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1 ble for determining the lowest triplet state energy level.
2 lar charge transfer and lowering of the LUMO energy level.
3 sists of naphtalene diimides having low LUMO energy level.
4 7) on selection of the optimal monochromatic energy level.
5 h delocalization of electrons near the Fermi energy level.
6 p and mixing of the frontier valence orbital energy levels.
7 e thermal quenching processes and activation energy levels.
8 rphometry is associated with decreased brain energy levels.
9 ransfer on the S1 states and anti-correlated energy levels.
10 e substituent effects on their HOMO and LUMO energy levels.
11 ven interactions leading to the splitting of energy levels.
12 nabolic environments in addition to cellular energy levels.
13 s evidence for partial unpinning of the TiO2 energy levels.
14 to a modification of the polymer electronic energy levels.
15 trum, consisting of highly degenerate Landau energy levels.
16 lectronic properties including HOMO and LUMO energy levels.
17 ale heating region is evaluated at different energy levels.
18 7C3-A20, a compound that stabilizes cellular energy levels.
19 cues such as nutrients, growth factors, and energy levels.
20 coupled with a matching donor with suitable energy levels.
21 ies, including atomic precision and discrete energy levels.
22 perovskites have a different composition and energy levels.
23 omain wall, displaying discrete quantum-well energy levels.
24 onal landscapes of proteins and their rugged energy levels.
25 able motor activity) and related subjective (energy) levels.
26 in the lowest-sodium model also varied with energy level (~0.5 mg/kcal) and ranged from 500 to 1250
27 ounts in the base model varied directly with energy level (1.0 mg Na/kcal) and ranged from 996 to 317
29 rm, allowing application at radiotherapeutic energy levels (50-350 MeV protons, 100-600 Mev/a.m.u car
32 ze the probability of sustaining appropriate energy levels across the entire foraging trajectory.
33 ectroporation catheter ablation with various energy levels after subxiphoid pericardial puncture.
34 ions play an important role in how molecular energy levels align to the graphene Dirac point, and may
35 R intraribbon heterostructures have a type-I energy level alignment and strongly localized interfacia
36 valent doping on charge-carrier dynamics and energy level alignment at the interface of perovskite NC
38 ood on the basis of a quantitative interface energy level alignment model, which indicates that bipol
39 pectroscopy (CMEAS), for the first time, the energy level alignment of a polymer:fullerene bulk heter
40 that the switch is due to the change in the energy level alignment of the redox states relative to t
41 of the morphology of the blend film and the energy level alignment on the efficiency of charge separ
42 ing molecular properties like solubility and energy level alignment while maintaining the high fissio
43 IPE spectrum contains information regarding energy level alignment within a complete, working molecu
44 ly considering the molecular interaction and energy level alignment, and highly efficient OPV devices
45 easurably inferior morphology and nonoptimal energy level alignment, resulting in PCEs of 5.34% and 4
46 voltaic characterizations disclosed that the energy level alignment, the molecular orbital profile, a
50 e lowest unoccupied molecular orbital (LUMO) energy level and a narrowing of the highest occupied mol
51 ong, it favors a higher ageostrophic kinetic energy level and an increase in surface chlorophyll conc
53 trated surface lowers transition metal redox energy level and consequently promotes the formation of
54 ults, to determine the localized As-impurity energy level and coupling parameters in the band anti-cr
56 e most probable state with relatively lowest energy level and lowest missing information compared to
61 ferences was greatest at lower monochromatic energy levels and at lower iodine concentrations (averag
62 n was used to identify optimal monochromatic-energy levels and compare them with single-energy CT.
66 to increase JSC , but also possess suitable energy levels and high mobility to afford high VOC and F
67 ring of phononic heat carriers with magnetic energy levels and increased phonon scattering due to enh
69 lving competing transitions between multiple energy levels and it has been difficult to precisely det
74 -ligand bond length can shift its electronic energy levels and predictably guide electron-transfer re
75 -withdrawing effect of F, and finally adjust energy levels and reduce bandgap, which is beneficial to
76 rd, we observe crossing and anti-crossing of energy levels and reveal the non-trivial topological mod
78 polymer semiconductors exhibiting different energy levels and structural order, ranging from amorpho
79 ed devices is attributed to a combination of energy levels and structured surface morphology that cau
80 city to synthesize ATP at physiological free energy levels and that the resulting changes to myocardi
82 requirement for proper alignment of material energy levels and the need to process emitting materials
83 terplay between the relative position of the energy levels and the polymer matrix microstructure.
