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1  and intensity, emitted from a hot object at thermal equilibrium.
2 pic scale phenomena can also be generated at thermal equilibrium.
3            However, much of nature is not in thermal equilibrium.
4 re often needed, and some systems are not in thermal equilibrium.
5 lations found in physical systems outside of thermal equilibrium.
6 rm numerous self-assembled structures out of thermal equilibrium.
7 ngle red population of mEos4b is observed at thermal equilibrium.
8 ules help to reduce inelastic loss, ensuring thermal equilibrium.
9 o exotic new phenomena that are forbidden in thermal equilibrium.
10 ow to 'paint' with bacteria, is forbidden in thermal equilibrium.
11        This means that they operate far from thermal equilibrium.
12 eds an initial supply of resources away from thermal equilibrium.
13 ectronic states of matter that are hidden in thermal equilibrium.
14 creasing the conversion 260-fold compared to thermal equilibrium.
15 essed when the unperturbed system approaches thermal equilibrium.
16 ty due to small nuclear spin polarization in thermal equilibrium.
17 uations have been much less explored even in thermal equilibrium.
18 CX(4) CM-1(-), with all four states being in thermal equilibrium.
19 f interacting linear harmonic oscillators in thermal equilibrium.
20 osed, but was later shown to be forbidden in thermal equilibrium.
21 oherent light, in a process that is far from thermal equilibrium.
22 ower, and low cost 405 nm laser perturbs the thermal equilibrium.
23 n the maximization of entropy in a system at thermal equilibrium.
24 bly well, even though the system is far from thermal equilibrium.
25 ck temperatures and pressures sapphire is in thermal equilibrium.
26 supply that serves to keep the system out of thermal equilibrium.
27 orces, assembling aggregates that are out of thermal equilibrium.
28 without ever perturbing the system away from thermal equilibrium.
29 an enhancement of approximately 170,000 over thermal equilibrium.
30 ecting their intrinsic fluctuations while in thermal equilibrium.
31 l mechanisms impacting the system's balanced thermal equilibrium.
32 esponse to external fields can be studied in thermal equilibrium.
33 termine the magnetic state of the islands in thermal equilibrium.
34 tion and force biochemical systems away from thermal equilibrium.
35 tive dispersive-wave-like characteristics in thermal equilibrium.
36 ons far larger than those for populations in thermal equilibrium.
37 glement order of condensed-matter systems in thermal equilibrium.
38 ncement of up to 1,400-fold as compared with thermal equilibrium.
39 ving the particle distributions back towards thermal equilibrium.
40  that are not ergodic, and thus do not reach thermal equilibrium.
41 ny degrees of freedom that does not approach thermal equilibrium.
42  too rapid to measure without disturbing the thermal equilibrium.
43 pump or otherwise drive the system away from thermal equilibrium.
44 t, quantifies a hair bundle's deviation from thermal equilibrium.
45 s and diffusion coefficients of molecules in thermal equilibrium.
46 ments revealed the signatures of the SRPT in thermal equilibrium, a kink and a softening, respectivel
47 ngly small simplifications, such as assuming thermal equilibrium across the liquid-vapor interface du
48                      Most flatbands exist in thermal equilibrium and cannot be easily created or anni
49  fluctuations of its net moment, which is in thermal equilibrium and has no imposed polarization grad
50 state displacement of (1)H polarization from thermal equilibrium and perpetual spin-lattice relaxatio
51  the filaments in the aligned domains are in thermal equilibrium and that the diffusion coefficient p
52 rse cascades of weak turbulence (WT) theory, thermal equilibrium, and a fourth spectrum (MMT; Majda,
53 on due to barriers, however, still occurs at thermal equilibrium, and anomalous subdiffusion due to a
54 e opposite angular momentum according to the thermal equilibrium as seen in the photoluminescence dec
55                                  Our test of thermal equilibrium as well as our variance analysis can
56  (at V = 0) is not one of simple associative thermal equilibrium, as previously supposed; rather, it
57 he abundances of all isotopologues driven to thermal equilibrium at 250 degrees C.
