VHF Josephson Arbitrary Waveform Synthesizer, IEEE Transactions On Applied Superconductivity

CREATE TABLE fig3_transfer_function (
  "frequency_dependence_of_the_measured_digitizer_voltage_b581b734" VARCHAR  -- Frequency Dependence Of The Measured Digitizer Voltage Generated By The VHF-JAWS From 1 KHz To 50.05 MHz (transfer Function Freq (Hz)). The Rms Voltage (transfer Function Voltage (mV)) Measured Across The 50 Ohm Input Impedance Of The Digitizer Is Used To Calculate The Output Power (transfer Function Power (dBm)). This Data Was Taken At An RF AWG Bias Pulse Amplitude Of 0.43 And A Dc Bias Current Of Zero.,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2
);

CREATE TABLE fig5_bottom_dc_qlr (
  "dc_bias_current_qlrs_the_first_three_columns_are_the_f_f42f2b66" VARCHAR  -- DC Bias Current QLRs. The First Three Columns Are The Flattened Data For A Density Plot Of The Total Harmonic Distortion (dBc) Versus DC Offset Current (mA) For Waveform Frequencies Up To 50.05 MHz. The Last Three Columns Are Data For The Black Dashed Scatter Plot, Which Denotes The QLR Margin Minimum (mA) And QLR Margin Maximum (mA). All Data Is Taken At A Default RF AWG Pulse Amplitude (0.43 AWG V (p-p)).,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2,
  "unnamed_3" VARCHAR  -- Unnamed: 3,
  "unnamed_4" VARCHAR  -- Unnamed: 4,
  "unnamed_5" VARCHAR  -- Unnamed: 5
);

CREATE TABLE fig5_top_dc_qlr (
  "dc_bias_current_qlrs_rms_voltage_magnitude_mv_vs_dc_of_093a1b48" VARCHAR  -- DC Bias Current QLRs. RMS Voltage Magnitude (mV) Vs DC Offset (mA) 50 KHz, 150 KHz, 5.5 MHz, 15.05 MHz, 30.05 MHz, And 50.05 MHz Waveforms. The Rms Voltage Values For The 30.05 MHz Tone Shown Here And In The Figure Are +5.5 MV Higher Than The Measured Values. This Addition Was Included For Visual Clarity.,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2
);

CREATE TABLE fig6_bottom_pulse_amp_qlr (
  "pulse_amplitude_qlrs_total_harmonic_distortion_dbc_vs__a8040b12" VARCHAR  -- Pulse Amplitude QLRs. Total Harmonic Distortion (dBc) Vs Programmed Peak-to-peak Amplitude (AWG V (p-p)) For 50 KHz, 150 KHz, 5.5 MHz, 15.05 MHz, 30.05 MHz, And 50.05 MHz Waveforms.,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2
);

CREATE TABLE fig6_top_pulse_amp_qlr (
  "pulse_amplitude_qlrs_rms_voltage_magnitude_mv_vs_progr_9e053504" VARCHAR  -- Pulse Amplitude QLRs. RMS Voltage Magnitude (mV) Vs Programmed Peak-to-peak Amplitude (AWG V (p-p)) For 50 KHz, 150 KHz, 5.5 MHz, 15.05 MHz, 30.05 MHz, And 50.05 MHz Waveforms. The Rms Voltage Values For The 30.05 MHz Tone Shown Here And In The Figure Are +5.5 MV Higher Than The Measured Values. This Addition Was Included For Visual Clarity.,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2
);

CREATE TABLE fig7_bottom_slope_phase (
  "the_phase_of_the_complex_slope_of_the_measured_feedthr_de9bc720" VARCHAR  -- The Phase Of The Complex Slope Of The Measured Feedthrough Error, Relative To The Output Waveform Phase At 0.43 AWG, As A Function Of Pulse Amplitude (over 0.4-0.5 AWG V (p-p)) As A Function Of Output Waveform Frequency (MHz). The Complex Slope Calculated From The Change In The Measured Output Voltage While The System Is Quantum-locked (qlr Slopes Phase, Radians Normalized To JJ Voltage) Agrees With That Of The 10 DB-adjusted Feedthrough Error Measured Directly By Significantly Attenuating The Pulses (feed Slopes Phase, Radians Normalized To JJ Voltage) To Remove The JJ Voltage Contribution. Standard Uncertainties Of The Slope Phases Based On The Linear Regression Are Included In Radians.,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2,
  "unnamed_3" VARCHAR  -- Unnamed: 3,
  "unnamed_4" VARCHAR  -- Unnamed: 4,
  "unnamed_5" VARCHAR  -- Unnamed: 5
);

CREATE TABLE fig7_top_slope_mag (
  "the_magnitude_of_the_complex_slope_of_the_measured_fee_f32f3143" VARCHAR  -- The Magnitude Of The Complex Slope Of The Measured Feedthrough Error As A Function Of Pulse Amplitude (over 0.4-0.5 AWG V (p-p)) As A Function Of Output Waveform Frequency (MHz). The Complex Slope Calculated From The Change In The Measured Output Voltage While The System Is Quantum-locked (qlr Slopes Mag, (mV / AWG V (p-p))) Agrees With That Of The 10 DB-adjusted Feedthrough Error Measured Directly By Significantly Attenuating The Pulses (feed Slopes Mag, (mV / AWG V (p-p))) To Remove The JJ Voltage Contribution. Standard Uncertainties Of The Slope Magnitudes Based On The Linear Regression Are Included In MV / AWG V (p-p).,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2,
  "unnamed_3" VARCHAR  -- Unnamed: 3,
  "unnamed_4" VARCHAR  -- Unnamed: 4,
  "unnamed_5" VARCHAR  -- Unnamed: 5
);

CREATE TABLE fig8_bottom_x_intercept (
  "the_x_intercepts_of_the_fits_in_fig8_top_are_plotted_i_db1ea539" VARCHAR  -- The X-intercepts Of The Fits In Fig8 Top Are Plotted In AWG V (p-p). We Observe A Non-zero X-intercept Above ~6 MHz. Standard Uncertainties Of The X-intercepts Based On The Linear Regression Are Included In AWG V (p-p).,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2
);

CREATE TABLE fig8_top_direct_feed (
  "rms_voltage_magnitude_mv_measured_by_the_dut_digitizer_31229e73" VARCHAR  -- RMS Voltage Magnitude (mV) Measured By The DUT Digitizer At The Pattern Frequency Which Is Entirely Due To The Feedthough Error (at Several Frequencies Up To 50 MHz). This Voltage Is Plotted Versus Programmed Peak-to-peak Pulse Amplitude (AWG V (p-p)). Data Is Taken After Inserting 10 DB Of Additional Attenuation So That The JJs Do Not Contribute To The Voltage Waveform. The Voltages Shown Here, And In The Figure, Are Scaled Up By +10 DB From The Measured Voltages (they Are 10 DB Larger) To Show The Feedthrough Error During Normal Operation. We Perform Linear Regressions Of These Voltages (fit Direct Feed MV, Fit Direct Feed Pulse Amp) Over The Previously Identified Global Pulse Amplitude Quantum Locking Range (0.4-0.5 AWG V (p-p)).,
  "unnamed_1" VARCHAR  -- Unnamed: 1,
  "unnamed_2" VARCHAR  -- Unnamed: 2,
  "unnamed_3" VARCHAR  -- Unnamed: 3,
  "unnamed_4" VARCHAR  -- Unnamed: 4
);