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Understanding the Phase of Responsivity and Noise Sources in Frequency-Domain Multiplexed Readout of Transition Edge Sensor Bolometers.
Farias, Nicole; Adkins, Tylor; de Haan, Tijmen; Lee, Adrian T; Lonappan, Anto; Russell, Megan; Suzuki, Aritoki; Siritanasak, Praween; Takatori, Sayuri; Westbrook, Benjamin.
Afiliación
  • Farias N; University of California Berkeley, Berkeley, CA 94720 USA.
  • Adkins T; University of California Berkeley, Berkeley, CA 94720 USA.
  • de Haan T; Institute of Particle and Nuclear Studies (IPNS), High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801 Japan.
  • Lee AT; International Center for Quantum-field Measurement Systems for Studies of the Universe and Particles (QUP), High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801 Japan.
  • Lonappan A; University of California Berkeley, Berkeley, CA 94720 USA.
  • Russell M; Institute of Particle and Nuclear Studies (IPNS), High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801 Japan.
  • Suzuki A; Lawrence Berkeley National Laboratory, Berkeley, CA 94720 USA.
  • Siritanasak P; University of Rome, 00185 Rome, Province of Rome Italy.
  • Takatori S; University of California, San Diego, San Diego, California 92093 USA.
  • Westbrook B; Lawrence Berkeley National Laboratory, Berkeley, CA 94720 USA.
J Low Temp Phys ; 216(1-2): 352-362, 2024.
Article en En | MEDLINE | ID: mdl-39070768
ABSTRACT
Cosmic microwave background (CMB) experiments have deployed focal planes with O ( 10 4 ) transition edge sensor (TES) bolometers cooled to sub-Kelvin temperatures by multiplexing the readout of many TES channels onto a single pair of wires. Digital Frequency-domain Multiplexing (DfMux) is a multiplexing technique used in many CMB polarization experiments, such as the Simons Array, SPT-3 G, and EBEX. The DfMux system studied here uses LC filters with resonant frequencies ranging from 1.5 to 4.5 MHz connected to an array of TESs. Each detector has an amplitude-modulated carrier tone at the resonant frequency of its accompanying LC resonator. The signal is recovered via quadrature demodulation where the in-phase (I) component of the demodulated current is in phase with the complex admittance of the circuit and the quadrature (Q) component is orthogonal to I. Observed excess current noise in the Q component is consistent with fluctuations in the resonant frequency. This noise has been shown to be non-orthogonal to the phase of the detector's responsivity. We present a detailed analysis of the phase of responsivity of the TES and noise sources in our DfMux readout system. Further, we investigate how modifications to the TES operating resistance and bias frequency can affect the phase of noise relative to the phase of the detector responsivity, using data from Simons Array to evaluate our predictions. We find that both the phase of responsivity and phase of noise are functions of the two tuning parameters, which can be purposefully selected to maximize signal-to-noise (SNR) ratio.
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Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: J Low Temp Phys Año: 2024 Tipo del documento: Article

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: J Low Temp Phys Año: 2024 Tipo del documento: Article