Noise properties of a Josephson parametric oscillator Gopika Lakshmi Bhai1 2Hiroto Mukai1 2Tsuyoshi Yamamoto3 4and Jaw-Shen Tsai1 2 3y 1Graduate School of Science Tokyo University of Science

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Noise properties of a Josephson parametric oscillator
Gopika Lakshmi Bhai,1, 2, Hiroto Mukai,1, 2 Tsuyoshi Yamamoto,3, 4 and Jaw-Shen Tsai1, 2, 3,
1Graduate School of Science, Tokyo University of Science,
1–3 Kagurazaka, Shinjuku, Tokyo 162–0825, Japan
2RIKEN Center for Quantum Computing (RQC), 2–1 Hirosawa, Wako, Saitama 351–0198, Japan
3Research Institute for Science and Technology, Tokyo University of Science,
1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan
4Secure System Platform Research Laboratories, NEC Corporation, Kawasaki, Kanagawa 211-0011, Japan
(Dated: January 19, 2023)
We perform the noise spectroscopy of a Josephson parametric oscillator (JPO) by implementing
a microwave homodyne interferometric measurement scheme. We observe the fluctuations in the
self-oscillating output field of the JPO for a long 10 s time interval in a single shot measurement and
characterize the phase and amplitude noise. Furthermore, we investigate the effects of the pump
strength on the output noise power spectra of the JPO. We found strong fluctuations in the phase
with a 1/f2characteristics in the phase noise power spectrum, which is suppressed by increasing
the pump strength.
I. INTRODUCTION
The study of noise in physical systems has a long his-
tory [1]. The measurement and performance aspects of
the physical systems have long been considered to be lim-
ited by the noise [2–5]. Various studies have been done
extensively to understand the noise sources and the pos-
sibility of evading the noise [6–11]. However, evading the
intrinsic noise of a physical system is highly challenging
and is a fundamental limitation [12–14]. Recently, sev-
eral advances have led to a renewed interest in the char-
acterization and mitigation of noise in the field of circuit
quantum electrodynamics (c-QED) [11, 15–17] — one of
the most promising candidates in quantum computing
and quantum information processing [18–20]. The ongo-
ing quest to build a quantum computer has intensified
the efforts to study the noise in qubits [11, 15, 16] — the
basic building block of a quantum computer. However,
the noise properties of other essential components used
for the readout of the qubit, such as Josephson paramet-
ric amplifier (JPA) or JPO, are rarely explored.
A typical c-QED measurement network operates at fre-
quencies of a few GHz and a temperature of around 10
mK. Quantum devices such as qubits are commonly read
out at a few photon regimes to protect from measure-
ment backaction [11, 21, 22]. Low noise amplification
of the signal is a practical need to detect weak photons
from the quantum devices operating in the microwave
regime. JPA, a typical parametric device consisting of
a superconducting resonator integrated with Josephson
elements [23–27] overcomes this obstacle by effectively
amplifying the signal by adding a minimum noise allowed
by the fundamental law of quantum mechanics [14, 28].
These devices have become an essential component of
the readout chain since they attain the quantum-limited
gopika.lakshmibhai@gmail.com
tsai@riken.jp
amplification by high-frequency modulation of the induc-
tance of the nonlinear Josephson element [26, 29, 30].
When the modulation amplitude exceeds the instabil-
ity threshold, self-sustained oscillations start to build
up [31], and it works as an oscillator — Josephson para-
metric oscillator [32–34]. Due to the new accessible pa-
rameter regimes as a consequence of the strong nonlin-
ear properties of JPO, notable studies have been done
demonstrating the generation of squeezed states [35, 36],
two-mode entanglement [36], cat state engineering [37–
40], high-fidelity qubit readout [32, 33, 41], etc. Nonethe-
less, the study of the noise properties of the JPO is left
unaddressed.
JPOs, like any other oscillators, have ubiquitous
noise properties, which gives rise to a finite oscillation
linewidth typically ranging from a few kHz to Hz de-
pending on the operating parameters [34, 42–45]. Sev-
eral unifying theories explain the noise characteristics of
an oscillator [46–48]. Over the last few decades, various
experimental and theoretical studies in the optical do-
main have investigated the noise properties of parametric
oscillators and lasers extensively [49–53]. Noise spectro-
scopic studies in the optics field show the limiting factor
of the finite linewidth of lasers [13, 54] described by the
celebrated work of Schawlow-Townes [55]. These theories
and experimental observations shed light on investigat-
ing the noise properties of the JPO in superconducting
circuit systems, where a detailed study of the noise prop-
