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1 (n)I(3n+1) (n = 2-4, BA= butylammonium, MA = methylammonium).
2  magnitude greater than that of MAPbI3 (MA = methylammonium).
3 onium uptake but reduced capacity to take up methylammonium.
4 alyzed had defects in accumulation of [(14)C]methylammonium.
5 s, the mutants were unable to transport [14C]methylammonium.
6 lica substrate and predict the adsorption of methylammonium.
7 vity to ammonium and to the transport analog methylammonium.
8 d accumulation of the ammonium analog [(14)C]methylammonium, a weak base, led to the proposal that me
9 lts are in accord with the view that Amt and methylammonium/ammonium permease proteins increase the r
10 lammonium transport B (AmtB) protein [called methylammonium/ammonium permeases (MEP)] that was observ
11 f enteric bacteria and their homologues, the methylammonium/ammonium permeases of Saccharomyces cerev
12 istant to oxidative stress relative to their methylammonium analogs.
13 cumulates much larger amounts of both [(14)C]methylammonium and [(14)C]methylglutamine in a washed ce
14                                              Methylammonium and ammonium (MEP) permeases of Saccharom
15   Large inward NH(4)(+) currents and sizable methylammonium and dimethylammonium currents were observ
16  cells so far have been obtained mainly with methylammonium and formamidinium mixed cations.
17        We find that hydrogen bonding between methylammonium and I(2) promotes triiodide formation, wh
18 ormance solar cells based on mixtures of Cs, methylammonium, and formamidinium.
19 nfer resistance to the toxic ammonium analog methylammonium are in AMT4 and a high proportion of spon
20 of formula MAPb(Br(x)I(1-x))(3), where MA is methylammonium, are of great interest for optoelectronic
21 ns (Cs (cesium), FA (formamidinium), and MA (methylammonium)) at room temperature.
22 c properties including better stability than methylammonium-based counterparts.
23                    Our approach reveals that methylammonium-based perovskites form densely packed, an
24 o strategies to boost stability of sensitive methylammonium-based Sn-Pb perovskite films and devices
25 n 0D metal-organic hybrid materials based on methylammonium bismuth halide (CH3NH3)3Bi2I9.
26 t time aryl-acetylene-based (4-ethynylphenyl)methylammonium (BMAA) and buta-1,3-diyne-1,4-diylbis(4,1
27 xciton quenching through a small increase in methylammonium bromide (MABr) molar proportion, and we s
28                                     A simple methylammonium bromide (MABr) treatment via spin-coating
29 ence band maximum (VBM)) of device-relevant, methylammonium bromide (MABr)-doped, formamidinium lead
30 uires spraying the material of interest with methylammonium bromide and observing whether photolumine
31                Poly(N-(3-dimethyl(ferrocenyl)methylammonium bromide)propyl acrylamide) (pFcAc) was gr
32 I(10) (x = 0-1, BA is n-butylammonium, MA is methylammonium) by the incorporation of a large EA catio
33 Sn(0.5)Pb(0.5)I(3) (FA = formamidinium, MA = methylammonium), can exhibit ideal band gaps of 1.27-1.3
34        We propose to replace the widely used methylammonium cation (CH3NH3(+)) by alternative molecul
35  electrogenic and transport the ammonium and methylammonium cation with high specificity.
36                               The absence of methylammonium cations in single layer perovskite accoun
37  alternating ordering of the guanidinium and methylammonium cations in the interlayer space (ACI).
38                           The application of methylammonium cations makes flexible perovskite solar m
39 ing the MOCP precursor solutions with excess methylammonium cations, the MOCPs form via a dynamic com
40 ra resulting from the rotation of aspherical methylammonium cations.
