Matthew C. Crowe

Mass Spectrometry of Small Bimetal Monolayer-Protected Clusters

Monolayer-protected clusters were prepared by procedures like those yielding Au25L18 (where L=-SCH2CH2Ph=-SC2Ph) but using, instead, mixtures of Au and Pd salts, as starting materials, with the intent of creating and characterizing Au25-xMxL18 clusters. Isolation of small nanoparticle product followed by partial ligand exchange to introduce thiolated poly(ethylene glycol) (SPEG=-S(CH2CH2O)5CH3) into the nanoparticle ligand shell enabled characterization of the Au25-xMxL18 content by positive mode electrospray ionization mass spectrometry (ESI-MS). For synthetic feed mole ratios of Au:Pd of 9:1 and 13:12, electrospray spectra of the PEGylated MPCs showed that the reaction and isolation produce a mixture of Au25(SC2Ph)18 and a mono-Pd nanoparticle Au24Pd(SC2Ph)18. A higher proportion of the mono-Pd nanoparticle is produced by the 13:12 mole ratio, and also when the thiol:metal ratio was lowered, according to ESI-MS and MALDI-TOF-MS. As the nanoparticle mixture is enriched, by solvent fractionations, in Au24Pd(SC2Ph)18 relative to Au25(SC2Ph)18, the distinctive optical and electrochemical signatures of Au25(SC2Ph)18 are replaced by Au24Pd(SC2Ph)18 nanoparticle responses, which are very different, even though only one Au atom is replaced by a Pd atom.

Energetics of adsorbed methanol and methoxy on Pt(111) by microcalorimetry.

The heat of adsorption and sticking probability of methanol were measured on clean Pt(111) at 100, 150, and 210 K and on oxygen-precovered Pt(111) at 150 K by single-crystal adsorption calorimetry (SCAC). On clean Pt(111) at 100 K, the heat of methanol adsorption was found to be 60.5 ± 0.8 kJ/mol in the limit of low coverage, resulting in a standard enthalpy of formation (ΔH(f)°) of CH(3)OH(ad) of -263 ± 0.8 kJ/mol. The results at 150 and 210 K on clean Pt(111) were indistinguishable from the energetics measured at 100 K in the same coverage range. Calorimetry of methanol on oxygen-precovered Pt(111) at 150 K yielded the energetics of adsorbed methoxy, giving ΔH(f)°[CH(3)O(ad)] = -170 ± 10 kJ/mol and a CH(3)O-Pt(111) bond enthalpy of 187 ± 11 kJ/mol. By use of these enthalpies, the dissociation of adsorbed methanol on Pt(111) to form methoxy and a hydrogen adatom is found to be uphill by +57 kJ/mol. At coverages below 0.2 monolayer (ML), the sticking probability for methanol on both surfaces at or below 150 K was >0.95. At 210 K, ∼80% of the methanol beam pulse transiently adsorbs to clean Pt(111) with a surface residence time of 238 ms and heat of adsorption of 61.2 ± 2.0 kJ/mol, giving a prefactor for methanol desorption of 4 × 10(15±0.5) s(-1). These measured energetics for methoxy and methanol were compared to density functional theory (DFT) calculations from previous literature, showing DFT to routinely underestimate the bond energy of both adsorbed methanol and methoxy by 15-52 kJ/mol.

Tandem Mass Spectrometry of Thiolate-Protected Au Nanoparticles NaxAu25(SC2H4Ph)18−y(S(C2H4O)5CH3)y

We report the first collision-induced dissociation tandem mass spectrometry (CID MS/MS) of a thiolate-protected Au nanoparticle that has a crystallographically determined structure. CID spectra assert that dissociation pathways for the mixed monolayer Na(x)Au(25)(SC(2)H(4)Ph)(18-y)(S(C(2)H(4)O)(5)CH(3))(y) centrally involve the semi-ring Au(2)L(3) coordination (L = some combination of the two thiolate ligands) that constitutes the nanoparticles protecting structure. The data additionally confirm charge state assignments in the mass spectra. Prominent among the fragments is [Na(2)AuL(2)](1+), one precursor of which is identified as another nanoparticle fragment in the higher m/z region. Another detected fragment, [Na(2)Au(2)L(3)](1+), represents a mass loss equivalent to an entire semi-ring, whereas others suggest involvement (fragmentation/rearrangement) of multiple semi-rings, e.g., [NaAu(3)L(3)](1+) and [NaAu(4)L(4)](1+). The detailed dissociation/rearrangement mechanisms of these species are not established, but they are observed in other mass spectrometry experiments, including those under non-CID conditions, namely, electrospray ionization mass spectrometry (ESI-MS) with both time-of-flight (TOF) and FT-ICR analyzers. The latter, previously unreported results show that even soft ionization sources can result in Au nanoparticle fragmentation, including that yielding Au(4)L(4) in ESI-TOF of a much larger thiolate-protected Au(144) nanoparticle under non-CID conditions.

Improved pyroelectric detectors for single crystal adsorption calorimetry from 100 to 350 K.

The adsorption of atoms and molecules on single crystal surfaces allows one to produce well-characterized atomic, molecular, or dissociated adsorbates. Microcalorimetric measurement of the resulting adsorption energies, i.e., single crystal adsorption calorimetry, allows determination of the standard enthalpies of formation of these adsorbates. Methods are described for making an improved heat detector for such measurements, which greatly improves the signal-to-noise ratio, particularly at low temperatures (down to 100 K). The heat detector is an adaptation of a previously introduced design, based on a metallized pyroelectric polymer (beta-polyvinylidene fluoride), which is pressed against the back of a single crystal during measurement but removed during sample preparation and annealing. The improvement is achieved by selectively etching the metal coating of the polymer, thus reducing the pyro- and piezoelectric noise from all nonessential regions of the polymer. We, furthermore, describe how to achieve a better thermal contact between the sample and the pyroelectric polymer, without increasing the thermal mass of the detector, resulting in significantly improved sensitivities for both 1 and 127 microm thick samples. The result is a detector which, using 1 microm samples, is approximately 40 times more sensitive at 100 K than the traditional polymer-based detector, showing a pulse-to-pulse standard deviation in the heat of adsorption of just 1.3 kJ/mol with gas pulses containing only 1.1% of a monolayer onto Pt(111), for which 1 ML (monolayer) is 1.5x10(15) species/cm(2). For measurements at 300 K, where especially pyroelectric noise is likely of less concern, the new design improves the sensitivity 3.6-fold compared to the traditional detector. These improvements are furthermore used to propose a new detector design that is able to measure heats of adsorption on samples as thick as 127 microm with reasonable sensitivity.

Adsorption Microcalorimetry: Recent Advances in Instrumentation and Application

Adsorption microcalorimetry measures the energetics of adsorbate-surface interactions and can be performed by use of several different techniques. This review focuses on three methods: single-crystal adsorption calorimetry (SCAC), isothermal titration calorimetry (ITC), and electrochemical adsorption calorimetry. SCAC is a uniquely powerful technique that has been applied to a variety of atoms and molecules that represent a large variety of well-defined adsorbate species on a wide range of single-crystal surfaces. ITC and electrochemical microcalorimetry are useful for studying adsorption energies in liquid solutions (on surfaces of suspended powders) and at the electrode-electrolyte interface, respectively. Knowledge of the energetics of adsorbate formation is valuable to ongoing research in many fields, including catalysis, fuel cells, and solar power. In addition, calorimetric measurements serve as benchmarks for the improvement of computational approaches to understanding surface chemistry. We review instrumentation and applications, emphasizing our own work.