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Josephson scanning tunneling spectroscopy in superconducting phases coexisting with pair-, charge- and spin-density-waves

Alyson Laskowski, Jasmin Bedow, Dirk K. Morr

Abstract

We demonstrate that the recent observations of spatial oscillations in the energy position of the superconducting coherence peaks in the cuprate, transition metal dichalcogenide, iron-based and heavy-fermion superconductors are consistent with the possible presence of a pair-, charge- or spin-density-wave phase. We show that for all three cases, the spatial oscillations of the superconducting order parameter, $Δ({\bf r})$ can be imaged via the critical Josephson current, $I_c({\bf r})$ measured in Josephson scanning tunneling spectroscopy experiments. Finally, we show that the spatial oscillations of the density waves and of $Δ({\bf r})$ exhibit relative phase shifts of $Δφ= 0$ or $π$ for a charge-density wave, and $Δφ=π/2$ for the spin-density wave.

Josephson scanning tunneling spectroscopy in superconducting phases coexisting with pair-, charge- and spin-density-waves

Abstract

We demonstrate that the recent observations of spatial oscillations in the energy position of the superconducting coherence peaks in the cuprate, transition metal dichalcogenide, iron-based and heavy-fermion superconductors are consistent with the possible presence of a pair-, charge- or spin-density-wave phase. We show that for all three cases, the spatial oscillations of the superconducting order parameter, can be imaged via the critical Josephson current, measured in Josephson scanning tunneling spectroscopy experiments. Finally, we show that the spatial oscillations of the density waves and of exhibit relative phase shifts of or for a charge-density wave, and for the spin-density wave.

Paper Structure

This paper contains 10 equations, 5 figures.

Figures (5)

  • Figure 1: Spatial and energy dependence of the LDOS for a mixed PDW phase with four different wavelengths: (a) $\lambda = 200 a_0 = 8\xi$, (b) $\lambda = 100 a_0 = 4\xi$, (c) $\lambda = 50 a_0 = 2\xi$, (d) $\lambda = 25 a_0 = \xi$ and (e) $\lambda = 4 a_0 = 0.16\xi$. (f)-(j) show the spatial dependence of the normalized Josephson critical current $I_{c}(\mathbf{r})/I_{c}^{\text{avg}}$ with $\Delta_{\text{tip}} = \Delta_0$ (dashed red) and of $\Delta(\mathbf{r})/\Delta_{0}$ (solid black) for the corresponding cases in (a)-(e). Parameters are $(\Delta_0, \Delta_\mathrm{PDW}, \mu_0, \Delta \mu, JS) = (0.05, 0.015, -3.6, 0,0)t$. For (a)-(e), we set $\Gamma = 0.0025t$, while for (f)-(j) $\Gamma = 0.1t$.
  • Figure 2: Spatial and energy dependence of the LDOS for a mixed CDW phase with four different wavelengths:(a) $\lambda = 200 a_0 = 8\xi$, (b) $\lambda = 100 a_0 = 4\xi$, (c) $\lambda = 50 a_0 = 2\xi$, (d) $\lambda = 25 a_0 = \xi$, and (e) $\lambda = 4 a_0 = 0.16\xi$. (f)-(j) show the spatial dependence of the normalized Josephson critical current $I_{c}(\mathbf{r})/I_{c}^{\text{avg}}$ with $\Delta_{\text{tip}} = \Delta_0$ (dashed red) and of $\Delta(\mathbf{r})/\Delta^{\text{avg}}$ (solid black) and charge density $\rho(\mathbf{r})$ (dashed blue) for the corresponding cases in (a)-(e). Parameters are $(\Delta_0, \Delta_\mathrm{PDW}, \mu_0, \Delta \mu, JS) = (0.05, 0, -3.6, 0.45, 0)t$. For (a)-(e), we set $\Gamma = 0.0025t$, while for (f)-(j) $\Gamma = 0.1t$.
  • Figure 3: (a) Spatial and energy dependence of the LDOS for a CSC phase with $\lambda = 200 a_0 = 8\xi$, for a more than half-filled electronic band. (b) Spatial dependence of the normalized Josephson critical current $I_{c}(\mathbf{r})/I_{c}^{\text{avg}}$ with $\Delta_{\text{tip}} = \Delta_0$ (dashed red) and of $\Delta(\mathbf{r})/\Delta^{\text{avg}}$ (solid black) and $\rho(\mathbf{r})$ (dashed blue), corresponding to (a). Parameters are $(\Delta_0, \Delta_\mathrm{PDW}, \mu_0, \Delta \mu, JS) = (0.05, 0, 3.6, 0.45, 0)t$. For (a), we set $\Gamma = 0.0025t$, while for (b) $\Gamma = 0.1t$.
  • Figure 4: Spatial and energy dependence of the LDOS for a mixed SDW phase with four different wavelengths: (a) $\lambda = 200 a_0 = 8\xi$, (b) $\lambda = 100 a_0 = 4\xi$, (c) $\lambda = 50 a_0 = 2\xi$, (d) $\lambda = 25 a_0 = \xi$, and (e) $\lambda = 8 a_0 = 0.32\xi$. (f)-(j) show the spatial dependence of the normalized Josephson critical current $I_{c}(\mathbf{r})/I_{c}^{\text{max}}$ with $\Delta_{\text{tip}} = \Delta_0$ (dashed red) and of $\Delta(\mathbf{r})/\Delta^{\text{max}}$ (solid black) for the corresponding cases in (a)-(e). The spatial dependence of the spin polarization $S(\mathbf{r})$ (dashed blue) is additionally shown in (f) and (g). Parameters are $(\Delta_0, \Delta_\mathrm{PDW}, \mu_0, \Delta \mu, JS) = (0.05, 0.0, -3.6, 0.0, 0.2)t$. For (a)-(e), we set $\Gamma = 0.0025t$, while for (f)-(j) $\Gamma = 0.1t$.
  • Figure 5: (a) Mixed PDW for wavelength $\lambda = 50 a_0 = 2\xi$ with same parameters as Fig. \ref{['fig:Fig2']}. (b) Mixed CDW for wavelength $\lambda = 50 a_0 = 2\xi$ with same parameters as Fig. \ref{['fig:Fig3']}. (c) Mixed SDW for wavelength $\lambda = 100 a_0 = 4\xi$ with same parameters as Fig. \ref{['fig:Fig4']}. (d) Figure 2(g) of Ref.Kong2025.