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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
28 s multiple segments at varying monochromatic energy levels (40-140 keV).
29 rm, allowing application at radiotherapeutic energy levels (50-350 MeV protons, 100-600 Mev/a.m.u car
30  single-energy multi-detector row CT at four energy levels (80, 100, 120, and 140 kVp).
31 ergy multi-detector row CT at four different energy levels (80, 100, 120, and 140 kVp).
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
37                                          The energy level alignment between the highest occupied mole
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
47 ayer and the substrate acts to influence the energy level alignment.
48 ese systems, such as engineering interfacial energy-level alignment and charge transfer (CT).
49                                              Energy level analysis of the three polymers demonstrated
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
52 acteristics of the cell such as respiration, energy level and apoptosis.
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
55 ross relevant inserts for each monochromatic energy level and iodine concentration.
56 e most probable state with relatively lowest energy level and lowest missing information compared to
57 poorer performance due to its low-lying LUMO energy level and nondisjointed HOMO/LUMO profile.
58                            The monochromatic energy level and the lesion iodine concentration had a s
59 f the variance is a function of the selected energy level and the lesion iodine content.
60  a shift toward lower energies of the ligand energy levels and a reduction of the HOMO-LUMO gap.
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.
63                       In addition to matched energy levels and complementary absorption spectrum with
64  orbital-lowest unoccupied molecular orbital energy levels and enhance the pai-conjugation.
65           Simultaneous control over both the energy levels and Fermi level, a key breakthrough for in
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
68          We use this method to determine the energy levels and interaction strengths of a fully conne
69 lving competing transitions between multiple energy levels and it has been difficult to precisely det
70 portant role in the cellular response to low energy levels and mediates AMPK-mTORC1 signaling.
71                               The electronic energy levels and optical transitions of a semiconductor
72                              By matching the energy levels and optimizing the molecular packing, high
73                    Twenty RCTs compared ESWT energy levels and placebo and consistently showed that h
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
77 porating BAI acceptor possess low-lying LUMO energy levels and small HOMO-LUMO gaps.
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
81                        Given the position of energy levels and the distribution of electronic couplin
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.
84 e at the desired electrochemical potentials (energy levels) and at different protein sites.
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
87 wth and metabolism in response to nutrients, energy levels, and growth factors.
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
96 erimentally only the electron densities and -energy levels are directly observable.
97                              These excitonic energy levels are experimentally found to be robust agai
98                                 The confined energy levels are highly sensitive to the specific nanos
99                                 Upon stress, energy levels are maintained by increased mitochondrial
100 he radical cation suggest that SOMO and HOMO energy levels are near-degenerate.
101             While the weakly interacting low-energy levels are used as memory to store classical info
102 able boron-doped PAHs (corresponding to LUMO energy levels as low as fullerenes).
103                              Moreover, their energy levels, as revealed by the intracellular ATP/ADP
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
106 t-times fluorinated derivative, with tunable energy levels based on mixing ratio.
107 es contain high protein, low cholesterol and energy levels, being its consumption recommended.
108                       Under an excitation at energy levels below 1.3 eV, VSiVC(0) are converted into
109 its allowed for fine control over electronic energy levels both in solution and in the bulk.
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
120 by monitoring the population of an auxiliary energy level coupled to the ground state.
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
123                                           An energy level diagram for fully decoupled electron- and p
124 ic voltammetry measurements of the ChaMs, an energy level diagram is constructed relating the ChaMs a
125                                           An energy-level diagram visualizing different photochemical
126 thick layer of a single molecule, but if the energy levels differed, the current voltage behavior exh
127 odel agrees well with that of the Fermi/HOMO energy level difference.
128 eneous N-QDCs with the standard deviation of energy level distribution sigma(epsilon) is a Lorentzian
129 reduction processes, and have low-lying LUMO energy levels down to -3.62 eV.
130 d lowest unoccupied molecular orbital (LUMO) energy level due to the fluorination of A units.
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
136 o a monoexponential decay, typical of single energy level emitters.
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
140                          We characterize the energy levels, excited state structures, and dynamics of
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
143                                      Precise energy levels for both the neutral and charged dark exci
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
147 cell growth and proliferation in response to energy levels, growth factors, and nutrients.
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
153 Cyclic voltammetry was used to determine the energy levels (HOMO and LUMO) in the bistriazines.
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
159       Our study confirms that the filling of energy levels in compressed atoms more closely follows t
160 ergetic offsets between the charge transport energy levels in different morphological phases of polym
161 ported by quantum-chemical simulation of SiV energy levels in small nanodiamonds.
162 e from Si and C impurities occupying shallow energy levels in the bandgap.
