Articles
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05/31/2023--
05/31/2023
Optoacoustic cooling of traveling hypersound waves
We experimentally demonstrate optoacoustic cooling via stimulated
Brillouin-Mandelstam scattering in a 50 cm-long tapered photonic crystal fiber.
For a 7.38 GHz acoustic mode, a cooling rate of 219 K from room temperature has
been achieved. As anti-Stokes and Stokes Brillouin processes naturally break
the symmetry of phonon cooling and heating, resolved sideband schemes are not
necessary. The experiments pave the way to explore the classical to quantum
transition for macroscopic objects and could enable new quantum technologies in
terms of storage and repeater schemes.
Laura Blázquez Martínez
Philipp Wiedemann
Changlong Zhu
Andreas Geilen
Birgit Stiller
09/25/2025--
09/25/2025
Strictly zero-dimensional biframes and Raney extensions
Raney extensions and strictly zero-dimensional biframes both faithfully
extend the dual of the category of $T_0$ spaces. We use tools from pointfree
topology to look at the connection between the two. Raney extensions may be
equivalently described as pairs $(L,\mathcal{F})$ where $L$ is a frame and
$\mathcal{F}\subseteq \mathcal{S}_{o}(L)$ a subcolocale containing all open
sublocales. Here, $\mathcal{S}_o(L)$ is the collection of all intersections of
open sublocales of $L$. Similarly, a strictly zero-dimensional biframe is a
pair $(L,\mathcal{D})$ where $\mathcal{D}\subseteq \mathcal{S}(L)$ is a codense
subcolocale. We show that there is an adjunction between certain subcolocales
of $\mathcal{S}_o(L)$ and codense subcolocales of $\mathcal{S}(L)$. We show
that the adjunction maximally restricts to an order-isomorphism between the
subcolocales of $\mathcal{S}_o(L)$ where the joins of open sublocales
distribute over binary meets, which we call the proper subcolocales, and what
we call the essential codense subcolocales. As an application of our main
result, we establish a bijection between proper Raney extensions and the
strictly zero-dimensional biframes $(L_1,L_2,L)$ such that $L$ is an essential
extension of $L_2$ in the category of frames. We show that this correspondence
cannot be made functorial in the obvious way, as a frame morphism $f:L\to M$
may lift to a map $f:(L,\mathcal{F})\to (L,\mathcal{G})$ of Raney extensions
without lifting to a map between the associated strictly zero-dimensional
biframes.
Anna Laura Suarez
03/06/2025--
03/06/2025
Innovating Bolometers' Mounting: A Gravity-Based Approach
Cryogenic calorimeters, also known as bolometers, are among the leading
technologies for searching for rare events. The CUPID experiment is exploiting
this technology to deploy a tonne-scale detector to search for neutrinoless
double-beta decay of $^{100}$Mo. The CUPID collaboration proposed an innovative
approach to assembling bolometers in a stacked configuration, held in position
solely by gravity. This gravity-based assembly method is unprecedented in the
field of bolometers and offers several advantages, including relaxed mechanical
tolerances and simplified construction. To assess and optimize its performance,
we constructed a medium-scale prototype hosting 28 Li$_2$MoO$_4$ crystals and
30 Ge light detectors, both operated as cryogenic calorimeters at the
Laboratori Nazionali del Gran Sasso (Italy). Despite an unexpected excess of
noise in the light detectors, the results of this test proved (i) a thermal
stability better than $\pm$0.5 mK at 10 mK, (ii) a good energy resolution of
Li$_2$MoO$_4$ bolometers, (6.6 $\pm$ 2.2) keV FWHM at 2615 keV, and (iii) a
Li$_2$MoO$_4$ light yield measured by the closest light detector of 0.36
keV/MeV, sufficient to guarantee the particle identification requested by
CUPID.
