Data for: Observing dynamical phases of BCS superconductors in a cavity QED simulator
Data files
Nov 20, 2023 version files 46.55 MB
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fig2b_expt_timetraces.csv
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fig2b_simfull_timetraces_finesample.csv
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fig2b_simfull_timetraces.csv
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fig2b_simideal_timetraces_finesample.csv
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fig2b_simideal_timetraces.csv
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fig2c_expt_avggap.csv
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fig2c_expt_lifetime.csv
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fig2c_simfull_avggap.csv
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fig2c_simideal_avggap.csv
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fig2d_expt_timetraces.csv
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fig3b_expt_timetraces.csv
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fig3b_simfull_timetraces_finesample.csv
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fig3b_simfull_timetraces.csv
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fig3b_simideal_timetraces_finesample.csv
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fig3b_simideal_timetraces.csv
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fig3d_expt_PSDs.csv
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fig3e_expt_oscamps.csv
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fig3e_simfull_oscamps.csv
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fig3e_simideal_oscamps.csv
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fig3f_expt_oscfreqs.csv
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fig3f_simfull_oscfreqs.csv
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fig3f_simideal_oscfreqs.csv
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fig4a_expt_timetraces.csv
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fig4a_simfull_timetraces_finesample.csv
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fig4a_simfull_timetraces.csv
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fig4a_simideal_timetraces_finesample.csv
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fig4a_simideal_timetraces.csv
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fig4b_expt_avggap.csv
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fig4b_simfull_avggap.csv
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fig4b_simideal_avggap.csv
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fig4c_expt_oscfreqs.csv
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fig4c_simfull_oscfreqs.csv
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fig4c_simideal_oscfreqs.csv
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figed4a_expt_timetraces.csv
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figed4a_peaktrough_times.csv
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figed4a_simfull_timetraces.csv
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figed4a_simideal_timetraces.csv
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figed4b_expt_higgsfreqs.csv
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figed4b_simideal_higgsfreqs.csv
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figed4c_expt_higgsfreqs_gap.csv
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figed4c_simideal_higgsfreqs_gap.csv
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README.md
Abstract
In conventional Bardeen-Cooper-Schrieffer (BCS) superconductors, electrons with opposite momenta bind into Cooper pairs due to an attractive interaction mediated by phonons in the material. While superconductivity naturally emerges at thermal equilibrium, it can also emerge out of equilibrium when the system's parameters are abruptly changed. The resulting out-of-equilibrium phases are predicted to occur in real materials and ultracold fermionic atoms but have not yet all been directly observed. Here we realise an alternate way to generate the proposed dynamical phases using cavity quantum electrodynamics (cavity QED). Our system encodes the presence or absence of a Cooper pair in a long-lived electronic transition in 88Sr atoms coupled to an optical cavity and represents interactions between electrons as photon-mediated interactions through the cavity. To fully explore the phase diagram, we manipulate the ratio between the single-particle dispersion and the interactions after a quench and perform real-time tracking of subsequent dynamics of the superconducting order parameter using non-destructive measurements. We observe regimes where the order parameter decays to zero (phase I), assumes a non-equilibrium steady-state value (phase II), or exhibits persistent oscillations (phase III). This opens up exciting prospects for quantum simulation, including the potential to engineer unconventional superconductors and to probe beyond mean-field effects like the spectral form factor, and for increasing coherence time for quantum sensing.
README: Data for: Observing Dynamical Phases of BCS Superconductors in a Cavity QED Simulator
https://doi.org/10.5061/dryad.7h44j100j
This repository contains the data (both experimental and from simulations) plotted in the associated manuscript.
