ライフサイエンスコーパス: superconducting

1 re integral to manipulating spintronic(1,2), superconducting(3,4), excitonic(5) and topological pheno

2 We show that the XFEL driven by a superconducting accelerator provides unprecedented beam

3 nt with a Luther-Emery liquid with power-law superconducting and charge density wave correlations ass

4 e parent state out of which the more fragile superconducting and correlated insulating ground states

5 We propose that the superconducting and correlated insulating orders are con

6 resulting in the appearance of gate-tunable superconducting and correlated insulating phases.

7 The coexistence of superconducting and correlated insulating states in magi

8 at temperatures well above the onset of the superconducting and correlated insulating states.

9 Between the superconducting and insulating regimes, we detected a ro

10 The discovery of superconducting and insulating states in magic-angle twi

11 ests that F-CDW correlations impact both the superconducting and normal state properties of YBCO.

12 However, integrating superconducting and optomechanical elements at cryogenic

13 salt-structured nitrides are known for their superconducting and refractory properties.

14 ffective interface system that provides both superconducting and topological states, opening a new ro

15 roach has been successfully applied to spin, superconducting, and Mott insulator systems.

16 nd isolators are disadvantageous in scalable superconducting architectures because they use magnetic

17 However, searching for superconducting aromatic molecular crystals remains elus

18 non of quantum wave mixing (QWM) on a single superconducting artificial atom.

19 om the ground state to an excited state of a superconducting artificial three-level atom can be track

20 ctor resulting in lower disparity and strong superconducting band gaps in the dominant crystal region

21 tic flux quantization in mesoscopic rings of superconducting beta-Bi(2)Pd thin films.

22 ons are resonantly coupled with photons in a superconducting cavity and a nanophotonic cavity at the

23 Here, we report an integrated superconducting cavity piezo-optomechanical platform whe

24 Here we consider a tunable superconducting cavity that can be used either as a tuna

25 nd fast characterization without requiring a superconducting cavity, thereby eliminating the need for

26 um interference devices (rf SQUIDs) inside a superconducting cavity.

27 demonstrate such coherence and control of a superconducting circuit incorporating graphene-based Jos

28 atible with a variety of quantum optical and superconducting circuit platforms, and already yields st

29 e we demonstrate a phase battery in a hybrid superconducting circuit.

30 Superconducting circuits are a competitive platform for

31 Our experiments demonstrate the power of superconducting circuits for studying strongly correlate

32 lopment, cavity quantum electrodynamics with superconducting circuits has emerged as a rich platform

33 Josephson junctions(1) converts macroscopic superconducting circuits into artificial atoms(2), enabl

34 Here we use superconducting circuits to explore strongly correlated

35 e will pave a new pathway of logical MBQC in superconducting circuits toward fault-tolerant quantum c

36 Superconducting circuits, for instance, have already bee

37 biquitously used in modern communication and superconducting circuits, this is the first time it has

38 ost structures become the building blocks of superconducting compounds at extreme conditions.

39 In contrast, for t' = 0, superconducting correlations fall off exponentially, whe

40 ctive interaction that drives unconventional superconducting correlations.

41 Their superconducting counterpart, the fully-gapped three-dime

42 he way for further exploration of this novel superconducting covalent metal.

43 It assigns optimal superconducting critical parameters to the unstrained st

44 hase shift in the quantum oscillation of the superconducting critical temperature.

45 nd SC are inhomogeneously distributed in the superconducting CuO(2) planes of LSCO.

46 e- and spin-density-wave (CDW/SDW) orders in superconducting cuprates has altered our perspective on

47 he primary field-induced state in underdoped superconducting cuprates is a PDW, with approximately ei

48 parent compound of high-[Formula: see text] superconducting cuprates is a unique Mott insulator cons

49 correlations are a ubiquitous feature of the superconducting cuprates, their disparate properties sug

50 een charge and lattice degrees of freedom in superconducting cuprates.

51 is a central enigma of the high-temperature superconducting cuprates.

