ライフサイエンスコーパス: hole

1 ) Schwarzchild radii for a 10(9)M((.)) black hole).

2 iezometers in the pristine catchment of Mule Hole.

3 ormed between the substrate and the oxyanion hole.

4 s, referred to as the North Atlantic warming hole.

5 dditionally showed an outer lamellar macular hole.

6 tual Coulomb attraction between electron and hole.

7 Arg residue in the formation of an oxyanion hole.

8 ng, indicating the localization of the doped holes.

9 r: mutated BEAT > original BEAT > knobs-into-holes.

10 depends on closure of nuclear envelope (NE) holes.

11 he study, of which 12 were secondary macular holes.

12 as well as on the carrier type, electrons or holes.

13 ly fragmented along with multiple nucleating holes.

14 internal structure of doped electrons versus holes.

15 of the spin-valley state of localized single holes.

16 waves(1) and in the first imaging of a black hole(2).

17 This phenomenon is likely to explain the 'k-hole', a state of oblivion likened to a near death exper

18 eve optimized contact for both electrons and holes, a doping-free logic inverter is demonstrated with

19 nthesised carbon-dots ((m)CD) possess unique hole-accepting nature, prolonging the electron lifetime

20 ed by scavenging of electrons by O(2) causes hole accumulation in the MHP film.

21 otocol has begun to heal the Antarctic ozone hole and avoided more global warming than any other trea

22 Herein we report the successful hole and electron doping of the transition-metal oxyhydr

23 mpared to Ru-complexes decreases the rate of hole and electron recombination and enhances the charge

24 igma(RT) <= 1.3 x 10(-2) S/cm) is enabled by hole and electron transport (mu(e)/mu(h) <= 5.70 x 10(-5

25 , all lying within 0.04 parsecs of the black hole and forming a class that is probably unique to this

26 n the process, penetrates through the narrow hole and generates highly nonuniform heating, which in t

27 nstrated no difference between the knob-into-hole and WT IgG4 molecules in E. coli.

28 can be controlled by varying the size of the hole and/or the duration of laser irradiation.

29 vent invasion of excess ER membranes into NE holes and a defective NE permeability barrier.

30 atment option especially in those with small holes and CME.

31 al reactions by electrochemical injection of holes and electrons, also known as "electrochemical cata

32 imentally extract the effective mass of both holes and electrons.

33 igned to equilibration between three surface holes and M(OH)-O-M(OH) sites.

34 hase and mitosis, so mechanisms that seal NE holes and protect its unique composition are critical fo

35 transmembrane dimers oligomerize into small holes and uncouple the proton gradient.

36 tates plays a key role in the study of black holes, and our work simulates such nontrivial structures

37 topology and quasiparticle band structure of hole- and electron-doped Sr(2)IrO(4) are striking given

38 that the lack of cross-reactivity in glycan hole antibodies is due to amino acid differences within

39 ontrast to previously described BG505 glycan hole antibodies, the B41-specific nAbs accommodate the >

40 The knob-into-hole approach is an effective way to produce bispecific

41 Suppression of segregation occurs when holes are extracted by a hole transport layer (spiro-OMe

42 especially through the formation of electron holes, are investigated.

43 amplify transport of ions, not electrons and holes as is done in electronic systems.

44 that is able to transport ions and electrons/holes, as tested in electrochemical absorption spectrosc

45 sion is driven by super-exchange and doublon-hole-assisted tunneling, and strongly violates the quant

46 Activity from the super-massive black hole at the Galactic Centre, which is coincident with th

47 nd long-lived charge carriers (electrons and holes) at room temperature in the dark, even long after

48 [Formula: see text] and [Formula: see text] hole bands near the [Formula: see text] and M point is o

49 in full control over shuttling electrons and holes between C(60), ZnP, and Fc is novel.

50 al tunneling of photogenerated electrons and holes between frontier orbitals of adjacent, weakly inte

51 an engineered glycosyltransferase, "bump-and-hole" (BH)-GalNAc-T2, boosts labeling in a programmable

52 finement of the electromagnetic field in the holes both by theoretical modelling and spectroscopic me

53 -OMeTAD) deposited on the MHP, thus avoiding hole build-up.

