11 research outputs found
Counterion Effect on Interfacial Water at Charged Interfaces and Its Relevance to the Hofmeister Series
Specific counterion
effects represented by Hofmeister series are
important for a variety of phenomena such as protein precipitations,
surface tensions of electrolytes solutions, phase transitions of surfactants,
etc. We applied heterodyne-detected vibrational sum-frequency generation
spectroscopy to study the counterion effect on the interfacial water
at charged interfaces and discussed the observed effect with relevance
to the Hofmeister series. Experiments were carried out for model systems
of positively charged cetyltrimethylammonium monolayer/electrolyte
solution interface and negatively charged dodecylsulfate monolayer/electrolyte
interface. At the positively charged interface, the intensity of the
OH band of the interfacial water decreases in the order of the Hofmeister
series, suggesting that the adsorbability of halide anions onto the
interface determines the Hofmeister order as previously proposed by
Zhang and Cremer (<i>Curr. Opin. Chem. Biol.</i> <b>2006</b>, <i>10</i>, 658–663). At the negatively charged
interfaces, on the other hand, the OH band intensity does not depend
significantly on the countercation, whereas variation in the hydrogen-bond
strength of the interfacial water is well correlated with the Hofmeister
order of the cation effect. These results provide new insights into
the molecular level mechanisms of anionic and cationic Hofmeister
effects
Spectroscopy and Dynamics of the Multiple Free OH Species at an Aqueous/Hydrophobic Interface
Sum frequency generation (SFG) spectra and free induction
decay
(FID) measurements of the H<sub>2</sub>O/octadecylsilane (ODS)/silica
interface in the free OH spectral region (∼3700 cm<sup>–1</sup>) show spatially inhomogeneous behavior. The SFG spectra and FIDs
suggest an inhomogeneous response of the free OH, consisting of at
least two distinct species at the interface with short and long coherence
times. In most areas of the sample, an OH band at ∼3680 cm<sup>–1</sup> with a short dephasing (<150 fs), assigned to
the free OH of water interacting with the hydrophobic methyl group
of ODS, was observed in agreement with previously reported SFG spectra
of the H<sub>2</sub>O/ODS/silica interface. In a small fraction (∼20%)
of the sample areas, a more intense peak at ∼3700 cm<sup>–1</sup> was observed in the SFG spectrum characterized by significantly
longer dephasing (∼760 fs) in the SFG-FID. Based on the peak
position, as well as control experiments on octadecydimethylmethoxysilane
(ODMS) monolayers and deuterium substitution experiments at the water/ODS/silica
interfaces, two possible assignments for the new feature are provided.
The long dephasing can be due to the free OH of the Si–OH of
incompletely cross-linked/tethered ODS molecules. Alternatively, a
contribution of water molecules trapped in nano pores of silica surface
and/or confined between the ODS molecules can explain the long coherence.
Either way, the long coherence can be attributed to the OH species
decoupled from bulk water
Observation of the Bending Mode of Interfacial Water at Silica Surfaces by Near-Infrared Vibrational Sum-Frequency Generation Spectroscopy of the [Stretch + Bend] Combination Bands
Vibrational sum-frequency generation (SFG) spectroscopy
of interfacial
water at mineral/aqueous interfaces is extended to the near-IR range
containing the low cross section stretch + bend combination bands
(ν<sub>comb</sub> = ν<sub>OH</sub> + δ<sub>HOH</sub>) of liquid water at silica surfaces near 5000–5300 cm<sup>–1</sup>, for the first time. The assignments of SFG spectra
are supported by FTIR and Raman spectroscopic measurements of the
bulk water ν<sub>comb</sub> modes. The SFG spectra contain significant
contributions from two combinations, [ν<sub>s</sub> + δ]
≈ 5060 cm<sup>–1</sup> and [ν<sub>as</sub> + δ]
≈ 5300 cm<sup>–1</sup>. These measurements provide the
first, to our knowledge, reported probe of the bending mode of water
at buried interfaces. The data suggest that the interfacial water
bending mode is blue-shifted from that of bulk water
The Topmost Water Structure at a Charged Silica/Aqueous Interface Revealed by Heterodyne-Detected Vibrational Sum Frequency Generation Spectroscopy
Despite
recent significant advances in interface-selective nonlinear
spectroscopy, the topmost water structure at a charged silica surface
is still not clearly understood. This is because, for charged interfaces,
not only interfacial molecules at the topmost layer but also a large
number of molecules in the electric double layer are probed even with
second-order nonlinear spectroscopy. In the present study, we studied
water structure at the negatively charged silica/aqueous interface
at pH 12 using heterodyne-detected vibrational sum frequency generation
spectroscopy, and demonstrated that the spectral component of the
topmost water can be extracted by examining the ionic strength dependence
of the Imχ<sup>(2)</sup> spectrum. The obtained Imχ<sup>(2)</sup> spectrum indicates that the dominant water species in the
topmost layer is hydrogen-bonded to the negatively charged silanolate
at the silica surface with one OH group. There also exists minor water
species that weakly interacts with the oxygen atom of a siloxane bridge
or the remaining silanol at the silica surface, using one OH group.
