ライフサイエンスコーパス: superconducting

1 ronic properties, ranging from insulating to superconducting.

2 phase transitions and also identify trivial-superconducting and commensurate/incommensurate charge-d

3 chnologically important thin films (e.g. for superconducting and magnetic devices), was analysed usin

4 Superconducting and topological states are two most intr

5 is the first 2D material that supports both superconducting and topological states, offering an exci

6 photon source based on a fully controllable superconducting artificial atom strongly coupled to an o

7 , we investigate the diffusive dynamics of a superconducting artificial atom under continuous homodyn

8 ields in two microwave cavities bridged by a superconducting artificial atom, which can also be viewe

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

10 for quantum information processing using the superconducting artificial atoms.

11 They become superconducting at temperatures (Tc) between approximate

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

13 d cuprates suppresses their high-temperature superconducting behaviour and reveals competing ground s

14 ferromagnetic (FM) stray fields, in both the superconducting behaviour of the film and the three-dime

15 vel negates the possibility of a topological superconducting behaviour on the surface.

16 In the doped compound BaPb0.72Bi0.28O3 (superconducting below TC = 7 K), a similar response was

17 ases were found to be dynamically stable and superconducting between 100 and 200 GPa.

18 nsition from pristine Bi2212 to a mixture of superconducting Bi2212 and semiconducting Bi2Sr2CuO6+del

19 While expensive avalanche photodiodes and superconducting bolometers are examples of detectors ach

20 Such performance is even comparable to superconducting bolometers, which however need to operat

21 ity layer by layer, because it contains both superconducting building blocks (Fe2As2 layers) and inte

22 e pairing mechanism in the recently-reported superconducting Ca-intercalated bilayer graphene.

23 d operations on a logical qubit encoded in a superconducting cavity resonator using four-component ca

24 o generate microwave photon Fock states in a superconducting circuit quantum electrodynamics system c

25 ogies, a design for a quantum memristor with superconducting circuits may be envisaged.

26 Superconducting circuits offer tremendous design flexibi

27 lts can be demonstrated experimentally using superconducting circuits where tuneable boundary conditi

28 This a challenge with superconducting circuits, as state-of-the-art architectu

29 tation using artificial-atoms, such as novel superconducting circuits, can be sensitively controlled

30 antization method, specifically designed for superconducting circuits, may be extended to other quant

31 y competing candidates for qubits, including superconducting circuits, quantum optical cavities, ultr

32 Thanks to the high level of control of superconducting circuits, we directly measure the extrac

33 imentally feasible with the state of the art superconducting circuits.

34 of transport phenomena in biomolecules with superconducting circuits.

35 ough continuous-variable entangled states in superconducting circuits.

36 y surface scattering, are smaller than their superconducting coherence lengths.

37 Remarkably superconducting coherence peaks are seen only on the ord

38 o further the development of SN2 cooled MgB2 superconducting coils for MRI applications.

39 tic fields generated by permanent magnets or superconducting coils has found applications in many fie

40 he existence of short-range correlations for superconducting compositions is uncertain.

41 ing properties at the surface of the related superconducting compounds might be different from the bu

42 ulators and evolve into paramagnons in doped superconducting compounds.

43 en the pump pulse is too weak to deplete the superconducting condensate, and for cuts inside the Ferm

44 also exceed the pair-breaking speed limit of superconducting condensate.

45 charge density waves, spin density waves and superconducting condensates.

46 nge interaction based on the coupling of the superconducting condensation energy to the magnetic stat

47 tion of the converse effect, that is, direct superconducting control of the magnetic state in GdN/Nb/

48 ements made at millikelvin temperatures of a superconducting coplanar waveguide resonator (CPWR) coup

49 l aluminium, which forms a proximity-induced superconducting Coulomb island (a 'Majorana island') tha

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

51 tly computed density of states (DOS) and the superconducting critical temperature T c .

52 rfluid density and a linear scaling with the superconducting critical temperature T c is observed und

53 culations on MnX (X = N, P, As, Sb) and find superconducting critical temperature TC of MnP sharply i

54 Superconducting critical temperature Tc(x) in ZrTe3-xSex

55 Their superconducting critical temperatures (Tc) were computed

56 ntial for exotic physics similar to high T C superconducting cuprates as they have similar crystal st

57 Although all superconducting cuprates display charge-ordering tendenc

58 res the collective spin excitations of doped superconducting cuprates remains under debate.

