ライフサイエンスコーパス: Bell

1 Bell inventory scores did not significantly differ accor

2 Bell non-locality between distant quantum systems--that

3 Bell tests - the experimental demonstration of a Bell in

4 Bell's palsy (BP) is an acute and idiopathic paralysis o

5 Bell's palsy is a common cranial neuropathy causing acut

6 Bell's palsy is a relatively common disease characterize

7 Bell's palsy is more prevalent in women who are either p

8 Bell-shaped cell spreading curves encompassing all subst

9 Bell-shaped pH versus rate profiles were observed for V(

10 Bell-shaped profiles were observed for k(cat) and k(cat)

11 Bell-shaped profiles were observed for kcat and kcat/Km

12 Bell-shaped relationships between adherence and resistan

13 Starting in 1965, Bell and others constructed mathematical inequalities wh

14 A Bell-type measurement performed on the hybrid state of s

15 tionally using transition state theory and a Bell tunneling correction yielded a value (1.58) far bel

16 We used the CNOT gate to generate a Bell state with 78% fidelity (corrected for errors in st

17 ducting phase qubits were used to generate a Bell-type state.

18 the presence of drives and dissipation is a Bell state, an essential building block for quantum info

19 We measure a Bell signal of 2.0732 +/- 0.0003, exceeding the maximum

20 No violation of a Bell inequality has been observed for a system entangled

21 Here we demonstrate the violation of a Bell inequality in a solid-state system.

22 The recently reported violation of a Bell inequality using entangled electronic spins in diam

23 tests - the experimental demonstration of a Bell inequality violation - are central to understanding

24 rified by way of the measured violation of a Bell inequality, and it can be used for communication pr

25 t starkly demonstrated by the violation of a Bell inequality.

26 Clauser-Horne-Shimony-Holt formulation of a Bell test to characterize entanglement between an artifi

27 een an artificial atom and a cat state, or a Bell-cat.

28 obtain a single quantum bit and to prepare a Bell state.

29 Here we report a Bell experiment that is free of any such additional assu

30 Utilizing a Bell-like model to describe a shedding rate which presum

31 -that is, joint correlations which violate a Bell inequality--can be verified without trusting the me

32 glet states and states that do not violate a Bell inequality.

33 s of the protocol is assessed by violating a Bell inequality, with the degree of violation determinin

34 ing, the isotopic data are consistent with a Bell tunneling correction factor of Q(H) = 12 and an ima

35 MAD2 complex is cell cycle regulated with a "Bell" shaped profile and peaks at prometaphase.

36 visualize certain four-level dynamics in a 'Bell frame' comprising an effective pair of uncoupled tw

37 best simulated by Monte Carlo with the above Bell parameters and an average of 1.48 bonds (n = 1 bond

38 This "axial" current is the chiral (Adler-Bell-Jackiw) anomaly investigated in quantum field theor

39 s cannot be attributed uniquely to the Adler-Bell-Jackiw chiral anomaly of bulk Dirac/Weyl fermions.

40 massless Dirac fermions, known as the Adler-Bell-Jackiw chiral anomaly, has also been observed.

41 Since being discovered by Alexander Bell, photoacoustics may again be seeing major resurgenc

42 , or any vaccine (all vaccines combined) and Bell's palsy (definite and probable cases combined).

43 um advantage in communication complexity and Bell nonlocality.

44 In comparison with entanglement and Bell nonlocality, Einstein-Podolsky-Rosen steering is a

45 fective colitis with colonic perforation and Bell Palsy (both possibly related).

46 , including squeezed states, Fock states and Bell states, plays an important role in quantum informat

47 Our measured value of the appropriate Bell's 'signal' is 2.25 +/- 0.03, whereas a value of 2 i

48 tically produce and stabilize an approximate Bell state of two trapped-ion quantum bits (qubits), ind

49 Necrotizing enterocolitis, defined as Bell stage 2 or greater by preplanned adjudication.

50 component of Q(12)/Q(13) = 1.028 (borrowing Bell's nomenclature for hydrogen tunneling corrections).

51 e representation of a new mother affected by Bell's palsy subsequent to her recent pregnancy.

52 es of transmission coefficients predicted by Bell's formula, kappaBell , agree well with multidimensi

53 loading rate dependence of F(R) predicted by Bell's model, we find that experimentally accessible par

54 The relationship proposed by Bell fit the data significantly the best and also predic

55 In this issue of Molecular Cell, Bell et al. identify an isoform of hTAF(II)80 that is in

56 the 1830s, several others (including Charles Bell, Francois-Amilcar Aran and Jean Cruveilhier) had al

57 ethanolic extracts from Melaphis chinensis (Bell), the Chinese Nutgall, exhibited strong inhibition

58 We find a violation of the CHSH-Bell inequality of 2.35 +/- 0.18, in agreement with the

59 We performed 245 trials that tested the CHSH-Bell inequality S </= 2 and found S = 2.42 +/- 0.20 (whe

60 of the second experiment and of the combined Bell tests.

