Crossing over universal scaling laws in two-dimensional driven dissipative condensates | Paper Citation Record

Observation 2f905e45-97c1-4aad-9dc1-a68fbfc279f9 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 1

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Observation da135c1c-a82c-47d1-978d-f54731930f2c · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 2

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Observation 56f5eb2e-9147-4c74-881b-f791de723c8b · outbound

This paper cites The average ⟨·⟩denotes both an average over independent realizations of the dynamics and an angular average over all directions at fixed distance ∆r=|∆r|.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates The average ⟨·⟩denotes both an average over independent realizations of the dynamics and an angular average over all directions at fixed distance ∆r=|∆r|

Reference 3

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Observation 491949d5-89ba-4363-8ba4-8cc6b5422f4f · outbound

This paper cites Indeed, under this condition, the microscopic model Eqs.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates Indeed, under this condition, the microscopic model Eqs

Reference 4

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Observation 9ac83bf8-d1aa-4e8e-b47b-2ea423005dcd · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 5

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Observation bf752dfd-ac28-421c-9fd2-40c44fe41e7e · outbound

This paper cites It con- sists of a 5λ/2 Ga 0.05Al0.95As microcavity surrounded by two Al 0.20Ga0.80As/Al0.05Ga0.95As distributed Bragg reflectors with 26 (38) pairs in the top (bottom) mirror.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates It con- sists of a 5λ/2 Ga 0.05Al0.95As microcavity surrounded by two Al 0.20Ga0.80As/Al0.05Ga0.95As distributed Bragg reflectors with 26 (38) pairs in the top (bottom) mirror

Reference 6

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Observation f9e743c1-ca0b-4337-8ee4-2a9bedca17c0 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 7

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Observation 873df4f6-b343-4f33-a2a2-eb502ce0c2dc · outbound

This paper cites A sketch of the optical setup is shown in Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates A sketch of the optical setup is shown in Fig

Reference 8

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Observation cd306d43-3148-47b4-9ef7-0c66739d5747 · outbound

This paper cites A PID controller stabilizes the intensity at the desired level for both long and short pulses.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates A PID controller stabilizes the intensity at the desired level for both long and short pulses

Reference 9

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Observation a8ae012e-2636-47af-997b-d75472bf8918 · outbound

This paper cites A retroreflector mounted on a high-precision motorized translation stage controls the path-length difference between arms.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates A retroreflector mounted on a high-precision motorized translation stage controls the path-length difference between arms

Reference 10

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Observation 3f358a29-02c3-4cf3-8b76-ac50022c9119 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 11

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Observation b32320be-61f5-420f-950d-12cf44e48aa6 · outbound

This paper cites It slightly varies with the exciton-photon detuning:m= 5.9× 10−5 me forℏδ=−5.2 meV (Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates It slightly varies with the exciton-photon detuning:m= 5.9× 10−5 me forℏδ=−5.2 meV (Fig

Reference 12

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Observation 3fd5ab83-049a-4f02-8ced-a4b5175208a0 · outbound

This paper cites S3 2 3, the first-order coherence function, g(1)(∆x,∆y,∆t) , is ex- tracted at each time delay ∆tfrom the fringe visibility of the corresponding interferogram.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates S3 2 3, the first-order coherence function, g(1)(∆x,∆y,∆t) , is ex- tracted at each time delay ∆tfrom the fringe visibility of the corresponding interferogram

Reference 13

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Observation b49d76b7-9703-4cf2-b83a-7354fdf4a8ea · outbound

This paper cites S4.Measurement of the gain-curvature coefficientγ 2.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates S4.Measurement of the gain-curvature coefficientγ 2

Reference 14

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Observation 11476026-ae93-446b-8d4a-f2766d7b76ba · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 15

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Observation 80064b9d-8d4f-47aa-aedc-3329abba8be2 · outbound

This paper cites (24) of Sec.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates (24) of Sec

Reference 16

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Observation 5298ca21-3eb7-4145-bcb3-43cc4cef6852 · outbound

This paper cites These dispersive branches are most pro- nounced close to the condensation threshold, where the condensed fraction only marginally exceeds the non-condensed one.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates These dispersive branches are most pro- nounced close to the condensation threshold, where the condensed fraction only marginally exceeds the non-condensed one

Reference 17

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Observation f40d8363-a724-4e6e-85fc-b44739c419c0 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 18

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Observation f9094229-7a09-419b-b73c-2c7e9b89d8b0 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 19

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Observation 75ae19b6-0a6b-4976-9269-d3805053059a · outbound

This paper cites S8a 1) and amplitudeA 0 =|FFT| (see Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates S8a 1) and amplitudeA 0 =|FFT| (see Fig

Reference 20

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Observation 74c05125-595f-4842-b105-b6c6fe4b0efb · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 21

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Observation db2da20f-061c-4996-beb1-906300e78aa1 · outbound

This paper cites The result is shown in Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates The result is shown in Fig

Reference 22

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Observation 7c5b9def-6470-4d53-8909-8ef11ce55668 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 23

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Observation 3d40e5ae-9be7-4cfe-831a-fce68514b3a4 · outbound

This paper cites bellow) the upper (resp.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates bellow) the upper (resp

Reference 24

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Observation 4a60b69f-cd6e-483e-b244-f8155cdd6274 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 25