58 00-fold in the (13) C NMR signal compared to thermal equilibrium at 9.4 T.
59 ntoxide, N(2)O(5), with which it is in rapid thermal equilibrium at lower tropospheric temperatures.
60 simplify the topology of DNA to levels below thermal equilibrium at the expense of ATP hydrolysis.
61 al origin-the radiative recombination of non-thermal-equilibrium band-edge carriers whose populations
62 sential way from those of systems in or near thermal equilibrium because of the flux of energy betwee
63 , leading to superthermal phonon bunching in thermal equilibrium between distinct modes.
64 ransition of PCB and to be essential for the thermal equilibrium between Pr and an intermediate state
65 mechano-stimulus photophysical behavior is a thermal equilibrium between the (1/3)LLCT states and a (
66 tive MW heating of polar solutes, perturbing thermal equilibrium between the solute and bulk solution
67      Preprocessed active site Cu(II) is in a thermal equilibrium between two species, an entropically
68 eshold, the polariton population splits to a thermal equilibrium Bose-Einstein distribution at in-pla
69 scribe systems residing out of the classical thermal equilibrium, both in stationary and nonstationar
70 tion of a mechanical ratchet is forbidden in thermal equilibrium, but becomes possible in systems out
71 pin interactions--under conditions of strict thermal equilibrium--by detecting and cross-correlating
72          Many-particle systems driven out of thermal equilibrium can show properties qualitatively di
73 ituents that are constantly driven away from thermal equilibrium can support spontaneous currents and
74 water hydroxyl hydrogen bond switching under thermal equilibrium conditions as T(aw) = 7 +/- 1 ps.
75 rivatives in room-temperature solution under thermal equilibrium conditions has been too fast to meas
76 us (Ht-M61A) at different temperatures under thermal equilibrium conditions were studied with infrare
77 ond complex were observed in real time under thermal equilibrium conditions with two-dimensional (2D)
78 and vitamin D allowed the calculation of the thermal equilibrium constants of the isomerization proce
79 rized state exponentially decays back to the thermal equilibrium, depending on the spin-lattice relax
80                                 Does overall thermal equilibrium exist between ions and electrons in
81       The global steady state of a system in thermal equilibrium exponentially favors configurations
82 a theoretical analysis of the active (out of thermal equilibrium) fluctuation of semiflexible polymer
83 ed, in this paper we propose a new notion of thermal equilibrium, focused on observables rather than
84               We characterise such notion of thermal equilibrium for an arbitrary observable via the
85 eveal fundamental barriers to staying out of thermal equilibrium for living systems.
86 and then thermalize, or find themselves near thermal equilibrium from the outset.
87 perature of arbitrarily complex materials in thermal equilibrium from X-ray Thomson scattering experi
88 etaT-cell receptor (TCR) operates outside of thermal equilibrium, harvesting energy via physical forc
89 suggest the smallest 2/3rds of species reach thermal equilibrium in <10s.
90        Moreover, we observe a deviation from thermal equilibrium in the resonant polariton population
91 rstanding how interacting particles approach thermal equilibrium is a major challenge of quantum simu
92 e total lattice motion at early times before thermal equilibrium is achieved.
93                       The relaxation back to thermal equilibrium is characterized by much slower time
94 pensating defects during processing close to thermal equilibrium is difficult because formation entha
95 -ion collision experiments well before local thermal equilibrium is established(1).
96                            The assumption of thermal equilibrium is made in nearly all computational
97          Quantum depletion of atomic BECs in thermal equilibrium is well understood theoretically but
98 esence of a temperature gradient, whereas in thermal equilibrium it is forbidden by the Bohr-van Leeu
99 hough superconductivity naturally emerges at thermal equilibrium, it can also emerge out of equilibri
100 erradiance in cytoskeletal protein fibers at thermal equilibrium, it is conjectured that the number o
101                                           At thermal equilibrium, ligand specificity is limited by th
102 ve the intrinsic thermal conductivity at the thermal equilibrium limit.