41 ctivity of (3'-trifluoromethoxybiphenyl-4-yl)methylammonium chloride (8) exceeded that of phenobarbit
42 ray structure of the receptor complexed with methylammonium chloride illuminates the basis of the mol
43 e that the readily accessible (biphenyl-4-yl)methylammonium chlorides (compound class B) exhibited a
44  present findings suggest that replacing the methylammonium component in CH3 NH3 PbI3 to a species wi
45  of gap states is either suppressed when the methylammonium concentration in mixed cation films is re
46                We close by demonstrating the methylammonium-containing perovskite solar cells showing
47 m)ethyl] methane-thiosulfonate (MTSET), both methylammonium-containing thiol-modifying reagents with
48       We confirmed that accumulation of [14C]methylammonium depends on its conversion to gamma-N-meth
49 ral phases and dipolar dynamics in the mixed methylammonium/dimethylammonium MA(1-x)DMA(x)PbBr(3) hyb
50 esulting from an interaction of charges with methylammonium dipoles.
51 nd 3D MA(0.5)FA(0.5)Pb(0.5)Sn(0.5)I(3) (MA = methylammonium, FA = formamidinium) perovskite composite
52 .7x)(X)(3-0.4x) (A = MA, FA; X = Br, I; MA = methylammonium, FA = formamidinium, en = ethylenediammon
53 Pb(Br(0.4) I(0.6) )(3) perovskite films (MA: methylammonium, FA: formamidinium) are studied under sol
54 (3), FAPbBr(3), CsPbI(3), and CsPbBr(3) (MA, methylammonium; FA(+), formamidinium), are used to synth
55  systematically tuning the cesium ratio of a methylammonium-free 1.8-electron volt mixed-halide perov
56 e p-i-n structure perovskite modules made of methylammonium-free formamidinium cesium lead iodide (FA
57                                              Methylammonium-free PSCs also benefit from a PNR interla
58                                          The methylammonium group is caged by three aromatic side cha
59 g, particularly through employing additional methylammonium halide over the stoichiometric ratio for
60 leaching for the selective release of excess methylammonium halides, we achieved full and even covera
61 airs of the amino acid analogues acetate and methylammonium in aqueous NaCl solutions of concentratio
62 uired for transport of the ammonium analogue methylammonium in washed cells, only in Saccharomyces ce
63 ed by increased ammonium-induced and reduced methylammonium-induced currents.
64  its volume expansion and fast reaction with methylammonium iodide (MAI)/formamidinium iodide (FAI) (
65                                              Methylammonium iodide is introduced in the fullerene lay
66  respect to decomposition to lead iodide and methylammonium iodide, even in the absence of ambient ai
67  and is ineffective when replacing MABr with methylammonium iodide.
68 polybases to induce the deprotonation of its methylammonium ions (MA(+)).
69 ture of the tetragonal structure is that the methylammonium ions do not sit centrally in the A-site c
70                       We have confirmed that methylammonium is not metabolized in the yeast S. cerevi
71 electric field applied to single crystals of methylammonium lead bromide (CH3 NH3 PbBr3 ) is varied,
72       Here, we synthesize single crystals of methylammonium lead bromide (CH3NH3PbBr3), characterise
73 ere, perovskite single-crystal FETs based on methylammonium lead bromide are studied and device insta
74 e of nanocrystal pinning, highly luminescent methylammonium lead bromide films are used to produce st
75 strate spin-polarized carrier injection into methylammonium lead bromide films from metallic ferromag
76 ing a small amount of neutral benzylamine to methylammonium lead bromide, which induces a proton tran
77 an der Waals (vdW) solids are realized using methylammonium lead halide (CH3 NH3 PbI3 ) as the organi
78  deposition of thick and continuous films of methylammonium lead halide (MAPbX(3); X = Br, I) from di
79 resence of a density of states in the gap of methylammonium lead halide films processed from DMSO-con
80 b-10 fs resolution pump-probe experiments on methylammonium lead halide perovskite films are describe
81                                              Methylammonium lead halide perovskite solar cells contin
82                                              Methylammonium lead halide perovskite-based solar cells
83 ystal nanowires, nanorods, and nanoplates of methylammonium lead halide perovskites (CH3NH3PbI3 and C
84                                              Methylammonium lead halide perovskites are attracting in
85        The discussion focuses principally on methylammonium lead iodide (CH(3)NH(3)PbI(3) or MAPbI(3)
86 Organic-inorganic hybrid perovskites such as methylammonium lead iodide (CH(3)NH(3)PbI(3)) are game-c
