Articles
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12/20/2003--
12/10/2003
Two Elementary Derivations of the Pure Fisher-Hartwig Determinant
We present two elementary derivations of the formula for the Toeplitz
determinant generated by a pure Fisher-Hartwig singularity.
Albrecht Boettcher
Harold Widom
09/02/2022--
08/02/2022
Unveiling the contribution of Pop III stars in primeval galaxies at redshift $\geq 6$
Detection of the first stars has remained elusive so-far but their presence
may soon be unveiled by upcoming JWST observations. Previous studies have not
investigated the entire possible range of halo masses and redshifts which may
help in their detection. Motivated by the prospects of detecting galaxies up to
$z\sim 20$ in JWST early data release, we quantify the contribution of Pop III
stars to high-redshift galaxies from $6 \leq z \leq 30$ by employing the
semi-analytical model A-SLOTH, which self-consistently models the formation of
Pop III and Pop II stars along with their feedback. Our results suggest that
the contribution of Pop III stars is the highest in low-mass halos of $\rm
10^7-10^9~M_{\odot}$. While high-mass halos $\rm \geq 10^{10}~M_{\odot}$
contain less than 1\% Pop III stars, they host galaxies with stellar masses of
$\rm 10^9~M_{\odot}$ as early as $z \sim 30$. Interestingly, the apparent
magnitude of Pop~III populations gets brighter towards higher redshift due to
the higher stellar masses, but Pop~III-dominated galaxies are too faint to be
directly detected with JWST. Our results predict JWST can detect galaxies up to
$z\sim 30$, which may help in constraining the IMF of Pop III stars and will
guide observers to discern the contribution of Pop~III stars to high-redshift
galaxies.
Shafqat Riaz
Tilman Hartwig
Muhammad A. Latif
07/16/2015--
05/01/2015
How an improved implementation of H2 self-shielding influences the formation of massive stars and black holes
High redshift quasars at z>6 have masses up to ~$10^9$ M$_\odot$. One of the
pathways to their formation includes direct collapse of gas, forming a
supermassive star, precursor of the black hole seed. The conditions for direct
collapse are more easily achievable in metal-free haloes, where atomic hydrogen
cooling operates and molecular hydrogen (H2) formation is inhibited by a strong
external UV flux. Above a certain value of UV flux (J_crit), the gas in a halo
collapses isothermally at ~$10^4$ K and provides the conditions for
supermassive star formation. However, H2 can self-shield, reducing the effect
of photodissociation. So far, most numerical studies used the local Jeans
length to calculate the column densities for self-shielding. We implement an
improved method for the determination of column densities in 3D simulations and
analyse its effect on the value of J_crit. This new method captures the gas
geometry and velocity field and enables us to properly determine the
direction-dependent self-shielding factor of H2 against photodissociating
radiation. We find a value of J_crit that is a factor of two smaller than with
the Jeans approach (~2000 J_21 vs. ~4000 J_21). The main reason for this
difference is the strong directional dependence of the H2 column density. With
this lower value of J_crit, the number of haloes exposed to a flux >J_crit is
larger by more than an order of magnitude compared to previous studies. This
may translate into a similar enhancement in the predicted number density of
black hole seeds.
Tilman Hartwig
Simon C. O. Glover
Ralf S. Klessen
Muhammad A. Latif
Marta Volonteri
11/20/2020--
10/12/2020
An accelerator facility for intermediate energy proton irradiation and testing of nuclear materials
The bulk irradiation of materials with 10-30 MeV protons promises to advance
the study of radiation damage for fission and fusion power plants. Intermediate
energy proton beams can now be dedicated to materials irradiation within
university-scale laboratories. This paper describes the first such facility,
with an Ionetix ION-12SC cyclotron producing 12 MeV proton beams. Samples are
mm-scale tensile specimens with thicknesses up to 300 um, mounted to a cooled
beam target with control over temperature. A specialized tensile tester for
radioactive specimens at high temperature (500+ {\deg}C) and/or vacuum
represents the conditions in fission and fusion systems, while a digital image
correlation system remotely measures strain. Overall, the facility provides
university-scale irradiation and testing capability with intermediate energy
protons to complement traditional in-core fission reactor and micro-scale ion
irradiation. This facility demonstrates that bulk proton irradiation is a
scalable and effective approach for nuclear materials research, down-selection,
and qualification.
S. J. Jepeal
A. Danagoulian
L. A. Kesler
D. A. Korsun
H. Y. Lee
N. Schwartz
B. N. Sorbom
E. Velez Lopez
Z. S. Hartwig
03/02/2020--
03/02/2020
Grothendieck rings of towers of twisted generalized Weyl algebras
Twisted generalized Weyl algebras (TGWAs) $A(R,\sigma,t)$ are defined over a
base ring $R$ by parameters $\sigma$ and $t$, where $\sigma$ is an $n$-tuple of
automorphisms, and $t$ is an $n$-tuple of elements in the center of $R$. We
show that, for fixed $R$ and $\sigma$, there is a natural algebra map
$A(R,\sigma,tt')\to A(R,\sigma,t)\otimes_R A(R,\sigma,t')$. This gives a tensor
product operation on modules, inducing a ring structure on the direct sum (over
all $t$) of the Grothendieck groups of the categories of weight modules for
$A(R,\sigma,t)$. We give presentations of these Grothendieck rings for $n=1,2$,
when $R=\mathbb{C}[z]$. As a consequence, for $n=1$, any indecomposable module
for a TGWA can be written as a tensor product of indecomposable modules over
the usual Weyl algebra. In particular, any finite-dimensional simple module
over $\mathfrak{sl}_2$ is a tensor product of two Weyl algebra modules.
