ライフサイエンスコーパス: bit

1 Here we describe a 160,000-bit molecular electronic memory circuit, fabricated at a

2 uces information transfer to approximately 1 bit at the single-cell level but allows 3-4 bits of info

3 This revealed mutual information values <1 bit, implying that individual GnRH-responsive cells cann

4 kappaB pathway is known to transmit merely 1 bit of information about stimulus level.

5 to an overall quality score compression of 1 bit per value with a negligible effect on variant callin

6 that the NF-kappaB network not only relays 1 bit of information to coordinate the all-or-nothing expr

7 xamined to date seem to transmit less than 1 bit of information.

8 ty of glomeruli activated above threshold (1 bit of information per glomerulus) and in the analog deg

9 SWNT-TFTs, a Monte Carlo simulation for a 1-bit adder circuit, as a reference, was conducted to demo

10 oduce a reprogrammable hologram based on a 1-bit coding metasurface, where the state of each unit cel

11 cept of a reprogrammable hologram based on 1-bit coding metasurfaces.

12 ly ordered units acting as the coded 0- or 1-bit, are introduced as a promising option for molecular

13 We show that 10-bit HiPR-FISH can distinguish between 1,023 isolates of

14 780-nm near-infrared light imaged onto a 12-bit charge-coupled device (CCD) camera in response to a

15 Images were captured as 12-bit tiff files and postprocessed to extract changes in r

16 Formula: see text] microlenses to capture 12-bit images of the pupil plane, and a superluminescent di

17 information storage density of 4.9 x 10(13) bit/inch(2).

18 2.5 metres with a spectral efficiency of ~16 bit s(-1) Hz(-1) using four independent orbital-angular

19 that the specific camera we used (with a 16-bit analog-to-digital converter) has sufficient dynamic

20 Here, we report a 16-bit coherent Ising machine based on a network of time-di

21 set, runs standard 32-bit instructions on 16-bit data and addresses, comprises more than 14,000 compl

22 This 16-bit microprocessor is based on the RISC-V instruction se

23 rs lack a -35 region, but have a 6.7 +/- 0.2 bit extended -10, almost the same information as the bip

24 The fabrication process for 5 Tb/in(2) bit patterns using solvent-assisted directed self-assemb

25 We implemented a 2-bit encoding for genotype data, and compared it against

26 Our system realizes the complete 2-bit logic flow and clocked control over state registrati

27 so reprogrammed to a functionally distinct 2-bit full adder with 32-set matched and complete logic ou

28 when building simple frequency tables from 2-bit encoded genotypes.

29 In general, the 2-bit encoding consumes less memory, and is slightly more

30 p penalties for a given matrix scaled in 1/3 bit units (e.g. BLOSUM50, PAM200) are q=25-0.1 * (target

31 device has the following characteristics: 3 bit MLC, electroforming-free, self-rectifying, much high

32 We show that a 3-bit barcode can be assigned with 94% accuracy by electro

33 A 3-bit organic complementary decoder is fabricated and used

34 n this work, we consider the use of 2- and 3-bit encoding schemes for genotype data.

35 We perform a comparison of 2- and 3-bit genotype encoding schemes for use in genotype counti

36 more efficient in some algorithms than the 3-bit encoding.

37 various bit-rates: from a 4-bit uniform to 3-bit non-uniform quantization in phase.

38 d compared it against a more commonly used 3-bit encoding scheme.

39 s containing millions of reads, even on a 32-bit desktop machine.

40 ep-learning accelerator components, and a 32-bit RISC-V ALU, based on our developed standard cell lib

41 as been tested to be compatible with both 32-bit and 64-bit Windows 7.

42 of libSBML and has been tested on Linux (32-bit Ubuntu 8.10 and 9.04).

43 the RISC-V instruction set, runs standard 32-bit instructions on 16-bit data and addresses, comprises

44 We successfully exchange a 1,366 bit random oblivious transfer string in ~3 min and inclu

45 ectral-density usage efficiency as high as 4 bit/s/Hz over 16 m in free space, wherein the BLD carrie

46 A high spectral efficiency of 8.0 +/- 0.4 (bit/s)/Hz in acoustic communication has been achieved us

47 and propagation length of 5 mm such that a 4-bit all-optical quantizer can be realized.

