirred: Toasting 30 years of kinetically roughened surfaces

The stochastic partial differential equation proposed nearly three decades ago by Kardar, Parisi and Zhang (KPZ) continues to inspire, intrigue and confound its many admirers. Here, we i) pay debts to heroic predecessors, ii) highlight additional, experimentally relevant aspects of the recently solved 1+1 KPZ problem, iii) use an expanding substrates formalism to gain access to the 3d radial KPZ equation and, lastly, iv) examining extremal paths on disordered hierarchical lattices, set our gaze upon the fate of $d$=$\infty$ KPZ. Clearly, there remains ample unexplored territory within the realm of KPZ and, for the hearty, much work to be done, especially in higher dimensions, where numerical and renormalization group methods are providing a deeper understanding of this iconic equation.

cond-mat.stat-mech

Universal aspects of curved, flat & stationary-state Kardar-Parisi-Zhang statistics

Motivated by the recent exact solution of the {\it stationary-state} Kardar-Parisi-Zhang (KPZ) statistics by Imamura & Sasamoto (Phys. Rev. Lett. {\bf 108}, 190603 (2012)), as well as a precursor experimental signature unearthed by Takeuchi (Phys. Rev. Lett. {\bf 110}, 210604 (2013)), we establish here the universality of these phenomena, examining scaling behaviors of directed polymers in a random medium, the stochastic heat equation with multiplicative noise, and kinetically roughened KPZ growth models. We emphasize the value of cross KPZ-Class universalities, revealing crossover effects of experimental relevance. Finally, we illustrate the great utility of KPZ scaling theory by an optimized numerical analysis of the Ulam problem of random permutations.

cond-mat.stat-mech

Tuning the trip to KPZ asymptopia

Because of a close blood relationship between directed percolation & directed polymers in random media, the latter's journey to asymptotic scaling can be greatly retarded by an uninformed choice of departure point; i.e., the bare-bond PDF employed in the transfer matrix study. Bisecting a gaussian noise distribution, examining DPRM scaling for left & right halves separately, and comparing results against the full PDF, reveals in the simplest possible manner the essence of this dilemma. Paradoxically, when the bare-bond PDF possesses a relative shortage [left demi-gaussian], rather than abundance [right demi-gaussian] of low energy bonds, much better scaling is achieved. This finding is somewhat counterintuitive since a zero-temperature DPRM seeks the globally minimal path through a random energy landscape. Nevertheless, the behavior is easily traced to the strong influence of the neighboring DP fixed point function. This note communicates, in part, unpublished work referenced in Phys. Rev. E58, R4096 (1998). We discovered, as well, that the RG road to asymptopia can be highly refined by bootstrapping the presumed universal distribution from the getgo...

cond-mat.stat-mech