Datasets:

nehathorat

/

image-demo125

like 0

<s> Bit error ratio of LDPC code after decoupled log-likelihood computation and belief-propagation algorithm. <e>

<s> Comparison of the randomness certification power of the new inequality (solid blue line) and the CHSH inequality (dashed red line). We plot upper bounds on the probability that Eve successfully guesses the outcome of the A0 measurement as a function of the noise parameter η. <e>

<s> C2N as a function of heliocentric distance z in units of R�. Filled circles denote the C2N derived using estimates of Dφ(s) by Armstrong et al. (1990), the open circle indicates C2N used for estimates of Dφ(s) by Anantharamaiah et al. (1994), and the filled boxes are for Spangler & Sakurai (1995). Data points in blue correspond to solar minimum, and data points in red correspond to solar maximum. <e>

<s> Variation of rAθ with axial position at the Axis-II cathode radius. The right scale is the equivalent normalized emittance corresponding to the flux linking the cathode. The location of the cathode is indicated by the vertical solid red line. <e>

<s> The Multi-MaxSense Algorithm <e>

<s> . Evolution of the weighting scheme for the joint simplicity and PDF refinement using the dynamic weighting scheme throughout the refinement as a function of proposed moves. <e>

<s> . All sensor-ID lists between 2 am and 6 am of the six days for deducing bedroom sensors in Milan. <e>

<s> Final occupation probabilities of the states |1〉 (red squares), |2〉 (green open symbols), and |3〉 (blue closed symbols) for the triangle model with strong decoherence (g/∆ = 4). More specifically, the symbols are: circles for Ĉ0:1, triangles for Ĉ1:3, inverted triangles for Ĉ3:1, and diamonds for Ĉ1:0. For comparison, we also show the occupation probabilities for the case g = 0: green x symbols for the state |2〉, blue stars for the state |3〉, and none for the state |1〉 because the probabilities coincide with those shown by the red squares. The solid, dashed, and dotted lines show the respective theoretical predictions obtained by assuming that the final occupation probabilities are determined by the sequence of three LZ processes at the three avoided crossings with no contribution from quantum interference terms. The blue symbols and the green symbols both exhibit rather irregular oscillations as functions of δ, and these oscillations also vary depending on the choice of Ĉ. While the details of these features cannot be explained easily without a quantitative analysis, the points to note in this figure are that the theoretical formulae (dashed and dotted lines) give good overall fits to the respective sets of simulation data and in particular that decoherence suppresses the quantum-interference-induced deviations from the results of the probability-based calculation. This behavior confirms that the main effect of the coupling to the environment is to suppress the quantum-interference effects between the three LZ processes. <e>

<s> Calculation of the magnetic field gradient ∂z|B| produced at the surface of the main mirror with currents set to I1 = I4 = 1.4 A, I2 = I3 = 3.5 A and without any external field applied. <e>

<s> . ∆Φ distributions for soft-soft, hard-hard, and soft-hard particle pairs in Au+Au collisions at √ sNN = 200GeV at centrality 30-40%. <e>