Judith Langer

Monodisperse Gold Nanotriangles: Size Control, Large-Scale Self-Assembly, and Performance in Surface-Enhanced Raman Scattering

Au nanotriangles display interesting nanoplasmonic features with potential application in various fields. However, such applications have been hindered by the lack of efficient synthetic methods yielding sufficient size and shape monodispersity, as well as by insufficient morphological stability. We present here a synthesis and purification protocol that efficiently addresses these issues. The size of the nanotriangles can be tuned within a wide range by simply changing the experimental parameters. The obtained monodispersity leads to extended self-assembly, not only on electron microscopy grids but also at the air-liquid interface, allowing transfer onto centimeter-size substrates. These extended monolayers show promising performance as surface-enhanced Raman scattering substrates, as demonstrated for thiophenol detection.

Sensing using plasmonic nanostructures and nanoparticles.

Nanoparticles are widely used in various fields of science and technology as well as in everyday life. In particular, gold and silver nanoparticles display unique optical properties that render them extremely attractive for various applications. In this review, we focus on the use of noble metal nanoparticles as plasmonic nanosensors with extremely high sensitivity, even reaching single molecule detection. Sensors based on plasmon resonance shifts, as well as the use of surface-enhanced Raman scattering and surface-enhanced fluorescence, will be considered in this work.

Infrared Spectra of Isolated Protonated Polycyclic Aromatic Hydrocarbon Molecules

Gas-phase infrared (IR) spectra of larger protonated polycyclic aromatic hydrocarbon molecules, H+PAH, have been recorded for the first time. The ions are generated by electrospray ionization and spectroscopically assayed by IR multiple-photon dissociation (IRMPD) spectroscopy in a Fourier transform ion cyclotron resonance mass spectrometer using a free electron laser. IRMPD spectra of protonated anthracene, tetracene, pentacene, and coronene are presented and compared to calculated IR spectra. Comparison of the laboratory IR spectra to an astronomical spectrum of the unidentified IR emission (UIR) bands obtained in a highly ionized region of the interstellar medium provides for the first time compelling spectroscopic support for the recent hypothesis that H+PAHs contribute as carriers of the UIR bands.

Star-shaped magnetite@gold nanoparticles for protein magnetic separation and SERS detection

A novel synthetic methodology for star shaped gold-coated magnetic nanoparticles is reported. The coating is performed in two steps: formation of gold nuclei at the surface of magnetite nanoparticles followed by growth of the gold nuclei into a complete star shaped shell. The star-shaped gold-coated magnetic nanoparticles thus obtained preserve the magnetic properties of the precursor magnetite nanoparticles, e.g. they can be easily separated with a magnet. In addition, the gold coating provides interesting optical properties while simultaneously allowing for biofunctionalization that may be advantageous for biological applications, such as (bio)detection via surface-enhanced Raman spectroscopy (SERS). As a proof-of-concept, a capping agent terminated with a nickel(II)-nitrilotriacetate group showing high affinity for histidine was used to modify the surface of the nanoparticles. The resulting star-shaped nanoparticles were used to selectively capture histidine-tagged maltose-binding protein from a crude cell extract. Finally, the performance of star shaped gold-coated magnetic nanoparticles as SERS platforms was demonstrated through the detection of Raman active dye (Astra Blue).