48 nstrate its practicality by implementing a 4-bit arithmetic logic unit consisting of 8 high-speed mic

49 it ripple carry adder with 48 p-bits and a 4-bit multiplier with 46 p-bits working in inverted mode a

50 ulate p-bits, and we present results for a 4-bit ripple carry adder with 48 p-bits and a 4-bit multip

51 g meta-layers at various bit-rates: from a 4-bit uniform to 3-bit non-uniform quantization in phase.

52 cquisition of sub-pulse duration range and 4-bit reflectivity information in the presence of high bac

53 8% of bits are copied correctly and 78% of 4-bit sequences are correct after two generations; roughly

54 urate enough for 1,000-fold replication of 4-bit sequences with 50% yield, replication of longer sequ

55 We demonstrate a 5-bit system capable of writing, erasing, and rewriting bi

56 blem sets with binary weights and 84% with 5-bit weight resolutions.

57 eprogrammed to implement a wide variety of 6-bit algorithms.

58 al antenna and capable of bit rates up to 60 bit/s.

59 The software library is designed for 64 bit Linux, OS X, or Windows on processors with SSE2, SSE

60 n runs on x86 compatible systems with the 64 bit Linux operating system and is freely available for a

61 The package is tested under Ubuntu 12.04 (64-bit), Java 7, glibc 2.15 and Cytoscape 3.1.0.

62 into the system architecture to realize a 64-bit full adder, which is also demonstrated through simul

63 ted to be compatible with both 32-bit and 64-bit Windows 7.

64 An installer for 64-bit Windows and a macOS app are available.

65 YAHA is currently supported on 64-bit Linux systems.

66 Requires 32 or 64-bit Linux system (tested on Fedora Core 8,10,11 and Ubun

67 C ++ and OpenMP, supports 64-bit Linux/Unix-like platforms.

68 sible atomic basis for these systems with 64-bit arithmetic, half-augmented-pVDZ, and the results wer

69 A compression of 0.68 bit per quality value is achieved using a more aggressiv

70 founded in 1994 by Adleman's solution of a 7-bit instance of the Hamiltonian path problem.

71 0-MHz catheter and digitized at 1 GHz with 8-bit resolution.

72 his approach, we experimentally generated 80 bit strong keys from human DNA, and used such a key to e

73 23.42 dB and effective number of bit is 3.89-bit.

74 A bit of information can be written optically in the chemi

75 ed within the cell biology community, I am a bit humbled by how long it took me to truly grasp his vi

76 Each node i is assigned a bit at time 0 and is a finite automaton with m bits of m

77 processing with <1.5 dB power penalties at a bit-error-rate of 2 x 10(-3).

78 Postconditioning has become a bit more controversial in the clinical literature; remot

79 We have developed BitPAl, a bit-parallel algorithm for general, integer-scoring glob

80 The sender encodes a bit sequence onto non-orthogonal quantum states and the

81 Feeling a bit cagey: morpholino-based antisense reagents have been

82 Furthermore we introduce a bit-by-bit analytical method which is agnostic to the sp

83 d can control the type I error rate and is a bit conservative when compared to the permutation method

84 ic exchange within one Archaean lineage is a bit like sex in eukaryotes - cells fuse and huge segment

85 circuits and implies a lower bound that is a bit stronger than that of Kabanets and Impagliazzo [Kaba

86 ption of rob, while decanoate represses it a bit.

87 ching ball, humans trigger their movements a bit earlier when the target arrives from above than from

88 We measure the work to erase a fraction of a bit of information and show that it is bounded by the Sh

89 f DNA, corresponding to the [0,1] state of a bit.