The CUPID Collaboration
K. Alfonso
A. Armatol
C. Augier
F. T. Avignone III
O. Azzolini
A. S. Barabash
G. Bari
A. Barresi
D. Baudin
F. Bellini
G. Benato
L. Benussi
V. Berest
M. Beretta
M. Bettelli
M. Biassoni
J. Billard
F. Boffelli
V. Boldrini
E. D. Brandani
C. Brofferio
C. Bucci
M. Buchynska
J. Camilleri
A. Campani
J. Cao
C. Capelli
S. Capelli
V. Caracciolo
L. Cardani
P. Carniti
N. Casali
E. Celi
C. Chang
M. Chapellier
H. Chen
D. Chiesa
D. Cintas
M. Clemenza
I. Colantoni
S. Copello
O. Cremonesi
R. J. Creswick
A. D'Addabbo
I. Dafinei
F. A. Danevich
F. De Dominicis
M. De Jesus
P. de Marcillac
S. Dell'Oro
S. Di Domizio
S. Di Lorenzo
V. Dompè
A. Drobizhev
L. Dumoulin
G. Fantini
M. El Idrissi
M. Faverzani
E. Ferri
F. Ferri
F. Ferroni
E. Figueroa-Feliciano
J. Formaggio
A. Franceschi
S. Fu
B. K. Fujikawa
J. Gascon
S. Ghislandi
A. Giachero
M. Girola
L. Gironi
A. Giuliani
P. Gorla
C. Gotti
C. Grant
P. Gras
P. V. Guillaumon
T. D. Gutierrez
K. Han
E. V. Hansen
K. M. Heeger
D. L. Helis
H. Z. Huang
M. T. Hurst
L. Imbert
A. Juillard
G. Karapetrov
G. Keppel
H. Khalife
V. V. Kobychev
Yu. G. Kolomensky
R. Kowalski
H. Lattaud
M. Lefevre
M. Lisovenko
R. Liu
Y. Liu
P. Loaiza
L. Ma
F. Mancarella
N. Manenti
A. Mariani
L. Marini
S. Marnieros
M. Martinez
R. H. Maruyama
Ph. Mas
D. Mayer
G. Mazzitelli
E. Mazzola
Y. Mei
M. N. Moore
S. Morganti
T. Napolitano
M. Nastasi
J. Nikkel
C. Nones
E. B. Norman
V. Novosad
I. Nutini
T. O'Donnell
E. Olivieri
M. Olmi
B. T. Oregui
S. Pagan
M. Pageot
L. Pagnanini
D. Pasciuto
L. Pattavina
M. Pavan
Ò. Penek
H. Peng
G. Pessina
V. Pettinacci
C. Pira
S. Pirro
O. Pochon
D. V. Poda
T. Polakovic
O. G. Polischuk
E. G. Pottebaum
S. Pozzi
E. Previtali
A. Puiu
S. Puranam
S. Quitadamo
A. Rappoldi
G. L. Raselli
A. Ressa
R. Rizzoli
C. Rosenfeld
P. Rosier
M. Rossella
J. A. Scarpaci
B. Schmidt
R. Serino
A. Shaikina
K. Shang
V. Sharma
V. N. Shlegel
V. Singh
M. Sisti
P. Slocum
D. Speller
P. T. Surukuchi
L. Taffarello
S. Tomassini
C. Tomei
A. Torres
J. A. Torres
D. Tozzi
V. I. Tretyak
D. Trotta
M. Velazquez
K. J. Vetter
S. L. Wagaarachchi
G. Wang
L. Wang
R. Wang
B. Welliver
J. Wilson
K. Wilson
L. A. Winslow
F. Xie
M. Xue
J. Yang
V. Yefremenko
V. I. Umatov
M. M. Zarytskyy
T. Zhu
A. Zolotarova
S. Zucchelli
02/08/2011--
02/08/2011
Complex connections with trivial holonomy
Given an almost complex manifold (M, J), we study complex connections with
trivial holonomy and such that the corresponding torsion is either of type
(2,0) or of type (1,1) with respect to J. Such connections arise naturally when
considering Lie groups, and quotients by discrete subgroups, equipped with
bi-invariant and abelian complex structures.
A. Andrada
M. L. Barberis
I. G. Dotti
10/13/2014--
10/13/2014
Binary orbits as the driver of gamma-ray emission and mass ejection in classical novae
Classical novae are the most common astrophysical thermonuclear explosions,
occurring on the surfaces of white dwarf stars accreting gas from companions in
binary star systems. Novae typically expel ~10^(-4) solar masses of material at
velocities exceeding 1,000 kilometres per second. However, the mechanism of
mass ejection in novae is poorly understood, and could be dominated by the
impulsive flash of thermonuclear energy, prolonged optically thick winds, or
binary interaction with the nova envelope. Classical novae are now routinely
detected in gigaelectronvolt gamma-ray wavelengths, suggesting that
relativistic particles are accelerated by strong shocks in the ejecta. Here we
report high-resolution radio imaging of the gamma-ray-emitting nova V959 Mon.
