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1 umes are governed by a single parameter--the effective temperature.
2 es interacting process using the language of effective temperature.
3 ferent samples onto columns kept at the same effective temperature.
4 luctuations in particle number can act as an effective temperature.
5 monopole-chain' states that exhibit negative effective temperatures.
6 que was used to lower the internal energies (effective temperatures ~100 K), yielding well-resolved s
8 ven by small-step motors are described by an effective temperature and are thus quiescent, at higher
10 the scaling relations between granule size, effective temperature and surface gravity that are predi
13 obtain a measurement of the transient local effective temperature at which a photo-isomerizing molec
14 ry also allows an estimate of nonequilibrium effective temperatures characterizing the response and f
15 onnecting cells, we create materials with an effective temperature coefficient of electrical resistan
17 an temperature of the device and thus allows effective temperature control without an additional sens
18 ients in resource availability can alter the effective temperature dependence of ecological processes
20 effective chemical potential or by a reduced effective temperature, depending on the spin current pol
23 th optical excitation and d.c. current, with effective temperatures exceeding several hundred kelvin.
24 ertainty may be the major contributor to the effective temperature factor (B-factor) describing contr
25 Raman emission may be used to determine the effective temperatures for both the vibrational modes an
26 sheared dense granular system, we extract an effective temperature from a relation connecting their d
27 at such a pumping can create remarkably high effective temperatures in a narrow spectral region of th
28 population of LFSs is a strong function of (effective) temperature in the ergodic liquid phase, risi
33 orm an explicit computation to show that the effective temperature measured from this relation coinci
36 es of the Great Eruption of eta Carinae, the effective temperature of its outburst is significantly l
38 ociation spectra of M(+)(H2O)(x=2-5)Ar (with effective temperatures of approximately 50-150 K, depend
45 thermometer that allows the assignment of an effective temperature (T(eff)) to each moiety in these c
46 ApNE solute so that it experiences a higher effective temperature than the measured temperature of t
47 imentation, but one essential ingredient--an effective temperature that provides a mechanism for ther
48 avior of the active process, we introduce an effective temperature that, for each frequency component
50 mulate a two-site Hubbard Hamiltonian at low effective temperatures with single-site resolution using
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