The authors consider the problem of estimating the density g of independent and identically distributed variables Xi, from a sample Z1, . . . , Zn where Zi = Xi + ÏƒÎµi, i = 1, . . . , n, Îµ is a noiseâ€¦ (More)

We consider the problem of estimating the density g of identically distributed variables Xi, from a sample Z1, . . . , Zn where Zi = Xi + ÏƒÎµi, i = 1, . . . , n and ÏƒÎµi is a noise independent of Xiâ€¦ (More)

Thermal conductivity measurements have been performed on the superconducting ferromagnet UCoGe down to very low temperature and under magnetic field. In addition to the electronic quasiparticleâ€¦ (More)

In the regression model with errors in variables, we observe n i.i.d. copies of (Y, Z) satisfying Y = fÎ¸0(X) + Î¾ and Z = X + Îµ involving independent and unobserved random variables X, Î¾, Îµ plus aâ€¦ (More)

Nowadays, superconductors serve in numerous applications, from high-field magnets to ultrasensitive detectors of radiation. Mesoscopic superconducting devices, referring to those with nanoscaleâ€¦ (More)

Consider an autoregressive model with measurement error: we observe Zi = Xi + Îµi, where Xi is a stationary solution of the autoregressive equation Xi = fÎ¸0(Xiâˆ’1) + Î¾i. The regression function fÎ¸0 isâ€¦ (More)

The thermal conductivity of YbRh_{2}Si_{2} has been measured down to very low temperatures under field in the basal plane. An additional channel for heat transport appears below 30 mK, both in theâ€¦ (More)

We consider a failure hazard function, conditional on a time-independent covariate Z, given by Î·Î³0(t)fÎ²0(Z). The baseline hazard function Î·Î³0 and the relative risk fÎ²0 both belong to parametricâ€¦ (More)