52 bands present in the CuO(2) sheets of doped superconducting cuprates.

53 to be a promising candidate for topological superconducting devices to detect and manipulate Majoran

54 basis for a unique family of spintronic and superconducting devices, the interface transport phenome

55 ical phase and to realize hybrid topological superconducting devices.

56 c order below 4 kelvin for doping beyond the superconducting dome in thin films of electron-doped La(

57 Magnetic fields suppress this superconducting dome, unveiling the quantum phase transi

58 We also observe three new superconducting domes at much lower temperatures, close

59 nets, states with non-zero Chern numbers and superconducting domes occur frequently across a wide ran

60 rs, the vacated phase space is taken over by superconducting domes that feature critical temperatures

61 the same anti-PbO type structure but is not superconducting down to 1.8 K.

62 the film in the maximum, R(max) prior to the superconducting drop of R(T), exceeds R(q) = h/4e(2).

63 optically sensitive materials are often not superconducting, efficient coupling between these two ch

64 ent is introduced in a weak link between two superconducting electrodes by Andreev reflections.

65 e-of-mass momentum is a spatially modulating superconducting energy gap Delta(r), where r is a positi

66 nts of FeSe and to measure the corresponding superconducting energy gaps.

67 ic requirement for higher magnetic fields in superconducting energy-efficient magnets means we must u

68 rich phase diagram of correlated insulating, superconducting, ferromagnetic and topological phases(1-

69 urrent density than a homogeneously disorder superconducting film.

70 from high-temperature cuprates to ultrathin superconducting films - that experience superconductor-t

71 cillations in nanopatterned high-temperature superconducting films.

72 Above the temperature of superconducting fluctuations, we found that the pseudoga

73 [Formula: see text], along with an onset of superconducting fluctuations.

74 idual samples, grains containing the largest superconducting fraction were isolated.

75 The d-wave superconducting gap opens along the pocket, revealing th

76 Well outside the superconducting gap region, the shot noise agrees quanti

77 olayer MgB2 make a major contribution to the superconducting gap spectrum and density of states, clea

78 nce patterns taken at the zero energy in the superconducting gap support the presence of the topologi

79 s spectroscopic signatures consistent with a superconducting gap(3,4), although a zero-resistance sta

80 Deep within the superconducting gap, shot noise is greatly enhanced, rem

81 and extending to biases much larger than the superconducting gap, there is a broad region in which th

82 a finite, flat density of states inside the superconducting gap, which is a hallmark of linearly dis

83 e continuum of electronic states outside the superconducting gap.

84 nsation of Cooper pairs and protected by the superconducting gap.

85 Our findings suggest that the large superconducting gaps observed in FeSe films grown on dif

86 Evidence of a superconducting glass state is presented, as demonstrate

87 The superconducting grains were then characterized with a se

88 ase(11,12) from which various insulating and superconducting ground-state phases emerge at low temper

89 f the upper critical fields mu(0)H(c2)(T) of superconducting H(3)S under a record-high combination of

90 ematic studies of electronic properties of a superconducting half-Heusler compound YPtBi, in its norm

91 ven by the spin Hall effect, combined with a superconducting heater-cryotron bit-select element.

92 a localized MZM at the interface between the superconducting helical edge channel and the iron cluste

93 ecifications appropriate for applications in superconducting high performance and quantum computing c

94 promising results of novel high-temperature superconducting (HTS) shim coil prototypes that circumve

95 g-factor and high carrier mobility, however superconducting hybrids in these 2DEGs remain unexplored

96 dictions, and have suggested a new family of superconducting hydrides that possess a clathrate-like s

97 gle-electron transport through a topological superconducting island via a mechanism referred to as te

98 anowire networks with a predefined number of superconducting islands.

99 cting parent compound K(2)Fe(4)Se(5) and the superconducting K(2-x) Fe(4+y) Se(5) samples.

100 nt is zero when the phase difference between superconducting leads is zero.