59 c double-layer (EDL) gating experiments with superconducting cuprates, our work shows that interfacin

60 tivity in the QH regime remain scarce, and a superconducting current through a QH weak link has been

61 here we show evidence for a p-wave triggered superconducting density of states in SLG.

62 redictions and could form the basis of novel superconducting devices based on reconfigurable vortex p

63 hers have been focused on the fabrication of superconducting devices capable of immobilizing vortices

64 1/f magnetic flux noise commonly observed in superconducting devices such as SQUIDs and qubits is sti

65 ical phase and to realize hybrid topological superconducting devices.

66 harge density wave (CDW) was found below the superconducting dome in YBa2Cu3O y when a high magnetic

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

68 f KxFe2-ySe2, which has pressure-induced two superconducting domes of SC I and SC II, was investigate

69 Neither phase at ambient pressure is superconducting down to 2 K.

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

71 n encapsulated graphene samples contacted by superconducting electrodes, in magnetic fields as high a

72 sing purely optomechanical interactions in a superconducting electromechanical circuit.

73 onductance peaks at zero-bias voltage in non-superconducting electronic transport through a 3D topolo

74 ms in mesoscopic superconductivity, scalable superconducting electronics, and new topological states

75 tum circuitry for novel high-speed low-power superconducting electronics.

76 de a means to reduce the size of SQUID-based superconducting electronics.

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

78 This superconducting exchange interaction is fundamentally di

79 l the intercalated compounds are found to be superconducting, exhibiting the same (within experimenta

80 standing of the structure and physics of the superconducting FeS.

81 he flow of individual magnetic vortices in a superconducting film is regulated by the magnetic potent

82 l hybrid system formed by a high-temperature superconducting film, patterned with antidots, and with

83 nfluence the critical current density of the superconducting film.

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

85 dependence of electric conductivity of thin superconducting films in the critical vicinity of superc

86 ween the anomalous pseudogap phase, enhanced superconducting fluctuations and giant anomalies in the

87 This increases the temperature range of superconducting fluctuations containing an overdamped Le

88 etism by far exceeding the standard Gaussian superconducting fluctuations is observed below T* approx

89 we revisit the design and fabrication of the superconducting flux qubit, achieving a planar device wi

90 We implement the protocol in a superconducting flux qubit, and rule out (by approximate

91 e superconductivity with a broad dome in the superconducting [Formula: see text] enclosing the nemati

92 In addition, a proximity-induced hard superconducting gap (with vanishing sub-gap conductance)

93 vity at Zeeman energies much larger than the superconducting gap can be understood only as the conseq

94 proximity effect, resulting in both a large superconducting gap Delta = 0.5 meV, and coherence lengt

95 0.25 As-quantum-well-Nb that results in hard superconducting gap detection in symmetric, planar, and

96 ure and the momentum dependence of the -wave superconducting gap determined from scanning tunnelling

97 An induced superconducting gap in Bi2Se3 was observed in the spectr

98 However the recent observation of a similar superconducting gap in single-unit-cell FeSe/STO(110) ra

99 quantum point contact (QPC), we find a hard superconducting gap in the tunnelling regime.

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

101 a ground-state property, independent of the superconducting gap.

102 (n) dome, the three maxima with accompanying superconducting gaps emerging consecutively as electrons

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

104 state and the two-dimensional surface state superconducting gaps observed in the angle-resolved phot

105 t should be possible to resolve two distinct superconducting gaps on the electron and hole Fermi surf

106 prompt gravity signal in data recorded by a superconducting gravimeter and broadband seismometers du

107 -fall gravimeters, spring-based gravimeters, superconducting gravimeters, and atom interferometers.

108 It would therefore be unexpected if a superconducting ground state would support spontaneous m

109 Magnetic and superconducting ground states can compete, cooperate and

110 A superconducting hard gap in hybrid superconductor-semico

111 shows that this layered chalcogenide remains superconducting in decompression down to 10.7 GPa.

112 The application of magnetic separation to superconducting inorganic phases is of particular intere

113 Each subband contributes to the superconducting instability and exhibits a gap in its en

114 we report the unprecedented enhancement of a superconducting instability by disorder in single crysta

115 network of crystalline nanowires coupled to superconducting islands.

116 anowire networks with a predefined number of superconducting islands.

117 lectronic heterostructure films of semi- and superconducting layers possess very different properties

118 junctions formed by InAs nanowires and Ti/Al superconducting leads.

