Hyo Jae Yoon

Allosteric supramolecular triple-layer catalysts

Chloride Control of a Catalyst Allosteric regulation of proteins and enzymes allows their conformation to be controlled by changes in the concentration of effector-binding molecules; reactivity can be controlled by changing access to the active catalytic site. The supramolecular control of conformation through multiple weaker interactions has been exploited in organometallic catalysts that can open or close access to reactive sites around a metal center. Yoon et al. (p. 66) now show how chloride ions can be used to control a rhodium polymerization catalyst in which two metal centers are bridged by a linker bearing aromatic groups. When Cl− is present, reactive sites remain available on the metal centers. When Cl− is removed by abstracting agents, aromatic groups on one of the other ligands on the Rh centers can bind to the linker to form a triple-layer sandwich structure. Formation of this supramolecular structure blocks access of reactants to the metal centers. A chloride ligand is used to control the access of reactants to a rhodium polymerization catalyst. Allosteric regulation of organometallic catalysts could allow for greater control over reactions. We report an allosteric supramolecular structure in which a monometallic catalytic site has been buried in the middle layer of a triple-layer complex. Small molecules and elemental anions can open and close this complex and reversibly expose and conceal the catalytic center. The ring-opening polymerization of ε-caprolactone can be turned on by the in situ opening of the triple-layer complex and then completely turned off by reforming it through the abstraction of Cl–, the allosteric effector agent, without appreciable loss of catalytic activity. This process can regulate the molecular weights of the resulting polymers.

Defining the Value of Injection Current and Effective Electrical Contact Area for EGaIn-Based Molecular Tunneling Junctions

Analysis of rates of tunneling across self-assembled monolayers (SAMs) of n-alkanethiolates SCn (with n = number of carbon atoms) incorporated in junctions having structure Ag(TS)-SAM//Ga2O3/EGaIn leads to a value for the injection tunnel current density J0 (i.e., the current flowing through an ideal junction with n = 0) of 10(3.6±0.3) A·cm(-2) (V = +0.5 V). This estimation of J0 does not involve an extrapolation in length, because it was possible to measure current densities across SAMs over the range of lengths n = 1-18. This value of J0 is estimated under the assumption that values of the geometrical contact area equal the values of the effective electrical contact area. Detailed experimental analysis, however, indicates that the roughness of the Ga2O3 layer, and that of the Ag(TS)-SAM, determine values of the effective electrical contact area that are ~10(-4) the corresponding values of the geometrical contact area. Conversion of the values of geometrical contact area into the corresponding values of effective electrical contact area results in J0(+0.5 V) = 10(7.6±0.8) A·cm(-2), which is compatible with values reported for junctions using top-electrodes of evaporated Au, and graphene, and also comparable with values of J0 estimated from tunneling through single molecules. For these EGaIn-based junctions, the value of the tunneling decay factor β (β = 0.75 ± 0.02 Å(-1); β = 0.92 ± 0.02 nC(-1)) falls within the consensus range across different types of junctions (β = 0.73-0.89 Å(-1); β = 0.9-1.1 nC(-1)). A comparison of the characteristics of conical Ga2O3/EGaIn tips with the characteristics of other top-electrodes suggests that the EGaIn-based electrodes provide a particularly attractive technology for physical-organic studies of charge transport across SAMs.

PCR-like Cascade Reactions in the Context of an Allosteric Enzyme Mimic

A supramolecular allosteric catalyst that exhibits a PCR-like cascade reaction is reported. The complex is triggered by a reaction with an acetate ion, which turns on a catalytic cascade that exponentially increases acetate ion concentration through an acyl transfer reaction.

The rate of charge tunneling through self-assembled monolayers is insensitive to many functional group substitutions.