54 fficient Coulomb screening of an electron or hole by extended ordering of dipoles from symmetry-broke

55 broader neutralization to the common glycan hole can be achieved, we immunized rabbits with B41 SOSI

56 suitable alternative to generate a high free hole carrier concentration for GaN.

57 grown under optimized conditions show a free hole carrier concentration with a maximum value of 6 x 1

58 CsClO(4)), to induce degenerate electron and hole carrier densities at the device contacts to form th

59 The high hole carrier mobility is uncommon for complex bulk mater

60 d that the mobility and concentration of the hole carriers both decreased upon increasing the target

61 from B41, a subtype B virus, shares a glycan hole centered on positions 230 and 289.

62 rs, oxygen vacancies, and nonbridging oxygen hole centers) convert CO(2) to methane with excellent pr

63 d time-resolved spectroscopies, such as core hole clock and laser flash photolysis measurements, we h

64 Eight eyes (89%) achieved successful hole closure and resolution of CME with concurrent impro

65 y, and not to epiretinal membrane or macular hole codes.

66 [Formula: see text] M ( ), implying a black hole companion of [Formula: see text] M ( ).

67 0-fold increase in the number of ~0.8 eV hot holes, compared to Au, and a threefold increase in the c

68 zed as a correlated nearly-complete electron-hole-compensated semimetal.

69 sis reveals that the nearly perfect electron-hole compensation could drive the appearance of non-satu

70 pacts of band convergence, vacancy-augmented hole concentration, and lattice softening, NaSn(m)SbTe(m

71 mula: see text], which rises with decreasing hole concentration, p.

72 ation of Fermi-surface reconstruction to two hole concentrations where the superconducting upper crit

73 Here, hole-conductive poly(3,4-ethylenedioxythiophene) (PEDOT)

74 ies such as the band alignment and resulting hole confinement.

75 ytoplasmic membranes directly adjacent to NE holes containing meiotic spindle microtubules.

76 eptor to facilitate charge separation, while holes could transfer to CuO(x) to avoid deep dehydrogena

77 laser to reveal the dynamics of the valence hole created by strong-field ionization and to track the

78 ion mechanism that is third order in surface-hole density, which is assigned to equilibration between

79 well as anatomic features on OCT, including hole diameter and presence of vitreomacular traction, ep

80 Average initial hole diameter was 79.6 mum (range, 44-132 mum).

81 The presence of a visible hole, diffuse fibrinopurulent exudate, intra-abdominal a

82 cooperative, multidentate, convergent sigma-hole donors, as shown by molecular dynamics simulations

83 Here, we synthesize and investigate hole-doped Sr(2-x)K(x)IrO(4) utilizing a combination of

84 CuO(2) sheets in cuprate superconductors and hole doping (Ni(1+/2+) , Ru(2+) ) or electron doping (Ni

85 ity of cation vacancies results in excessive hole doping and frustrates the ability to control the th

86 elical ordering of electric dipoles by light hole doping of the quadruple perovskite BiMn(7)O(12) In

87 the intrinsic behaviour of Sr(2)IrO(4) upon hole doping remains enigmatic.

88 suggest that Ti atoms effectively introduce hole doping, thus rapidly decreases the total energy of

89 Upon hole doping, we observe the formation of a coherent, two

90 itical transition temperature (T (c)), light hole-doping to the parent compound, which is an antiferr

91 primary H/D KIE leads to the inference that hole-driven scission of the O-H bond in H(2) O is a crit

92 ble consequences, e.g., negatively affecting hole/electron conduction and severely shortening device

93 DFT analysis of Y6 crystals reveals hole/electron reorganization energies of as low as 160/1

94 Upon free electron-hole encounters at later times, both charge-transfer sta

95 data to guide mutations in the BG505 glycan hole epitope in an attempt to broaden the reactivity of

96 were that autologous NAbs to the N289 glycan hole epitope were consistently induced in mice given sol

97 505-specific nAbs bind to overlapping glycan hole epitopes.