119 r copper oxides was recently shown to induce superconducting-like optical properties at temperatures

120 so confirmed that the fluxoid state inside a superconducting loop can be manipulated using primarily

121 In a heavily overdoped, metallic but non-superconducting LSCO (x = 0.35) film, the spin asymmetry

122 Less-doped, superconducting LSCO films show no magnetic moment in ne

123 circuit boards and installed within a single superconducting magnet and vacuum system.

124 An efficient cooling system and the superconducting magnet are essential components of magne

125 conjunction with a magnesium diboride (MgB2) superconducting magnet.

126 raction technique has been implemented using superconducting magnetic Wollaston prisms in both single

127 Superconducting materials in the Meissner phase are idea

128 The use of superconducting materials in the prisms allows high neut

129 and MnSb may be the more potential Mn-based superconducting materials.

130 Here, we demonstrate theoretically a superconducting memory based on solitonic long Josephson

131 amplifier combined with high-quality-factor superconducting microresonators cooled at millikelvin te

132 o image Cooper pair tunnelling from a d-wave superconducting microscope tip to the condensate of the

133 By coupling donor spins in silicon to a superconducting microwave cavity with a high quality fac

134 ilicon nitride nanomembranes for integrating superconducting microwave circuits with planar acoustic

135 nsitions, glitches in pulsars, and losses in superconducting microwave circuits, and it limits the cu

136 We present superconducting nanowire single-photon detectors (SSPDs)

137 Secondly, the superconducting nature of a topological superconductor i

138 er-sized Py ferromagnetic disks covered by a superconducting Nb thin film.

139 rface-structural modulation of the ultrathin superconducting NbSe2 by polar reductive hydrazine molec

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

141 to induce ferromagnetism in two-dimensional superconducting NbSe2, representing the freestanding cas

142 High transparency superconducting niobium titanium nitride contacts are ma

143 its high purity and the possibility that its superconducting order parameter has odd parity.

144 cted, for the first time, the existence of a superconducting order parameter in a band far from the F

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

146 on due to the d(s(+/-))-wave symmetry of the superconducting order parameter, it has also been propos

147 phase transition dramatically affecting the superconducting order parameter.

148 nteger larger than 2Delta/eVSD and Delta the superconducting order parameter.

149 MnP and trace its pressure evolution towards superconducting order via measurements in a diamond anvi

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

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

152 several candidates, including memristive and superconducting oscillators, a proof of concept of neuro

153 of the Fe d-orbitals is intertwined with the superconducting pairing in Fe-based materials, our resul

154 estigation of the nature of charge order and superconducting pairing in NbSe2 and related TMDCs.

155 n any attempt to understand the mechanism of superconducting pairing in these materials.

156 f the effects of nematic fluctuations on the superconducting pairing interaction in this family of co

157 eractions have been suggested to mediate the superconducting pairing, both in the orbital and in the

158 With the short-range p-wave superconducting pairing, multifarious topological quantu

159 device to image vortices penetrating into a superconducting Pb film at rates of tens of GHz and movi

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

161 lower or even ambient pressures with better superconducting performance.

162 ture of the proton fundamentally changes the superconducting phase diagram of H3S.

163 The unusual dependence of the superconducting phase diagram of lithium on its atomic m

164 The superconducting phase in iron-based high-[Formula: see t

165 It has been proposed that the superconducting phase is body-centered cubic H3 S (Im3 m

166 of unconventional superconductors and their superconducting phase is important for understanding the

167 he c-axis changes around 12 GPa, where a new superconducting phase of SC II appears.

168 at about 3 K suggests that there is a second superconducting phase that may be associated with a sing

169 ossover (a mystery for over 30 years), and a superconducting phase which may involve spin triplet Coo

170 netic multipolar ordered and possible d-wave superconducting phases in doped Sr2IrO4 have reinforced

171 s with strain engineering, or unconventional superconducting phases.

172 Here we develop a hybrid superconducting-photonic circuit system to show how thes

173 -based materials, our results imply that the superconducting properties at the surface of the related

174 f dimensionality and electron correlation on superconducting properties has remained unclear.

175 mple is the deterministic enhancement of the superconducting properties of materials.

176 ffers an alternative route for modifying the superconducting properties via a shockwave treatment.

177 Several superconducting properties were observed, revealing the

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

179 ents combining magnonic elements with planar superconducting quantum devices.

