Most of this division was absorbed into the
Optical Technology Division
Molecular Physics Division
Technical Highlights
- FTMW Spectrometer Development for Analytical Applications. A number
of recent improvements in Fourier-transform microwave spectroscopy (FTMS) have
increased the detectability limits for gas phase species down to the
10 ppb to 100 ppb range. This high sensitivity coupled with
100 % species selectivity, millisecond response times and complete
automation of the instrument provides analytical chemists with a new technique
for the determination of trace gas species that are present in industrial
chemical processes. The technique can be used either in-lieu-of or as a
complementary detection technique to gas chromatography mass spectrometric
techniques (GCMS) for the detection of gas phase species.

Figure 1: Comparison of the signal-to-noise ratio for 1 gas pulse
and 100 gas pulses of a 120 ppb sample of acrolein in Neon carrier
gas showing a minimum detectable signal of approximately 2 ppb for a
100 pulse average.
Sensitivity tests of the new spectrometer were carried out using 800 ppm
samples of acrolein (CH2 = CHCHO) and propionaldehyde
(CH3CH2CHO). Using these samples and the known isotopic
abundances of 13C = 1.1 %,
18O = 0.2 %, and
2H = 0.015 %, single shot (one gas pulse from the
pulsed nozzle) detection limits of approximately 40 ppb were attained.
Averaging for 100 nozzle pulses yielded a signal-to-noise ratio of 35/1
on transitions of the monodeuterated isotopes in natural abundance. This
corresponds to detection limits of approximately 3 ppb. Additional
improvements in the instrument's detection system and software modifications
should yield another order of magnitude improvement in sensitivity.
Advantages of the new technique in monitoring trace gas constituents include
the 100 % certainty of the identity of the species being monitored. Using
a pulsed molecular beam nozzle in conjunction with a specially designed flow
nozzle which operates at up to 30 Hz repetition rates allows rapid
response to changes in industrial process flow streams. The cooling provided
by the pulsed molecular beam permits larger molecular species to be monitored
with the same ease as smaller species since only the lowest rotational energy
levels will of any species will be populated at the 1 K temperature of
the molecular beam. (R.D. Suenram and F.J. Lovas)
- Large Amplitude Internal Motions - Cooperative Effects.
Cooperative effects involving large numbers of molecules play an important
role in condensed phase chemical and biochemical reactions, but such
cooperative effects are thought to be driven by a succession of nearest
neighbor interactions.
Figure 2: Spectral trace of the J = 2-1 region of the
methanol dimer showing the complex spectrum that results from the facile
tunneling and internal rotations of the methyl groups. Under non-tunneling
conditions only three peaks would be present.
Since many cooperative effects are equivalent to a collection of internal
rotations about C-C single bonds, and since we noted several years ago that a
substantial reduction in barrier height to methyl group internal rotation was
produced in methanol when the methanol was hydrogen bonded to other
molecular species, we have investigated a larger class of methanol dimers with
a view to barrier determination and elucidation of any large changes observed.