85 lens was enhanced from 7.4 to 11 mm at this energy level, and peak pressure (41 MPa) and maximum cav
86 quantum transition between avoided crossing energy levels, and also results in unexpected magnetic b
88 The extended photoresponse, well-matched energy levels, and high hole mobility from optimized BHJ
89 transfer characteristics, easy tenability of energy levels, and low production cost, organic semicond
90 of the few open quantum systems in which the energy levels, and not just the excited-state lifetimes,
91 s in solids or in molecules possess discrete energy levels, and the associated quantum states can be
92 ignals, including growth factors, nutrients, energy levels, and various stress conditions, regulates
93 of strong coupling in WSe(2)/WS(2), that is, energy-level anticrossing and oscillator strength redist
94 l glycolysis.SIGNIFICANCE STATEMENT Neuronal energy levels are critical for proper CNS function, but
95 hole-transport materials (HTMs) with tunable energy levels are designed and synthesized for efficient
104 ements and bond distortions that control the energy levels at the valence and conduction band edges,
105 omogeneity translates into a distribution of energy levels, band gaps, work functions, and other char
110 mi-elliptic bands to free-atom-like discrete energy levels, bridging the complexity of electronic des
111 e these variations by adjusting the electron energy levels, but the more ambitious goal of creating q
112 ell lifetime whereas increasing the cellular energy level by AMP-activated kinase (AMPK) activation d
113 del predictions that decreasing the cellular energy level by glucose starvation decreases leader cell
114 ivation of interface states and alignment of energy levels by intrinsic molecular polarization, as we
115 f virtual monochromatic images at an optimal energy level can overcome renal cyst pseudoenhancement.
116 , they go through a sequence of states whose energy levels can be computed and arranged into a step-b
117 n of semiconducting polymer frontier orbital energy levels can drive spectral shifts of SWNT hole pol
118 ur model shows that increasing intracellular energy levels can increase the number of supported stabl
119 tion that acts as a "dopant," introducing an energy level closer to the electrodes' Fermi level than
121 -Zener formula in the vicinity of an avoided energy-level crossing will cause considerable errors due
122 phase-controlled pulses with up to a 100 muJ energy level, depending on the filling gas, pressure and
124 ic voltammetry measurements of the ChaMs, an energy level diagram is constructed relating the ChaMs a
126 thick layer of a single molecule, but if the energy levels differed, the current voltage behavior exh
128 eneous N-QDCs with the standard deviation of energy level distribution sigma(epsilon) is a Lorentzian
131 ctric field causes a shift in the electronic energy levels due to the Stark effect, which induces a t
132 the mitochondrial apoptotic pathway and cell energy level during differentiation of mESCs into the ca
133 capture the overpopulation of high internal energy levels during the excitation phase and also the d
134 hase and also the depletion of high internal energy levels during the quasi-steady-state (QSS) dissoc
135 a thin polymer interlayer with intermediate energy levels, electrons and holes can effectively shutt
137 conductor nanomaterials feature size-tunable energy level engineering, which considerably expands the
138 nstrate that side-chain conjugation can tune energy levels, enhance absorption, and electron mobility
139 acceptor material, including more favorable energy levels, enhanced light absorption and stronger in
141 Here we show that, owing to the much higher energy level for the Cu 3d(10) orbitals than for the Ag
142 of these compounds; i.e., (1) the lower HOMO energy levels for BN anthracenes stabilize the molecules
144 rmination of the valence and conduction band energy levels for noncovalently modified (6,5) chirality
145 ns were retrospectively reconstructed at VMI energy levels from 40 to 140 keV in 5-keV increments and
146 In obesity, fundamental reductions in brain energy levels, gray matter density, and cortical metabol
148 inverted populations of atomic and molecular energy levels have been predicted theoretically to exhib
149 nt method to optimize the hybrid structure's energy levels, here comprising ZnO and a tailored ladder
150 ymers with high molar absorptivity, suitable energy levels, high charge carrier mobility and high sol
151 layers in perovskite solar cells with ideal energy levels, high charge mobilities and improved therm
152 have deep highest occupied molecular orbital energy levels, high crystallinity, optimal bulk-heteroju