90 Although we know quite a bit about the mechanisms that control Schwann cell devel

91 These outcomes differ quite a bit from previous approaches that incorporate allometrie

92 n peers as a group were extremely or quite a bit involved in human rights abuses included 50% (42/83)

93 This delineation will entail quite a bit of cell biology.

94 nderstanding of the term has changed quite a bit since 1910, particularly in light of modern molecula

95 clinically based nosology, still has quite a bit to teach modern psychiatry and can be a more generat

96 cantly more hand/foot toxicity (eg, "quite a bit" of cold-induced hand/foot pain 26% FLOX v 2.6% FULV

97 LR of 0.44 (95% CI, 0.24-0.82) for "quite a bit" or "extremely confident.

98 0, "not at all"; 1, "a little"; 2, "quite a bit"; or 3, "very much." Summing the six symptom scores

99 wers were "not at all," "a little," "quite a bit," and "very much." Analysis was limited to the first

100 further posited that ether radicals react a bit more slowly than ketyl radicals because they lack th

101 While reading a bit of information stored in the magnetostrictive nanoma

102 A bubble traveling in a channel represents a bit, providing us with the capability to simultaneously

103 OM can integrate these models will require a bit more math.

104 ment of work, which may make the situation a bit more competitive and thus drives attention toward bo

105 n did those who considered their body size a bit too large (0.21 vs. 0.38 BMI units; P = 0.009).

106 was similar to the classic methods though a bit lower in total content.

107 Using a bit-level coding scheme for SNP data and parallelized co

108 Using a bit-string shape space, both similar and complementary a

109 l after 24 d of storage whereas thymol was a bit more effective in encapsulated WO-TAGs.

110 plitude modulation (16-QAM OFDM) data with a bit error rate (BER) of 3.1 x 10(-3) over a 60-cm free-s

111 ploited to implement a memory element with a bit retention time of 11 h.

112 these memory elements is roughly 8 pJ with a bit-select element, designed to achieve a minimum overhe

113 lectro-optic switching at 11 Gb s(-1) with a bit-switching energy as low as 22 fJ.

114 After traveling the world a bit, Calisher joined the faculty of Colorado State Unive

115 Writing a bit is usually achieved by rotating the magnetization of

116 e important for flux-logic devices, where a 'bit' might be represented by a pancake vortex stack, and

117 mapping with supervised learning to achieve bit error rates as low as 0.11% for single reads, withou

118 mus is required for both circuits to achieve bit error rates below 10(-3), which is a putative thresh

119 eams with both multiplexed channels achieved bit error rates (BERs) of <3.8 x 10(-3).

120 roach to reliably protecting a qubit against bit-flip errors.

121 They also bit, retrieved, and attempted to eat model fish made of

122 igh-density recording on portable disks, and bit densities of approximately 100 Gbit inch(-2) have be

123 Here we demonstrate such phase- and bit-flip error correcting codes in a superconducting cir

124 te performance with an increase in range and bit rate, when compared with conventional threshold dete

125 or more than a week at room temperature, and bit level ratios (0:1) of the conductivity-type memory h

126 sequence gap-filled gene feature annotation, bit-block encoded genotypes and sectional fast access to

127 cuitry, we implemented the antiferromagnetic bit cell in a standard printed circuit board managed and

128 The single-atom bit represents the ultimate limit of the classical appro

129 n-volatile strain switching at the attojoule/bit level(5-7), with immediate applications in ultrafast

130 The human brain is easily the most baffling bit of biology on the planet.

131 um entropy decoding can give slightly better bit-error-rates than the maximum likelihood approach, co

132 r level of security than conventional binary-bit architecture with the same key size.

133 local patches of the ground surface, bit by bit, from near to far, but not in the reverse direction.

134 Bit by bit, we are coming to understand how this may occur, but

135 Furthermore we introduce a bit-by-bit analytical method which is agnostic to the specific

136 tance descriptors are held as pre-calculated bit strings permitting fast and efficient similarity and

137 T2): T1 measures the lifetime of a classical bit, in this case embodied by a spin oriented either par

138 Whilst classical bit-flip detection can be realized via a linear array of

139 ught a consensus majority for each component bit within the message - was consistently the most succe

140 r of mismatches) between their corresponding bit vectors.

141 bined with a superconducting heater-cryotron bit-select element.

142 In memories of this sort, storing a data bit means increasing the size of one polar region at the

143 s using the chirality of Skyrmions as a data bit.

144 ssical bits that are subject to only digital bit-flip errors, quantum bits are susceptible to a much

145 each member contains a unique barcode; each bit in the barcode is signalled by the presence or absen

146 right voltage polarity, one can write either bit deterministically.