The ionic strength dependence of the Imχ<sup>(2)</sup> spectrum
indicates that this water structure of the topmost layer is unchanged
in a wide ionic strength range from 0.01 to 2 M
Three Distinct Water Structures at a Zwitterionic Lipid/Water Interface Revealed by Heterodyne-Detected Vibrational Sum Frequency Generation
Lipid/water interfaces and associated interfacial water
are vital
for various biochemical reactions, but the molecular-level understanding
of their property is very limited. We investigated the water structure
at a zwitterionic lipid, phosphatidylcholine, monolayer/water interface
using heterodyne-detected vibrational sum frequency generation spectroscopy.
Isotopically diluted water was utilized in the experiments to minimize
the effect of intra/intermolecular couplings. It was found that the
OH stretch band in the Imχ<sup>(2)</sup> spectrum of the phosphatidylcholine/water
interface exhibits a characteristic double-peaked feature. To interpret
this peculiar spectrum of the zwitterionic lipid/water interface,
Imχ<sup>(2)</sup> spectra of a zwitterionic surfactant/water
interface and mixed lipid/water interfaces were measured. The Imχ<sup>(2)</sup> spectrum of the zwitterionic surfactant/water interface
clearly shows both positive and negative bands in the OH stretch region,
revealing that multiple water structures exist at the interface. At
the mixed lipid/water interfaces, while gradually varying the fraction
of the anionic and cationic lipids, we observed a drastic change in
the Imχ<sup>(2)</sup> spectra in which spectral features similar
to those of the anionic, zwitterionic, and cationic lipid/water interfaces
appeared successively. These observations demonstrate that, when the
positive and negative charges coexist at the interface, the H-down-oriented
water structure and H-up-oriented water structure appear in the vicinity
of the respective charged sites. In addition, it was found that a
positive Imχ<sup>(2)</sup> appears around 3600 cm<sup>–1</sup> for all the monolayer interfaces examined, indicating weakly interacting
water species existing in the hydrophobic region of the monolayer
at the interface. On the basis of these results, we concluded that
the characteristic Imχ<sup>(2)</sup> spectrum of the zwitterionic
lipid/water interface arises from three different types of water existing
at the interface: (1) the water associated with the negatively charged
phosphate, which is strongly H-bonded and has a net H-up orientation,
(2) the water around the positively charged choline, which forms weaker
H-bonds and has a net H-down orientation, and (3) the water weakly
interacting with the hydrophobic region of the lipid, which has a
net H-up orientation
Vibrational Sum Frequency Generation by the Quadrupolar Mechanism at the Nonpolar Benzene/Air Interface
The interface selectivity of vibrational
sum frequency generation
(VSFG) spectroscopy is explained under the dipole approximation as
resulting from the breakdown of inversion symmetry at the interface.
From this viewpoint, VSFG is not expected to occur at the interface
consisting of centrosymmetric molecules, because the inversion symmetry
is preserved even at the interface. In reality, however, VSFG at the
nonpolar benzene/air interface has been observed with traditional
homodyne-detected VSFG. Here we report a heterodyne-detected VSFG
study of the benzene/air interface. The result strongly indicates
that VSFG at this interface cannot be explained within the framework
of the dipole approximation. The selection rule and polarization dependence
of the observed VSFG signal show that the quadrupole transition plays
an essential role because of the field discontinuity at the interface.
This finding implies the applicability of interface-selective VSFG
to the nonpolar interfaces comprising centrosymmetric molecules, which
opens a new possibility of VSFG spectroscopy
Water Structure at the Buried Silica/Aqueous Interface Studied by Heterodyne-Detected Vibrational Sum-Frequency Generation
Complex χ<sup>(2)</sup> spectra of buried silica/isotopically
diluted water (HOD-D<sub>2</sub>O) interfaces were measured using
multiplex heterodyne-detected vibrational sum frequency generation
spectroscopy to elucidate the hydrogen bond structure and up/down
orientation of water at the silica/water interface at different pHs.
