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1 osed, but was later shown to be forbidden in thermal equilibrium.
2 n the maximization of entropy in a system at thermal equilibrium.
3 bly well, even though the system is far from thermal equilibrium.
4 ck temperatures and pressures sapphire is in thermal equilibrium.
5 supply that serves to keep the system out of thermal equilibrium.
6 without ever perturbing the system away from thermal equilibrium.
7 an enhancement of approximately 170,000 over thermal equilibrium.
8 ecting their intrinsic fluctuations while in thermal equilibrium.
9 esponse to external fields can be studied in thermal equilibrium.
10 termine the magnetic state of the islands in thermal equilibrium.
11 tion and force biochemical systems away from thermal equilibrium.
12 tive dispersive-wave-like characteristics in thermal equilibrium.
13 ons far larger than those for populations in thermal equilibrium.
14 glement order of condensed-matter systems in thermal equilibrium.
15 ncement of up to 1,400-fold as compared with thermal equilibrium.
16 ving the particle distributions back towards thermal equilibrium.
17 that are not ergodic, and thus do not reach thermal equilibrium.
18 ny degrees of freedom that does not approach thermal equilibrium.
19 too rapid to measure without disturbing the thermal equilibrium.
20 pump or otherwise drive the system away from thermal equilibrium.
21 t, quantifies a hair bundle's deviation from thermal equilibrium.
22 s and diffusion coefficients of molecules in thermal equilibrium.
23 oherent light, in a process that is far from thermal equilibrium.
24 ngly small simplifications, such as assuming thermal equilibrium across the liquid-vapor interface du
25 fluctuations of its net moment, which is in thermal equilibrium and has no imposed polarization grad
26 state displacement of (1)H polarization from thermal equilibrium and perpetual spin-lattice relaxatio
27 the filaments in the aligned domains are in thermal equilibrium and that the diffusion coefficient p
28 rse cascades of weak turbulence (WT) theory, thermal equilibrium, and a fourth spectrum (MMT; Majda,
29 on due to barriers, however, still occurs at thermal equilibrium, and anomalous subdiffusion due to a
31 (at V = 0) is not one of simple associative thermal equilibrium, as previously supposed; rather, it
32 ntoxide, N(2)O(5), with which it is in rapid thermal equilibrium at lower tropospheric temperatures.
33 sential way from those of systems in or near thermal equilibrium because of the flux of energy betwee
34 tive MW heating of polar solutes, perturbing thermal equilibrium between the solute and bulk solution
35 eshold, the polariton population splits to a thermal equilibrium Bose-Einstein distribution at in-pla
36 tion of a mechanical ratchet is forbidden in thermal equilibrium, but becomes possible in systems out
37 pin interactions--under conditions of strict thermal equilibrium--by detecting and cross-correlating
38 water hydroxyl hydrogen bond switching under thermal equilibrium conditions as T(aw) = 7 +/- 1 ps.
39 rivatives in room-temperature solution under thermal equilibrium conditions has been too fast to meas
40 us (Ht-M61A) at different temperatures under thermal equilibrium conditions were studied with infrare
41 ond complex were observed in real time under thermal equilibrium conditions with two-dimensional (2D)
42 and vitamin D allowed the calculation of the thermal equilibrium constants of the isomerization proce
43 a theoretical analysis of the active (out of thermal equilibrium) fluctuation of semiflexible polymer
44 ed, in this paper we propose a new notion of thermal equilibrium, focused on observables rather than
48 pensating defects during processing close to thermal equilibrium is difficult because formation entha
49 esence of a temperature gradient, whereas in thermal equilibrium it is forbidden by the Bohr-van Leeu
54 always a class of observables which exhibits thermal equilibrium properties and we give a recipe to e
55 e of two forms of bound CO that are in rapid thermal equilibrium rather than two distinct protein pop
59 decrease in bending stiffness are present in thermal equilibrium, such as regions in which DNA melts
60 low-dimensional dynamical phenomena far from thermal equilibrium that exhibit some conservation law.
61 ssembling particles that is allowed to reach thermal equilibrium, the energy of a given microscopic a
62 rs of magnitude higher than that expected at thermal equilibrium; the expansion is highly anisotropic
66 mechanics is the definition of the notion of thermal equilibrium, which can be given as the state tha
67 ission of photoexcited electrons that are in thermal equilibrium with a semiconductor lattice, avoidi
68 of filamentous (F-)actin and microtubules at thermal equilibrium with high spatial and temporal resol
69 nene gives a pi-complex of the norbornene in thermal equilibrium with its carbene isomer; at 90 degre
70 sition states along the reaction path are in thermal equilibrium with solvent, our ME results show th
71 is that the diffusing particle cannot be in thermal equilibrium with the binding sites; an equilibra
73 emented by using spins that rapidly get into thermal equilibrium with the environment, e.g., electron
74 roughly consistent with predictions based on thermal equilibrium with the planets' received radiation
75 ecules forming the chain are in chemical and thermal equilibrium with the surrounding bath, we observ
76 phonon modes, which drive the lattice toward thermal equilibrium with the well-known negative thermal
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