8 research outputs found
Microhydration of Dibenzo-18-Crownâ6 Complexes with K<sup>+</sup>, Rb<sup>+</sup>, and Cs<sup>+</sup> Investigated by Cold UV and IR Spectroscopy in the Gas Phase
In
this Article, we examine the hydration structure of dibenzo-18-crown-6
(DB18C6) complexes with K<sup>+</sup>, Rb<sup>+</sup>, and Cs<sup>+</sup> ion in the gas phase. We measure well-resolved UV photodissociation
(UVPD) spectra of K<sup>+</sup>·DB18C6·(H<sub>2</sub>O)<sub><i>n</i></sub>, Rb<sup>+</sup>·DB18C6·(H<sub>2</sub>O)<sub><i>n</i></sub>, and Cs<sup>+</sup>·DB18C6·(H<sub>2</sub>O)<sub><i>n</i></sub> (<i>n</i> = 1â8)
complexes in a cold, 22-pole ion trap. We also measure IR-UV double-resonance
spectra of the Rb<sup>+</sup>·DB18C6·(H<sub>2</sub>O)<sub>1â5</sub> and the Cs<sup>+</sup>·DB18C6·(H<sub>2</sub>O)<sub>3</sub> complexes. The structure of the hydrated complexes
is determined or tentatively proposed on the basis of the UV and IR
spectra with the aid of quantum chemical calculations. Bare complexes
(K<sup>+</sup>·DB18C6, Rb<sup>+</sup>·DB18C6, and Cs<sup>+</sup>·DB18C6) have a similar boat-type conformation, but the
distance between the metal ions and the DB18C6 cavity increases with
increasing ion size from K<sup>+</sup> to Cs<sup>+</sup>. Although
the structural difference of the bare complexes is small, it highly
affects the manner in which each is hydrated. For the hydrated K<sup>+</sup>·DB18C6 complexes, water molecules bind on both sides
(top and bottom) of the boat-type K<sup>+</sup>·DB18C6 conformer,
while hydration occurs only on top of the Rb<sup>+</sup>·DB18C6
and Cs<sup>+</sup>·DB18C6 complexes. On the basis of our analysis
of the hydration manner of the gas-phase complexes, we propose that,
for Rb<sup>+</sup>·DB18C6 and Cs<sup>+</sup>·DB18C6 complexes
in aqueous solution, water molecules will preferentially bind on top
of the boat conformers because of the displaced position of the metal
ions relative to DB18C6. In contrast, the K<sup>+</sup>·DB18C6
complex can accept H<sub>2</sub>O molecules on both sides of the boat
conformation. We also propose that the characteristic solvation manner
of the K<sup>+</sup>·DB18C6 complex will contribute entropically
to its high stability and thus to preferential capture of K<sup>+</sup> ion by DB18C6 in solution
FranckâCondon-like Progressions in Infrared Spectra of Biological Molecules
Infrared
spectra in the NH stretch region are often used for structure
determination of gas-phase biological molecules. Vibrational couplings
complicate the structure determination process by giving rise to additional
vibrational bands along with the expected fundamental transitions.
We present an example of a strong anharmonic coupling in a biological
molecule, Ac-Phe-Ala-LysH<sup>+</sup>, which causes the appearance
of long vibrational progressions in the infrared spectrum. By analyzing
the spectra of the ground and the electronically excited state, we
determined that the coupling occurs between the NH stretch (Ï<sub>NH</sub>) and a low-frequency torsion of the phenyl ring (Ï<sub>Ï</sub>). We describe the vibrational progressions using a
BornâOppenheimer-like separation of the high-frequency stretch
and low-frequency torsion with a quartic Taylor expansion for the
potential energy surface that accounts for the equilibrium distance
and frequency change of the torsional vibration upon the NH stretch
excitation. We also demonstrate that small conformational changes
in the peptide are sufficient to break this coupling
Cryogenic Spectroscopy and Quantum Molecular Dynamics Determine the Structure of Cyclic Intermediates Involved in Peptide Sequence Scrambling
Collision-induced dissociation (CID)
is a key technique used in
mass spectrometry-based peptide sequencing. Collisionally activated
peptides undergo statistical dissociation, forming a series of backbone
fragment ions that reflect their amino acid (AA) sequence. Some of
these fragments may experience a âhead-to-tailâ cyclization,
which after proton migration, can lead to the cyclic structure opening
in a different place than the initially formed bond. This process
leads to AA sequence scrambling that may hinder sequencing of the
initial peptide. Here we combine cryogenic ion spectroscopy and <i>ab initio</i> molecular dynamics simulations to isolate and
characterize the precise structures of key intermediates in the scrambling
process. The most stable peptide fragments show intriguing symmetric
cyclic structures in which the proton is situated on a <i>C</i><sub>2</sub> symmetry axis and forms exceptionally short H-bonds
(1.20 Ă
) with two backbone oxygens. Other nonsymmetric cyclic
structures also exist, one of which is protonated on the amide nitrogen,
where ring opening is likely to occur
Infrared Spectroscopy as a Probe of Electronic Energy Transfer
We
have combined electronic and vibrational spectroscopy in a cryogenic
ion trap to produce highly resolved, conformer-selective spectra for
the ground and excited states of a peptide containing two chromophores.
