Results 51 to 60 of about 5,079,022 (381)
Le Journal de Physique Colloques, 1988 The exponent β that describes the sinusoidally modulate d ↔ paramagnetic phase transition crosses over from a value of 0.39 near TN to a mean field value away from TN. Electrical resistivity measurements near TN are given for the c axis and the critical behaviour is discussed.
G.H.F. Brits +2 more
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Target Localization with Unknown Transmit Power and Path-Loss Exponent Using a Kalman Filter in WSNs
Sensors, 2020 We present a novel hybrid localization algorithm for wireless sensor networks in the absence of knowledge regarding the transmit power and path-loss exponent.
SeYoung Kang, TaeHyun Kim, WonZoo Chung
doaj +1 more source
Critical exponents of Nikolaevskii turbulence [PDF]
Physical Review E, 2005 9 pages, 6 ...
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Critical Tsallis exponent in heavy ion reaction [PDF]
, 2001 The numerical solution of the nonlocal kinetic equation allows to simulate heavy ion reactions around Fermi energy. The expansion velocity and density profile show specific radial dependence which can be described with a Tsallis exponent of $q=5/3$. This
Morawetz, Klaus
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New Journal of Physics, 2019 We investigate the non-equilibrium dynamics across the miscible–immiscible phase separation in a binary mixture of Bose–Einstein condensates. The excitation spectra reveal that the Landau critical velocity vanishes at the critical point, where the ...
Xunda Jiang +3 more
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Groundstates of nonlinear Choquard equations: Hardy–Littlewood–Sobolev critical exponent [PDF]
, 2014 We consider nonlinear Choquard equation where N ≥ 3, V ∈ L∞(ℝN) is an external potential and Iα(x) is the Riesz potential of order α ∈ (0, N). The power in the nonlocal part of the equation is critical with respect to the Hardy–Littlewood–Sobolev ...
Vitaly Moroz, Jean Van Schaftingen
semanticscholar +1 more source
Dimensional Dependence of Critical Exponent of the Anderson Transition in the Orthogonal Universality Class [PDF]
, 2014 We report improved numerical estimates of the critical exponent of the Anderson transition in Anderson’s model of localization in d = 4 and 5 dimensions.
Yoshiki Ueoka, K. Slevin
semanticscholar +1 more source
Critical exponent for the quantum spin Hall transition in Z_2 network model
, 2011 We have estimated the critical exponent describing the divergence of the localization length at the metal-quantum spin Hall insulator transition. The critical exponent for the metal-ordinary insulator transition in quantum spin Hall systems is known to ...
Kobayashi, K., Ohtsuki, T., Slevin, K.
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The Oslo model, hyperuniformity, and the quenched Edwards-Wilkinson model [PDF]
, 2016 We present simulations of the 1-dimensional Oslo rice pile model in which the critical height at each site is randomly reset after each toppling. We use the fact that the stationary state of this sandpile model is hyperuniform to reach system of sizes $>
Dhar, Deepak +2 more
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Critical Exponents for Random Knots [PDF]
Physical Review Letters, 2000 The size of a zero thickness (no excluded volume) polymer ring is shown to scale with chain length $N$ in the same way as the size of the excluded volume (self-avoiding) linear polymer, as $N^ $, where $ \approx 0.588$. The consequences of that fact are examined, including sizes of trivial and non-trivial knots.
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