98 shold energy for impact ionization while the holes experience the multiple valence minibands scatteri

99 r illumination through a combination of fast hole extraction and minimized nonradiative recombination

100 ending in perovskite effectively facilitates hole extraction to hole transport layer and expels elect

101 The accelerated hole extraction was linked to a low ideality factor of 1

102 ed charge carriers at the p-n junction, with holes flowing to the p-side and electrons flowing to the

103 beta3 strand necessary to form the oxyanion hole for acylation and also traps ceftriaxone in a nonca

104 Also, more microscopic holes, fragments, strips in treated samples were observe

105 ormational dynamics induced by the knob-into-hole framework, and the conformational stability is simi

106 n emission following the Auger decay of O 2s holes from adsorbed oxygen and oxide surfaces are very e

107 Such (m)CD rapidly extracts holes from CN and prevents the surface adsorption of met

108 s for photoexcited carriers is the escape of holes from trap states, which prolongs the apparent life

109 Eyes with full-thickness macular hole (FTMH, 12/72 eyes, 16.7%) displayed a "sunflower" e

110 onent is introduced, which provides a second hole-generation and transporting mechanism to minimize t

111 gainst catalytic proposals invoking oxyanion hole geometric discrimination between the ground state a

112 1/2 species indicate a ligand-based electron hole, giving this complex an Fe(II)-thiyl radical electr

113 olated resonance associated with the valence hole (H(2)O(+)/OH) enabled straightforward detection.

114 Although both the electron/hole high mobilities have been calculated for BAs, there

115 This is ascribed to the percolation hole hopping on the surface states.

116 jected electron and the oxidized sensitizer (hole hopping) are both operative in the composite mechan

117 Injection of holes, i.e. formation of the TPP radical cation, inside

118 s of the Milky Way host a supermassive black hole identified with the position of the radio and infra

119 layer of the GaAs substrate and metallic via-holes implemented in the central patch of each row const

120 the local hyperfine fields for electron and hole in Alq(3): B(hf1) = (0.63 +/- 0.01) mT (electron),

121 Accretion onto the supermassive black hole in some active galactic nuclei (AGN) drives relativ

122 cluded lattice in 196 eyes (54.0%), atrophic holes in 126 eyes (34.7%), retinal tears in 111 eyes (30

123 on emission following the relaxation of O 1s holes in [Formula: see text].

124 es from separated transport of electrons and holes in [WO(4) ](-2) and [Bi(2) O(2) ](+2) layers respe

125 ient recombination of injected electrons and holes in a confined 2D channel.

126 he size of and distance between the circular holes in a hexagonal or square lattice structure.

127 arrays of optically addressable spin-valley holes in a solid state platform.

128 y leads to the co-existence of electrons and holes in an undoped semiconductor.

129 iers) with electrons occupying Cu center and holes in ligands.

130 rays made of nanoantennas represented by the holes in NPG.

131 However, there are still major holes in our understanding of T. gondii biology, includi

132 the exact function of plasmon-generated hot holes in regulating the morphology of nanostructures has

133 tive interaction among the electrons and the holes in semiconductors usually leads to s-wave excitons

134 flipping could be completely inhibited when holes in the bilayer were backfilled with bovine serum a

135 layer can efficiently separate electrons and holes in the intralayer excitons with a type II alignmen

136 It is time for policymakers to plug the holes in the ozone hole treaty.

137 After degradation, holes in the PCL films exposed to pH 0 were observed, an

138 in the TCO can travel back to recombine with holes in the perovskite layer.

139 lts provide further insight into the role of holes in the phase segregation of MHPs and hole mobility

140 insertion of opportunely designed nanometric holes in the photonic circuit, which are available for a

141 To ensure sufficient photogenerated holes in the rear subcell, a small amount of an infrared

142 terspecific variation in the geometry of the holes in the structures, and verify with finite-differen

143 hat the presence of visual impairment on pin-hole increased significantly with increasing age (odds r

144 For the use of the black-hole indicator dye, the calix[4]pyrrole was modified wit

145 nteractions, which simultaneously accelerate hole injection and hinder excessive electron injection.

146 nanoscopic mechanism of sequential electron-hole injection for exciton generation in nanocrystal-bas

147 s us to explain behavior related to electron/hole injection from the tip, interaction with UV light,

148 While hole injection into neutral quantum dots is generally co

149 rge-confinement-enhanced sequential electron-hole injection mechanism probed at the single-nanocrysta

150 tralization strategy of a conducting-polymer hole-injection layer is used to prevent detrimental surf

151 tantially increased affinity through a sigma-hole interaction.

152 vskites, unraveling the key role of electron-hole interactions and dielectric screening.