61 To date, Bell tests have relied on careful calibration of measure

62 By realizing a fully deterministic Bell-state measurement combined with real-time feed-forw

63 The scheme allows direct Bell state generation with an observed maximum fidelity

64 stages of idiopathic facial paralysis (i.e., Bell's palsy), but their effectiveness is uncertain.

65 le children in elementary schools of eastern Bell County, Texas.

66 e 125 pN were considerably lower than either Bell or Hookean spring model predictions, suggesting the

67 emonstrate the stabilization of an entangled Bell state of a quantum register of two superconducting

68 tions, we have prepared ions in an entangled Bell state with 97% fidelity-about six times better than

69 ary outcomes were necrotising enterocolitis (Bell stage 2 or 3), blood culture positive sepsis more t

70 une Seung and colleagues describe the Eugene Bell Foundation's experience of treating MDR-TB in North

71 to evaluate the fidelity to a time-evolving Bell state, revealing entanglement between photons emitt

72 the assumption that hidden parameters exist, Bell tacitly makes a variety of other assumptions that c

73 the assumption that hidden parameters exist, Bell tacitly makes a variety of other assumptions; for i

74 mputational studies, which employed extended Bell theory to predict the force dependence of the activ

75 nergies is obtained from the minimal (Eyring-Bell-Evans) model using the local coordinate common to a

76 and whose radiographs fulfilled criteria for Bell's stage 2 or 3 necrotising enterocolitis.

77 e exponential force dependence expected from Bell's equation.

78 rofile associated with humans suffering from Bell's Palsy or Moebius Syndrome.

79 ely, and using Kramers-based theories (e.g., Bell-Evans and Dudko-Hummer-Szabo models), we extract th

80 squeezed state in the context of generalized Bell inequalities.

81 In 1903, Alexander Graham Bell developed a design principle to generate lightweigh

82 herpes zoster and 1 DZB(-)MMF(+) subject had Bell's palsy possibly related to VZV.

83 We derive the hierarchical Bell model, a theory that explicitly considers the hiera

84 ieved by a variant of the techniques used in Bell-type proofs but only for a subclass of objective lo

85 For instance, Bell assumes that the hidden parameters do not depend on

86 In this issue, Bell et al. (), drawing on the unique 50-year data set a

87 More than 50 years ago, John Bell proved that no theory of nature that obeys locality

88 that behave consistently within the Kramers-Bell-Evans model of force-mediated dissociation.

89 We validate this platform by measuring Bell inequality violations and performing quantum state

90 sepsis, necrotising enterocolitis (modified Bell stage >/=2), or death in infants 32 weeks' gestatio

91 from a set of suitably chosen multiparticle Bell tests, we identify conditions bounding the quality

92 , we connect the violation of a multipartite Bell inequality with the amount of tripartite entangleme

93 ated a propensity score for the risk of NEC (Bell's stage 2 or 3) after day 7 of life.

94 n archaeological sites of the Late Neolithic Bell Beaker Complex and the Early Bronze Age from the Le

95 Numerous Bell inequality tests have been reported; however, all e

96 The experimentally observed Bell-Evans-Polanyi correlations, in the presence of stro

97 ber 1999, there were 1,181 incident cases of Bell's palsy among US service members.

98 potential contributors to the development of Bell's palsy, but the precise cause remains unclear.

99 ld ion flows corresponding to experiments of Bell and Miller.

100 ions): these correlations violate a form of Bell's inequality.

101 as evidenced by their violation of a form of Bell's inequality.

102 -mediated aggregation using the formalism of Bell where the forward rate of bond formation dictated a

103 ent lifetimes, we derive a generalization of Bell's formula that is formally exact within the framewo

104 The celebrated inequalities of Bell are based on the assumption that local hidden param

105 However, the well known inequalities of Bell are based on the assumption that local hidden param

106 blished studies on the medical management of Bell's palsy and highlight strategies in the surgical ma

107 We argue that the mathematical model of Bell excludes a large set of local hidden variables and

108 s presenting within 72 hours of the onset of Bell palsy?

109 a knowledge of the clinical presentation of Bell's palsy.

110 We show that the known proofs of Bell's inequalities contain algebraic manipulations that

111 rends, and demographic correlates of risk of Bell's palsy during a 2-year period.

112 1.31) were independent predictors of risk of Bell's palsy.

113 at certain vaccines may increase the risk of Bell's palsy.