101 n which the phase difference phi between the superconducting leads represents an additional tuning kn

102 n surface states, that is proximitized by Al superconducting leads.

103 mputing schemes utilizing Josephson junction superconducting logic, this obstacle is exacerbated by t

104 By contrast, superconducting magnets are widespread owing to their lo

105 paradigm of constructing quench-predictable superconducting magnets from Bi-2212.

106 s high as those generated by low-temperature superconducting magnets.

107 perature that has been confirmed so far in a superconducting material.

108 the design or predict the properties of new superconducting materials.

109 ironments, which simplifies integration with superconducting materials.

110 re helpful for a better understanding on the superconducting mechanism.

111 The world's first superconducting megahertz repetition rate hard X-ray fre

112 The development of superconducting memory and logic based on magnetic Josep

113 ization between bosonic qubits stored in two superconducting microwave cavities.

114 ive measurements that are implemented with a superconducting microwave cavity having the role of the

115 In conjunction with recently demonstrated superconducting microwave Chern insulators, we expect th

116 0.42 GHz) hypersonic phononic crystal with a superconducting microwave circuit.

117 inearity and single-mode squeezing(1,3) in a superconducting microwave resonator(4).

118 we present a 'bottom-up' method to create 3D superconducting nanostructures with prescribed multiscal

119 le grating with a single-element propagating superconducting nanowire detector of ultraslow-velocity

120 rate for the first time optical readout of a superconducting nanowire single-photon detector (SNSPD)

121 id-infrared emission spectrometer based on a superconducting nanowire single-photon detector, we obse

122 logical insulator Bi2Se3 thin films grown on superconducting NbSe2 single crystals.

123 ingle-particle tunneling measurements on the superconducting nickelate thin films.

124 lid structure, following by its coating with superconducting niobium (Nb).

125 inge states of bismuth(111) films grown on a superconducting niobium substrate and decorated with mag

126 High transparency superconducting niobium titanium nitride contacts are ma

127 Here we investigate superconducting niobium-titanium-nitride (Nb(1-x)Ti(x)N)

128 ing by coupling acoustic phonon sources with superconducting or spin qubits.

129 Moreover, the superconducting order parameter in T d-MoTe2 is determin

130 ed as a direct signature of an odd frequency superconducting order.

131 ng overall a-lattice parameter, it increases superconducting-ordering temperature in optimally cobalt

132 se to give rise to the exotic p-wave nematic superconducting pairing in the M(x)Bi(2)Se(3) (M = Cu, S

133 on-phonon interaction can induce more exotic superconducting pairing than the s-wave, consistent with

134 ns indicates a highly unconventional type of superconducting pairing.

135 te penetration of super-fast vortices into a superconducting Pb film at rates of tens of GHz and velo

136 l analysis indicates that the winding of the superconducting phase can induce a transition to a topol

137 ow-disorder devices reveal details about the superconducting phase diagram and its relationship to th

138 endence on temperature, and around which the superconducting phase forms a dome-shaped area in the ph

139 Here, we approach the superconducting phase from the more conventional overdop

140 The exact superconducting phase of K(2-x) Fe(4+y) Se(5) has so far

141 This superconducting phase stability suggests that UTe(2) is

142 llective quasicharge variable instead of the superconducting phase(23,24).

143 s a strong coupling between charge, spin and superconducting phase, able to break the phase rigidity

144 o increase the doping all the way to the non-superconducting phase.

145 electronic bands and strongly correlated and superconducting phases in magic-angle twisted bilayer gr

146 d-child' relation between the insulating and superconducting phases in moire graphene, and suggests a

147 meteorites are chemically inhomogeneous, and superconducting phases in them could potentially be minu

148 Here, we report the identification of superconducting phases in two meteorites, Mundrabilla, a

149 ating Majorana modes and probing topological superconducting phases in two-dimensional systems.

150 isplaying insulating(3-6), magnetic(7,8) and superconducting phases(4-6).

151 relationship to the principal pseudogap and superconducting phases.