154 ne) was found to have lower frontier orbital energy levels (HOMO/LUMO=-5.9/-4.0 eV) than poly(3-hexyl
155 sample when measured directly at the 186 keV energy level if the attenuation of the high TDS of the f
156 lbenzene) based layer, a molecule whose HOMO energy level in a vacuum is close to the Fermi level of
157 he correct ordering of singlet excited-state energy levels in a pentacene molecule (E (S1) < E (D)) f
158 The SnRK1 protein kinase balances cellular energy levels in accordance with extracellular condition
160 ergetic offsets between the charge transport energy levels in different morphological phases of polym
163 tic activity is due to aligning the protonic energy levels in the PCET steps, while improving the act
164 toelectron spectroscopy to characterize hole energy levels in the polymer phases of polymer:fullerene
165 allenge of controlling molecular packing and energy levels in the solid state precludes clear determi
166 e demonstrate voltage tunability of the spin energy-levels in a single quantum dot by modifying how s
167 the ternary copolymers show up-shifted LUMO energy levels, increased electron mobilities, and improv
169 tunnelling spectroscopy we obtain charge and energy-level information for these boron nitride defect
170 nanocomposite resulted in spatially varying energy levels inside the nanocomposite that enhanced the
172 a higher lowest unoccupied molecular orbital energy level (IOIC2: -3.78 eV vs IHIC2: -3.86 eV), broad
173 w enthalpy of formation, and that the defect energy level is a shallow donor to the conduction band r
174 tion to variationally computed rovibrational energy levels is investigated, employing triatomic AB[Fo
175 The measurement and understanding of their energy levels is key to scientific and technological pro
177 anging molecular structure will alter system energy levels leading to a change in the transport barri
178 proach was used to investigate the effect of energy level, lesion size, lesion iodine content, and im
179 rapamycin prevented the increase in cellular energy levels, lysosomal biogenesis, and endocytic uptak
180 ed highest occupied molecular orbital (HOMO) energy level mainly due to the additional octyl on the D
181 ures and of the medium can produce transient energy level matching among multiple electronic states.
183 by leveraging on van der Waals coupling and energy level matching between two-dimensional Ruddlesden
184 ubility in common solvents and features good energy level matching with poly(3-hexylthiophene) (P3HT)
185 Cs) provides higher carrier mobility, better-energy level matching, and superior stability, as well a
186 enhanced head CT scans at 65-75 keV (optimal energy levels) maximizes image quality compared with sca
187 onventional CdSe/ZnS QDs, which have a large energy level mismatch between CdSe and ZnS and thus show
189 ed in detecting and interpreting nutrient or energy levels-most notably, the insulin/insulin-like gro
190 The practice of comparing host and dopant energy levels must consider the long-range electrostatic
192 ergy drink is not efficacious in enhancing s-energy levels, nor any related cognitive or behavioral v
193 plays a critical role in regulating cellular energy levels, observations that have broad implications
195 luence of conformational aspects on the HOMO energy level of anellated 1,4-thiazine paves the way to
197 ore requires the knowledge of the nature and energy level of low-lying excited states that could be c
198 nique for examining position of the impurity energy level of p-type dopants in nitride semiconductors
199 formation is due to the lowering of the HOMO energy level of the aryl moiety to reduce the process of
200 ngs are shown to dramatically lower the LUMO energy level of the carboxonium electrophile (compared t
201 sor system; it can encode sensitivity to the energy level of the cell and creates independent topolog
203 e lowest unoccupied molecular orbital (LUMO) energy level of the porphyrins and, consequently, facili
206 l monochromatic images were reconstructed at energy levels of 40-140 keV (in 10-keV increments) in ei
207 substrate, with the goal of influencing the energy levels of a coadsorbed chromophore, is explored.
208 resolution, in the vacant space between two energy levels of a given resonance band, a new band appe
210 effect of a dense plasma environment on the energy levels of an embedded ion is usually described in
212 (3) modification of g-C3N4 with well-matched energy levels of another semiconductor or a metal as a c
214 es, approaches can be devised to control the energy levels of cation sublattices in semiconductors.