87 rst time on a hole conductor-free mesoscopic methylammonium lead iodide (CH(3)NH(3)PbI(3)) perovskite
88                                Thin films of methylammonium lead iodide (CH(3)NH(3)PbI(3), MAPI) are
89 e activation energies for ionic migration in methylammonium lead iodide (CH3NH3PbI3) are derived from
90             Metal halide perovskites such as methylammonium lead iodide (CH3NH3PbI3) are generating g
91 ention is given to the prototypical compound methylammonium lead iodide (CH3NH3PbI3) due to the prepo
92            Hybrid halide perovskites such as methylammonium lead iodide (CH3NH3PbI3) exhibit unusuall
93 ct visualization of hot-carrier migration in methylammonium lead iodide (CH3NH3PbI3) thin films by ul
94                                       Cesium methylammonium lead iodide (Cs(x) MA(1-x) PbI(3) ) nanoc
95 n the absorption properties of formamidinium/methylammonium lead iodide (FA(x)MA(1-x)PbI(3), x = 0 to
96 roelectric (PFE) polymers are doped into the methylammonium lead iodide (MAPbI(3) ) layer and/or inse
97 skite thin films coated by QA, PSCs based on methylammonium lead iodide (MAPbI(3) ) showed significan
98 ide salts, apply them as capping layers onto methylammonium lead iodide (MAPbI(3)) films, age them un
99  engineering of low-temperature blade-coated methylammonium lead iodide (MAPbI(3)) perovskite films.
100 hancing hole extraction from polycrystalline methylammonium lead iodide (MAPbI(3)) perovskite to the
101 ully demonstrate the potential of the hybrid Methylammonium lead iodide (MAPbI(3)) perovskite-based s
102 rformance perovskite photovoltaic absorbers, methylammonium lead iodide (MAPbI3) and formamidinium le
103 Here we show that intrinsic doping surges in methylammonium lead iodide (MAPbI3) crystals as a respon
104 area, orientationally pure crystalline (OPC) methylammonium lead iodide (MAPbI3) hybrid perovskite fi
105            The PSCs fabricated with LBSO and methylammonium lead iodide (MAPbI3) show a steady-state
106               Hybrid perovskites, especially methylammonium lead iodide (MAPbI3), exhibit excellent s
107                                              Methylammonium lead iodide (MAPI) cells of the design FT
108 e when compared to the typical 3D perovskite methylammonium lead iodide (MAPI); direct evidence for t
109 uddlesden-Popper perovskite, n-butylammonium methylammonium lead iodide (nBA-MAPI), compared to that
110 trochemical (PEC) solar cell based on p-type methylammonium lead iodide (p-MeNH3PbI3) perovskite with
111 during the two-step sequential deposition of methylammonium lead iodide and formamidinium lead iodide
112                                        Using methylammonium lead iodide and formamidinium lead iodide
113 e structures and report polymorphs found for methylammonium lead iodide and formamidinium lead iodide
114           Three-dimensional perovskites like methylammonium lead iodide are determined to be ferroela
115         Here we show that iodide ions in the methylammonium lead iodide migrate via interstitial site
116                                              Methylammonium lead iodide perovskite (MAPbI3 ), a proto
117 s exhibit a higher PLQY than the standard 3D methylammonium lead iodide perovskite although this is a
118                                              Methylammonium lead iodide perovskite can make high-effi
119                                              Methylammonium lead iodide perovskite has attracted cons
120 ) as an interfacial layer between TiO(2) and methylammonium lead iodide perovskite is probed to reduc
121 een a range of different polymer films and a methylammonium lead iodide perovskite layer was used as
122  figure of merit of radiative efficiency for Methylammonium Lead Iodide perovskite solar cells and, t
123              Here we turn to polycrystalline methylammonium lead iodide perovskite, which has emerged
124 t carrier scattering with optical phonons in methylammonium lead iodide perovskite.
125  comparable to those of the state-of-the-art methylammonium lead iodide perovskites, favorable effect
126 n the thickness direction (for example, from methylammonium lead iodide, MAPbI(3), to MAPb(0.5)Sn(0.5
127    Here, we demonstrate that by assembling a methylammonium lead tri-bromide perovskite single crysta
128 , that is, greater than 20%, normally employ methylammonium lead tri-iodide with a sub-optimal bandga
129 -the-art narrowband photodetectors made from methylammonium lead trihalide perovskite single crystals
130 he morphology and luminescence properties of methylammonium lead trihalide perovskite thin films.