Jonas T. Hartwig
Daniele Rosso
12/12/2018--
11/21/2018
On the Detection of Supermassive Primordial Stars
The collapse of supermassive primordial stars in hot, atomically-cooled halos
may have given birth to the first quasars at $z \sim$ 15 - 20. Recent numerical
simulations of these rapidly accreting stars reveal that they are cool, red
hypergiants shrouded by dense envelopes of pristine atomically-cooled gas at
6,000 - 8,000 K, with luminosities $L$ $\gtrsim$ 10$^{10}$ L$_{\odot}$. Could
such luminous but cool objects be detected as the first stage of quasar
formation in future near infrared (NIR) surveys? We have now calculated the
spectra of supermassive primordial stars in their birth envelopes with the
Cloudy code. We find that some of these stars will be visible to JWST at $z
\lesssim$ 20 and that with modest gravitational lensing Euclid and WFIRST could
detect them out to $z \sim$ 10 - 12. Rather than obscuring the star, its
accretion envelope enhances its visibility in the NIR today by reprocessing its
short-wavelength flux into photons that are just redward of the Lyman limit in
the rest frame of the star.
Marco Surace
Daniel J. Whalen
Tilman Hartwig
Erik Zackrisson
S. C. O. Glover
Samuel Patrick
Tyrone E. Woods
Alexander Heger
Lionel Haemmerlé
01/07/2004--
01/07/2004
Applications and generalizations of Fisher-Hartwig asymptotics
Fisher-Hartwig asymptotics refers to the large $n$ form of a class of
Toeplitz determinants with singular generating functions. This class of
Toeplitz determinants occurs in the study of the spin-spin correlations for the
two-dimensional Ising model, and the ground state density matrix of the
impenetrable Bose gas, amongst other problems in mathematical physics. We give
a new application of the original Fisher-Hartwig formula to the asymptotic
decay of the Ising correlations above $T_c$, while the study of the Bose gas
density matrix leads us to generalize the Fisher-Hartwig formula to the
asymptotic form of random matrix averages over the classical groups and the
Gaussian and Laguerre unitary matrix ensembles. Another viewpoint of our
generalizations is that they extend to Hankel determinants the Fisher-Hartwig
asymptotic form known for Toeplitz determinants.
P. J. Forrester
N. E. Frankel
08/07/2024--
08/02/2023
Eigenvectors of Toeplitz matrices from Fisher-Hartwig symbols with greater than, or equal to, one singularity
Asymptotically, we analytically derive the form of eigenvectors for two
Fisher-Hartwig symbols besides those which were previously investigated in a
$2016$ work due to Movassagh and Kadanoff, in which the authors characterized
the eigenpairs of Toeplitz matrices generated by Fisher-Hartwig symbols with
one singularity. To perform such computations, we extend their methods which
consists of formulating an eigenvalue problem, obtained by a Wiener-Hopf
method, from which a suitable winding number is defined for passing to Fourier
space, and introducing a factorization dependent upon the winding number, for
other Fisher-Hartwig symbols which have previously been defined in the
literature. Following the computations required for the proof after obtaining
the asymptotic approximation of the eigenvectors, we provide a table from which
eigenvalues of one Fisher-Hartwig symbol for different complex valued functions
$b$ can be inferred.
Pete Rigas
02/01/2021--
04/08/2020
Radio Power from a Direct-Collapse Black Hole in CR7
The leading contenders for the seeds of the first quasars are direct collapse
black holes (DCBHs) formed during catastrophic baryon collapse in
atomically-cooled halos at $z \sim$ 20. The discovery of the Ly$\alpha$ emitter
CR7 at $z =$ 6.6 was initially held to be the first detection of a DCBH,
although this interpretation has since been challenged on the grounds of
Spitzer IRAC and Very Large Telescope X-Shooter data. Here we determine if
radio flux from a DCBH in CR7 could be detected and discriminated from
competing sources of radio emission in the halo such as young supernovae and H
II regions. We find that a DCBH would emit a flux of 10 - 200 nJy at 1.0 GHz,
far greater than the sub-nJy signal expected for young supernovae but on par
with continuum emission from star-forming regions. However, radio emission from
a DCBH in CR7 could be distinguished from free-free emission from H II regions
by its spectral evolution with frequency and could be detected by the Square
Kilometer Array in the coming decade.
Daniel J. Whalen
Mar Mezcua
Avery Meiksin
Tilman Hartwig
Muhammad A. Latif
07/16/2019--
03/28/2019
On the Detection of Supermassive Primordial Stars. II. Blue Supergiants
Supermassive primordial stars in hot, atomically-cooling haloes at $z \sim$
15 - 20 may have given birth to the first quasars in the universe. Most
simulations of these rapidly accreting stars suggest that they are red, cool
hypergiants, but more recent models indicate that some may have been bluer and
hotter, with surface temperatures of 20,000 - 40,000 K. These stars have
spectral features that are quite distinct from those of cooler stars and may
have different detection limits in the near infrared (NIR) today. Here, we
present spectra and AB magnitudes for hot, blue supermassive primordial stars
calculated with the TLUSTY and CLOUDY codes. We find that photometric
detections of these stars by the James Webb Space Telescope (JWST) will be
limited to $z \lesssim$ 10 - 12, lower redshifts than those at which red stars
can be found, because of quenching by their accretion envelopes. With moderate
gravitational lensing, Euclid and the Wide-Field Infrared Space Telescope
(WFIRST) could detect blue supermassive stars out to similar redshifts in
wide-field surveys.
Marco Surace
Erik Zackrisson
Daniel J. Whalen
Tilman Hartwig
S. C. O. Glover
Tyrone E. Woods
Alexander Heger
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