At its conception, the field of molecular electronics promised to provide the ability to engineer the rate of charge transport, by design of the molecular structure of electronic junctions.[1] The hypothesis was that the electronic and geometrical structure of molecules in a junction would have a significant and predictable effect on the rate and mechanism of charge transport through their influence on the energetic topography of the tunneling barrier. Here we show the preparation and electrical characterization of junctions (Figure 1) of the structure AgTS/S(CH2)4CONH(CH2)2R//Ga2O3/EGaIn (AgTS = template-stripped silver surface[2]; R = tail group; EGaIn = eutectic gallium and indium alloy; Ga2O3 = a passivating metal oxide film on the surface of the EGaIn[3–5]) including a range of common aliphatic, aromatic, and heteroaromatic organic tail groups. We demonstrate that the rate of charge transport across these self-assembled monolayers (SAMs) is surprisingly insensitive to changes in the structure of the organic molecules of which they are composed. This study is based on a physical-organic design: that is, the information it provides comes from comparisons of rates of tunneling across related structures, rather than from the interpretation of the absolute values of single measurements. Figure 1 A) Schematic description of tunneling junction consisting of a template-stripped Ag bottom-electrode supporting a SAM, and contacted by a Ga2O3/EGaIn top-electrode. B) A schematic of one junction. C) The numbering system based on non-hydrogen atoms in ... Targets for shaping the tunneling barriers of molecular junctions have included electron–donor–bridge–acceptor molecules,[1a,6] molecular quantum dot systems,[7] aromatic molecules,[8] and complex organic molecules with multiple functional groups.[9] Many of these studies ostensibly shaping the tunneling barriers of molecular junctions have, however, been difficult to interpret because, when they were carried out, there were no experimental systems that generated well-characterized, statistically validated data. This paper characterizes the rates of charge transport by tunneling across a series of molecules—arrayed in SAMs—containing a common head group and body (HS(CH2)4CONH(CH2)2-) and structurally varied tail groups (-R); these molecules are assembled in junctions of the structure AgTS/SAM//Ga2O3/EGaIn. Over a range of common aliphatic, aromatic, and heteroaromatic organic tail groups, changing the structure of R does not significantly influence the rate of tunneling. In making these measurements, we utilize C12 and C18 alkanethiols as calibration standards to allow comparison with results from other types of junctions. Limited studies[4,5,10–15] of charge transport using a range of junctions have described the relation between molecular structure and the rate of tunneling. For example, Venkataraman et al.[14] reported that the rate of charge transport through a series of diaminobenzenes depends on the alignment of the metal Fermi level to the closest molecular orbital. Chiechi and Solomon et al.[15] compared the rate of charge transport through three different anthracene derivatives of approximately the same thickness, and concluded that conjugation influences the rate of charge transport. Studies exploring the correlation between molecular structure and charge transport based on systematic physical–organic measurements of the rate of charge transport over a wide range of structures are sparse. This paper describes tunneling rates through SAMs of molecules with a variety of molecular structures including aromatic, heterocyclic, and aliphatic moieties. We have previously examined ferrocene-terminated SAMs[4] and SAMs comprising odd-and even-numbered n-alkanethiolates.[5]

Replacing –CH2CH2- with -CONH- Does Not Significantly Change Rates of Charge Transport Through AgTS-SAM//Ga2O3/EGaIn Junctions

This paper describes physical-organic studies of charge transport by tunneling through self-assembled monolayers (SAMs), based on systematic variations of the structure of the molecules constituting the SAM. Replacing a -CH(2)CH(2)- group with a -CONH- group changes the dipole moment and polarizability of a portion of the molecule and has, in principle, the potential to change the rate of charge transport through the SAM. In practice, this substitution produces no significant change in the rate of charge transport across junctions of the structure Ag(TS)-S(CH(2))(m)X(CH(2))(n)H//Ga(2)O(3)/EGaIn (TS = template stripped, X = -CH(2)CH(2)- or -CONH-, and EGaIn = eutectic alloy of gallium and indium). Incorporation of the amide group does, however, increase the yields of working (non-shorting) junctions (when compared to n-alkanethiolates of the same length). These results suggest that synthetic schemes that combine a thiol group on one end of a molecule with a group, R, to be tested, on the other (e.g., HS~CONH~R) using an amide-based coupling provide practical routes to molecules useful in studies of molecular electronics.

Replacing Ag(TS)SCH(2)-R with Ag(TS)O(2)C-R in EGaIn-based tunneling junctions does not significantly change rates of charge transport.

This paper compares rates of charge transport by tunneling across junctions with the structures Ag(TS) X(CH2 )2n CH3  //Ga2 O3  /EGaIn (n=1-8 and X= SCH2  and O2 C); here Ag(TS) is template-stripped silver, and EGaIn is the eutectic alloy of gallium and indium. Its objective was to compare the tunneling decay coefficient (β, Å(-1) ) and the injection current (J0 , A cm(-2) ) of the junctions comprising SAMs of n-alkanethiolates and n-alkanoates. Replacing Ag(TS) SCH2 -R with Ag(TS) O2 C-R (R=alkyl chains) had no significant influence on J0 (ca. 3×10(3)  A cm(-2) ) or β (0.75-0.79 Å(-1) )-an indication that such changes (both structural and electronic) in the Ag(TS) XR interface do not influence the rate of charge transport. A comparison of junctions comprising oligo(phenylene)carboxylates and n-alkanoates showed, as expected, that β for aliphatic (0.79 Å(-1) ) and aromatic (0.60 Å(-1) ) SAMs differed significantly.