The data show that vibrational coupling (inter- and/or intramolecular
coupling) plays a significant role in determining the χ<sup>(2)</sup> spectral feature of silica/H<sub>2</sub>O interfaces and
indicate that the doublet feature in the H<sub>2</sub>O spectra does
not represent two distinct water structures (i.e., the ice- and liquid-like
structures) at the silica/water interface. The observed pH dependence
of the imaginary χ<sup>(2)</sup> spectra is explained by (1)
H-up oriented water donating a hydrogen bond to the oxygen atom of
silanolate, which is accompanied by H-up water oriented by the electric
field created by the negative charge of silanolate, (2) H-up oriented
water which donates a hydrogen bond to the neutral silanol oxygen,
and (3) H-down oriented water which accepts hydrogen bonds from the
neutral silanol and donates hydrogen bonds to bulk water molecules.
The broad continuum of the OH stretch band of HOD-D<sub>2</sub>O and
a long tail in the low frequency region represent a wide distribution
of strong hydrogen bonds at the silica/water interface, particularly
at the low pH
Partially Hydrated Electrons at the Air/Water Interface Observed by UV-Excited Time-Resolved Heterodyne-Detected Vibrational Sum Frequency Generation Spectroscopy
Hydrated
electrons are the most fundamental anion species, consisting
only of electrons and surrounding water molecules. Although hydrated
electrons have been extensively studied in the bulk aqueous solutions,
even their existence is still controversial at the water surface.
Here, we report the observation and characterization of hydrated electrons
at the air/water interface using new time-resolved interface-selective
nonlinear vibrational spectroscopy. With the generation of electrons
at the air/water interface by ultraviolet photoirradiation, we observed
the appearance of a strong transient band in the OH stretch region
by heterodyne-detected vibrational sum-frequency generation. Through
the comparison with the time-resolved spectra at the air/indole solution
interface, the transient band was assigned to the vibration of water
molecules that solvate electrons at the interface. The analysis of
the frequency and decay of the observed transient band indicated that
the electrons are only partially hydrated at the water surface, and
that they escape into the bulk within 100 ps
Cooperative Hydrogen-Bond Dynamics at a Zwitterionic Lipid/Water Interface Revealed by 2D HD-VSFG Spectroscopy
Molecular-level elucidation
of hydration at biological membrane
interfaces is of great importance for understanding biological processes.
We studied ultrafast hydrogen-bond dynamics at a zwitterionic phosphatidylcholine/water
interface by two-dimensional heterodyne-detected vibrational sum frequency
generation (2D HD-VSFG) spectroscopy. The obtained 2D spectra confirm
that the anionic phosphate and cationic choline sites are individually
hydrated at the interface. Furthermore, the data show that the dynamics
of water at the zwitterionic lipid interface is not a simple sum of
the dynamics of the water species that hydrate to the separate phosphate
and choline. The center line slope (CLS) analysis of the 2D spectra
reveals that ultrafast hydrogen-bond fluctuation is not significantly
suppressed around the phosphate at the zwitterionic lipid interface,
which makes the hydrogen-bond dynamics look similar to that of the
bulk water. The present study indicates that the hydrogen-bond dynamics
at membrane interfaces is not determined only by the hydrogen bond
to a specific site of the interface but is largely dependent on the
water dynamics in the vicinity and other nearby moieties, through
the hydrogen-bond network
Unified Molecular View of the Air/Water Interface Based on Experimental and Theoretical χ<sup>(2)</sup> Spectra of an Isotopically Diluted Water Surface
The energetically unfavorable termination of the hydrogen-bonded network of water molecules at the air/water interface causes molecular rearrangement to minimize the free energy. The long-standing question is <i>how water minimizes the surface free energy</i>. The combination of advanced, surface-specific nonlinear spectroscopy and theoretical simulation provides new insights. The complex χ<sup>(2)</sup> spectra of isotopically diluted water surfaces obtained by heterodyne-detected sum frequency generation spectroscopy and molecular dynamics simulation show excellent agreement, assuring the validity of the microscopic picture given in the simulation. The present study indicates that there is no ice-like structure at the surfacein other words, there is no increase of tetrahedrally coordinated structure compared to the bulkbut that there are water pairs interacting with a strong hydrogen bond at the outermost surface. Intuitively, this can be considered a consequence of the lack of a hydrogen bond toward the upper gas phase, enhancing the lateral interaction at the boundary. This study also confirms that the major source of the isotope effect on the water χ<sup>(2)</sup> spectra is the intramolecular anharmonic coupling, i.e., Fermi resonance