131                           Single crystals of methylammonium lead trihalide perovskites (MAPbX3; MA =
132 o characterize the ionic defect landscape in methylammonium lead triiodide (MAPbI(3)) perovskites in
133  cells made with HaPs, especially tetragonal methylammonium lead triiodide (MAPbI3).
134                 The spectral response of the methylammonium lead triiodide single crystal solar cells
135                                         Thin methylammonium lead triiodide single crystals with tuned
136 e nanoscale photoconductivity imaging on two methylammonium lead triiodide thin films with different
137 /- 0.1 meV are identified in polycrystalline methylammonium lead triiodide, which mainly stay at grai
138 anging the surface chemistry and suppressing methylammonium loss.
139 , 2D perovskites contain a monocation [e.g., methylammonium (MA(+) ) or formamidinium (FA(+) )].
140 BX(3), where A is a monovalent cation (e.g., methylammonium (MA(+)), Cs(+)), B is the divalent metal
141                 Specifically, we investigate methylammonium (MA(+)), formamidinium (FA(+)), and guani
142 and 4-(aminomethyl)piperidinium) (4AMP); A = methylammonium (MA) and formamidinium (FA)).
143 vealed that the local environment around the methylammonium (MA) cation in MAPbBr3 hybrid perovskite
144 acancies (H(v)) at both N and C atoms of the methylammonium (MA) cation in MAPbI(3) efficiently passi
145 lations to study the dynamics of the organic methylammonium (MA) cation orientation in a range of pur
146  phases by empirically alloying with cesium, methylammonium (MA) cations, or both.
147 rough the effect of isotopic labeling of the methylammonium (MA) component on the dielectric permitti
148  is used as an additive, and eliminated when methylammonium (MA) is replaced with cesium or formamidi
149 cs in hybrid mixed-cation formamidinium (FA)/methylammonium (MA) lead halide perovskites.
150 , demonstrated on the formamidinium (FA) and methylammonium (MA) mixed-cation perovskite system FA(1-
151 o PbBr(6) octahedra, butylammonium (BA), and methylammonium (MA) molecule tilting motion that leads t
152 kites (2FBZ)(2)(A)(n-1)Pb(n)I(3n+1) with A = methylammonium (MA) or formamidinium (FA) and n = 2, 3.
153  prepared suspensions of APbBr(3) (A = Cs or methylammonium (MA)) type perovskite colloids (ca. 2-100
154 obutylammonium (c-C4A), combining these with methylammonium (MA), and found that the middle cation, c
155 e-cation solid alloys of formamidinium (FA), methylammonium (MA), cesium, and rubidium lead halides w
156 A)Pb(2)I(7) where BA = butylammonium and A = methylammonium (MA), formamidinium (FA), dimethylammoniu
157 (A' = 4-(aminomethyl)pyridinium (4AMPY), A = methylammonium (MA), n = 1-4).
158 rochemical impedance spectroscopy (EIS) with methylammonium (MA)-, formamidinium (FA)-, and MA(x)FA(1
159  and grain anchoring to successfully prepare methylammonium (MA)-free and phase-pure stable a-FAPbI(3
160 ciency (PCE) of triple-A cation (cesium (Cs)/methylammonium (MA)/formaminidium (FA)) perovskite solar
161 xation dynamics in LHP NCs with cesium (Cs), methylammonium (MA, CH(3)NH(3)(+)), and formamidinium (F
162 A(3) Ru(2) X(9) (X=Br) based upon the use of methylammonium (MA=CH(3) NH(3) (+) ) on the perovskite A
163 ts, with the general formula AM(II)I(3) (A = methylammonium, MA; M(II) = Sr, Sm, Eu, and A = formamid
164                                              Methylammonium-mediated phase-evolution behavior of FA1-
165 he reaction of superoxide (O2 (-) ) with the methylammonium moiety of the perovskite absorber.