Fluorination, and Tunneling across Molecular Junctions

This paper describes the influence of the substitution of fluorine for hydrogen on the rate of charge transport by hole tunneling through junctions of the form Ag(TS)O2C(CH2)n(CF2)(m)T//Ga2O3/EGaIn, where T is methyl (CH3) or trifluoromethyl (CF3). Alkanoate-based self-assembled monolayers (SAMs) having perfluorinated groups (R(F)) show current densities that are lower (by factors of 20-30) than those of the homologous hydrocarbons (R(H)), while the attenuation factors of the simplified Simmons equation for methylene (β = (1.05 ± 0.02)n(CH2)(-1)) and difluoromethylene (β = (1.15 ± 0.02)n(CF2)(-1)) are similar (although the value for (CF2)n is statistically significantly larger). A comparative study focusing on the terminal fluorine substituents in SAMs of ω-tolyl- and -phenyl-alkanoates suggests that the C-F//Ga2O3 interface is responsible for the lower tunneling currents for CF3. The decrease in the rate of charge transport in SAMs with R(F) groups (relative to homologous R(H) groups) is plausibly due to an increase in the height of the tunneling barrier at the T//Ga2O3 interface, and/or to weak van der Waals interactions at that interface.

Introducing Ionic and/or Hydrogen Bonds into the SAM//Ga 2 O 3 Top- Interface of Ag TS /S(CH 2 ) n T//Ga 2 O 3 /EGaIn Junctions

Junctions with the structure Ag(TS)/S(CH2)nT//Ga2O3/EGaIn (where S(CH2)nT is a self-assembled monolayer, SAM, of n-alkanethiolate bearing a terminal functional group T) make it possible to examine the response of rates of charge transport by tunneling to changes in the strength of the interaction between T and Ga2O3. Introducing a series of Lewis acidic/basic functional groups (T = -OH, -SH, -CO2H, -CONH2, and -PO3H) at the terminus of the SAM gave values for the tunneling current density, J(V) in A/cm(2), that were indistinguishable (i.e., differed by less than a factor of 3) from the values observed with n-alkanethiolates of equivalent length. The insensitivity of the rate of tunneling to changes in the terminal functional group implies that replacing weak van der Waals contact interactions with stronger hydrogen- or ionic bonds at the T//Ga2O3 interface does not change the shape (i.e., the height or width) of the tunneling barrier enough to affect rates of charge transport. A comparison of the injection current, J0, for T = -CO2H, and T = -CH2CH3--two groups having similar extended lengths (in Å, or in numbers of non-hydrogen atoms)--suggests that both groups make indistinguishable contributions to the height of the tunneling barrier.

Aziridine in polymers: a strategy to functionalize polymers by ring-opening reaction of aziridine

A novel method for the post-modification of polymers was demonstrated using an aziridine-incorporated copolymer. The side-chain length of the copolymer was extended via the Lewis acid-assisted ring-opening of the aziridine moieties in the copolymer.

Formation of Triboelectric Series via Atomic-Level Surface Functionalization for Triboelectric Energy Harvesting

Triboelectric charging involves frictional contact of two different materials, and their contact electrification usually relies on polarity difference in the triboelectric series. This limits the choices of materials for triboelectric contact pairs, hindering research and development of energy harvest devices utilizing triboelectric effect. A progressive approach to resolve this issue involves modification of chemical structures of materials for effectively engineering their triboelectric properties. Here, we describe a facile method to change triboelectric property of a polymeric surface via atomic-level chemical functionalizations using a series of halogens and amines, which allows a wide spectrum of triboelectric series over single material. Using this method, tunable triboelectric output power density is demonstrated in triboelectric generators. Furthermore, molecular-scale calculation using density functional theory unveils that electrons transferred through electrification are occupying the PET group rather than the surface functional group. The work introduced here would open the ability to tune triboelectric property of materials by chemical modification of surface and facilitate the development of energy harvesting devices and sensors exploiting triboelectric effect.