180 While individual superconducting quantum dots have been explored, control

181 Here, we implement a random access superconducting quantum information processor, demonstra

182 ng scanning tunneling spectroscopy, scanning superconducting quantum interference device (SQUID) magn

183 Here, we use a nanoscale scanning superconducting quantum interference device to image vor

184 Here we report a nano-thermometer based on a superconducting quantum interference device with a diame

185 icrowave photons, based on three equidistant superconducting quantum interference devices (SQUIDs) on

186 Future quantum networks, in which superconducting quantum processors are connected via opt

187 Superconducting quantum systems (artificial atoms) have

188 ly electric-field-tunable spin-polarized and superconducting quasi-2D electron system (q2DES) can be

189 s, we found that the relaxation component of superconducting quasiparticles persisted from the superc

190 ity that encodes quantum information about a superconducting qubit and converts information into work

191 e and demonstrate a read-out technique for a superconducting qubit by dispersively coupling it with a

192 em comprising the dressed states of a driven superconducting qubit coupled to a microwave resonator.

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

194 elength converter, it could pave the way for superconducting qubit processors with multiplexed on-chi

195 spin-based systems could be used to advance superconducting qubit science.

196 between KZM in the Ising model and LZT in a superconducting qubit system.

197 s and quantum interference phenomena for the superconducting qubit systems driven by intense ac field

198 wave resonator that is strongly coupled to a superconducting qubit using piezoelectric transduction w

199 ion probes of non-commuting observables to a superconducting qubit.

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

201 between them to investigate the dynamics of superconducting qubits in transverse, longitudinal, and

202 s (SAWs) can be piezoelectrically coupled to superconducting qubits, and confined in high-quality Fab

203 In the context of superconducting qubits, we implement a pumping sequence

204 Using a chain of nine superconducting qubits, we implement a technique for res

205 motion to nonlinear quantum objects such as superconducting qubits.

206 Bulk niobium Superconducting Radio-Frequency cavities are a leading a

207 uperconductivity (MoTe2 was discovered to be superconducting recently) and their topological order.

208 We employ a tunable quarter wavelength superconducting resonator and modulate its resonant freq

209 n be tested with current technology by using superconducting resonators with tunable boundary conditi

210 the eigenmodes of a linear array of coupled superconducting resonators.

211 By revealing the tunability of the superconducting response through doping and confinement

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

213 ich cause the decay of persistent current in superconducting rings and the appearance of resistance i

214 Spin filter superconducting S/I/N tunnel junctions (NbN/GdN/TiN) sho

215 HTS with ferromagnetic order, fluctuating in superconducting samples and static beyond the supercondu

216 Recently, the superconducting semimetal FeSe with a transition tempera

217 lanced-detection scheme in SS-OCT, even when superconducting single-photon detectors were used.

218 tatistics with two monolithically integrated superconducting single-photon detectors.

219 critical temperature (Tc) control in FM/S/FM superconducting spin valves (SSVs) and critical current

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

221 rovide important insight for spintronics and superconducting spintronics where engineering tunable ma

222 the active control of the magnetic state in superconducting spintronics.

223 The transition separates the (presumably) superconducting state at H < Hc from a "Hall-insulator"

224 alitative understanding of the nature of the superconducting state itself has been achieved.

225 ntly slower buildup of quasiparticles in the superconducting state than in the normal state.

226 conducting quasiparticles persisted from the superconducting state up to at least 70 K in the normal

227 clude time-reversal symmetry breaking in the superconducting state with zero-field muSR experiments.

228 ocal signal is significantly enhanced in the superconducting state, being associated with unprecedent

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

230 A sharp spin resonance develops in the superconducting state, whose energy ( approximately 4 me

231 glement of these two states, the topological superconducting state, will give rise to even more exoti

232 a zero-field magnetic instability inside the superconducting state.

233 lly drops to zero as the system falls into a superconducting state.

234 excitons that form inside the unconventional superconducting state.

235 lass' response and the resonance mode in the superconducting state.

236 be a magnon-like excitation appearing in the superconducting state.

237 also act as an organizing principle for the superconducting state.

238 practically identical characteristics in the superconducting state.

239 g the proximity between these very different superconducting states and identifying experimental para

240 e is the appearance of highly conducting and superconducting states at the interface between LaAlO3 a

241 be helpful in understanding low temperature superconducting states of these topological materials.

242 d a rich phase diagram for these topological superconducting states.

