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Atmospheric processes affecting the separation of volcanic ash and SO2 in volcanic eruptions: inferences from the May 2011 Grímsvötn eruption
The separation of volcanic ash and sulfur dioxide
(SO2) gas is sometimes observed during volcanic eruptions.
The exact conditions under which separation occurs are not
fully understood but the phenomenon is of importance because
of the effects volcanic emissions have on aviation, on
the environment, and on the earth’s radiation balance. The
eruption of Grímsvötn, a subglacial volcano under the Vatnajökull
glacier in Iceland during 21–28 May 2011 produced
one of the most spectacular examples of ash and SO2 separation,
which led to errors in the forecasting of ash in the
atmosphere over northern Europe. Satellite data from several
sources coupled with meteorological wind data and photographic
evidence suggest that the eruption column was unable
to sustain itself, resulting in a large deposition of ash,
which left a low-level ash-rich atmospheric plume moving
southwards and then eastwards towards the southern Scandinavian
coast and a high-level predominantly SO2 plume travelling
northwards and then spreading eastwards and westwards.
Here we provide observational and modelling perspectives
on the separation of ash and SO2 and present quantitative
estimates of the masses of ash and SO2 that erupted,
the directions of transport, and the likely impacts. We hypothesise
that a partial column collapse or “sloughing” fed
with ash from pyroclastic density currents (PDCs) occurred
during the early stage of the eruption, leading to an ash-laden
gravity intrusion that was swept southwards, separated from
the main column. Our model suggests that water-mediated
aggregation caused enhanced ash removal because of the
plentiful supply of source water from melted glacial ice and
from entrained atmospheric water. The analysis also suggests
that ash and SO2 should be treated with separate source
terms, leading to improvements in forecasting the movement
of both types of emissions
An efficient quantum algorithm for the hidden subgroup problem in extraspecial groups
Extraspecial groups form a remarkable subclass of p-groups. They are also
present in quantum information theory, in particular in quantum error
correction. We give here a polynomial time quantum algorithm for finding hidden
subgroups in extraspecial groups. Our approach is quite different from the
recent algorithms presented in [17] and [2] for the Heisenberg group, the
extraspecial p-group of size p3 and exponent p. Exploiting certain nice
automorphisms of the extraspecial groups we define specific group actions which
are used to reduce the problem to hidden subgroup instances in abelian groups
that can be dealt with directly.Comment: 10 page
Eludicating Heavy‐Atom‐Tunneling Kinetics in the Cope Rearrangement of Semibullvalene
In this work, we characterize the temperature dependence of kinetic properties in heavy atom tunneling reactions by means of molecular dynamics simulations, including nuclear quantum effects (NQEs) via Path Integral theory. To this end, we consider the prototypical Cope rearrangement of semibullvalene. The reaction was studied in the 25-300 K temperature range observing that the inclusion of NQEs modifies the temperature behavior of both free energy barriers and dynamical recrossing factors with respect to classical dynamics. Notably, while in classical simulations the activation free energy shows a very weak temperature dependence, it becomes strongly dependent on temperature when NQEs are included. This temperature behavior shows a transition from a regime where the quantum effects are limited and can mainly be traced back to zero point energy, to a low temperature regime where tunneling plays a dominant role. In this regime, the free energy curve tunnels below the potential energy barrier along the reaction coordinate, allowing much faster reaction rates. Finally, the temperature dependence of the rate constants obtained from molecular dynamics simulations was compared with available experimental data and with semi-classical transition state theory calculations, showing comparable behaviors and similar transition temperatures from thermal to (deep) tunneling regime.When heavy atom tunneling regime is attained, the free energy reaction profile tunnels below the potential energy profile due to the inclusion of nuclear quantum effects. Ring Polymer Molecular Dynamics simulations are able to provide free energy and rate constants describing this phenomenon. Here we use the Cope's rearrangement of semibullvalene as prototypical reaction. imag
Semiconductor quantum plasmonics
We investigate the frontier between classical and quantum plasmonics in
highly doped semiconductor layers. The choice of a semiconductor platform
instead of metals for our study permits an accurate description of the quantum
nature of the electrons constituting the plasmonic response, which is a crucial
requirement for quantum plasmonics. Our quantum model allows us to calculate
the collective plasmonic resonances from the electronic states determined by an
arbitrary one-dimensional potential. Our approach is corroborated with
experimental spectra, realized on a single quantum well, in which higher order
longitudinal plasmonic modes are present. We demonstrate that their energy
depends on the plasma energy, as it is also the case for metals, but also on
the size confinement of the constituent electrons. This work opens the way
towards the applicability of quantum engineering techniques for semiconductor
plasmonics
When Quantum Fluctuations Meet Structural Instabilities: The Isotope- and Pressure-Induced Phase Transition in the Quantum Paraelectric NaOH
Anhydrous sodium hydroxide, a common and structurally simple compound, shows
spectacular isotope effects: NaOD undergoes a first-order transition, which is
absent in NaOH. By combining ab initio electronic structure calculations with
path integrals, we show that NaOH is an unusual example of a quantum
paraelectric: zero-point quantum fluctuations stretch the weak hydrogen bonds
(HBs) until they become unstable and break. By strengthening HBs via isotope
substitution or applied pressure, the system can be driven down to a
broken-symmetry antiferroelectric phase. We also provide a simple quantitative
criterion for HB breaking in layered crystals and show that nuclear quantum
effects are crucial in paraelectric to ferroelectric transitions in
hydrogen-bonded hydroxides
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