153 original BEAT, mutated BEAT, and "knobs-into-holes" interfaces, suggested a cooperative assembly proc

154 At low temperatures holes introduced via substitution of La by Sr segregate

155 llent thermal stability, dual functionality (hole/ions transportation), one-dimensional (1D) lamellar

156 n emission following the Auger decay of O 2s hole is nearly as efficient as electron emission followi

157 show that the recent North Atlantic warming hole is of anthropogenic origin.

158 nogens remains difficult.IMPORTANCE A glycan hole is one of the most dominant autologous neutralizing

159 ectively transfer photoexcited electrons and holes is an important endeavor toward achieving high-eff

160 nal survival was affected by accumulation of holes, leading to users discarding nets.

161 al in the treatment of large stage 4 macular hole (MH) > 400 mum and to evaluate reconstructive anato

162 g which factors influence idiopathic macular hole (MH) size is important because it is a major progno

163 stabilize inverted ILM flap onto the macular hole (MH) were reviewed.

164 ed for vitreomacular traction (VMT), macular hole (MH), and epiretinal membrane (ERM) according to th

165 iques are used for the management of macular holes (MHs).

166 For topological hole minibands tuned to have a finite Chern number, we f

167 transport characteristics with electron and hole mobilities approaching 0.40 and 0.07 cm(2) V(-1) s(

168 iadiazole, are imperative for achieving high hole mobilities in this relatively amorphous polymer.

169 they also increase the average electron and hole mobility by at least 2-fold.

170 f holes in the phase segregation of MHPs and hole mobility in perovskite solar cells.

171 ) measurements demonstrate that 1 displays a hole mobility of 0.31 cm(2) V(-1) s(-1), and the 1-C(70)

172 OFETs fabricated with 1 and 2 both exhibited hole mobility of 10(-5) and 10(-3) cm(2)/(V s), respecti

173 he delaminated FL-BP crystals exhibit a high hole mobility of 76 cm(2) V(-1) s(-1) and an on/off rati

174 cture, reduces the bandgap and increases the hole mobility of alpha-FAPbI(3).

175 We achieve an effective hole mobility of ~35 cm(2 )V(-1 )s(-1), on/off current r

176 ogues have been able to match or surpass the hole mobility that can be obtained by IDT-BT.

177 At half-filling of the first hole moire superlattice band, we observe a Mott insulati

178 nd the conformational impact by the knob and hole mutations, we combined size-exclusion chromatograph

179 nds, often dubbed the North Atlantic warming hole (NAWH).

180 larger image dataset obtained from the Woods Hole Oceanographic Institution.

181 lexation induces a polarisation of the sigma hole of ChB and XB heteroditopic receptor donors as a si

182 nstraints are lifted, and SrNi(4+) O(3) with holes on adjacent O anions is stabilized as a perovskite

183 ing hysteresis and promoting stable electron holes on O(2-) that are revealed by X-ray absorption spe

184 Localization of holes on the iodide site in the MHP induces instability

185 ve been developed, patterning closely spaced holes on the nanoscale in graphene nanoribbons is still

186 ppearance of positively charged areas (sigma-holes) on the surface of the iodine substituents in I(4)

187 Hole or electron doping of phases prepared by topochemic

188 rder of the vitreomacular interface (macular hole or epimacular membrane).

189 plex curved and multi-connected shapes (e.g. holes or sharp-to-smooth mating edges).

190 dissipation occurs ~1 parsec from the black hole (or ~10(4) Schwarzchild radii for a 10(9)M((.)) bla

191 ombination of an inversion layer, induced by holes (or electrons) at the interface of the semiconduct

192 s of compact objects (neutron stars or black holes) or relativistic shocks launched from such objects

193 at 370 nm, followed by delocalization of the hole over the T(4) segment.

194 ost a long-lived "dark" exciton, an electron-hole pair in a spin-triplet configuration.

195 inding energy-the energy binding an electron-hole pair through the electrostatic Coulomb force-indepe

196 e tribovoltaic effect, in which the electron-hole pairs at the sliding interface are excited by the e

197 The electron-hole pairs at the sliding interface are subsequently sep

198 s of freedom of excitons, which are electron-hole pairs bound by the Coulomb attraction in a photoexc

199 ton is the bosonic quasiparticle of electron-hole pairs bound by the Coulomb interaction(1).