152 e, a probe that is uniquely sensitive to the superconducting precursor, to uncover remarkable univers

153 ntally implement two quantum algorithms on a superconducting processor.

154 The remarkable high-pressure superconducting properties observed in the niobium-titan

155 Superconducting properties of Cr(0.0005)NbSe(2) (T(c)~6.

156 iour and an associated distinct weakening of superconducting properties.

157 Strong superconducting proximity effect and easy preparation of

158 rovides a comprehensive understanding of the superconducting proximity effect observed in QAH-superco

159 The superconducting proximity effect on the topological insu

160 Superconducting proximity pairing in helical edge modes,

161 f quantum states between microwave frequency superconducting quantum circuits and optical photons in

162 n and indispensable in the readout chains of superconducting quantum circuits.

163 miniature quantum memory elements in hybrid superconducting quantum circuits.

164 text] often dominate the loss mechanisms in superconducting quantum computation.

165 ill be critical for realizing fault-tolerant superconducting quantum computers.

166 ents combining magnonic elements with planar superconducting quantum devices.

167 onductivity, our devices are compatible with superconducting quantum electrodynamics architectures(11

168 ronomy(1), dark-matter axion searches(2) and superconducting quantum information science(3,4).

169 dependent low-spin states were recorded with superconducting quantum interference device (SQUID) meas

170 ), respectively, as shown by resistivity and superconducting quantum interference device (SQUID) meas

171 Superconducting quantum interference device (SQUID) meas

172 lux that it generates upon passage through a superconducting quantum interference device (SQUID)(4).

173 l known quantum phenomenon in a conventional superconducting quantum interference device (SQUID).

174 Here we use a nanoscale on-tip scanning superconducting quantum interference device (SQUID-on-ti

175 These flakes are characterized by superconducting quantum interference device magnetometry

176 n InAs/Al Josephson junctions measured via a superconducting quantum interference device.

177 sign consists of an array of radio-frequency superconducting quantum interference devices (rf SQUIDs)

178 ment of a variety of applications such as 3D Superconducting Quantum interference Devices (SQUIDs) fo

179 ecades earlier, where a double-planar SQUID (Superconducting Quantum Interference Devices) gradiomete

180 the magnetic field vector, highly sensitive Superconducting Quantum Interference Filters (SQIFs), an

181 demonstrate our approach experimentally on a superconducting quantum processor, building three-qubit

182 onstrate this error mitigation protocol on a superconducting quantum processor, enhancing its computa

183 , and offers an appealing platform to bridge superconducting quantum processors and optical telecommu

184 of quantum states between remotely connected superconducting quantum processors(1).

185 eport on the creation and investigation of a superconducting quasi-1D material with long-range ordere

186 ation of the quasiparticle excitation of the superconducting qubit and quantum entanglement between q

187 Three fundamental types of superconducting qubit are known(5), each reflecting a di

188 ineered non-Gaussian dephasing noise using a superconducting qubit as a sensor.

189 ping efficient, low-noise devices that match superconducting qubit frequencies (gigahertz) and bandwi

190 icular, piezo-mechanics operating at typical superconducting qubit frequencies features low thermal e

191 present measurements of a device in which a superconducting qubit is coupled to a SAW cavity, realis

192 al piezoelectric resonators with a microwave superconducting qubit on the same chip.

193 porating our Josephson-based isolator into a superconducting qubit setup, we demonstrate fast, high-f

194 o-level system such as a single spin(2-4), a superconducting qubit(5-7) or a single optical emitter(8

195 Here we introduce the missing superconducting qubit, 'blochnium', which exploits a coh

196 he emission and recapture of a phonon by one superconducting qubit, quantum state transfer between tw

197 Using a gigahertz superconducting qubit, we observed the quantization of a

198 frequency excitation of a transmon-a type of superconducting qubit-into an optical photon.

199 readout resonator coupled with an ancillary superconducting qubit.