147 lled domain wall traps facilitate electrical bit selection in a magnetic nanowire register.

148 ction of classical states from environmental bit-flip errors and demonstrate the suppression of these

149 includes membrane inhibitors that are every bit as important as those in plasma.

150 as a targeting signal has proved to be every bit as important to eukaryotic cells as the better under

151 cell layer that is teeming with life, every bit as active as any other organ in the body.

152 There exist bit-vector techniques to solve the fixed-length approxim

153 tion and observation and, yes, still, a fair bit of luck.

154 ectrical energy consumptions of only 0.07 fJ bit(-1) at 50 Gbit s(-1), 0.3 fJ bit(-1) at 200 Gbit s(-

155 , 0.3 fJ bit(-1) at 200 Gbit s(-1), and 2 fJ bit(-1) at 400 Gbit s(-1).

156 nly 0.07 fJ bit(-1) at 50 Gbit s(-1), 0.3 fJ bit(-1) at 200 Gbit s(-1), and 2 fJ bit(-1) at 400 Gbit

157 NOT gate with an energy dissipation of ~1 fJ/bit at 640 Gb/s and use it as a building block for an XN

158 which becomes impractically large, > 0.1 fJ/bit per gate, for signal speeds just over several GHz.

159 rated design for a compact, sub-volt, sub-fJ/bit, hyperuniform-clad, electrically controlled resonant

160 oding along large-angle bending channels for bit-error-free acoustic data transmission in an underwat

161 igital logic circuits, culminating in a four-bit square-root circuit that comprises 130 DNA strands.

162 at computes the square-root function of four-bit input numbers.

163 switching in magnetic media supporting high bit densities no longer takes place at well-defined fiel

164 High-bit-rate long-distance quantum communication is a propos

165 work, determination, foresight, and a little bit of luck.

166 Together, a little bit of reciprocal altruism can, however, greatly reduce

167 thology would go in future decades, a little bit to my gut instincts and innate ability to spot up-an

168 By using two vertices to encode each logical bit, we obtain universal computation.

169 ted that the CoFeB clocking system has lower bit-density than in Ni or Terfenol-D systems due to its

170 te, allowing rapid rewriting of the magnetic bit.

171 des can become aware of knowing the majority bit and stop communicating.

172 nsus with high probability on their majority bit.

173 oth 4-channel multiplexing schemes, measured bit error rates (BERs) of < 10(-6) are achieved over a d

174 ng distinct performance metrics across multi-bit memory capacity, low-power operation, endurance, ret

175 oupled nanomagnets, as demonstrated by multi-bit computing gates.

176 eful for the development and tuning of multi-bit storable organic nanocomposite memory device systems

177 d displacement to develop a rewritable multi-bit DNA memory system.

178 Due to nanoscale bit size, a single computer hard disk is now able to sto

179 edicting the thermal transients for the next bit to be received.

180 thors' findings argue that platelets are not bit part players, but rather fully fledged, critical mem

181 ably sized electrical antenna and capable of bit rates up to 60 bit/s.

182 se ratio is 23.42 dB and effective number of bit is 3.89-bit.

183 It can be extended to arbitrary number of bit streams.

184 It also has a better tolerance of bit errors and of finite-sized-key effects.

185 Moreover, the use of bit strings points to the importance of certain molecula

186 roposed weighted GO transfer method based on bit-score and a logarithmic transformation of CHI-square

187 imum energy dissipation required to gain one bit of information.

188 ectures of gates discovered we implement one bit half-adder and controlled-not circuits in the F-acti

189 We demonstrate the protection of one bit of quantum information against all collective noise

190 from the reservoir at temperature T per one bit of created information.

191 We perform a one-bit full-addition operation on a quantum computer using

192 down-sampled pixels is converted into a one-bit representation with delta modulation (DM).

193 e; they can correct any single phase-flip or bit-flip error on one of the three qubits, depending on

194 dels based on global molecular properties or bit strings point to a small advantage of the latter for

195 sensor prototypes produce a digitized output bit (that is, a large and sharp off-to-on state transiti

196 n to this problem but improvements in output bit rate, power consumption, and design complexity must

197 y role is played by a probabilistic bit (a p-bit)-a robust, classical entity fluctuating in time betw

198 ith the first, thus correlating the second p-bit stream with the first.