166 )MA(n-1)Sn(n)I(3n+1) (BA, butylammonium; MA, methylammonium; n = 1, 3, 5) superlattice by chemical ep
167 PEA: R/S-beta-methylphenylethylammonium; MA: methylammonium; n = 1-3).
168                              Accumulation of methylammonium occurs within seconds and appears to refl
169                                       Excess methylammonium oleate from the reaction mixture in the M
170 ng in isolated ASn(x)Pb(1-x)I(3) (where A is methylammonium or a mixture of formamidinium and cesium)
171 emperatures, increasing organic cation (e.g. methylammonium) or decreasing inorganic cation (e.g. ces
172               The ammonium transporter (AMT)/methylammonium permease (MEP)/Rhesus glycoprotein (Rh) f
173 iated by the ubiquitous ammonium transporter/methylammonium permease/rhesus protein (Amt/Mep/Rh) fami
174                           Two genes encoding methylammonium permeases (MEPs) were identified from eac
175 thylammonium transport proteins (also called methylammonium permeases), are gas channels for NH(3), w
176  the four commonly studied formamidinium and methylammonium perovskites, HC(NH2)2PbI3, HC(NH2)2PbBr3,
177 , subsequent energy-dependent utilization of methylammonium precludes its use in assessing active tra
178 oup both hydrogen bonds and ion pairs to the methylammonium proton.
179                                              Methylammonium recognition involves two aromatic residue
180  AMT4 gene, and the insert cosegregated with methylammonium resistance in genetic crosses.
181                           All 16 spontaneous methylammonium-resistant mutants that we analyzed had de
182 tions with the organic part of the material (methylammonium), resulting in the MAPbI3 decomposition a
183                     The binding of charged N-methylammonium species to the functionalized SWCNTs was
184                   Further browning in AS and methylammonium sulfate seeds was triggered by cloud even
185 amine, tetraethylammonium (TEA), tri-n-butyl-methylammonium (TBuMA), and N'-methylnicotinamide (NMN).
186 ixed-organic-cation perovskite formamidinium methylammonium tin iodide ( FAMASnI3 ) as an absorber la
187 ng so-called "hollow" ethylenediammonium and methylammonium tin iodide ({en}MASnI3) perovskite as abs
188 sed on alloyed perovskite solid solutions of methylammonium tin iodide and its lead analogue (CH3NH3S
189 ects on the crystallization of the lead-free methylammonium tin triiodide (CH3NH3SnI3) perovskite fil
190 romide, which induces a proton transfer from methylammonium to benzylamine and enables crystallizatio
191 cteria, however, ATP-dependent conversion of methylammonium to gamma-N-methylglutamine by glutamine s
192 ma-1 mutant of N. crassa largely metabolized methylammonium to methylglutamine.
193 ranscribed and Chlamydomonas is sensitive to methylammonium toxicity.
194                                 The ammonium/methylammonium transport (Amt) proteins of enteric bacte
195 function of three homologues of the ammonium/methylammonium transport B (AmtB) protein [called methyl
196 heir only known paralogues, the ammonium and methylammonium transport proteins (also called methylamm
197  members of the Rh superfamily, the ammonium/methylammonium transport proteins, are bidirectional cha
198 lock for alpha7 nAChRs, i.e., 3alpha-azido-N-methylammonium tropane, was used for additional in situ
199 d with different degrees of defect in [(14)C]methylammonium uptake.
200 activity, as judged by measurements of [14C]-methylammonium uptake.
201 ansitions and optical behavior of MAPbI3 (MA=methylammonium) using in situ synchrotron X-ray diffract
202  employing an infrared pump pulse tuned to a methylammonium vibration, we observe slow, nanosecond-lo
203                             Concentration of methylammonium was most easily studied in strains that l
204 xchange experiments on MA(2)CrCl(4) (MA(+) = methylammonium), which instead show 3D exchange.
205 =2), AMP = 4-(aminomethyl)piperidinium; MA = methylammonium), which shows an out-of-plane polarizatio
206         Notably, mixed-cation (formamidinium-methylammonium) wide-bandgap perovskite films are prone
207 d or greater) defects in the accumulation of methylammonium, with little accompanying defect in the i

 
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