Infrared spectra of protonated neurotransmitters: serotonin

The gas-phase IR spectrum of the protonated neurotransmitter serotonin (5-hydroxytryptamine) was measured in the fingerprint range by means of IR multiple photon dissociation (IRMPD) spectroscopy. The IRMPD spectrum was recorded in a Fourier transform ion cyclotron resonance mass spectrometer coupled to an electrospray ionization source and an IR free electron laser. Quantum chemical calculations at the B3LYP and MP2 levels of theory using the cc-pVDZ basis set yield six low-energy isomers in the energy range up to 40 kJ/mol, all of which are protonated at the amino group. Protonation at the indole N atom or the hydroxyl group is substantially less favorable. The IRMPD spectrum is rich in structure and exhibits 22 distinguishable features in the spectral range investigated (530-1885 cm(-1)). The best agreement between the measured IRMPD spectrum and the calculated linear IR absorption spectra is observed for the conformer lowest in energy at both levels of theory, denoted g-1. In this structure, one of the three protons of the ammonium group points toward the indole subunit, thereby maximizing the intramolecular NH(+)-π interaction between the positive charge of the ammonium ion and the aromatic indole ring. This mainly electrostatic cation-π interaction is further stabilized by significant dispersion forces, as suggested by the substantial differences between the DFT and MP2 energies. The IRMPD bands are assigned to individual normal modes of the g-1 conformer, with frequency deviations of less than 29 cm(-1) (average <13 cm(-1)). The effects of protonation on the geometric and electronic structure are revealed by comparison with the corresponding structural, energetic, electronic, and spectroscopic properties of neutral serotonin.

Low energy electron driven reactions in single formic acid molecules (HCOOH) and their homogeneous clusters

Low energy (0-3 eV) electron attachment to single formic acid (FA) and FA clusters is studied in crossed electron/molecular beam experiments. Single FA molecules undergo hydrogen abstraction via dissociative electron attachment (DEA) thereby forming HCOO(-) within a low energy resonance peaking at 1.25 eV. Experiments on the isotopomers HCOOD and DCOOH demonstrate that H/D abstraction occurs at the O-H/O-D site. In clusters, electron attachment is strongly enhanced leading to a variety of negatively charged complexes with the dimer M2(-) (M[triple bond]HCOOH) and its dehydrogenated form M (M-H)(-) as the most abundant ones. Apart from the homologous series containing the non-dissociated (Mn(-)) and dehydrogenated complexes (M(n-1) (M-H)(-), n > or = 1) further products are observed indicating that electron attachment at sub-excitation energies (approximately 1 eV) can trigger a variety of chemical reactions. Among these we detect the complex H2O (M-H)(-) which is interpreted to arise from a reaction initiated in the cyclic hydrogen bonded dimer target. In competition to hydrogen abstraction yielding the dehydrogenated complex M (M-H)(-) the abstracted hydrogen atom can react with the opposite FA molecule forming H2O and HCO with the polar water molecule attached to the closed shell HCOO(-) ion. The FA dimer can thus be used as a model system to study the response of a hydrogen bridge towards dehydrogenation in DEA.

Infrared spectra of protonated polycyclic aromatic hydrocarbon molecules: Azulene

The infrared (IR) spectrum of protonated azulene (AzuH(+), C(10)H(9)(+)) has been measured in the fingerprint range (600-1800 cm(-1)) by means of IR multiple photon dissociation (IRMPD) spectroscopy in a Fourier transform ion cyclotron resonance mass spectrometer equipped with an electrospray ionization source using a free electron laser. The potential energy surface of AzuH(+) has been characterized at the B3LYP/6-311G(**) level in order to determine the global and local minima and the corresponding transition states for interconversion. The energies of the local and global minima, the dissociation energies for the lowest-energy fragmentation pathways, and the proton affinity have been evaluated at the CBS-QB3 level. Comparison with calculated linear IR absorption spectra supports the assignment of the IRMPD spectrum to C4-protonated AzuH(+), the most stable of the six distinguishable C-protonated AzuH(+) isomers. Comparison between Azu and C4-AzuH(+) reveals the effects of protonation on the geometry, vibrational properties, and the charge distribution of these fundamental aromatic molecules. Calculations at the MP2 level indicate that this technique is not suitable to predict reliable IR spectra for this type of carbocations even for relatively large basis sets. The IRMPD spectrum of protonated azulene is compared to that of isomeric protonated naphthalene and to an astronomical spectrum of the unidentified IR emission bands.

Infrared spectra of the protonated neurotransmitter histamine: competition between imidazolium and ammonium isomers in the gas phase.

