In the quest to understand high-temperature superconductivity in copper oxides, debate has been focused on the pseudogap—a partial energy gap that opens over portions of the Fermi surface in the ‘normal’ state above the bulk critical temperature1. The pseudogap has been attributed to precursor superconductivity, to the existence of preformed pairs and to competing orders such as charge-density waves1,2,3,4. A direct determination of the charge of carriers as a function of temperature and bias could help resolve among these alternatives. Here we report measurements of the shot noise of tunnelling current in high-quality La2−xSrxCuO4/La2CuO4/La2−xSrxCuO4 (LSCO/LCO/LSCO) heterostructures fabricated using atomic layer-by-layer molecular beam epitaxy at several doping levels. The data delineate three distinct regions in the bias voltage–temperature space. Well outside the superconducting gap region, the shot noise agrees quantitatively with independent tunnelling of individual charge carriers. Deep within the superconducting gap, shot noise is greatly enhanced, reminiscent of multiple Andreev reflections5,6,7. Above the critical temperature and extending to biases much larger than the superconducting gap, there is a broad region in which the noise substantially exceeds theoretical expectations for single-charge tunnelling, indicating pairing of charge carriers. These pairs are detectable deep into the pseudogap region of temperature and bias. The presence of these pairs constrains current models of the pseudogap and broken symmetry states, while phase fluctuations limit the domain of superconductivity.
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The data used to produce the figures in the main text as well as in the Extended Data are provided with the paper. Data are also available online at https://doi.org/10.6084/m9.figshare.8247140 through the Springer Nature Research Data Support Service.
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Y. Zhang helped with TEM sample preparation and S. Yang with STEM EDX spectroscopy data acquisition. We are also grateful to P. Lee, S. Kivelson, D. Scalapino, J. Kono, M. Foster, T. C. Wu, J. C. Cuevas, P. Samuelsson, A. Gozar and I. Drozdov for their comments and questions. The research at Brookhaven National Laboratory, including heterostructure synthesis and characterization and device fabrication, was supported by the US Department of Energy, Basic Energy Sciences, Materials Sciences and Engineering Division. X.H. was supported by the Gordon and Betty Moore Foundation’s EPiQS Initiative through grant GBMF4410. The work at the University of Connecticut was supported by the US state of Connecticut. The research at Rice University was supported by the US Department of Energy, Basic Energy Sciences, Experimental Condensed Matter Physics award DE-FG02-06ER46337. Some of the Rice noise measurement hardware were acquired through National Science Foundation award DMR-1704264.
The authors declare no competing interests.
Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Extended data figures and tables
a, LSCO/LCO/LSCO film is grown on top of an LSAO substrate with a thin layer of in situ-deposited Au covering the film. b, The film is etched into about 20-μm-sized bars defined photolithographically. This is a deep etch all the way into the substrate. c, A second dry etch step removes part of the top LSCO and middle LCO layers, and stops in the middle of the bottom LSCO layer, creating mesas of 10–20 μm in diameter. d, A thick layer of Al2O3 (100 nm) is evaporated to isolate the future Au contacts (all 150 nm thick, one at the top and two at the bottom), to avoid parallel conduction paths. e, Contacts are defined lithographically and Au is evaporated to make contact with the top and bottom LSCO layers. f, A false-coloured scanning electron microscopy image of the device. g, STEM cross-section of a representative device structure, showing the atomic perfection of the ALL-MBE process.
a, R–T measurement on the Hall bar device fabricated in this film shows the superconducting transition temperature Tc = 38 K. b, Tunnelling differential conductance in a trilayer junction fabricated in this film. c, log–log plot of the I–V characteristics of two x = 0.15 tunnel junction devices, demonstrating device-to-device reproducibility and lack of any supercurrent down to pA levels at dilution refrigerator temperatures. Source data
a, Diagram of the two-channel cross-correlation method. b, The equivalent circuit diagram can be modeled as an RSCP circuit, where is is the noise source, RS is the (bias-dependent) differential resistance of the sample, CP is the parasitic capacitance in the system, and vna is the input voltage noise of the preamplifier.
Extended Data Fig. 5 RSCP model fitting, noise PSD calibration and example spectra of an LSCO tunnel junction.
a, The PSD of the JN voltage noise in a 2.17 kΩ resistor at T = 300 K, measured by the cross-correlation method. The red line is a fit based on the RSCP model. b, The JN voltage noise of various resistors at 300 K. The voltage noise SV has a simple linear dependence on the resistance of the resistor that is used as a calibration reference. c, The JN noise is also linearly dependent on temperature for a fixed resistor (2.17 kΩ). d, For a fixed resistor (2.17 kΩ), the JN noise is independent of the bias current, as expected for a macroscopic diffusive conductor. e–j, Example spectra of an LSCO tunnel junction for x = 0.15, recorded at T = 50 K. The d.c. bias current is marked for each panel. Red dashed lines are fits based on the RSCP circuit model. The sharp spikes result from environmental pickup of specific frequencies, and the fitting procedure is not influenced by these. Such environmental pickup is larger at the lowest temperatures below Tc. Source data
a, A relatively flat region (red) is selected to analyse the distribution of variations in the PSD. Sharp spikes are the environmental pickup of discrete frequencies; these are not used in the fitting procedure. b, c, The normalized PSD distribution in the selected region for a 96 s averaging time (b) and a 6 s averaging time (c). The red line is the Gaussian fit to the distribution. d, The standard deviation of the distribution for different averaging times. Source data
a–d, Noise measurements (blue points with error bars) and differential conductance (green) as a function of bias and temperature for a commercial Nb/AlOx/Nb tunnel junction that exhibits Josephson supercurrent below Tc = 9 K. The error bars combine in quadrature the systematic uncertainty described in Methods section ‘Error analysis’ and the standard error of the noise fitting parameter for each bias. e, Inferred pair fraction z as a function of bias and temperature for this device. The red dash–dotted line is the superconducting gap region outside which z = 0 is expected from the BCS theory for the measured value of Tc. The green dashed line is V = kBT/e. As eV/kBT → 0, determining z via noise measurements is not possible (see Methods). The grey region indicates where the uncertainty in z exceeds 0.5, on the basis of the systematic standard deviation of the noise ratio of ±0.015, as described in Methods section ‘Error analysis’. Source data
Noise data from Fig. 3 plotted as a function of bias current instead of bias voltage, and the noise data at 5 K compared with expectations of a very simplified MAR model. a–d, The red dashed line shows the single-charge tunnelling Poissonian expectation 2eIcoth(eV(I)/2kBT), based on the measured I(V) at each temperature. e, f, The red traces assume a bias-dependent effective charge based on kinetically allowed Andreev processes (q∗ = ne with 2Δ/n < eV < 2Δ/(n − 1), for n = 2, 3, …) for a fixed isotropic gap Δ, combined with a finite temperature expectation for the noise SI = 2q∗(V) × Icoth(q∗(V) × V/2kBT). Source data