These spectra permit us to determine the precise three-dimensional
structure of the peptide and give insight into the migration of the
electronic excitation from phenylalanine to tyrosine because changes
in the excited-state infrared spectra are sensitive to localization
of the electronic energy in each chromophore. The well-controlled
experimental conditions make this result a stringent test for theoretical
methods dealing with electronic energy transfer
New Approach for the Identification of Isobaric and Isomeric Metabolites
The structural elucidation
of metabolite molecules is important
in many branches of the life sciences. However, the isomeric and isobaric
complexity of metabolites makes their identification extremely challenging,
and analytical standards are often required to confirm the presence
of a particular compound in a sample. We present here an approach
to overcome these challenges using high-resolution ion mobility spectrometry
in combination with cryogenic vibrational spectroscopy for the rapid
separation and identification of metabolite isomers and isobars. Ion
mobility can separate isomeric metabolites in tens of milliseconds,
and cryogenic IR spectroscopy provides highly structured IR fingerprints
for unambiguous molecular identification. Moreover, our approach allows
one to identify metabolite isomers automatically by comparing their
IR fingerprints with those previously recorded in a database, obviating
the need for a recurrent introduction of analytical standards. We
demonstrate the principle of this approach by constructing a database
composed of IR fingerprints of eight isomeric/isobaric metabolites
and use it for the identification of these isomers present in mixtures.
Moreover, we show how our fast IR fingerprinting technology allows
to probe the IR fingerprints of molecules within just a few seconds
as they elute from an LC column. This approach has the potential to
greatly improve metabolomics workflows in terms of accuracy, speed,
and cost
UV and IR Spectroscopy of Cryogenically Cooled, Lanthanide-Containing Ions in the Gas Phase
We
measure UV and IR spectra in the gas phase for EuOH<sup>+</sup>, EuCl<sup>+</sup>, and TbO<sup>+</sup> ions, which are produced by an electrospray
ionization source and cooled to âŒ10 K in a cold, 22-pole ion
trap. The UV photodissociation (UVPD) spectra of these ions show a
number of sharp, well-resolved bands in the 30000â38000 cm<sup>â1</sup> region, although a definite assignment of the spectra
is difficult because of a high degree of congestion. We also measure
an IR spectrum of the EuOH<sup>+</sup> ion in the 3500â3800
cm<sup>â1</sup> region by IRâUV double-resonance spectroscopy,
which reveals an OH stretching band at 3732 cm<sup>â1</sup>. We perform density functional theory (DFT) and time-dependent DFT
(TD-DFT) calculations of these ions in order to examine the nature
of the transitions. The DFT results indicate that the states of highest-spin
multiplicity (octet for EuOH<sup>+</sup> and EuCl<sup>+</sup> and
septet for TbO<sup>+</sup>) are substantially more stable than other
states of lower-spin multiplicity. The TD-DFT calculations suggest
that UV absorption of the EuOH<sup>+</sup> and EuCl<sup>+</sup> ions
arises from EuÂ(4f) â EuÂ(5d,6p) transitions, whereas electronic
transitions of the TbO<sup>+</sup> ion are mainly due to the electron
promotion of OÂ(2p) â TbÂ(4f,6s). The UVPD results of the lanthanide-containing
ions in this study suggest the possibility of using lanthanide ions
as âconformation reportersâ for gas-phase spectroscopy
for large molecules
Ion Selectivity of Crown Ethers Investigated by UV and IR Spectroscopy in a Cold Ion Trap
Electronic and vibrational spectra of benzo-15-crown-5
(B15C5)
and benzo-18-crown-6 (B18C6) complexes with alkali metal ions, M<sup>+</sup>âąB15C5 and M<sup>+</sup>âąB18C6 (M = Li, Na,
K, Rb, and Cs), are measured using UV photodissociation (UVPD) and
IRâUV double resonance spectroscopy in a cold, 22-pole ion
trap. We determine the structure of conformers with the aid of density
functional theory calculations. In the Na<sup>+</sup>âąB15C5
and K<sup>+</sup>âąB18C6 complexes, the crown ethers open the
most and hold the metal ions at the center of the ether ring, demonstrating
an optimum matching in size between the cavity of the crown ethers
and the metal ions. For smaller ions, the crown ethers deform the
ether ring to decrease the distance and increase the interaction between
the metal ions and oxygen atoms; the metal ions are completely surrounded
by the ether ring. In the case of larger ions, the metal ions are
too large to enter the crown cavity and are positioned on it, leaving
one of its sides open for further solvation. Thermochemistry data
calculated on the basis of the stable conformers of the complexes
suggest that the ion selectivity of crown ethers is controlled primarily
by the enthalpy change for the complex formation in solution, which
depends strongly on the complex structure
The Structure of the Protonated Serine Octamer
The
amino acid serine has long been known to form a protonated
âmagic-numberâ cluster containing eight monomer units
that shows an unusually high abundance in mass spectra and has a remarkable
homochiral preference. Despite many experimental and theoretical studies,
there is no consensus on a Ser<sub>8</sub>H<sup>+</sup> structure
that is in agreement with all experimental observations. Here, we
present the structure of Ser<sub>8</sub>H<sup>+</sup> determined by
a combination of infrared spectroscopy and ab initio molecular dynamics
simulations. The three-dimensional structure that we determine is
âŒ25 kcal mol<sup>â1</sup> more stable than the previous
most stable published structure and explains both the homochiral preference
and the experimentally observed facile replacement of two serine units