2010
DOI: 10.1063/1.3459142
|View full text |Cite
|
Sign up to set email alerts
|

High-speed phonon imaging using frequency-multiplexed kinetic inductance detectors

Abstract: We present a measurement of phonon propagation in a silicon wafer utilizing an array of frequency-multiplexed superconducting resonators coupled to a single transmission line. The electronic readout permits fully synchronous array sampling with a per-resonator bandwidth of 1.2 MHz, allowing submicrosecond array imaging. This technological achievement is potentially vital in a variety of low-temperature applications, including single-photon counting, quantum-computing, and dark-matter searches. (C) 2010 America… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
99
0

Year Published

2011
2011
2015
2015

Publication Types

Select...
8
1

Relationship

3
6

Authors

Journals

citations
Cited by 98 publications
(103 citation statements)
references
References 13 publications
(7 reference statements)
2
99
0
Order By: Relevance
“…If we assume that α particles were irradiated at the position of the resonator which gave a higher pulse height, we may be able to estimate the propagation velocity of athermal phonons. From the distance between the adjacent resonators of 1.6 mm, we make a rough estimation of the velocity to be 1.1-1.3 km/s, which is comparable to the results obtained by Swenson et al [5].…”
Section: Resultssupporting
confidence: 76%
“…If we assume that α particles were irradiated at the position of the resonator which gave a higher pulse height, we may be able to estimate the propagation velocity of athermal phonons. From the distance between the adjacent resonators of 1.6 mm, we make a rough estimation of the velocity to be 1.1-1.3 km/s, which is comparable to the results obtained by Swenson et al [5].…”
Section: Resultssupporting
confidence: 76%
“…Unlike traditional bolometric instruments, NIKA uses KIDs. The KIDs are superconducting resonators whose resonance frequency (∼1−2.5 GHz) changes linearly with the absorbed optical power (see for example Swenson et al 2010). Each resonator can be modeled by a complex transfer function in frequency with a real part I (in-phase) and imaginary part Q (quadrature; Grabovskij et al 2008).…”
Section: Observations With Nikamentioning
confidence: 99%
“…Obtaining a similar surface with KIDs would require hundreds of pixels for each LD, which is not a realistic option for experiments with ∼1000 detectors. This problem can be overcome following the phonon-mediated approach developed for Neutron Tansmutation Doped Ge thermistors 10 and for Transition Edge Sensors 11 , and recently proposed also for KIDs 12,13 .…”
Section: Introductionmentioning
confidence: 99%