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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
13 cumulates much larger amounts of both [(14)C]methylammonium and [(14)C]methylglutamine in a washed ce
15 Large inward NH(4)(+) currents and sizable methylammonium and dimethylammonium currents were observ
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
24 o strategies to boost stability of sensitive methylammonium-based Sn-Pb perovskite films and devices
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
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
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
37 alternating ordering of the guanidinium and methylammonium cations in the interlayer space (ACI).
39 ing the MOCP precursor solutions with excess methylammonium cations, the MOCPs form via a dynamic com
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
47 m)ethyl] methane-thiosulfonate (MTSET), both methylammonium-containing thiol-modifying reagents with
49 ral phases and dipolar dynamics in the mixed methylammonium/dimethylammonium MA(1-x)DMA(x)PbBr(3) hyb
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
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
64 its volume expansion and fast reaction with methylammonium iodide (MAI)/formamidinium iodide (FAI) (
66 respect to decomposition to lead iodide and methylammonium iodide, even in the absence of ambient ai
69 ture of the tetragonal structure is that the methylammonium ions do not sit centrally in the A-site c
71 electric field applied to single crystals of methylammonium lead bromide (CH3 NH3 PbBr3 ) is varied,
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
83 ystal nanowires, nanorods, and nanoplates of methylammonium lead halide perovskites (CH3NH3PbI3 and C
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
89 e activation energies for ionic migration in methylammonium lead iodide (CH3NH3PbI3) are derived from
91 ention is given to the prototypical compound methylammonium lead iodide (CH3NH3PbI3) due to the prepo
93 ct visualization of hot-carrier migration in methylammonium lead iodide (CH3NH3PbI3) thin films by ul
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
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
113 e structures and report polymorphs found for methylammonium lead iodide and formamidinium lead iodide
117 s exhibit a higher PLQY than the standard 3D methylammonium lead iodide perovskite although this is a
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
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.
132 o characterize the ionic defect landscape in methylammonium lead triiodide (MAPbI(3)) perovskites in
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
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
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
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
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
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
166 )MA(n-1)Sn(n)I(3n+1) (BA, butylammonium; MA, methylammonium; n = 1, 3, 5) superlattice by chemical ep
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
173 iated by the ubiquitous ammonium transporter/methylammonium permease/rhesus protein (Amt/Mep/Rh) fami
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
182 tions with the organic part of the material (methylammonium), resulting in the MAPbI3 decomposition a
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
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
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
205 =2), AMP = 4-(aminomethyl)piperidinium; MA = methylammonium), which shows an out-of-plane polarizatio
207 d or greater) defects in the accumulation of methylammonium, with little accompanying defect in the i