3 research outputs found
Surface Effect of Alumina on the First Electronic Transition of Liquid Water Studied by Far-Ultraviolet Spectroscopy
The
first electronic transition (<i>AÌ</i> â <i>XÌ</i>) of liquid water (H<sub>2</sub>O and D<sub>2</sub>O) on an α-alumina substrate was studied using variable angle
attenuated total reflection far-ultraviolet (VA-ATR-FUV) spectroscopy
in the wavelength region 140â180 nm (8.86â6.89 eV).
A variation in the penetration depth of the evanescent wave of a probe
light (25â19 nm) directly determined individual FUV spectra
associated with bulk water (distance from the alumina surface >2
nm)
and interfacial water (<2 nm). We found that the <i>AÌ</i> â <i>XÌ</i> band of the interfacial water
was markedly blue-shifted and red-tailed relative to the bulk water.
The electronic state difference of the interfacial water from the
bulk water mainly arose from the hydrogen-bond structure and energy
affected by the alumina surface
Electronic Transitions of Protonated and Deprotonated Amino Acids in Aqueous Solution in the Region 145â300 nm Studied by Attenuated Total Reflection Far-Ultraviolet Spectroscopy
The
electronic transitions of 20 naturally occurring amino acids
in aqueous solution were studied with attenuated total reflection
far-ultraviolet (ATR-FUV) spectroscopy in the region from 145 to 300
nm. From the measured ATR spectra of sample solutions, the FUV absorption
spectra attributed to the amino acids were separated from the intense
solvent absorption by using a modified KramersâKronig transformation
method. The FUV absorption spectra of the amino acids reflect the
protonation states of the backbone and side-chain structures. The
contributions of the side chains to the spectra were also examined
from the difference spectra subtracting the corresponding Gly spectrum
from each spectrum. The observed spectra were compared mostly with
the electronic transition studies of the molecular fragments of the
amino acids in gas phase. The FUV spectra of the amino acids exhibited
the intra- and intermolecular electronic interactions of the soluteâsolute
as well as the soluteâsolvent, and those are essential factors
to elucidate UV photochemical processes of the amino acids in aqueous
solution
Hydration States of Poly(<i>N</i>âisopropylacrylamide) and Poly(<i>N</i>,<i>N</i>âdiethylacrylamide) and Their Monomer Units in Aqueous Solutions with Lower Critical Solution Temperatures Studied by Infrared Spectroscopy
The coil-to-globule transition of polyÂ(<i>N</i>-isopropylacrylamide)
(PNiPA) and polyÂ(<i>N</i>,<i>N</i>-diethylacrylamide)
(PdEA) in aqueous solutions has recently received substantial interest
in its drastic change in the hydration state from a hydrated random
coil to a hydrophobic globule for practical applications: drug delivery
and tissue engineering. In this report, the hydration states of PNiPA
and PdEA in aqueous solutions were investigated by IR spectroscopy
in the amide I, NâH and CâH stretching band regions
as compared with those of their repeat units, <i>N</i>-isopropylpropionamide
(NiPP) and <i>N</i>,<i>N</i>-diethylpropylacrylamide
(dEP) in aqueous and cyclohexane solutions in combined with their
phase diagrams. The IR spectral changes in the amide I and CâH
stretching band regions of <i>N</i>-alkylamides and <i>N</i>,<i>N</i>-dialkylamides including NiPP and dEP
in aqueous solutions with varying concentration was characteristic
due to different amideâamide interaction; the amideâamide
interaction for <i>N</i>-alkylamide (Cî»O···HâN
hydrogen bond) is stronger than that for <i>N</i>,<i>N</i>-dialkylamide (dipolar interaction). It is found that almost
all amide groups of PNiPA in aqueous solution forms the intramolecular
Cî»O···HâN hydrogen bond even in the coil
state and that the amide group of PNiPA is less hydrated than that
of PdEA in spite of the similar degree of hydration to alkyl groups.
The IR spectral changes in the amide I and CâH stretching band
regions of PNiPA and PdEA in aqueous solutions with heat are ascribed
to the dehydration of the amide and alkyl groups from the coil state
to the globule one