199 s of the two MTJs (high or low) encode the p-bit values (1 or 0) in the two streams.

200 of a significant reduction in the energy per bit compared with conventional transistors.

201 dths while consuming subpicojoule energy per bit, vastly eclipsing performance of prior nanostructure

202 sub-pA operation current and femtojoule per bit energy consumption.

203 d be below 1 volt and single femtojoules per bit, respectively.

204 GHz modulation speed and less than 1 fJ per bit energy of operation, which is orders of magnitude lo

205 w-voltage (0.5 VPP) and efficient 0.9 fJ per bit error-free operation.

206 e additional energy consumption (0.24 fJ per bit for a total energy consumption below 1.03 J per bit)

207 a total energy consumption below 1.03 J per bit).

208 unction this is [Formula in text] joules per bit (kB is Boltzmann's constant and T is the absolute te

209 gnal power requirements to a few photons per bit.

210 In the case of a phi-bit, the coherent superposition of states in the directi

211 tion of an ultrasonic pseudospin i.e., a phi-bit.

212 We also demonstrate phi-bit gate operations on the coherent superposition analog

213 oinositide signaling landscape is physically bit mapped so that eukaryotic cells are able to convert

214 The key role is played by a probabilistic bit (a p-bit)-a robust, classical entity fluctuating in

215 fidelity and the coherence time of a quantum bit (qubit) are important benchmarks for quantum computa

216 Complete control of the state of a quantum bit (qubit) is a fundamental requirement for any quantum

217 f a simple quantum system, such as a quantum bit (qubit) or a cavity mode, in the presence of decoher

218 f the simplest platforms to encode a quantum bit (qubit), the elementary unit of future quantum compu

219 ral two-level system for realizing a quantum bit in the solid state.

220 be deterministically positioned in a quantum bit or qubit.

221 A quantum bit stored in a single trapped ytterbium ion (Yb+) is te

222 ures the corresponding lifetime of a quantum bit, encoded in the phase of the quantum state.

223 for this spin to be operational as a quantum bit, full quantum control is essential.

224 llator-a 'quantum drum'-coupled to a quantum bit, which is used to measure the quantum state of the r

225 ystem that extends the lifetime of a quantum bit.

226 ry to exploit a physical system as a quantum bit.

227 apping this property onto an ancilla quantum bit, whose only role is to facilitate quantum state mani

228 e field-effect transistors (FET) and quantum bit (qubit) devices.

229 One proposal for a solid-state-based quantum bit (qubit) is to control coupled electron spins on adja

230 te, we perform a single pass of both quantum bit- and phase-flip error correction and demonstrate the

231 t disturbing the coherence of an ion quantum bit in an adjacent site.

232 quantum states by encoding a logical quantum bit (qubit) in multiple physical qubits.

233 entanglement between a single matter quantum bit (qubit) and a telecommunications (telecom)-wavelengt

234 m information across a wide range of quantum bit (qubit) frequencies-from a few kilohertz for transit

235 tion has stimulated investigation of quantum bit (qubit) readout techniques, which for many condensed

236 l therefore be facilitated if qubit (quantum bit) error rates are far below the so-called fault-toler

237 plexity can be reduced by separating quantum bit (qubit) manipulation from measurement and by providi

238 l DQD may be used to obtain a single quantum bit and to prepare a Bell state.

239 In contrast to a single quantum bit, an oscillator can store multiple excitations and co

240 ndividually addressable, solid-state quantum bit (qubit), even at room temperature.

241 ters in diamond offers a solid-state quantum bit and enables high-precision magnetic-field sensing on

242 ate system, namely a superconducting quantum bit (qubit) coupled to a microwave cavity.

243 wever, by coupling a superconducting quantum bit (qubit) to signals on a microwave transmission line,

244 cavity containing a superconducting quantum bit (qubit), and track the individual quantum trajectori

245 f states offers this protection, the quantum bit was encoded in a proper noiseless subsystem.

246 um dot-photonic crystal cavity based quantum-bit.

