2019
DOI: 10.1103/physreva.99.053819
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Wave breaking and formation of dispersive shock waves in a defocusing nonlinear optical material

Abstract: We theoretically describe the quasi one-dimensional transverse spreading of a light beam propagating in a nonlinear optical material in the presence of a uniform background light intensity. For short propagation distances the pulse can be described within a nondispersive (geometric optics) approximation by means of Riemann's approach. For larger distances, wave breaking occurs, leading to the formation of dispersive shocks at both edges of the beam. We describe this phenomenon within Whitham modulation theory,… Show more

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Cited by 28 publications
(39 citation statements)
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“…Consequently, small oscillating fluctuations of the beam intensity field on top of a fixed background are described by the standard Bogoliubov theory [18][19][20][21], as was recently confirmed experimentally [14,17]. Large perturbations on top of a small background on the other hand lead to the creation of dispersive shock waves [22][23][24][25]. Recently, this platform was also exploited to explore the generation of topological defects and the associated turbulence [26,27], as well as analogue cosmological Sakharov oscillations in the density-density correlations of a quantum fluid of light [28,29].…”
Section: Introductionmentioning
confidence: 83%
See 1 more Smart Citation
“…Consequently, small oscillating fluctuations of the beam intensity field on top of a fixed background are described by the standard Bogoliubov theory [18][19][20][21], as was recently confirmed experimentally [14,17]. Large perturbations on top of a small background on the other hand lead to the creation of dispersive shock waves [22][23][24][25]. Recently, this platform was also exploited to explore the generation of topological defects and the associated turbulence [26,27], as well as analogue cosmological Sakharov oscillations in the density-density correlations of a quantum fluid of light [28,29].…”
Section: Introductionmentioning
confidence: 83%
“…The = case is instead used to define the norm N r (q ⊥ ) of the -th Bogoliubov mode. These conditions summarize as i X † 0, (q ⊥ )Π * 0, (q ⊥ ) − Π T 0, (q ⊥ )X 0, (q ⊥ ) = N r (q ⊥ )δ (24) (in this section we do not sum over repeated indices). Notice that the norm is real and can be either positive or negative.…”
Section: Properties Of Bogoliubov Modes and Orthonormalization Relationsmentioning
confidence: 99%
“…Near this edge, solutions of Whitham's equations are selfsimilar and depend on the variable z = x/t 1/3 . Although this solution can be obtained in analytic form [43,44], the self-similarity domain is relatively small, and we do not discuss this theory here. The solution of Whitham's equations in the entire DSW domain was obtained in [29,44].…”
Section: Motion Of Edges Of Dispersive Shock Wavesmentioning
confidence: 99%
“…Although this solution can be obtained in analytic form [43,44], the self-similarity domain is relatively small, and we do not discuss this theory here. The solution of Whitham's equations in the entire DSW domain was obtained in [29,44]. In approaching the small-amplitude edge, the DSW evolution again becomes self-similar, with the modulation parameters depending on z = x/t.…”
Section: Motion Of Edges Of Dispersive Shock Wavesmentioning
confidence: 99%
“…In optics, the hydrodynamics interpretation relies on the Madelung transforms which identify the light intensity to the fluid density and the phase gradient to the fluid velocity [18]. Recently several works have studied analytically shock wave formation in one and two dimensions [19,20]. Optical systems allow for repeatable experiments and precise control of the experimental parameters.…”
Section: Introductionmentioning
confidence: 99%