These efforts provide a wide variety of benchmark measurements for use by
those involved in developing new algorithms for treating weak interactions in
these systems (Biosym, a current ATP Awardee). The species that have been
studied, include methanol dimer, methanol-water, methanol-formamide,
methanol-carbon monoxide and methanol-hydrogen cyanide. One of the general
structural features common to these species is that the hydroxyl hydrogen of
methanol is not involved in hydrogen bonding. The two exceptions are the
methanol dimer itself in which the OH group of one monomer binds to the
O atom of the other and methanol-formamide which has a doubly hydrogen
bonded structure. The methanol dimer, as well as methanol-water, are rather
complicated systems and required the development of extensive new theory in
order to achieve an adequate description of all internal motions. A simplified
model employing the internal axis method could be used to extract internal
rotation barriers from all the molecules studied, however, leading to the
following V3 barriers: (CH3OH)2
V3(donor) = 191 cm-1, V3
(acceptor) = 136 cm-1 CH3OH·CO
V3 = 183 cm-1;
CH3OH·HCN V3 = 137 cm-1; and
NH2COH·CH3OH V3 =
231 cm-1. Comparison of these effective barrier heights
with free methanol (373 cm-1) indicates a substantial
reduction upon dimer formation. These barrier heights are unexpectedly
sensitive to deuteration of the hydroxyl hydrogen not involved in the hydrogen
bond, suggesting that the librational motion of the OH group contributes to
this effective lowering of the barrier, and modeling this motion can explain
the large discrepancy. This work has been carried out in collaboration with
M. Tretyakov and S. Belov, Institute of Applied Physics, Russia,
W. Stahl, University of Kiel, Germany, P. Stockman and
G. Blake, California Institute of Technology, J. Sobhanadri, Indian
Institute of Technology, Madras, India, N. Ohashi, Kanazawa University,
Japan, and guest worker J. Ortigoso, Instituto de Estructura
de la Materia, Madrid, Spain. (F.J. Lovas, J.T. Hougen,
R.D. Suenram and G.T. Fraser)
- High Resolution IR Studies of Atmospheric Molecules. The burgeoning
importance of remote-sensing Fourier-transform infrared spectroscopy as a new
technique for detecting and monitoring fugitive emissions at chemical plant
boundaries has sparked renewed interest in this area. This is in addition to
the on-going NASA sponsored work in the division. Much of the frequency and
intensity data resulting from this effort winds up in the HITRAN tables, an
exhaustive compilation of the spectrum of the atmosphere produced by the Air
Force Geophysics Laboratory.
As a result of the recent volcanic activity in the Philippines and Japan, and
the emission of great quantities of SO2 into the atmosphere, it was
discovered that the spectral data for SO2 and SO3 in the
HITRAN tables was inadequate. As a result, an extensive study of the
fundamental and a number of overtone and combination bands of SO2
is being carried out in collaboration with J.-M. Flaud of LPMA in Paris.
A global fitting of the (010), (020), (100) and (001) levels has been made
resulting in much improved spectroscopic parameters. In addition the
ν1 + ν3,
2ν1 + ν3, 2ν3 and
3ν3 bands have been studied and an excellent set of rotational
and vibrational anharmonic constants and intensity parameters has been
obtained.
The HOCl molecule is one of the species involved in the stratospheric ozone
reactions. In collaboration with James Burkholder of NOAA, we have just
finished a study of the a-,b-type hybrid ν1 band of this
molecule. Since this band falls in the intense water region in the 3 µm
region, it is not of great importance directly for remote sensing purposes
except in the far wings of the band; however, the improved ground state
rotational constants derived permit calculation of the far IR spectrum with a
uncertainty of better than ±0.001 cm-1.
Molecular beam spectra of several bands of N2O3 and
N2O4 have been obtained and completely analyzed. The
cooling obtained in the molecular beam experiments greatly simplifies the
spectra, and facilitates the line assignment. Also in a collaborative effort
with DuPont, the beam spectrum of chlorine nitrate has been obtained, and a
band analysis is in progress.
At the request of NASA, we have also been studying the collision induced
absorption in the fundamental bands of N2 and O2 in
order to permit modeling of the background continuum produced by these
molecules in the 1600 cm-1 and 2340 cm-1
regions. Laboratory measurement requires long paths (80 m) and high
pressure [1.2 MPa (12 atm.)]. Initial measurements were plagued by
ppb amounts of impurities. This problem has recently been solved, and we
expect to finish this project in the next three months. (W.J. Lafferty
and A. Andrews)
- Collisional Studies of Atmospheric Molecules. There is currently
an increased level of activity in remote-sensing Fourier transform infrared
spectroscopy for use in identifying and quantifying multiple toxic gases
simultaneously. In efforts aimed at developing the requisite models for
treating the effects of line broadening in these complex systems we are
continuing our work on collisional lineshapes with emphasis on the phenomenon
of line mixing in heavily overlapped spectra. We have recorded self-,
N2- and Ar-broadened combination band Q branches in HCN and HCCH
from the well-resolved Doppler limit at low pressures to the blended contours
at atmospheric pressures using a tunable difference-frequency laser
spectrometer. At lower pressures where the lines are not overlapped, the
broadening coefficients as a function of rotational quantum number J are
independent of vibrational level and can be modelled successfully using an
energy-corrected-sudden (ECS) approximation scaling law for self-broadened HCN
and with simpler empirical energy-gap fitting laws for the other collision
partners. No empirical collision dynamics model was found suitable for all
cases. At higher pressures where overlap is severe, line mixing, manifest as a
non-additive superposition of Lorentzian lines, strongly affects the blended
contours, and indicates that the coupling between lines varies from 30 %
to 64 % of the collisional broadening. The decoupling presumably arises
from collisional energy transfer to the other member of the l-type
doublet not observed in the Q-branch transitions of these II-Σ bands. A
vibrational angular momentum coupling model recently proposed by a French
group to account for line mixing in infrared Q branches of CO2 does
not seem to work for the similar molecules studied here, so we have utilized
empirical coupling factors to fit our observed contours.