erties of the JPO is yet to be investigated.
In this work, we present the experimental study of
the noise characterization of a JPO pumped above its
parametric threshold, where the phase coherence of the
output photons from the oscillator is investigated. We
perform the spectral analysis of noise in the phase and
amplitude quadrature at low frequencies and explore the
possible noise sources in JPO.
arXiv:2210.15116v2 [quant-ph] 17 Jan 2023
2
II. EXPERIMENTAL SETUP
Our device consists of a λ/4 resonator made with
a segment of coplanar waveguide (CPW) terminated
by a dc superconducting quantum interference device
(SQUID) [26]. The CPW resonator is fabricated by etch-
ing out the sputtered niobium on a silicon wafer [56].
The Josephson junctions are then made by standard
double-angle shadow evaporation of aluminum [Fig. 1(b,
c)]. The presence of the SQUID makes the reso-
nance frequency of the resonator tunable by a vari-
able Josephson inductance LJwhich follows a relation
LJ= Φ0/(4πIc|cos (πΦdc/Φ0)|). Here, Icis the criti-
cal current through the junction, Φdc is the dc magnetic
flux through the SQUID, and Φ0is the flux quantum.
By changing the flux through the dc-SQUID Φdc, the
Josephson inductance can be varied.
An input signal and a pump signal are applied to the
device through the attenuated lines with filters to the
respective ports on the chip. On-chip dc bias is applied
through the same pump line using a bias-tee. The mea-
surements of the device are carried out in a cryogenic
environment using a dilution refrigerator at the base tem-
perature of 10 mK [Fig. 1(a)]. The output signal from
the device is routed through a microwave filter, circula-
tor, and isolator, which is amplified using a high-electron-
mobility transistor (HEMT) at 4K. The output signal is
then further amplified at room temperature using R.T
amplifiers.
At first, we characterize the system dynamics by scan-
ning the resonator frequency dependence on the applied
magnetic flux using a dc source. A weak probe signal is
coupled to the cavity through a circulator in the mix-
ing chamber, and the output from the device is ana-
lyzed using a vector network analyzer (VNA) by mea-
suring the complex reflection coefficient S11. The bare
resonator frequency in the absence of flux was found to
be ωr0/2π= 6.239 GHz. The estimated critical current
for each Josephson junction is 1.89 µA which is obtained
from fitting the resonator spectrum. The external and
internal cavity loss are found to be κext/2π= 11 MHz
and κint/2π= 0.3 MHz at a flux bias of Φdc/Φ0= 0.35
with a resonance frequency of ωr/2π= 5.94 GHz. To fur-
ther characterize the operational properties of the JPA,
we apply a pump signal with a frequency ωp2ωrwhere
ωris the resonator frequency at a specific flux point. The
pump photons interact with the incoming signal photons
and generate an amplified signal with an approximate
gain of 20 dB at pump power, Pp=63.4 dBm.
To investigate the photon generation, we apply the
pump signal at twice the resonance frequency in the ab-
sence of the input signal and examine the output from
the JPA by increasing the pump power Pp. As the
pump power increases beyond the parametric instabil-
ity threshold, self-sustained oscillations build up expo-
nentially in time inside the cavity. This can be under-
stood as a second-order phase transition from a ground
state below the threshold to an excited state above the
HEMT/ R.T.amps
Isolator
Circulator
LPF
BiasTee
dB
Attenuator
100 mK
800 mK
4 K
50 K
Output InputDC biasPump
JPO chip
300 K
20 dB
20 dB
10 dB
10 dB 0 dB
6 dB
10 dB
0 dB
20 dB
20 dB
10 dB 6 dB
10 dB 20 dB
20 dB
(a)
10 mK
R
H
(b) (c)
ωs
x 2
JPO
φ
I
Q
RF
LO
att
HPF
BPF
ADC
I(t)
Q(t)
(d)
doubler phase
shifter
Cryostat
HR
pump line
dc-SQUID
50 μm500 nm
sωs
~1.6 GHz
~12 GHz
(8.4 -13
GHz)
(4.9 - 6.2
GHz)
FIG. 1. (a) Schematic illustration of the cryogenic microwave
measurement setup. (b) Scanning electron microscope (SEM)
image showing SQUID consisting of two parallelly connected
Josephson junctions. The SQUID made of aluminum is gal-
vanically coupled to the central conductor of the CPW pat-
terned on a niobium film which is deposited on a silicon sub-
strate through sputtering. There are ground plane holes to
pin the trapped flux on the chip. (c) SEM image showing
Josephson junction made of Al/AlOx/Al. (d) Microwave in-
terferometric setup to measure the phase noise of the JPO:
input lines are color-coded with the cryogenic circuit lines in
Fig. 1(a), which describes the signal flow.
摘要:

NoisepropertiesofaJosephsonparametricoscillatorGopikaLakshmiBhai,1,2,HirotoMukai,1,2TsuyoshiYamamoto,3,4andJaw-ShenTsai1,2,3,y1GraduateSchoolofScience,TokyoUniversityofScience,1{3Kagurazaka,Shinjuku,Tokyo162{0825,Japan2RIKENCenterforQuantumComputing(RQC),2{1Hirosawa,Wako,Saitama351{0198,Japan3Resea...

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