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Many superconducting devices rely on the finite gap in the excitation spectrum of a superconductor: thanks to this gap, at temperatures much smaller than the critical one the number of excitations (quasiparticles) that can impact the…

Superconductivity · Physics 2024-09-05 P. B. Fischer , G. Catelani

In the superconducting state, the presence of a finite gap in the excitation spectrum implies that the number of excitations (quasiparticles) is exponentially small at temperatures well below the critical one. Conversely, minute…

Superconductivity · Physics 2023-05-31 P. B. Fischer , G. Catelani

The response of superconducting pair-breaking detectors is dependent on the details of the quasiparticle distribution. In Kinetic Inductance Detectors (KIDs), where both pair breaking and non-pair breaking photons are absorbed…

Superconductivity · Physics 2015-04-29 Tejas Guruswamy , David J. Goldie , Stafford Withington

Thin-film superconductors with thickness 30 to 500 nm are used as non-equilibrium quantum detectors for photons, phonons or more exotic particles. One of the most basic questions in determining their limiting sensitivity is the efficiency…

Superconductivity · Physics 2014-03-26 T. Guruswamy , D. J. Goldie , S. Withington

We study the effect of non-equilibrium quasiparticles on the operation of a superconducting device (a qubit or a resonator), including heating of the quasiparticles by the device operation. Focusing on the competition between heating via…

Mesoscale and Nanoscale Physics · Physics 2019-01-31 G. Catelani , D. M. Basko

Understanding the detailed behaviour of superconducting pair breaking photon detectors such as Kinetic Inductance Detectors requires knowledge of the nonequilibrium quasiparticle energy distributions. We have previously calculated the…

Superconductivity · Physics 2016-03-23 Tejas Guruswamy , David J. Goldie , Stafford Withington

We have calculated the non-equilibrium quasiparticle and phonon distributions $f(E)$, $n(\Omega)$, where $E$ and $\Omega$ are the quasiparticle and phonon energies respectively, generated by the photons of the probe signal of a low…

Superconductivity · Physics 2015-06-11 D. J. Goldie , S. Withington

Exchanging energy below the superconducting gap introduces quasiparticle energy distributions in superconducting quantum circuits, which will be responsible for their decoherence. This study examines the impact of quasiparticle energy on…

Measuring the internal quality factor of coplanar waveguide superconducting resonators is an established method of determining small losses in superconducting devices. Traditionally, the resonator losses are only attributed to two-level…

Quantum Physics · Physics 2025-07-25 Ashish Alexander , Christopher G. Weddle , Christopher J. K. Richardson

In a superconductor absorption of photons with an energy below the superconducting gap leads to redistribution of quasiparticles over energy and thus induces a strong non-equilibrium quasiparticle energy distribution. We have measured the…

Superconductivity · Physics 2014-02-04 P. J. de Visser , D. J. Goldie , P. Diener , S. Withington , J. J. A. Baselmans , T. M. Klapwijk

We perform time resolved photoelectron spectroscopy measurements of optimally doped $\tn{Bi}_2\tn{Sr}_2\tn{CaCu}_2\tn{O}_{8+\delta}$ (Bi-2212) and $\tn{Bi}_2\tn{Sr}_{2-x}\tn{La}_{x}\tn{Cu}\tn{O}_{6+\delta}$ (Bi-2201). The electrons dynamics…

Superconductivity · Physics 2016-03-18 C. Piovera , Z. Zhang , M. d'Astuto , A. Taleb-Ibrahimi , E. Papalazarou , M. Marsi , Z. Z. Li , H. Raffy , L. Perfetti

Photoexcited quasiparticle relaxation dynamics are investigated in a $YBa_{2}Cu_{3}O_{7-\delta}$ superconductor as a function of doping $\delta$ and temperature $T$ using ultrafast time-resolved optical spectroscopy. A model calculation is…

Superconductivity · Physics 2009-10-31 V. V. Kabanov , J. Demsar , B. Podobnik , D. Mihailovic

The correlated polar semimetal Ca$_3$Ru$_2$O$_7$ exhibits a rich phase diagram including two magnetic transitions ($T_N$=56 K and $T_C$=48 K) with the appearance of an insulating-like pseudogap (at $T_C$). In addition, there is a crossover…

Low temperature Kinetic Inductance Detectors (KIDs) are attractive candidates for producing quantumsensitive, arrayable sensors for astrophysical and other precision measurement applications. The readout uses a low frequency probe signal…

Instrumentation and Detectors · Physics 2014-01-13 D. J. Goldie , S. Withington

The density of quasiparticles typically observed in superconducting qubits exceeds the value expected in equilibrium by many orders of magnitude. Can this out-of-equilibrium quasiparticle density still possess an energy distribution in…

Propagation and relaxation of nonequilibrium quasiparticles in superconductors are of key importance for functioning of numerous nanoscale devices, enabling operation of some of them, and limiting the performance of the others. The…

Superconductivity · Physics 2020-10-21 Maciej Zgirski , Marek Foltyn , Alexander Savin , Andrii Naumov , Konrad Norowski

Nonequilibrium quasiparticle (QP) and phonon dynamics are central to the operation of superconducting devices. Superconducting detectors, such as the superconducting nanowire single-photon detector, perform best when a large QP population…

Ultrafast time-resolved optical spectroscopy in high-temperature superconductors enables the direct real-time measurement of non-equilibrium quasiparticle recombination dynamics. In addition, it also gives detailed information about the…

Superconductivity · Physics 2007-05-23 D. Mihailovic , J. Demsar

Non-equilibrium quasiparticle excitations degrade the performance of a variety of superconducting circuits. Understanding the energy distribution of these quasiparticles will yield insight into their generation mechanisms, the limitations…

Mesoscale and Nanoscale Physics · Physics 2018-10-16 K. Serniak , M. Hays , G. de Lange , S. Diamond , S. Shankar , L. D. Burkhart , L. Frunzio , M. Houzet , M. H. Devoret

The performance and scalability of superconducting quantum circuits are fundamentally constrained by non-equilibrium quasiparticles, which induce microwave losses that limit resonator quality factors and qubit coherence times. Understanding…

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