We have also studied self-, N2-, O2-, H2-,
Ar- and He-broadening of the ν1 band of ammonia with the
difference-frequency laser. A systematic J and K dependence of the broadening
coefficients is observed, with striking similarities for N2,
O2 and Ar and for H2 and He buffer gases. Self
broadening is adequately explained by Anderson-Tsao-Curnutte theory which,
however, fails in the cases of the non-polar buffer gases studied. Dicke
narrowing is evident at intermediate pressures, yielding an average narrowing
coefficient and an optical diffusion constant for each buffer gas. The
broadening coefficients are in good agreement with ground-state inversion
measurements except for H2. We are currently studying Ar broadening
of HF for comparison with recent "exact" quantum mechanical
calculations from a very realistic intermolecular potential obtained from high
resolution microwave and infrared spectra of the Ar-HF van der Waals species.
Our initial results appear to be in excellent agreement, with an as yet
unexplained lineshape asymmetry observed. (A. Pine)
- Free Internal Rotors. Most of the metalorganic molecules used in
semiconductor MOCVD and MOMBE processing and fabrication are di- or trimethyl
metals exhibiting facile internal rotation of the methyl groups. This internal
rotation leads to extremely congested and complicated spectra which have not
been adequately studied in the infrared. To test the feasibility of such
studies for the NIST Semiconductor Initiative, we have recorded a low
temperature spectrum of a prototype species, dimethylacetylene (a.k.a. DMA,
C4H6, H3C-C ≡ C-CH3,
2-butyne), using a tunable-laser difference-frequency spectrometer and a White
cell cooled to approximately 195 K. Most of the free internal rotor
structure of the molecule has been resolved and the low energy torsional hot
bands have been suppressed. The spectrum is under analysis by P.R. Bunker
of the National Research Council of Canada, Ottawa, Canada and
C. di Lauro of the University of Naples, Italy.
(A. Pine)
- Submillimeter Molecular-Beam Spectrometer for the Investigation of
Weakly Bound Complexes Based on Phase-Locked Backward-Wave Oscillators.
Phase-locked Russian-made backward wave oscillators have been coupled to an
electric-resonance optothermal molecular-beam spectrometer to allow the study
of the submillimeter and far-infrared spectra of weakly bound complexes and
stable molecules. The rapid scanning and double-resonance capabilities of the
spectrometer simplify the quantum-state assignment of complex spectra. Initial
studies were undertaken on isotopic water dimer to unravel the complex
tunneling dynamics of the various isotopomers. The spectra will be used to
more fully characterize the pair potential of water. The goal is to achieve a
reliable intermolecular potential for water to allow for the accurate
computer modeling of the properties of water. Spectra have also obtained and
analyzed for deuterated ammonia dimer and the ammonia hydrogen-sulfide
complex.

Figure 3: Q-branch spectrum of water dimer obtained using NIST's EROS
molecular beam instrument using a computer-driven, phase-locked Russian BWO
source.