200 on-resonant photoexcitation of free electron-hole pairs have been challenging to directly probe becau

201 By optically exciting electron-hole pairs in a crystalline silicon membrane, we single

202 e alkanol-oxidation by photoexcited electron-hole pairs on a polymeric semiconductor.

203 und and trapped excitons as well as electron-hole pairs originating from their disintegration.

204 iency through the production of two electron-hole pairs per incident photon.

205 Generation of electron-hole pairs via symmetry-breaking charge separation (SB-C

206 Molecular triplet excitons (bound electron-hole pairs) are 'dark states' because of the forbidden n

207 much smaller mass, excitons (bound electron-hole pairs) are expected to condense at considerably hig

208 lomb attraction between interfacial electron-hole pairs.

209 TAC donor as well as the spatially separated hole-particle wavefunctions, three of the five compounds

210 re, >=20% increase in time to complete the 9-Hole Peg Test [9HPT], >=20% increase in time to perform

211 ctions in the spinal cord and brain of the 9-Hole Peg Test and cortical thickness and spinal cord gre

212 cus on quarter filling, corresponding to one hole per moire unit cell.

213 que and reveal a Mott insulator state at one hole per superlattice site and surprising insulating pha

214 he 6th month of follow up, the outer retinal hole persist in OCT in 80% of cases.

215 e used to access different parts of electron-hole phase diagram, including BEC-BCS crossover, enablin

216 pulses to non-resonantly excite an electron-hole plasma and show the formation of two-dimensional ex

217 The electron-hole plasma in charge-neutral graphene is predicted to r

218 , two-band Fermi surface, consisting of both hole pockets centred at (pai, 0) and electron pockets ce

219 tochastic fluctuations of the photogenerated hole population lead to spontaneous fluorescence switchi

220 racting with the supermassive Galactic black hole, possibly enhancing its accretion activity.

221 Relatively, holes predominantly bleach inter-chain interactions with

222 ize ratio between the smaller and the larger hole presented.

223 inherently fluorescent guest dye or a black-hole quencher from the receptor's cavity by means of com

224 efficiency of charge injection and electron-hole recombination.

225 these CFC banks could delay Antarctic ozone hole recovery by about six years and contribute 9 billio

226 New evidence shows that closure of NE holes relies on regulated de novo lipid synthesis, provi

227 Macular hole reopening occurred in 7 eyes (8.0%).

228 lecular basis of this strain-specific glycan hole response.

229 rane (ILM) flap for the treatment of macular hole retinal detachment (MHRD).

230 minimized nonradiative recombination at the hole-selective interface.

231 ethyl-substituted carbazole monolayer as the hole-selective layer in the perovskite cell.

232 Because the holes self-trap, the band-edge luminescence is weak; hen

233 he greatly accelerated photoinduced electron-hole separation and transfer, which benefited the photoc

234 lude that even for the immunodominant glycan hole shared between BG505 and B41, the prospect of desig

235 Thus, even for the immunodominant glycan hole shared between BG505 and B41, the prospect of desig

236 ons, excitons, phonons, polarons, electrons, holes, spins, ions and molecules, we illustrate the curr

237 Specifically, it is found that hot holes stabilized by surface adsorbed iodide enable the s

238 fs and 4.3 +/- 0.4 fs are obtained for core-hole states parallel to the bond and 6.5 +/- 0.6 fs and

239 , where the tidal interaction with the black hole stretches them along the orbit) and they show both

240 fusion protein fabricated a vertical through-hole structure with improved mechanical properties, and

241 excitons(16-18)-bound pairs of electrons and holes that reside either in a single layer (intralayer e

242 xcitation can generate charges (electron and holes) that can later recombine to form singlet excitons

243 mT (electron), B(hf2) = (0.24 +/- 0.01) mT (hole); the separation rates for singlet and triplet pola

244 of zebrafish for using the larger available hole to pass an obstacle.

245 Coulombic attraction can cause electrons and holes to encounter each other at interfaces close to whe

246 wave (SAW) and is transported to a region of holes to form an exciton.

247 er with the kinetics limited by diffusion of holes to the local trap clusters.

248 oduction and feeding of ER membranes into NE holes together with ESCRT-mediated remodeling is require

249 d of hurricane passage near Thatchpoint Blue Hole (TPBH) on Abaco Island, The Bahamas.