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
168                In contrast, low nutrient and energy levels induce FOXO1 activity.
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
171 llapse, that is, the coalescence of discrete energy levels into a continuous band.
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
176            An anticrossing of the driven dot energy levels is observed when the Zeeman and valley spl
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.
182                                    Also, the energy level matching between the conduction bands of Cd
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
188                                         Fine energy-level modulations of small-molecule acceptors (SM
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
191 , due to fractal nature, generation of newer energy levels never stops.
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
194  Importantly, this effect was observed at an energy level of 50.25 keV, but not with 50.0 keV.
195 luence of conformational aspects on the HOMO energy level of anellated 1,4-thiazine paves the way to
196  motions, is found to depend strongly on the energy level of local mesoscale eddy variability.
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
202 efect state that resides below the predicted energy level of the dark excitons.
203 e lowest unoccupied molecular orbital (LUMO) energy level of the porphyrins and, consequently, facili
204                         As we correlate each energy level of the resonance band of organic jelly, as
205 ced at small negative potentials giving LUMO energy levels of -3.57 to -3.74 eV.
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
209 oposal of quantum jumps between two discrete energy levels of an atom(1).
210  effect of a dense plasma environment on the energy levels of an embedded ion is usually described in
211 estimated by calculations only involving the energy levels of an isolated neutral atom.
212 (3) modification of g-C3N4 with well-matched energy levels of another semiconductor or a metal as a c
213 off-resonance light can be used to shift the energy levels of atoms, molecules, and solids.
214 es, approaches can be devised to control the energy levels of cation sublattices in semiconductors.
215 vskite solar cells comes from the nonmatched energy levels of charge transport layers.
216 er, unlike conventional semiconductors where energy levels of defects are well documented, they are e
217  from the favorable alignment of interfacial energy levels of DMASnBr(3) and g-C(3) N(4) .
218                  Furthermore, the electronic energy levels of even the same spin are dense on the sca
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
221 , we implement a technique for resolving the energy levels of interacting photons.
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
229                                          The energy levels of the donor-acceptor conjugates were fine
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
233                           The structures and energy levels of the molecular layers included donor mol
234 ffectively impact the optical properties and energy levels of the molecules.
235 vice resistances track with the valence band energy levels of the PM(n) wire, which were modulated vi
236 t the local electric field that broadens the energy levels of the PNA nucleobases.
237                                     The HOMO energy levels of the polymers can be progressively incre
238                                 The relative energy levels of the possible transition states of the I
239             The precisely controlled triplet energy levels of the quantum dot photocatalysts facilita
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
243                 A dynamic model based on the energy levels of the two early charge-separated states,
244                                     When the energy levels of the two molecular layers were similar,
245 nate leads to a splitting of the vibrational energy levels of the umbrella mode.
246 ded crossings of the quantum mechanical spin energy-levels of radicals formed in cryptochromes.
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
250                       The effect of acceptor energy level on electron transfer rate in blends of the
251                            Modulation of its energy level on the energy landscape in photosynthetic v
252  they represent physiological states such as energy level or stress in response to environmental and
253                                We found that energy-level ordering is inverted with respect to visibl
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.
256 s were reconstructed in 10-keV increments at energy levels ranging from 40 to 140 keV.
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)
258              Virtual monochromatic images at energy levels ranging from 80 to 140 keV did not show ps
259  occurred on virtual monochromatic images at energy levels ranging from 90 to 140 keV.
260                 Additionally, dipole-induced energy-level realignment between the two binary segments
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: -
263 of the gate is simply to shift the molecular energy levels relative to the metal Fermi level.
264              We show the analogy between the energy level schemes of the special pair and of the lase
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
267                                        These energy level shifts may play a major role in PSC perform
268  is electronic in origin and will modify the energy-level spectrum and electronic and magnetic proper
269               The strategy for tailoring the energy level splitting of Ln ions by the highly designab
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
273 er band gaps are narrowed mainly due to LUMO energy level stabilization.
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
282           For each vascular compartment, the energy level that provided optimal evaluation on virtual
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
285           It affects mitochondrial function, energy levels, the lipid environment, and transcriptomic
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
289                             First, a shallow energy level traps a photoexcited electron.
290                                        Here, energy level tuning and molecular doping are combined to
291                               Therefore, the energy level tuning effect has a crucial impact on the m
292 ive metabolism modes paradoxically increases energy levels under substrate restriction.
293 favor of the T form, which moves to a higher energy level upon oxygen release.
294 rturbation theory calculations of electronic energy levels, we determined the band edge positions of
295 tenuation for each insert and reconstruction energy level were recorded.
296 g electrochemical and computational studies, energy levels were established to visualize excited stat
297 al estimations of frontier molecular orbital energy levels, which are reported and discussed.
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

 
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