216 er, unlike conventional semiconductors where energy levels of defects are well documented, they are e
219 ) and phi of 5-17 and computed HOMO and LUMO energy levels of fragments of 5-17, i.e., 8-vinyl 9-Me-a
220 the confined electronic orbitals and related energy levels of individual semiconductor quantum dots h
222 hibited by the difficulty in determining the energy levels of molecules after being perturbed by inte
223 onal theory for calculations of valence band energy levels of nanoscale precipitates of CdS, CdSe, Zn
224 e potentiometric valence and conduction band energy levels of semiconducting carbon nanotubes; (ii) p
225 omophore, is a versatile method to shift the energy levels of such chromophores with respect to the b
226 es of the model quartic potential and in the energy levels of the [H, C, N] potential energy surface.
227 sis of the DFT calculations of the HOMO-LUMO energy levels of the chiral forms, these compounds can b
228 paring the singly occupied molecular orbital energy levels of the corresponding phosphine radical cat
230 p to 0.33 A impart remarkable effects on the energy levels of the frontier orbitals of Au25(SR)18(-)
231 nductors with appropriate bandgaps, suitable energy levels of the frontier orbitals, and high intrins
232 ion via Channel I and II pathways, including energy levels of the materials involved, exciton diffusi
235 vice resistances track with the valence band energy levels of the PM(n) wire, which were modulated vi
240 that through crossconjugation the electronic energy levels of the radical cation state may be control
241 duce disorder to study the statistics of the energy levels of the system as it undergoes the transiti
242 g, electronic inductive effects modulate the energy levels of the system resulting in compression of
247 ent obstacle to that end is the unfavourable energy level offset at hybrid inorganic/organic structur
248 at increases the driving force, which is the energy level offset between the conduction band energy o
249 at exhibits the smallest donor/acceptor LUMO energy level offset, the photocurrent quantum yield fall
252 they represent physiological states such as energy level or stress in response to environmental and
254 -D structure, donor state density, and Fermi energy level position are critical for maintaining the s
255 ld exceeds the separation between rotational energy levels, preventing state-selective ionisation.
257 ad an energy fluence of 9 mW/cm(2) and total energy levels ranging from 5.4 J/cm(2) up to 10 J/cm(2)
261 alent to a Nernst distribution for one redox energy level, redox site coverage is both underestimated
262 occupied molecular orbital (LUMO) (-3.80 eV) energy levels relative to ITIC1 (HOMO: -5.48 eV; LUMO: -
265 The network is also modular, containing energy level sensing proteins that connect to four outpu
266 ments so far have not shown valley-selective energy level shifts in fields accessible in the laborato
268 is electronic in origin and will modify the energy-level spectrum and electronic and magnetic proper
270 aspects of upconversion processes, including energy level splitting, transition probability, line bro
271 ns in the host materials can determine their energy level splitting, which is of vital importance to
272 zed as the host material to embed Eu(3+) and energy-level splitting was achieved for tuning its photo
274 store classical information (bits), the high-energy levels strongly interact with neighboring magnets
275 r centres are generated, and their symmetry, energy level structure, magnetic and optical properties,
276 increased visible light absorption, altered energy level structures, and variable cage geometries, w
277 rphinato)zinc(II) moiety with low-lying pai*-energy levels, sufficiently destabilize MC states and st
278 the regional and gene-specific responses to energy levels suggest a complex, interactive network whe
279 re generally poorly conducting because their energy levels tend to lie far from the Fermi energy of t
280 cross a range of mood/cognitive/behavioral/s-energy-level tests after consumption of the energy drink
281 1.42 eV redox, respectively) and higher HOMO energy levels than those of their pentacene analogues (2
283 m(2) attributable to the proper alignment of energy levels that led to the efficient harvesting of ex
284 PDK1-3 and PDH phosphorylation and decreased energy levels that were significantly ameliorated after
286 sparency, good conductivity, and appropriate energy levels, the solar-cell efficiency and lifetime ar
287 re hydrophobic and have slightly higher LUMO energy levels, thus providing better device performance
288 , this dye possesses favorable HOMO and LUMO energy levels to render efficient sensitizing action in
294 rturbation theory calculations of electronic energy levels, we determined the band edge positions of
296 g electrochemical and computational studies, energy levels were established to visualize excited stat
298 ers as the dipole layer to tune the relative energy levels, which can potentially maximize the open c
299 gth of electrons, metal NCs exhibit discrete energy levels, which in turn result in the emergence of
300 mic diarylethene moieties possessing similar energy levels yet different propensity to aggregate with