The isotopic ammonia dimer will allow us to address the apparent disagreement
between ab initio theory and experiment on the equilibrium structure of
the (NH3)2. Part of this effort has been carried out to
provide experimentally derived benchmarks for the new ab initio and
molecular mechanics algorithms being developed by Biosym, an ATP Participant
in their quest to develop a better understanding of the complex interactions
possible between drugs and biological molecules. (G.T. Fraser,
R.D. Suenram, E. Karyakin, and G. Hilpert)
- An Evaluation of Theoretical Compressibility Factors for the
CH4/H2O System. Accurate intermolecular potentials
are required by the natural gas and chemical industry for the calculation of
second-viral coefficients and compressibility factors for gases of varying
composition. Potentials of interest for natural gas transport include those
for CH4·CH4, CH4·H2O,
and CH4·H2S. In an effort to test and improve the
available intermolecular potentials for the
CH4·H2O system we have examined the microwave
spectrum of the C4H·H2O complex. The rotational
spectrum is extremely complex due to the weak anisotropy of the potential
which allows hindered rotation of the CH4 and H2O
subunits. The spectroscopic constants obtained from isotopic studies
determine the minimum energy configuration for the potential, which has the
H2O subunit proton donating to the CH4. This disagrees
with the results of a recent ab initio quantum mechanical
calculation of the potential energy surface which has a minimum energy
geometry in which the CH4 is hydrogen bonding to the oxygen of the
H2O unit. The large amplitude motions sample large regions of the
intermolecular potential, allowing a quantitative characterization of the
anisotropy of the interaction. The present results suggest a revaluation of
compressibility factors and second-viral coefficients calculated from the
recent ab initio potential surface. (R.D. Suenram,
G.T. Fraser, F.J. Lovas, and Y. Kawashima)
- Spectra of Molecular Reaction Intermediates in Chemical Vapor
Deposition and Plasma Processing. A special effort has recently been
started to obtain previously unavailable information on the molecular energy
levels of free radicals and molecular ions which may be formed during the
course of chemical vapor deposition and plasma processing. The interaction of
neon atoms excited to 16.6 eV to 16.8 eV with precursor molecules is
exceptionally well suited to that task. Their interaction with BF3
has yielded infrared absorptions of all three vibrational fundamentals and one
combination band (ν1 + ν3) of the
BF2 free radical, as well as absorptions which have been assigned
to the stretching fundamentals of BF3+, the ground state
structure of which is distorted as a result of interaction with a low-lying
degenerate excited electronic state. Photodecomposition of
BF3+ in the red spectral region leads to growth in the
ν3 infrared absorption of BF2+. Before
these studies, the positions of two of the vibrational fundamentals of
BF2 had been determined, one of them with 30 cm-1
uncertainty. No spectroscopic data for BF2+ and no
quantitative vibrational data for BF3+ were available.
The infrared spectral data for BF2 and for
BF2+ are in excellent agreement with recent
ab initio calculations of the molecular energy levels of these
species performed by Drs. Karl Irikura and Jeffrey Hudgens, of the Chemical
Kinetics and Thermodynamics Division. The analogous experiments on
NF3 have led to the assignment of the ν 3 fundamental
and the ν1 + ν3 combination band of
NF2+, in good agreement with the positions obtained in
a recent ab initio calculation, and to the tentative spectroscopic
identification of NF3+. (M.E. Jacox)
- Vibrational and Electronic Energy Levels of Small Polyatomic Transient
Molecules. There have been two major outputs in this ongoing project,
supported in part by the Standard Reference Data Program. A 461-page monograph
presenting gas-phase and matrix-isolation spectroscopic data for 1582 species
and their fully deuterium-substituted counterparts [M.E. Jacox,
Vibrational and Electronic Energy Levels of Polyatomic Transient
Molecules, J. Phys. Chem. Ref. Data, Monograph 3 (1994)] has
been completed and proofread. The computer-searchable version of these data
(NIST VEEL-Standard Reference Database #26, Version 3) was also prepared,
and will be ready for distribution in early 1994. Users may search by
molecule, by wavenumber range, or by wavelength range.
(M.E. Jacox)
- Substrate to Adsorbate Energy Transfer. In a joint research effort
involving scientists in the Molecular Physics Division and the Surface and
Microanalysis Science Division, picosecond lasers were used to determine the
rates and mechanisms for energy to flow from a metal substrate to the
vibrational modes of chemisorbed molecules. Such information is critically
important to understanding chemical reactivity at surfaces since sticking,
desorption, surface mobility and chemical reactions are activated by
vibrational excitation. The coupling of optical radiation to surface reactions
is receiving attention in the fields of catalysis, semiconductor processing,
and solar energy conversion.