We find that its ejecta were shaped by the motion of the binary system: some
gas was expelled rapidly along the poles as a wind from the white dwarf, while
denser material drifted out along the equatorial plane, propelled by orbital
motion. At the interface between the equatorial and polar regions, we observe
synchrotron emission indicative of shocks and relativistic particle
acceleration, thereby pinpointing the location of gamma-ray production. Binary
shaping of the nova ejecta and associated internal shocks are expected to be
widespread among novae, explaining why many novae are gamma-ray emitters.
Laura Chomiuk
Justin D. Linford
Jun Yang
T. J. O'Brien
Zsolt Paragi
Amy J. Mioduszewski
R. J. Beswick
C. C. Cheung
Koji Mukai
Thomas Nelson
Valerio A. R. M. Ribeiro
Michael P. Rupen
J. L. Sokoloski
Jennifer Weston
Yong Zheng
Michael F. Bode
Stewart Eyres
Nirupam Roy
Gregory B. Taylor
07/31/2024--
07/31/2024
In-plane dielectric constant and conductivity of confined water
Water is essential for almost every aspect of life on our planet and,
unsurprisingly, its properties have been studied in great detail. However,
disproportionately little remains known about the electrical properties of
interfacial and strongly confined water where its structure deviates from that
of bulk water, becoming distinctly layered. The structural change is expected
to affect water's conductivity and particularly its polarizability, which in
turn modifies intermolecular forces that play a crucial role in many physical
and chemical processes. Here we use scanning dielectric microscopy to probe the
in-plane electrical properties of water confined between atomically flat
surfaces separated by distances down to 1 nm. For confinement exceeding a few
nm, water exhibits an in-plane dielectric constant close to that of bulk water
and its proton conductivity is notably enhanced, gradually increasing with
decreasing water thickness. This trend abruptly changes when the confined water
becomes only a few molecules thick. Its in-plane dielectric constant reaches
giant, ferroelectric-like values of about 1,000 whereas the conductivity peaks
at a few S/m, close to values characteristic of superionic liquids. We
attribute the enhancement to strongly disordered hydrogen bonding induced by
the few-layer confinement, which facilitates both easier in-plane polarization
of molecular dipoles and faster proton exchange. This insight into the
electrical properties of nanoconfined water is important for understanding many
phenomena that occur at aqueous interfaces and in nanoscale pores.
R. Wang
M. Souilamas
A. Esfandiar
R. Fabregas
S. Benaglia
H. Nevison-Andrews
Q. Yang
J. Normansell
P. Ares
G. Ferrari
A. Principi
A. K. Geim
L. Fumagalli
04/17/2018--
04/17/2018
ALMA observations of polarization from dust scattering in the IM Lup protoplanetary disk
We present 870 $\mu$m ALMA observations of polarized dust emission toward the
Class II protoplanetary disk IM Lup. We find that the orientation of the
polarized emission is along the minor axis of the disk, and that the value of
the polarization fraction increases steadily toward the center of the disk,
reaching a peak value of ~1.1%. All of these characteristics are consistent
with models of self-scattering of submillimeter-wave emission from an optically
thin inclined disk. The distribution of the polarization position angles across
the disk reveals that while the average orientation is along the minor axis,
the polarization orientations show a significant spread in angles; this can
also be explained by models of pure scattering. We compare the polarization
with that of the Class I/II source HL Tau. A comparison of cuts of the
polarization fraction across the major and minor axes of both sources reveals
that IM Lup has a substantially higher polarization fraction than HL Tau toward
the center of the disk. This enhanced polarization fraction could be due a
number of factors, including higher optical depth in HL Tau, or scattering by
larger dust grains in the more evolved IM Lup disk. However, models yield
similar maximum grain sizes for both HL Tau (72 $\mu$m) and IM Lup (61 $\mu$m,
this work). This reveals continued tension between grain-size estimates from
scattering models and from models of the dust emission spectrum, which find
that the bulk of the (unpolarized) emission in disks is most likely due to
millimeter (or even centimeter) sized grains.