103               The diffusive model in a local thermal equilibrium medium has been well established for
104                                          Low thermal-equilibrium nuclear spin polarizations and the n
105 perpolarized (i.e., polarized far beyond the thermal equilibrium) nuclear spins can result in the rad
106 atures, we found underpopulation relative to thermal equilibrium of [Formula: see text] and spin-latt
107 the spin dynamics and approach towards local thermal equilibrium of a macroscopic ensemble of S = 3 c
108 ted the relaxation by rapidly perturbing the thermal equilibrium of the sample.
109 nal conversion and vibrational relaxation to thermal equilibrium on the dipeptide ground state occurs
110 ch, the acidity of the merocyanine form, the thermal equilibrium position between the spiropyran and
111 sitions but normal if the particles start at thermal equilibrium positions.
112 always a class of observables which exhibits thermal equilibrium properties and we give a recipe to e
113 e of two forms of bound CO that are in rapid thermal equilibrium rather than two distinct protein pop
114 MR experiment, while the chiral auxiliary at thermal equilibrium remained unobserved.
115 closed quantum systems can effectively reach thermal equilibrium, resolving the apparent incongruity
116 let charge-transfer state, assuring a solely thermal equilibrium route for an effective spin-flip pro
117      The appearance of these structures in a thermal equilibrium state (with the same average energy)
118 entration of 1.5 mM compared with that under thermal equilibrium state.
119 t of bath temperature, and for detecting non-thermal equilibrium states.
120 decrease in bending stiffness are present in thermal equilibrium, such as regions in which DNA melts
121 ensity fluctuations far larger than those in thermal equilibrium systems.
122 low-dimensional dynamical phenomena far from thermal equilibrium that exhibit some conservation law.
123 rmation driven by interacting proteins under thermal equilibrium that nucleate following diffusive co
124 ssembling particles that is allowed to reach thermal equilibrium, the energy of a given microscopic a
125          Likewise, for systems prepared near thermal equilibrium, the response to the driving is bare
126 rs of magnitude higher than that expected at thermal equilibrium; the expansion is highly anisotropic
127 fications gives rise to a continuous, out-of-thermal equilibrium transition through different methyla
128 patially homogeneous polariton condensate in thermal equilibrium, up to very high condensate fraction
129          The Brownian motion of molecules at thermal equilibrium usually has a finite correlation tim
130  several orders of magnitude relative to its thermal equilibrium value and offers a promising route t
131  a cavity can induce novel quantum phases in thermal equilibrium via symmetry breaking.
132 of the solution and surface, indicating that thermal equilibrium was attained rapidly.
133                       Individual polymers at thermal equilibrium were exposed to an elongational flow
134 mechanics is the definition of the notion of thermal equilibrium, which can be given as the state tha
135 st in two different conformational states at thermal equilibrium, which limits their effective photoc
136 ission of photoexcited electrons that are in thermal equilibrium with a semiconductor lattice, avoidi
137 an experimentally accessible qubit is not in thermal equilibrium with a surrounding spin bath, are pe
138 rk, producing optimized structures of DNA at thermal equilibrium with built-in or user-generated elas
139 nergy flux serves to heat the surface out of thermal equilibrium with bulk material, thus enabling lo
140 of filamentous (F-)actin and microtubules at thermal equilibrium with high spatial and temporal resol
141 nene gives a pi-complex of the norbornene in thermal equilibrium with its carbene isomer; at 90 degre
142 sition states along the reaction path are in thermal equilibrium with solvent, our ME results show th
143  is that the diffusing particle cannot be in thermal equilibrium with the binding sites; an equilibra
144 ements at low E/N ratios where ions are near thermal equilibrium with the buffer gas.
145 emented by using spins that rapidly get into thermal equilibrium with the environment, e.g., electron
146 nt chunks of contaminant that do not achieve thermal equilibrium with the fuel throughout the burn ph
147 roughly consistent with predictions based on thermal equilibrium with the planets' received radiation
148 ecules forming the chain are in chemical and thermal equilibrium with the surrounding bath, we observ
149 phonon modes, which drive the lattice toward thermal equilibrium with the well-known negative thermal

 
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