In these experiments, carbon monoxide, CO, chemisorbed on a Cu(100) crystal
initially at a temperature T = 100 K was studied, and
the results compared to our previous data for CO on Pt(111) and to theory for
CO/Cu (done at AT&T Bell Labs). A short duration (< 1 ps) visible
or UV laser pump pulse created hot electrons (characterized by temperature
Te) and hot lattice phonons (characterized by temperature
Tlat) in the near-surface region of the Cu substrate. In our
experiments the maximum temperatures following the pump were
Te = 300 K and
Tlat = 130 K. The increased energy in the
electronic and lattice degrees of freedom then caused vibrational excitation
of the low frequency (ν = 32 cm-1) frustrated
translation mode of CO. The coupling time of the vibration to the electrons
was τe = 4.8 ps and the coupling time to the
phonons was Tlat = 3.8 ps. Essentially the
same values were found for visible and for UV excitation of the Cu, proving
that ballistic electrons did not excite the CO vibrations, contrary to many
predictions.
These were the first measurements of τe and τe,
independently, for any system. We compared our results to dozens of recently
published theoretical models. Only one (due to Tully at AT&T Bell Labs and
Head-Gordon at U.C. Berkeley) correctly predicted significant coupling of this
vibrational mode both to electrons and phonons. The coupling (damping) rates
are key parameters in understanding surface processes like sticking and
diffusion, and these benchmark measurements are very important in guiding the
modelling of such processes.
We developed the experimental methods for studying vibrational dynamics on
surfaces, performed the first benchmark measurements, and established the
coupling times and mechanisms for different adsorbate modes (i.e., the
internal CO stretch and the Cu-CO frustrated translation) on metal surfaces;
this expanded our previous studies of molecules on semiconductor and
dielectric substrates. Such measurements, built upon earlier NIST work, are
now being done elsewhere (e.g., AT&T Bell Labs, IBM, F.O.M. Amsterdam,
U. Penn, U. Chicago, Tokyo Inst. Tech.). (T.A. Germer,
R.R. Cavanagh, E.J. Heilweil, and J.C. Stephenson)
- Ultrafast Metal-Carbonyl Photochemistry. Femtosecond broadband
infrared studies of metal-carbonyl photochemistry were undertaken to identify
mechanisms and rates for CO-ligand ejection, solvation, intermediate cooling,
and fragment chemical reaction. These initial microscopic processes govern the
outcome of many industrial applications of metal-carbonyls: gasification and
liquefaction of coal, enhanced oil recovery, and initiation of polymerization
reactions. Without high time-resolution spectroscopic methods, detailed
pictures of these important reactive species have been primarily speculative
and elusive.
In the photochemistry of M(CO)6 (M = Cr, Mo, W), for
example, the dominant photoproduct following UV excitation in n-hexane at
298 K is M(CO)5(n-hexane). A significant fraction of all three
photoproducts are formed with vibrationally excited CO-stretches which relax
in approximately 160 ps; the W and Mo photoproducts are formed with
similar amounts of CO-stretch vibrational excitation, but the Cr photoproduct
is formed with less. However, experiments which examined metal dicarbonyls
such as CpCo(CO)2 (Cp = η-C5H5)
found no CO-stretch excitation in the monocarbonyl photoproduct. The reason
for these distinctions is unclear, and while we hypothesize the larger organic
ligands of the dicarbonyls may act as energy sinks, molecular modelling and
theory is needed to clarify these measurements.
Observations have also been made for UV photolysis of the dimer species
[CpFe(CO)2]2 in room temperature n-hexane. Our
sub-picosecond results determined that only the parent trans isomer is
responsible for all observable photochemical reactions. The lack of two
distinct CO-stretching bands for the CpFe(CO)2 radical (formed by
Fe-Fe bond cleavage) indicates it is a symmetric species with opposing CO
ligands. This structural assignment has never been correctly made until now.
Identification of the Cp(CO)Fe(µ-CO)2FeCp(n-hexane) solvated
species has been tentatively made along with its tetrahydrofuran (THF) analog.
We find another mechanistic pathway produces the triply-bridged species,
[CpFe(µ-CO)3FeCp], which forms and vibrationally cools in about
70 ps after terminal CO-elimination from the dimer.