200 n-insulator platform is compatible with both superconducting qubits and silicon photonics, and its no

201 Spin qubits and superconducting qubits are among the promising candidate

202 Superconducting qubits are one of the leading platforms

203 quantum walks on a quantum processor, using superconducting qubits as artificial atoms and tomograph

204 oss-Kerr interaction induced by intermediary superconducting qubits between neighbouring cavities und

205 ntum state in such a conversion process with superconducting qubits has not yet been achieved.

206 However, the coherence of superconducting qubits is affected by the breaking of Co

207 ould ultimately limit the coherence times of superconducting qubits of the type measured here to mill

208 magnetic field, allowing it to coexist with superconducting qubits on the same chip.

209 at can be directly interfaced with NbN-based superconducting qubits or SiC-based spin qubits.

210 n the giant-atom regime have been limited to superconducting qubits that couple to short-wavelength s

211 ng qubit, quantum state transfer between two superconducting qubits with a 67% efficiency, and, by pa

212 ave photons in a one-dimensional array of 12 superconducting qubits with short-range interactions.

213 mes of roughly 100 microseconds reported for superconducting qubits(15) and matches the timescales of

214 ort the use of a processor with programmable superconducting qubits(2-7) to create quantum states on

215 positioning of artificial atoms realized as superconducting qubits(8) along a one-dimensional wavegu

216 structure can be controlled and detected by superconducting qubits, enabling the coherent generation

217 ing two-photon quantum walks by exciting two superconducting qubits, we observed the fermionization o

218 erface with leading quantum hardware such as superconducting qubits.

219 ns, enabling the quantum entanglement of two superconducting qubits.

220 cold atoms, trapped ions, Rydberg atoms, and superconducting qubits.

221 Superconducting resonators with high quality factors hav

222 rally set by the applied field, controls the superconducting response.

223 ifts with annealing time was observed in the superconducting samples only.

224 of these nano-scale phase admixtures in the superconducting samples.

225 The direct identification of the nodal superconducting (SC) gap structure is challenging, partl

226 ation measurements show that polycrystalline superconducting (SC) K(1.9)Fe(4.2)Se(5) has a critical t

227 ng the pair density wave (PDW), in which the superconducting (SC) order parameter is oscillatory in s

228 to TSC using magnetic flux applied to a full superconducting shell surrounding a semiconducting nanow

229 elastic neutron scattering measurements on a superconducting single crystal of Sr(0.1)Bi(2)Se(3), a p

230 ence of the topological superconductivity in superconducting Sn(1-) (x) Pb(x) Te.

231 so discuss the recent observation of a large superconducting spin-valve effect with a T c change 1 K

232 alous phase, and opens new opportunities for superconducting spintronics, and new possibilities for r

233 lous Josephson effect-the hallmark effect of superconducting spintronics-which can be characterized b

234 n developing of a field of research known as superconducting spintronics.

235 Isostructural examples include bulk superconducting Sr(2)RuO(4) (ref.

236 phase width of 0.01<x<0.04 and identify the superconducting state below 8 K, which in contrast to ea

237 ansition between a trivial and a topological superconducting state by controlling the phase differenc

238 , a record-high pressure up to which a known superconducting state can continuously survive.

239 udogap state from which the high-temperature superconducting state emerges.

240 This implies that an inhomogeneous superconducting state exists, in which some regions show

241 relativistic' physics of a proximity-induced superconducting state in a topological Kondo insulator.

242 In this study we observed the reproducible superconducting state in Cd(3)As(2) thin films without a

243 e we use high magnetic fields to destroy the superconducting state in FeSe(1-x)S(x) and follow the ev

244 e control, on the micrometer scale, over the superconducting state in samples of the heavy-fermion su

245 The superconducting state is formed by the condensation of C

246 The superconducting state is observed over a broad pressure

247 In that context, the superconducting state of the quasi-two-dimensional and s

248 By investigating the bulk superconducting state via dc magnetization measurements,

249 ing line(6) and the possible transition to a superconducting state(7).