247 Such observables, typically multi-quantum-bit parities, must correspond to a special symmetry prop

248 The simplest of these are three-quantum-bit (three-qubit) codes, which map a one-qubit state to

249 Although fast, 180-picosecond, two-quantum-bit (two-qubit) operations can be realized using nearest

250 a plan for the implementation of two-quantum-bit gates in a quantum computing architecture with natur

251 h this approach, two-dimensional (2D) random bit arrays are created that can offer ternary-bit archit

252 Such an exchange requires a common random bit sequence, called a key, to be shared secretly betwee

253 emonstrate a reliable high-speed true random bit generator (TRBG) device based on the unpredictable e

254 transmit much more than just one regulatory bit.

255 KGGSeq's bit-block genotype format used 1.5% or less space to fle

256 (state-of-the-art implementation of Myers's bit-vector algorithm) and Parasail (state-of-the-art seq

257 er the best previous algorithm (Gene Myers's bit-vector algorithm).

258 Based on a modified Myers's bit-vector dynamic programming algorithm, Btrim can hand

259 antage to open the way for three- or several-bit electronics.

260 gle atoms and molecules has allowed a single bit of information to be represented by a single atom or

261 ch that each simple FSM operates on a single bit position in the input (five bits are sufficient for

262 the receiver randomly dictates how a single bit should be calculated from the sequence.

263 (MD) can convert into free energy per single bit of information obtained in a measurement.

264 zymatic toehold creation that enables single-bit random-access and in-memory computations.

265 ent experiment has realized geometric single-bit gates in a superconducting system.

266 the atoms in the heat bath are given a small bit of quantum coherence.

267 cleus of eukaryotic cells; it is the 'sticky bit' that remains after aggressive DNAse digestion and s

268 can develop a double-well potential to store bit information.

269 ermine a separation distance; the streaming "bit signal" contains all the information needed.

270 Measurements show superior bit error rate performance with an increase in range and

271 canning local patches of the ground surface, bit by bit, from near to far, but not in the reverse dir

272 power loss, intermodal crosstalk, and system bit error rate (BER).

273 it arrays are created that can offer ternary-bit architecture by determining the connection yield and

274 The bit-parallel approach represents individual cells in an

275 the homologous protein, and then assign the bit-score as weights to GO features.

276 ending its permanence in the dark beyond the bit retention time.

277 the whole of the sequence, cannot guess the bit value correctly.

278 en demonstrated using recent advances in the bit writing and reading techniques.

279 that the far-field spatial variation of the bit error rate is different from that of the emitted pow

280 The benefits of the bit strings are in accord with the use of fragment-based

281 is paper concentrates on advancements to the bit error rate (BER) performance.

282 owth under near-optimal conditions where the bit copying error rate is <0.2%.

283 This bit-split organization of the Aho-Corasick implementatio

284 o an electronic circuit operating as a three-bit address decoder.

285 We then show how to map peptides to bit vectors such that the distance between any two pepti

286 tion, serves as the physical basis for a two-bit conditional quantum logic gate.

287 operation of purely mechanical one- and two-bit memory storage prototypes.Origami is a popular metho

288 ate the operation of mechanical one- and two-bit memory storage.

289 Using this approach we created two-bit digital-to-analog converters, which should be useful

290 al logic circuits for a set-reset latch, two-bit shift register, leading-edge detector, digital-to-an

291 ach more appealing is the realization of two-bit mechanical memory, in which two pairs of TCO cells a

292 memory organization is limited by unreliable bit operation and high write loads.

293 in RAM, xMAN can scan through genomes using bit shifting operation and achieve at least one order of

294 ring out error-abundant sequence pairs using bit-parallel and SIMD-parallel operations.

295 stic levitation using meta-layers at various bit-rates: from a 4-bit uniform to 3-bit non-uniform qua

296 that the metasurfaces are capable of varying bit error rates in response to different waveforms.

297 pper, is developed based on a new vectorized bit-vector algorithm, which simultaneously calculates th

298 The wasps bit and carried off second instars whole, whereas third

299 nd a 4 x 4 array can be fully addressed with bit select error rates of 10(-6).

300 angular momentum channels are recovered with bit-error rates below 3.8 x 10(-3).