Studies of the industrial agent CpCo(CO)2 (Vollhardt's catalyst) in
neat n-hexane, neat 1-hexene and solvent mixtures have revealed rich solvent
substitution chemistry under ambient thermal conditions. The
-HC=CH2 end of 1-hexene displaces initially coordinated n-hexane
and preferentially associates with the de-liganded metal center to form a
stable species. This displacement reaction was observed in real time for
moderately high concentrations of 1-hexene (0.1-2.0 Molar). Solvation
takes place at nearly the diffusion-controlled rate so that substitution
occurs for each encounter of solvent with solute.
During our examination of the above and other metal-carbonyl photochemistries,
we have discovered previously unknown reactive species and identified several
misconceptions of the mechanistic pathways leading to final products. Since
reactive transients are produced in several picoseconds in these systems,
discrepancies in spectral assignments and interpretation of complex long-time
dynamics must clearly be rationalized over all observable time-scales.
(T. Dougherty and E.J. Heilweil)
- Interactions of laser cooled atoms. Advances in laboratory
techniques for laser cooling and trapping of neutral atoms at temperatures
below 1 mK offer many new opportunities to science and technology, such as
greatly improved atomic clocks, the optical manipulation of atomic beams, and
applications of optical lattices, atom cavities and atom optics. The
interactions between laser cooled and trapped atoms exhibit new and unusual
physics which must be understood in order to make optimal use of this new
technology: for example, collisions between cooled atoms strongly affect cold
atomic sources or optical lattices at high fill factors or interfere with
precise frequency measurements in atomic clocks. Paul Julienne from the
Molecular Theory Group, in conjunction with collaborators outside NIST, have
done pioneering research in the unique physics of these collisions at
temperatures below 1 mK, supported in part by a NIST Competency Program
and in part by the Office of Naval Research. The interactions of ground state
atoms are relatively short range, and collisions of ground state atoms are
strongly dependent on quantum effects associated with the long De Broglie
wavelength and are extremely sensitive to the details of the atomic
interaction potentials. When a light field is present, excited molecular
states have a profound effect on the interactions, due to the very long range
of the resonant dipole-dipole potential. Recent experiments at NIST and
elsewhere have measured high resolution molecular spectra due to the
photoassociation of the two colliding atoms to make excited molecular
vibrational states. Such spectra permit the very accurate characterization of
the long range interactions between the atoms, both in the ground and excited
states. A knowledge of these interactions is necessary for the accurate
simulation of the properties of trapped atoms. In collaboration of
C.J. Williams of the University of Chicago, we have calculated very good
agreement with experimental spectra at NIST, including the effect of molecular
hyperfine structure. Refinements in the calculations will permit the very
accurate determination of ground and excited state potentials and accurate
simulation of the effects of interatomic interactions when the light is
detuned more than a few linewidths below atomic resonance for the cooling
transition. Cold collisions of laser excited atoms are also strongly
influenced by excited state radiative decay during the time of interaction,
and these collisions are typical of a large class of open quantum systems, in
which a quantum subsystem couples dissipatively to its environment. Such
systems must be described by a density matrix rather than a wavefunction. We
are developing new computational algorithms, in collaboration of
K. Burnett and K.A. Suominen of Oxford University, for describing
open collisions using new Monte Carlo wavefunction simulations. Normal
wavefunction evolution methods are used, but at each time step a random number
is used to determine if photon emission has occurred, and the wavefunction is
readjusted accordingly. We have used these methods to calculate the quantum
mechanical evolution of typical collisions that result in loss of atoms from
magneto-optical traps. For these cases the light is detuned up to a few
linewidths to the red of atomic resonance. With Y.B. Band of Ben Gurion
University we also have developed quantum methods based on using complex
potentials to simulate the effect of decay. This method only treats the case
of low laser power, whereas the Monte Carlo method treats the arbitrary power
case. Both the complex potential and Monte Carlo quantum methods were compared
to semiclassical models at temperatures from 10 µK to 10 mK. We show
that a simple Landau-Zener semiclassical model of the dynamics works much
better than a semiclassical optical Bloch equation treatment. Simple two state
models of the quantum process do not agree very well with measured trap loss
rates, and multichannel models that treat hyperfine structure will be
necessary for quantitative modeling of the small detuning case.
(P. Julienne and F. Mies)
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