250 Hole transfer from nanocrystals to tetracene is energeti

251 e interfacial energetics on the electron and hole transfer rates separately.

252 cleation and growth, heterojunction electron-hole transfer, electronic structure, and luminescence wi

253 er electron-transfer coupling with near-zero hole-transfer coupling and thereby contributes to the lo

254 for stronger oxidants, leading to a smaller hole-transfer effective tunneling barrier height.

255 c acid (DTTDC), an electron-rich linker with hole transport ability.

256 sm is suggested to understand the particular hole transport behavior in p-DSCs, in which the hole tra

257 ectro-active units that serve as electron or hole transport channels for solar energy harvesting and

258 tion (with I(-)/I(3)(-) as redox couple) and hole transport in NiO-based p-DSCs.

259 egation occurs when holes are extracted by a hole transport layer (spiro-OMeTAD) deposited on the MHP

260 e effectively facilitates hole extraction to hole transport layer and expels electrons toward cathode

261 on transport layer/perovskite and perovskite/hole transport layer interfaces for high-efficiency and

262 he energy barrier between the perovskite and hole transport layer.

263 ar materials for application as electron and hole transport layers in perovskite solar cells with ide

264 tected near the interface of perovskites and hole transport layers, where a large density of nanocrys

265 re prepared and were found to operate in the hole transport regime with an average charge carrier mob

266 e transport behavior in p-DSCs, in which the hole transport time is independent of light intensity.

267 CQD solar cells, since these employ a p-type hole-transport layer (HTL) implemented using 1,2-ethaned

268 spite the use of undoped Spiro-OMeTAD as the hole-transport material (HTM).

269 Devices with SBA-based hole transporting layers (HTL) attain efficiencies on pa

270 t that the C(8) -BTBT-rich phase acts as the hole-transporting channel, while the quantum wells in (P

271 Herein, a unique strategy of "transparent hole-transporting frameworks" is proposed.

272 A hole-transporting large-bandgap polymer (poly[bis(4-phen

273 lls (PSCs) composed of organic polymer-based hole-transporting materials (HTMs) are considered to be

274 Three hole-transporting materials (HTMs) were prepared followi

275 Four spirobisacridine (SBA) hole-transporting materials were synthesized and employe

276 ayer only in the visible region, keeping the hole-transporting pathways as well as the optimized film

277 s, which likely contributes to the excellent hole-transporting properties.

278 (photo) conductivity and finally limits the hole-transporting property of the rear subcell.

279 a high yield of photoluminescence-quenching hole trapping on the EDL.

280 carrier trapping process(10,11), we reveal a hole-trapping character with the kinetics limited by dif

281 policymakers to plug the holes in the ozone hole treaty.

282 s to analyze the dynamics of an axisymmetric hole undergoing capillary collapse in a fluid sheet of s

283 e, which permits separation of electrons and holes upon defect formation, and only allows carriers to

284 es for electrons and more disperse bands for holes upon optical or thermal excitation.

285 ke a contribution to in the top of the heavy hole valence band and raise its energy.

286 states and decrease the energy of the light hole valence band.

287 prevalence of visual impairment based on pin-hole value was 1.7 +/- 0.3% using World Health Organizat

288 luence of 4 intraoperative findings [visible hole (VH), diffuse fibrinopurulent exudate (DFE) extendi

289 ies of [Formula: see text] eV to create O 2s holes via matter-antimatter annihilation.

290 ng, a 2 L bottle cap with a 1.25 cm diameter hole was used for filtering.

291 ons showing sheet-like transient electron or hole wave functions in LHPs.

292 If a neovascularization or macular hole were present, bilateral occurrence was frequent (33

293 and 13.8% of perfluorodecalin eyes; retinal holes were found in 14.6% of PFO eyes and in none of the

294 It includes a maximal density of holes, which increases throughput in automated cryo-EM w

295 e host-guest-induced release of an "electron hole" will translate to various forms of non-encapsulate

296 adical anion upon reaction of photogenerated holes with an electron donor, which plays a key role in

297 ssays, we demonstrate that TMD2 forms stable holes with an estimated diameter of 2 nm, as long as the

298 n generation and separation of electrons and holes with high charge transfer kinetics.

299 ontributing factors to RDs included atrophic holes within peripheral avascular retina, visible vitreo

300 Herein, we discover that those hot holes work with surface adsorbates collectively to contr