114 ing the MWI, I show that the quantum side of Bell's inequality, generally believed nonlocal, is reall

115 es (e.g., reactivation of herpes simplex) of Bell's palsy.

116 hy of the state produced, and make a test of Bell's inequality with non-identical atoms.

117 vir to oral corticosteroids for treatment of Bell palsy was associated with a higher proportion of pe

118 lished guidelines for the acute treatment of Bell's palsy advocate for steroid monotherapy, although

119 proven to be efficacious in the treatment of Bell's palsy and should be offered to patients presentin

120 rapy have been proposed for the treatment of Bell's palsy for many years, the clinical efficacy of th

121 of antiviral medications in the treatment of Bell's palsy.

122 However, complete verification of Bell non-locality requires high detection efficiencies,

123 CHSH (Clauser-Horne-Shimony-Holt) version of Bell's inequality for this novel entangled state and fin

124 ble: it is a consequence of the violation of Bell inequalities by entangled quantum systems.

125 tified randomness, based on the violation of Bell inequalities.

126 ts with massive particles, this violation of Bell's inequality was obtained by use of a complete set

127 demonstrated and used to show violations of Bell's inequality and to implement simple quantum algori

128 description of pulling experiments based on Bell's expression for the force-induced rupture rate is

129 dely used phenomenological approach based on Bell's formula, but also free energies of activation.

130 cal nor a mathematical basis but is based on Bell's translation of the concept of Einstein locality i

131 code qubits in either an even or odd parity Bell state, conditioned on the syndrome qubit state.

132 e six states reported, namely the odd-parity Bell states and the W state, were not actually produced.

133 ocol and physical implementation for partial Bell-state measurements of Fermionic qubits, allowing fo

134 ce of local hidden variables does not permit Bell-type proofs to go forward.

135 field loss, trigeminal neuralgia, recurrent Bell's palsy, and pulsatile tinnitus.

136 iled to form membrane tethers, the regressed Bell parameters (consistent with single bond Monte Carlo

137 The self-report Bell Object Relations Reality Testing Inventory was admi

138 Here we report on data from a second Bell experiment using the same experimental setup with m

139 a beneficial role in select cases of severe Bell's palsy.

140 ing measurement statistics that violate some Bell inequality.

141 both quantum state tomography and the strict Bell-CHSH test, both of which confirm a high level of on

142 The Bell frame constitutes a promising tool for control of m

143 The Bell inequalities are based on a mathematical model of t

144 The Bell-Evans-Polanyi principle does not account for the ob

145 subsequent pan-European cultures such as the Bell Beakers expanding out of Iberia in the Late Neolith

146 Because the Bell inequality was designed to test for non-classical b

147 -force distributions were well fitted by the Bell model.

148 hree selectin dissociation constants fit the Bell and Hookean spring models of force-driven bond brea

149 l evidence of continuing traditions from the Bell Beaker Complex to the Early Bronze Age.

150 Linearity in the Bell-Evans-Polayni graph and the finding of a large kine

151 antum correlations exists in the form of the Bell inequalities, measurements of which provide strong

152 ser-Horne-Shimony-Holt (CHSH) version of the Bell inequality.

153 ns that surpass the classical maximum of the Bell inequality.

154 Interestingly, application of the Bell model shows two energy barriers that correlate with

155 quantum value to the classical value of the Bell quantity becomes unbounded with the increase in the

156 n the constraint and a generalization of the Bell-Colella-Glaz algorithm to treat time-dependent cons

157 Our approach is a generalization of the Bell-Colella-Glaz predictor-corrector method for incompr

158 Unstressed k(off) values based on the Bell model were 2.4, 2.6, 2.8, 3.8 s(-1) for P-selectin,

159 Based on the Bell-Evans-Polanyi principle, it is demonstrated how the

160 According to the Bell model, at short times of contact between cell and v

161 in a rich dynamical evolution, where the two Bell-frame qubits undergo entangling-disentangling oscil

162 of a CHSH (Clauser-Horne-Shimony-Holt)-type Bell inequality on entangled states composed of differen

163 hus directly tests the principles underlying Bell's inequality.

164 s are intrinsically anti-bunched and violate Bell's inequality by 17 standard deviations High-visibil

165 of these operations are necessary, violating Bell inequalities (i) with certainty using unaligned, bu

166 re observed in this category: (1) volitional Bell's phenomenon and (2) intorsion with fixation.

167 s that remove this need for trust, even when Bell non-locality is not present.

168 resemble the clinical signs associated with Bell's Palsy and Moebius Syndrome in humans.

169 zed, factorial trial involving patients with Bell's palsy who were recruited within 72 hours after th

170 In patients with Bell's palsy, early treatment with prednisolone signific

171 he chances of full recovery in patients with Bell's palsy.