The datasets were acquired with the Labber software and can be openend with the Labber databrowser.
In order to execute the scripts the Labber python API must be installed.

Fig 1: Analysis script: SOIPaperStabilityDiagram.py
c) '2021//01//Data_0111\PLL-PLR_largerLB' 

d, e, f) '2020//09//Data_0922\FunnelvsAngle' 
Description: The dataset contains the Funnel measurements as a function of magnetic field angle.
It is a 3-dimensional dataset. x-axis: Bfield strength, y-axis: detuning, z-axis: magnetic field angle 

Fig 2: Analysis script: SOIPaperRabivsAngleFigure (contains also simulations of the frequencies overlaid on the FFT in b) and d))
a) '2020//11//Data_1123//Rabiat2mTvsAngle' (b) is FFT of a))
Description: measurement of ST0 oscillations at 2mT vs magnetic field angle. the x-axis is duration, the y-axis is magnetic field angle.

c)'//2020//1123\Rabiat2mTvsAngleRamped' (d) is FFT of c))
Description: measurement of ST- oscillations at 2mT vs magnetic field angle. the x-axis is duration, the y-axis is magnetic field angle.

Fig 3: script SOIPaperLZFigure
b) c)

2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_90_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_85_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_80_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_75_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_70_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_65_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_60_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_55_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_50_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_45_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_40_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_35_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_30_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_25_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_20_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_15_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_10_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_5_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_0_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-5_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-10_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-15_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-20_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-25_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-30_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-35_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-40_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-45_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-50_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-55_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-60_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-65_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-70_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-75_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-80_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-85_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2
2020//11//Data_1127//LandauZenerTrasition_8mVdetuning_20_mT_-90_deg_20timesi_StartTime0times100QuarterSamplingRateReverseRamp_2


Fig 4:
simulation script SOIPaperFunnelFigureSupplementary.py

Fig S1: Analysis script: SOIPaperStabilityDiagram.py


Fig S2:
b) '//2020//08//Data_0810//ConfigForRamseyOutRB+100mV.hdf5'

Fig S3: script: SOIPaperRabiinPlaneFigure.py
a)'//2020//1116\RabiInPlaneHalfamplitude_4' 
b) FFT of a)

Fig S4: script: SOIPaperRabiinPlaneFigure.py
The script also contains the simulations overlaid to the FFTs.
a) '//2020//1116//Rabi5degHalfamplitude' 
b) FFT of a)
c) '//2020//1116//Rabi10degHalfamplitude' 
d) FFT of c)
e) '//2020//1116//Rabi20degHalfamplitude'
f) FFT of e)
g) '//2020//1116//Rabi30degHalfamplitude'
h) FFT of g)


Fig S5: '2020//12//Data_1214\FunnelVsangle'
the funnel vs angle on the other (1,1)->(0,2) transition

Fig S6: Simulations contained in script SOIPaperLZFigure

Fig S7: Analysis done on data from Fig 3. Analysis script SOIPaperLZFigure

Fig S8: Data is from Fig S4.