Charles L. H. Hull
Haifeng Yang
Zhi-Yun Li
Akimasa Kataoka
Ian W. Stephens
Sean Andrews
Xuening Bai
L. Ilsedore Cleeves
A. Meredith Hughes
Leslie Looney
Laura M. Pérez
David Wilner
03/18/2005--
03/18/2005
Yang-Yang Anomalies and Coexistence Diameters: Simulation of Asymmetric Fluids
A general method for estimating the Yang-Yang ratio, ${\cal R}_{\mu}$, and
the coexistence-curve diameter of a model fluid via Monte Carlo simulations is
presented on the basis of data for a hard-core square-well (HCSW) fluid and the
restricted primitive model (RPM) electrolyte. The isothermal minima of
$Q_{L}\equiv< m^{2}>^{2}_{L}/< m^{4}>_{L}$ are evaluated at $T_{c}$ in an
$L\times L\times L$ box where $m = \rho - <\rho>_{L}$ is the density
fluctuation. The ``complete'' finite-size scaling theory for the
$Q_{\scriptsize min}^{\pm}(T_{c};L)$ incorporates pressure mixing in the
scaling fields, thereby allowing for a Yang-Yang anomaly.
Young C. Kim
04/24/2023--
01/10/2023
Pseudopotential Bethe-Salpeter calculations for shallow-core x-ray absorption near-edge structures: excitonic effects in Al2O3
We present an ab initio description of optical and shallow-core x-ray
absorption spectroscopies in a unified formalism based on the pseudopotential
plane-wave method at the level of the Bethe-Salpeter equation (BSE) within
Green's functions theory. We show that norm-conserving pseudopotentials are
reliable and accurate not only for valence, but also for semicore electron
excitations. In order to validate our approach, we compare BSE absorption
spectra obtained with two different codes: the pseudopotential-based code EXC
and the all-electron full-potential code Exciting. We take corundum
$\alpha$-Al$_2$O$_3$ as an example, being a prototypical material that presents
strong electron-hole interactions for both valence and core electron
excitations. We analyze in detail the optical absorption spectrum as well as
the Al L$_1$ and L$_{2,3}$ edges in terms of anisotropy, crystal local fields,
interference and excitonic effects. We perform a thorough inspection of the
origin and localization of the lowest-energy excitons, and conclude
highlighting the purely electronic character off the pre-edge of L$_1$ and the
dichroic nature of the optical and L$_{23}$ spectra.
M. Laura Urquiza
Matteo Gatti
Francesco Sottile
04/22/2025--
05/05/2024
Raney extensions: a pointfree theory of T_0 spaces based on canonical extension
We introduce a pointfree version of Raney duality. Our objects are
\emph{Raney extensions} of frames, pairs $(L,C)$ where $C$ is a coframe and
$L\subseteq C$ is a subframe that meet-generates it and whose embedding
preserves strongly exact meets. We show that there is a dual adjunction between
$\mathbf{Raney}$ and $\mathbf{Top}$, with all $T_0$ spaces as fixpoints,
assigning to a space $X$ the pair $(\Omega(X),\mathcal{U}(X))$, with
$\mathcal{U}(X)$ are the intersections of open sets. We show that for every
Raney extension $(L,C)$ there are subcolocale inclusions
$\mathcal{S}_c(L)^{op}\subseteq C\subseteq \mathcal{S}_o(L)$ where these are
the opposite of the frame of joins of closed sublocales and the coframe of
intersections of open sublocales. We thus exhibit a symmetry between these two
well-studied structures in pointfree topology. The spectra of these are,
respectively, the classical spectrum $\mathsf{pt}(L)$ of the underlying frame
and its $T_D$ spectrum $\mathsf{pt}_D(L)$. This confirms the view advanced in
\cite{banaschewskitd} that sobriety and the $T_D$ property are mirror images of
each other, and suggests that the symmetry above is a pointfree view of it. All
Raney extensions satisfy some variation of the properties \emph{density} and
\emph{compactness} from the theory of canonical extensions. We characterize
sobriety, the $T_1$, and the $T_D$ axioms in terms of density and compactness
of $(\Omega(X),\mathcal{U}(X))$. We characterize frame morphisms $f:L\to M$
that extend to Raney morphisms $\overline{f}:(L,C)\to (M,D)$. We use this
result to exhibit the existence of various free and cofree constructions. We
use Raney extensions to give a new perspective on canonical extension
generalized to frames as well as $T_D$ duality.
Anna Laura Suarez
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