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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 ed at the constituent level and at different effective temperatures.
6 monopole-chain' states that exhibit negative effective temperatures.
7 que was used to lower the internal energies (effective temperatures ~100 K), yielding well-resolved s
9 ven by small-step motors are described by an effective temperature and are thus quiescent, at higher
11 the scaling relations between granule size, effective temperature and surface gravity that are predi
15 istance are studied, from which we obtain an effective temperature at each microwave power level.
16 obtain a measurement of the transient local effective temperature at which a photo-isomerizing molec
17 ensemble with large entropy and well-defined effective temperature becomes locally indistinguishable
18 ces with measured distances and an estimated effective temperature between that of Jupiter (170 K) an
20 ing episode is caused by the dropping of its effective temperature by at least 170 K on 2020 January
21 ry also allows an estimate of nonequilibrium effective temperatures characterizing the response and f
22 onnecting cells, we create materials with an effective temperature coefficient of electrical resistan
24 plified by their superior clinical score and effective temperature control compared with their wild-t
25 an temperature of the device and thus allows effective temperature control without an additional sens
27 ients in resource availability can alter the effective temperature dependence of ecological processes
29 effective chemical potential or by a reduced effective temperature, depending on the spin current pol
32 repared in local thermal states at different effective temperatures, employing a Nuclear Magnetic Res
33 th optical excitation and d.c. current, with effective temperatures exceeding several hundred kelvin.
34 ertainty may be the major contributor to the effective temperature factor (B-factor) describing contr
35 Raman emission may be used to determine the effective temperatures for both the vibrational modes an
37 sheared dense granular system, we extract an effective temperature from a relation connecting their d
38 nteractions under three conditions: (i) high effective temperature, (ii) translation invariance, and
39 at such a pumping can create remarkably high effective temperatures in a narrow spectral region of th
40 population of LFSs is a strong function of (effective) temperature in the ergodic liquid phase, risi
42 ance and reliability, population density and effective temperature influence the cost-to-benefit asse
43 tial relationship between vapor pressure and effective temperature is determined as a function of app
48 orm an explicit computation to show that the effective temperature measured from this relation coinci
50 the atmosphere of a cool brown dwarf with an effective temperature of 380 K in a spectrum taken with
52 s ferooxidans microorganisms with an optimum effective temperature of around 30 degrees C (referred t
53 es of the Great Eruption of eta Carinae, the effective temperature of its outburst is significantly l
56 ociation spectra of M(+)(H2O)(x=2-5)Ar (with effective temperatures of approximately 50-150 K, depend
61 The latter, sometimes termed the fictive (or effective) temperature, plays important roles in nonequi
62 uced resonance measurement to demonstrate an effective temperature reduction by a factor of ~25, i.e.
63 t comfortable state, with a neutral Standard Effective Temperature (SET) range of 13.0 to 22.73 degre
64 an be mapped on each other by introducing an effective temperature shift of [Formula: see text] K.
66 uch as reaction mechanisms, catalysis, local effective temperatures, surface interactions, and charge
69 thermometer that allows the assignment of an effective temperature (T(eff)) to each moiety in these c
70 ApNE solute so that it experiences a higher effective temperature than the measured temperature of t
71 imentation, but one essential ingredient--an effective temperature that provides a mechanism for ther
72 avior of the active process, we introduce an effective temperature that, for each frequency component
74 mulate a two-site Hubbard Hamiltonian at low effective temperatures with single-site resolution using