Description of the data and file structure
Files are named according to the following naming convention: [ASSOCIATED FIGURE]_[DATA SOURCE]_[DESCRIPTION OF DATA].csv
. See the explanation below:
[ASSOCIATED FIGURE]
references the figure of the manuscript where the data is plotted. This repository contains data fromfig2
,fig3
,fig4
, andfiged4
, which are the four figures containing experimental data. All of these figures contain sub-panels which are labeled alphabetically. For example, data from Fig. 3, panel f is referenced byfig3f
.[DATA SOURCE]
specifies whether the data is derived from raw experimental data (expt
) or from theoretical simulations (simideal
orsimfull
). Note that many figure panels feature data from multiple sources. For clarity, we have uploaded data from different sources as separate files. We use two different models to simulate our system (see manuscript for a detailed description of how the models are defined).simideal
refers to so-called "ideal" simulations as described in the paper, which ignore single-particle dissipation and motion of our atoms along the cavity axis.simfull
refers to "full" simulations of the experiment, which attempt to capture all technical details of the experiment.
[DESCRIPTION OF DATA]
is meant to be a short semantic identifier describing the type of data included in the file. We define the identifiers here:- Files labeled with
timetraces
contain time dynamics of the order parameter ΔBCS. The first column is time expressed in μs. The remaining columns describe ΔBCS for different values of our control parameters (χN, δs, φ0). We indicate the value of any scanned parameters in the header text: for example, the headerchiN_0.109_MHz
indicates that this column was taken at χN = 2π * 0.109 MHz.timestraces_finesample
files represent simulation data with a parameter sweep finer than what is realized in the experiment. These files are larger due to the many parameter values simulated.
- Files labeled with
oscfreqs
oroscamps
measure the oscillation frequency or amplitude of ΔBCS. These values are plotted against the relevant control parameter in the first column. - Files labeled with
avggap
measure the average value of ΔBCS at long times (as defined in the manuscript), plotted against the relevant control parameter. - Files labeled with
lifetime
measure the 1/e coherence time of ΔBCS. - Files labeled with
PSDs
describe the power spectra of ΔBCS. - Files labeled with
peaktrough_times
measure the detected time positions of the first peak and trough of curves in Extended Data Fig. 4. - Files labeled with
higgsfreqs
measure the oscillation frequency of transient "Higgs"-like behavior in Extended Data Fig. 4, plotted against the control parameter φ0. These frequencies are inferred from the peak and trough times frompeaktrough_times
files.higgsfreqs_gap
files also report the Higgs oscillation frequency, this time plotted against the quantity 2Δ∞ as defined in the manuscript.
- Files labeled with
The data is expressed in the same units present in the figures. For completeness, we describe the units here:
- Time values are written in units of μs, indicated by the header label
"Time_us"
. - Frequency values are expressed in MHz and represent cycles/sec as opposed to angular units. These column headings are typically written like
"fosc_MHz"
. - The control parameter φ0, representing an initial phase spread of the atomic ensemble as defined in the manuscript, is reported in units of π as indicated in the header
phi0_pi
. For example, a reported value of 0.418 indicates that φ0 = 0.418π. - Plots of the order parameter ΔBCS are typically unitless and normalized to the initial value.
- The exception to this is in Extended Data Fig. 4a (
figed4a
), which plots ΔBCS as a frequency in MHz. - Data representing oscillation amplitudes in time traces of ΔBCS are also unitless and are normalized in the same way as ΔBCS itself.
- The exception to this is in Extended Data Fig. 4a (
- The power spectral densities (PSDs) from
fig3d
are expressed in arbitrary units.
Below, we describe how error bars are reported:
- All error bars represent the standard error of the mean for the relevant quantity.
- Error bars are reported a separate column and are typically indicated in the header with a
d
in front of the measured value. For example, the error bars for oscillation frequencies reported asfoscs_MHz
are labeled with a headerdfoscs_MHz
. - For some traces, we provide both statistical error bars and uncertainties to systematic corrections. These are reported as separate columns and are indicated by, for example,
dfoscs_stat_MHz
anddfoscs_sys_MHz
respectively. - For some traces, we allow for asymmetric error bars. These are expressed with
l
orr
characters, representing left-hand and right-hand errors respectively. For example:dfl_MHz
,dfr_MHz
.