243 ractions selectively favours two topological superconducting states: interpocket paired state with Ch

244 suppressed and destroyed for x</=0.035, the superconducting strength evolves non-monotonically with

245 e state at high fields and temperatures made superconducting strips a mainstream of superconductivity

246 ing at P = 1 atm, and some form metallic and superconducting symmetrically bonded AuHAu sheets under

247 g digitized adiabatic quantum computing in a superconducting system.

248 n-Abelian anyons include p-wave superfluids, superconducting systems with strong spin-orbit coupling,

249 d to a significant ( 70%) suppression of the superconducting T c for pair-forming electron-phonon cou

250 -temperature phase stiffness on the critical superconducting temperature is generally linear, but wit

251 are homogeneous; variations in the critical superconducting temperature within a film are very small

252 electron-doped TMDs have recently been found superconducting, the observed superconductivity is unlik

253 coating the inner wall of an SRF cavity with superconducting thin films increases Hvp.

254 ging from liquid helium, ultracold atoms and superconducting thin films to ensembles of spins.

255 form kinetic inductance characterizations of superconducting thin films.

256 Here we investigate strongly disordered superconducting TiN films and demonstrate universality o

257 tomic layers, leading to the transition from superconducting to an unusual Mott insulating state emer

258 phous materials; e.g., it has a well-defined superconducting transition along with an exceptional rob

259 Superconducting transition appears at 8 GPa with a criti

260 A sharp superconducting transition at approximately 3.2 K was ob

261 and heat capacity measurements reveal a bulk superconducting transition at Tc =1.36 K.

262 /3-ySbySexTe6-x revealed a dependence of the superconducting transition on composition that can incre

263 ser deposition (PLD) enables improving their superconducting transition temperature (T c) by more tha

264 We find that the superconducting transition temperature (T c) increases f

265 The pressure dependence of the superconducting transition temperature (Tc) and unit cel

266 A superconducting transition temperature (Tc) as high as 1

267 The superconducting transition temperature (TC) in a FeSe mo

268 It sets in far above the superconducting transition temperature and competes with

269 an archetypical cuprate YBa2Cu3O6.54 at its superconducting transition temperature approximately 60

270 m of LO phonons opens the path to increasing superconducting transition temperature in bulk transitio

271 the valence electron count dependence of the superconducting transition temperature in the high-entro

272 Even though the gap forms around the superconducting transition temperature of lead, we do no

273 The superconducting transition temperature of tetragonal FeS

274 on-scattering results for HgBa2CuO(4+delta) (superconducting transition temperature Tc approximately

275 In particular, the superconducting transition temperature Tc calculated for

276 covered sulfur hydride superconductor with a superconducting transition temperature Tc of 203 kelvin

277 asymmetric dome of the dynamical mean-field superconducting transition temperature Tc(d), the maximu

278 te theoretically all-electric control of the superconducting transition temperature using a device co

279 ble S approximately Gi(1/2)(T/Tc) (Tc is the superconducting transition temperature) that has been ac

280 perties at temperatures far greater than the superconducting transition temperature, Tc.

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

282 a rare-earth metal) exhibit the highest bulk superconducting transition temperatures (Tc) up to 55 K

283 f these properties generates remarkably high superconducting transition temperatures above 80 K at an

284 The superconducting transition temperatures are highest for

285 coupling leads to reasonably high calculated superconducting transition temperatures for these materi

286 H8, C2/m-SnH12 and C2/m-SnH14 exhibit higher superconducting transition temperatures of 81, 93 and 97

287 One is a publicly accessible superconducting transmon device (www.

288 On the other hand, effect of chirality on superconducting transport has not been known.

289 The qubit is a superconducting two-level system and the bipartite quant

290 behavior has not, however, been found in the superconducting upper critical field H c2.

291 The superconducting volume fraction of oriented single cryst

292 d interface density correlates well with the superconducting volume measured.

293 copy has been used to directly visualise the superconducting vortex behavior in hybrid structures con

294 We have studied the pinning of added free superconducting vortices as a function of the magnetisat

295 icroscopy to image magnetic bifurcations and superconducting vortices, while high resolution scanning

296 c Mott transition in a system of interacting superconducting vortices.

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

298 ng rings and the appearance of resistance in superconducting wires.

299 converted into a metallic phase that becomes superconducting with a record Tc of approximately 200 K.

300 ort on the realization of the process in the superconducting Xmon and phase qutrits--two ladder-type