250 eld Hc2, a fundamental characteristic of the superconducting state, has been subject to strong contro

251 reversed electrochemically to reinstate the superconducting state.

252 topological quantum phase transition in the superconducting state.

253 tent with a drop in spin polarization in the superconducting state.

254 energy excitations that are protected in the superconducting state.

255 e repeatedly and reliably between normal and superconducting states demonstrate the great potential o

256 emonstrated in the correlated insulating and superconducting states observed in magic-angle twisted-b

257 iton trapping(2-5), host Mott insulating and superconducting states(6) and act as unique Hubbard syst

258 fect the phase diagram of the correlated and superconducting states.

259 e Bean-Livingston barrier at the edge of the superconducting strip in an external magnetic field.

260 Transport characteristics of nano-sized superconducting strips and bridges are determined by an

261 Studies of nanoscale superconducting structures have revealed various physica

262 ogy of a two-component (electron and proton) superconducting superfluid condensate(2,3).

263 onality to combine the two worlds of quantum superconducting systems and photonics systems.

264 er with developing SDW stripe order near the superconducting T(c).

265 n of practical, large-scale systems based on superconducting technologies.

266 oundaries, giving a larger T(N) and a higher superconducting temperature (T(c)) upon the application

267 ange metal phases, and ultimately their high superconducting temperatures.

268 be stabilized in two slightly different non-superconducting tetragonal phases, PI and PII, through t

269 ich allows rapid and safe quenching from the superconducting to the normal state(5-10).

270 Superconducting topological crystalline insulators are e

271 tion, our investigations have determined the superconducting transition by focusing on the detailed t

272 The volume fraction of superconducting transition strongly depends on the annea

273 45% without structural phase transition, the superconducting transition temperature (T(C) ) increases

274 h a slope that scales monotonically with the superconducting transition temperature (T(C) with H = 0)

275 The increase in superconducting transition temperature (T(C)) of Sn nano

276 t Mott state as a strategy for enhancing the superconducting transition temperature in cuprates.

277 that, in FeSe/SrTiO(3) heterostructures, the superconducting transition temperature in FeSe monolayer

278 y-fermion superconductor UTe(2), which has a superconducting transition temperature of 1.6 kelvin(5).

279 ng from elemental precursors, with a maximum superconducting transition temperature of 287.7 +/- 1.2

280 response of Nd(0.8)Sr(0.2)NiO(2) indicate a superconducting transition temperature of about 9 to 15

281 honon softening has a major influence on the superconducting transition temperature of Sn nanostructu

282 The highest superconducting transition temperature of the monolayer

283 X-ray scattering, were used to calculate the superconducting transition temperature using the Allen-D

284 sults showing the pressure dependence of the superconducting transition temperature, T(c), near to op

285 f T(C) show an increase compared to the bulk superconducting transition temperature.

286 FeSe which is a pseudogaped metal above the superconducting transition temperature.

287 The superconducting transition temperatures ( T(c)) of the d

288 e have discovered a common resurgence of the superconducting transition temperatures (T(c)s) of the m

289 The sharpest superconducting transition was observed for diamond grow

290 wurtzite nitrides and rocksalt structure of superconducting transition-metal nitrides.

291 (3)/FeTe heterostructure associated with the superconducting transition.

292 MFMMS measurements detected superconducting transitions in samples from each, above

293 trapped atomic ions(11,12) or cavity-coupled superconducting transmons(13).

294 ruction to two hole concentrations where the superconducting upper critical fields are found to be en

295 temperature (T (c)) of ~31 K with a varying superconducting volume fraction, which strongly depends

296 We examine driven superconducting vortices interacting with quenched disor

297 ects in irradiated-annealed high temperature superconducting wires based on epitaxial Y(Dy)BCO film.

298 However, superconducting wires for high-field-magnet applications

299 -treatment (HT) temperature theta in Nb(3)Sn superconducting wires made by the restacked-rod process

300 The fast optical generation of superconducting zero resistance state is non-volatile bu