The infrared (IR) spectrum of protonated histamine (histamineH(+)) was recorded in the 575-1900 cm(-1) fingerprint range by means of IR multiple photon dissociation (IRMPD) spectroscopy. The IRMPD spectrum of mass-selected histamineH(+) ions was obtained in a Fourier transform ion cyclotron resonance mass spectrometer coupled to an electrospray ionization source and an IR free electron laser. A variety of isomers were identified and characterized by quantum chemical calculations at the B3LYP and MP2 levels of theory using the cc-pVDZ basis set. The low-energy isomers are derived from various favourable protonation sites--all of which are N atoms--and different orientations of the ethylamine side chain with respect to the heterocyclic imidazole ring. The measured IRMPD spectrum was monitored in the NH(3) loss channel and exhibits 14 bands in the investigated spectral range, which were assigned to vibrational transitions of the most stable isomer, denoted A. This imidazolium-type isomer A with protonation at the imidazole ring and gauche conformation of the ethylamine side chain is significantly stabilized by an intramolecular ionic Nπ-H(+)···Nα hydrogen bond to the ethylamino group. The slightly less stable ammonium-type isomer B with protonation at the ethylamino group is only a few kJ mol(-1) higher in energy and may also provide a minor contribution to the observed IRMPD spectrum. Isomer B is derived from A by simple proton transfer from imidazole to the ethylamino group along the intramolecular Nπ-H(+)···Nα hydrogen bond via a low barrier, which is calculated to be of the order of 5-15 kJ mol(-1). Significantly, the most stable structure of isolated histamineH(+) differs from that in the condensed phase by both the protonation site and the conformation of the side chain, emphasizing the important effects of solvation on the structure and function of this neurotransmitter. The effects of protonation on the geometric and electronic structure of histamine are evaluated by comparing the calculated properties of isomer A with those of the most stable structure of neutral histamine A(n).

Negative ion formation from low energy (0–15 eV) electron impact to CF2Cl2 under different phase conditions

Negative ion formation following low energy (0–10 eV) electron attachment to free and bound CF2Cl2 molecules is studied in (1) a molecular beam experiment (single molecules, homogeneous clusters, and mixed CF2Cl2/NH3 clusters) and (2) a UHV surface experiment where desorption of negative ions from condensed CF2Cl2 is observed. From single gas phase CF2Cl2 molecules we observe Cl− and F− generated via dissociative electron attachment from a resonance near 0 eV and 3 eV, respectively, as the most abundant ions. From homogeneous clusters (CF2Cl2)n, we additionally detect undissociated complexes of the form (M)n−(M=CF2Cl2) including the stabilized monomer CF2Cl2− and also “solvated fragment ions” of the form Mn⋅X−(X=Cl, F). Their relative abundance vs size (n) of the final product varies in a significant different way between (M)n− and Mn⋅X− reflecting the different relaxation probabilities in the initial cluster. In the desorption spectra, the dominant low energy Cl− gas phase resonance is strongly suppresse...

Vibrational Spectra and Structures of Neutral SimCn Clusters (m + n = 6): Sequential Doping of Silicon Clusters with Carbon Atoms

Vibrational spectra of mixed silicon carbide clusters Si(m)C(n) with m + n = 6 in the gas phase are obtained by resonant infrared-vacuum-ultraviolet two-color ionization (IR-UV2CI for n ≤ 2) and density functional theory (DFT) calculations. Si(m)C(n) clusters are produced in a laser vaporization source, in which the silicon plasma reacts with methane. Subsequently, they are irradiated with tunable IR light from an IR free electron laser before they are ionized with UV photons from an F(2) laser. Resonant absorption of one or more IR photons leads to an enhanced ionization efficiency for Si(m)C(n) and provides the size-specific IR spectra. IR spectra measured for Si(6), Si(5)C, and Si(4)C(2) are assigned to their most stable isomers by comparison with calculated linear absorption spectra. The preferred Si(m)C(n) structures with m + n = 6 illustrate the systematic transition from chain-like geometries for bare C(6) to three-dimensional structures for bare Si(6). In contrast to bulk SiC, carbon atom segregation is observed already for the smallest n (n = 2).