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      Distinguishing coherent and thermal photon noise in a circuit QED system

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          Abstract

          In the cavity-QED architecture, photon number fluctuations from residual cavity photons cause qubit dephasing due to the AC Stark effect. These unwanted photons originate from a variety of sources, such as thermal radiation, leftover measurement photons, and crosstalk. Using a capacitively-shunted flux qubit coupled to a transmission line cavity, we demonstrate a method that identifies and distinguishes coherent and thermal photons based on noise-spectral reconstruction from time-domain spin-locking relaxometry. Using these measurements, we attribute the limiting dephasing source in our system to thermal photons, rather than coherent photons. By improving the cryogenic attenuation on lines leading to the cavity, we successfully suppress residual thermal photons and achieve \(T_1\)-limited spin-echo decay time. The spin-locking noise spectroscopy technique can readily be applied to other qubit modalities for identifying general asymmetric non-classical noise spectra.

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          Rapid Driven Reset of a Qubit Readout Resonator

          , , (2015)
          Using a circuit QED device, we demonstrate a simple qubit measurement pulse shape that yields fast ring-up and ring-down of the readout resonator regardless of the qubit state. The pulse differs from a square pulse only by the inclusion of additional constant-amplitude segments designed to effect a rapid transition from one steady-state population to another. Using a Ramsey experiment performed shortly after the measurement pulse to quantify the residual population, we find that compared to a square pulse followed by a delay, this pulse shape reduces the timescale for cavity ring-down by more than twice the cavity time constant. At low drive powers, this performance is achieved using pulse parameters calculated from a linear cavity model; at higher powers, empirical optimization of the pulse parameters leads to similar performance.
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            Microwave attenuators for use with quantum devices below 100 mK

            To reduce the level of thermally generated electrical noise transmitted to superconducting quantum devices operating at 20 mK, we have developed thin-film microwave power attenuators operating from 1 to 10 GHz. The 20 dB and 30 dB attenuators are built on a quartz substrate and use 75 nm thick films of nichrome for dissipative components and 0.001 mm thick silver films as hot electron heat sinks. The noise temperature of the attenuators was quantified by connecting the output to a 3D cavity containing a transmon qubit and extracting the dephasing rate of the qubit as a function of temperature and dissipated power P_d in the attenuator. The minimum noise temperature T_n of the output from the 20 dB attenuator was T_n less than and equal to 53 mK for no additional applied power and T_n about 120 mK when dissipating 30 nW. In the limit of large dissipated power (P_d > 1 nW) we find T_n proportional to P_d^(1/5.4), consistent with detailed thermal modeling of heat flow in the attenuators.
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              Author and article information

              Journal
              01 January 2018
              Article
              1801.00467
              6b5249ab-952a-4bb7-abab-4abbd021b6ab

              http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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