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Observation ccd3c46d-2995-42c7-bf75-725ba4e9939b · outbound

This paper cites We replicate and flip this quadrant to replace{k≤0, E≥0} and{k≥0, E≤0}(see Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates We replicate and flip this quadrant to replace{k≤0, E≥0} and{k≥0, E≤0}(see Fig

Reference 26

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Observation d8e5b803-227c-431f-9ddd-3e165bfc5a35 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 27

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Observation acb668d1-6b50-447a-b9f5-2c8a44379b26 · outbound

This paper cites The result is shown in Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates The result is shown in Fig

Reference 28

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Observation d0e8b563-3371-49dd-af91-4f8904cc23af · outbound

This paper cites We plot the spatial (temporal) experimental decay in logarithmic scales as a function of the expected KPZ scaling ∆r 2χ (∆t2β) (see Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates We plot the spatial (temporal) experimental decay in logarithmic scales as a function of the expected KPZ scaling ∆r 2χ (∆t2β) (see Fig

Reference 29

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Observation 1968a090-a403-458f-8d30-430ba3ed1887 · outbound

This paper cites 4 The phase diagram in Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates 4 The phase diagram in Fig

Reference 30

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Observation dd884797-e49d-4cf8-893d-810ff310a2b1 · outbound

This paper cites We first demonstrate additional data collapses onto the universal KPZ scaling function for different pump powers, using the dataset presented in Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates We first demonstrate additional data collapses onto the universal KPZ scaling function for different pump powers, using the dataset presented in Fig

Reference 31

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Observation 21881a7b-60a7-4105-9021-9201ba97eed4 · outbound

This paper cites The numerical integration is performed relying on two numerical schemes, used to propagate in time its deterministic and stochastic contributions respectively.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates The numerical integration is performed relying on two numerical schemes, used to propagate in time its deterministic and stochastic contributions respectively

Reference 32

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Observation 530f55fc-cc07-4ad6-9d41-29993c1c4b9b · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 33

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Observation 26cc0877-96e8-4d8d-b8a1-a6feef468eb6 · outbound

This paper cites Within Bogoliubov theory, it is signaled by a positive imaginary part of the excitation spectrum [33].

Crossing over universal scaling laws in two-dimensional driven dissipative condensates Within Bogoliubov theory, it is signaled by a positive imaginary part of the excitation spectrum [33]

Reference 34

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Observation c41feb02-ece5-4f7d-82b6-424e3b2ab9be · outbound

This paper cites 2 and 3 of the main text are closely reproduced.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates 2 and 3 of the main text are closely reproduced

Reference 35

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Observation f5789c91-f382-4cb4-b78c-6832820d2b0c · outbound

This paper cites We found that both KPZ and EW regimes are robust against variations of the pumping rateptrp, up to the onset of modula- tion instability.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates We found that both KPZ and EW regimes are robust against variations of the pumping rateptrp, up to the onset of modula- tion instability

Reference 36

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Observation 7455c006-b6b1-4aef-98df-b08fd7d00f98 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 37

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Observation 3adf07fc-0ad4-4ce3-b94b-b057e013bdaa · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 38

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Observation 6adb66f0-eb00-4480-9e75-408c91b73bcc · outbound

This paper cites The corresponding distance is denotedR NOS.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates The corresponding distance is denotedR NOS

Reference 39

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Observation aa8c299d-5f64-4dc8-8d38-3a43c4bcde63 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 40

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Observation 9a8f9a80-2de7-442f-9177-ed176bb04cc5 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 41

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Observation 77004a26-5d1b-47c2-b0e6-afece934e9b6 · outbound

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Crossing over universal scaling laws in two-dimensional driven dissipative condensates Unresolved cited work

Reference 42

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Observation 617475cb-4cb7-446f-bb7e-d1932b14c69d · outbound

This paper cites For instance, if two opposite charge defects are mutually the nearest neighbors of each other, they are classified as forming a dipole.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates For instance, if two opposite charge defects are mutually the nearest neighbors of each other, they are classified as forming a dipole

Reference 43

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Observation f6552627-e9b4-4460-8f86-ea6b58e7322b · outbound

This paper cites A typical instantaneous phase heat map after clustering is displayed in Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates A typical instantaneous phase heat map after clustering is displayed in Fig

Reference 44

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Observation 872f61ae-e671-4b23-89f1-7f1cdecc7ebe · outbound

This paper cites [49], which investigates the BKT tran- sition in semiclassical Monte Carlo simulations of 2D quasi-BECs at thermal equilibrium.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates [49], which investigates the BKT tran- sition in semiclassical Monte Carlo simulations of 2D quasi-BECs at thermal equilibrium

Reference 45

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Observation db6a3923-bd44-4f30-9bb2-d59ffe42749e · outbound

This paper cites The probability distribution of vortex (respectively antivortex) lifetimes is displayed in Fig.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates The probability distribution of vortex (respectively antivortex) lifetimes is displayed in Fig

Reference 46

Resolution: verified fuzzy; raw_fallback, observed 2026-08-10T12:05:43.772287Z

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Observation 363c1374-62b7-4dae-9292-65aa7370d8d6 · outbound

This paper cites Results in the KPZ regime are presented in Figs.

Crossing over universal scaling laws in two-dimensional driven dissipative condensates Results in the KPZ regime are presented in Figs

Reference 47

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