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 t the responses encoded only approximately 1 bit/s about constant-velocity stimuli but up to 29 bits/

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

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

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

7 However, B-form DNA can support only 1 bit of sequence conservation via contacts into the minor

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

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

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

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

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

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

14 ease digestion to manipulate strands of a 10-bit binary RNA library, we developed a molecular algorit

15 igitized with a 0.175-mm pixel size and a 10-bit gray scale.

16 780-nm near-infrared light imaged onto a 12-bit charge-coupled device (CCD) camera in response to a

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

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

19 2.5 metres with a spectral efficiency of ~16 bit s(-1) Hz(-1) using four independent orbital-angular

20 Five observers evaluated 20 16-bit posteroanterior digital chest radiographs compressed

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

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

23 The system was based on a high-speed, 16-bit AD/DA acquisition board that allowed high scan rates

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

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

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

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

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

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

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

31 The authors successfully reconstructed 24-bit color, 100 degrees field-of-view, composite retinal

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

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

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

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

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

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

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

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

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

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

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

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

44 The 32-bit Windows application START is implemented using Visua

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

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

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

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

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

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

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

59 + and R and supported on 64-bit Linux and 64-bit MS Windows.

60 ttp://bioinf.scri.ac.uk/tablet in 32- and 64-bit versions.

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

62 e/ as a self-contained binary package for 64-bit Linux computers and as python source-code.

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

64 implemented in C++ and R and supported on 64-bit Linux and 64-bit MS Windows.

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 ttp://bioinf.hutton.ac.uk/tablet in 32 or 64-bit versions for Windows, OS X, Linux or Solaris.

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

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

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

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

72 read the computed radiographs by using an 8-bit, 1,684 x 2,048-pixel display.

73 0-MHz catheter and digitized at 1 GHz with 8-bit resolution.

74 real time with a digitizer at 500 MHz with 8-bit resolution.

75 23.42 dB and effective number of bit is 3.89-bit.

76 and applied it to a 3 x 3 chessboard as a 9-bit instance of this problem.

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

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

79 Careful design of the COBE satellite, and a bit of luck, allowed the 30 &mgr;K fluctuations in the C

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

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

82 to invade into the TFT population, becomes a bit larger than predicted by the deterministic model.

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

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

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

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

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

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

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

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

91 prediction was remarkably accurate, if not a bit understated, for the reactivity of these compounds.

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

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

94 Although we know quite a bit about the epidemiology of Salmonella infection among

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

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

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

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

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

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

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

102 0, "not at all"; 1, "a little"; 2, "quite a bit"; or 3, "very much." Summing the six symptom scores

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

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

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

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

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

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

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

110 It costs 10(4) ATP molecules to transmit a bit at a chemical synapse, and 10(6)-10(7) ATP for grade

111 per unit bandwidth, is needed to transmit a bit, and more if quantized channels are used with photon

112 flickering" alpha-helical structure, until a bit of tertiary structure forms that stabilizes the syst

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

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

115 A single-electron memory, in which a bit of information is stored by one electron, is demonst

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

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

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

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

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

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

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

123 ng publicly available compound databases and bit string descriptors.

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

125 parameters, such as topological indices, and bit strings representing the presence or absence of cert

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

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

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

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

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

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

132 ion of a reversible, bistable nanotube-based bit.

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

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

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

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

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

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

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

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

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

142 r of mismatches) between their corresponding bit vectors.

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

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

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

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

157 presents a challenge to reaching even higher bit densities.

158 nd raw variant calls are available at http://bit.ly/1g8XqRt scripts and miscellaneous data at https:/

159 Source code and documentation are at http://bit.ly/pihelper.

160 nd a SPARQL endpoint, is available at http://bit.ly/TCGARoadmap.

161 A video tutorial is available at http://bit.ly/TCGARoadmapTutorial.

162 or (2) that each time a bird sings, a little bit of learning-motor engrainment-occurs, adding to memo

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

187 ally), and the energy dissipation ℰ per bit may be much less than the thermal energy scale kBT (

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

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

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

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

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

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

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

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

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

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

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

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

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

201 mputation is based on implementing a quantum bit with two optical modes containing one photon.

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

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

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

205 ystem that extends the lifetime of a quantum bit.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

232 transmit much more than just one regulatory bit.

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

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

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

236 Scan bit maps from the extensive LSC analyses confirmed that

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

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

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

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

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

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

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

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

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

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

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

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

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

250 The bit-parallel approach represents individual cells in an

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

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

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

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

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

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

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

258 is system to inbred mouse strains, the third bit of good fortune was the availability at the National

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

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

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

262 e minimal energy requirement per transmitted bit.

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

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

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

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

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

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

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

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

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

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

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

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