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"Mathematical physics"
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A certain uncertainty : nature's random ways
\"Based around a series of real-life scenarios, this engaging introduction to statistical reasoning will teach you how to apply powerful statistical, qualitative and probabilistic tools in a technical context. From analysis of electricity bills, baseball statistics, and stock market fluctuations, through to profound questions about physics of fermions and bosons, decaying nuclei, and climate change, each chapter introduces relevant physical, statistical and mathematical principles step-by-step in an engaging narrative style, helping to develop practical proficiency in the use of probability and statistical reasoning. With numerous illustrations making it easy to focus on the most important information, this insightful book is perfect for students and researchers of any discipline interested in the interwoven tapestry of probability, statistics, and physics\"-- Provided by publisher.
Symmetry TFTs from String Theory
by
Bonetti, Federico
,
Hosseini, Saghar S.
,
Apruzzi, Fabio
in
Classical and Quantum Gravitation
,
Complex Systems
,
Mathematical and Computational Physics
2023
We determine the
d
+
1
dimensional topological field theory, which encodes the higher-form symmetries and their ’t Hooft anomalies for
d
-dimensional QFTs obtained by compactifying M-theory on a non-compact space
X
. The resulting theory, which we call the Symmetry TFT, or SymTFT for short, is derived by reducing the topological sector of 11d supergravity on the boundary
∂
X
of the space
X
. Central to this endeavour is a reformulation of supergravity in terms of differential cohomology, which allows the inclusion of torsion in cohomology of the space
∂
X
, which in turn gives rise to the background fields for discrete (in particular higher-form) symmetries. We apply this framework to 7d super-Yang Mills, where
X
=
C
2
/
Γ
ADE
, as well as the Sasaki–Einstein links of Calabi–Yau three-fold cones that give rise to 5d superconformal field theories. This M-theory analysis is complemented with a IIB 5-brane web approach, where we derive the SymTFTs from the asymptotics of the 5-brane webs. Our methods apply to both Lagrangian and non-Lagrangian theories, and allow for many generalisations.
Journal Article
Trick or truth? : the mysterious connection between physics and mathematics
The prize-winning essays in this book address the fascinating but sometimes uncomfortable relationship between physics and mathematics. Is mathematics merely another natural science? Or is it the result of human creativity? Does physics simply wear mathematics like a costume, or is math the lifeblood of physical reality? The nineteen wide-ranging, highly imaginative and often entertaining essays are enhanced versions of the prize-winning entries to the FQXi essay competition âءءTrick or Truthâءء, which attracted over 200 submissions. The Foundational Questions Institute, FQXi, catalyzes, supports, and disseminates research on questions at the foundations of physics and cosmology, particularly new frontiers and innovative ideas integral to a deep understanding of reality, but unlikely to be supported by conventional funding sources.
Higher Gauging and Non-invertible Condensation Defects
by
Shao, Shu-Heng
,
Roumpedakis, Konstantinos
,
Seifnashri, Sahand
in
Classical and Quantum Gravitation
,
Complex Systems
,
Mathematical and Computational Physics
2023
We discuss invertible and non-invertible topological condensation defects arising from gauging a discrete higher-form symmetry on a higher codimensional manifold in spacetime, which we define as higher gauging. A
q
-form symmetry is called
p
-gaugeable if it can be gauged on a codimension-
p
manifold in spacetime. We focus on 1-gaugeable 1-form symmetries in general 2+1d QFT, and gauge them on a surface in spacetime. The universal fusion rules of the resulting invertible and non-invertible condensation surfaces are determined. In the special case of 2+1d TQFT, every (invertible and non-invertible) 0-form global symmetry, including the
Z
2
electromagnetic symmetry of the
Z
2
gauge theory, is realized from higher gauging. We further compute the fusion rules between the surfaces, the bulk lines, and lines that only live on the surfaces, determining some of the most basic data for the underlying fusion 2-category. We emphasize that the fusion “coefficients” in these non-invertible fusion rules are generally not numbers, but rather 1+1d TQFTs. Finally, we discuss examples of non-invertible symmetries in non-topological 2+1d QFTs such as the free
U
(1) Maxwell theory and QED.
Journal Article
Symmetry TFTs for Non-invertible Defects
by
Zheng, Yunqin
,
Ohmori, Kantaro
,
Kaidi, Justin
in
Boundary conditions
,
Classical and Quantum Gravitation
,
Complex Systems
2023
Given any symmetry acting on a
d
-dimensional quantum field theory, there is an associated
(
d
+
1
)
-dimensional topological field theory known as the Symmetry TFT (SymTFT). The SymTFT is useful for decoupling the universal quantities of quantum field theories, such as their generalized global symmetries and ’t Hooft anomalies, from their dynamics. In this work, we explore the SymTFT for theories with Kramers-Wannier-like duality symmetry in both
(
1
+
1
)
d and
(
3
+
1
)
d quantum field theories. After constructing the SymTFT, we use it to reproduce the non-invertible fusion rules of duality defects, and along the way we generalize the concept of duality defects to
higher
duality defects. We also apply the SymTFT to the problem of distinguishing intrinsically versus non-intrinsically non-invertible duality defects in
(
1
+
1
)
d.
Journal Article
Non-invertible Condensation, Duality, and Triality Defects in 3+1 Dimensions
by
Córdova, Clay
,
Hsin, Po-Shen
,
Lam, Ho Tat
in
Classical and Quantum Gravitation
,
Complex Systems
,
Mathematical and Computational Physics
2023
We discuss a variety of codimension-one, non-invertible topological defects in general 3+1d QFTs with a discrete one-form global symmetry. These include condensation defects from higher gauging of the one-form symmetries on a codimension-one manifold, each labeled by a discrete torsion class, and duality and triality defects from gauging in half of spacetime. The universal fusion rules between these non-invertible topological defects and the one-form symmetry surface defects are determined. Interestingly, the fusion coefficients are generally not numbers, but 2+1d TQFTs, such as invertible SPT phases,
Z
N
gauge theories, and
U
(
1
)
N
Chern-Simons theories. The associativity of these algebras over TQFT coefficients relies on nontrivial facts about 2+1d TQFTs. We further prove that some of these non-invertible symmetries are intrinsically incompatible with a trivially gapped phase, leading to nontrivial constraints on renormalization group flows. Duality and triality defects are realized in many familiar gauge theories, including free Maxwell theory, non-abelian gauge theories with orthogonal gauge groups,
N
=
1
,
and
N
=
4
super Yang-Mills theories.
Journal Article
Approximate Unitary t-Designs by Short Random Quantum Circuits Using Nearest-Neighbor and Long-Range Gates
by
Mehraban, Saeed
,
Harrow, Aram W.
in
Classical and Quantum Gravitation
,
Complex Systems
,
Mathematical and Computational Physics
2023
We prove that
poly
(
t
)
·
n
1
/
D
-depth local random quantum circuits with two qudit nearest-neighbor gates on a
D
-dimensional lattice with
n
qudits are approximate
t
-designs in various measures. These include the “monomial” measure, meaning that the monomials of a random circuit from this family have expectation close to the value that would result from the Haar measure. Previously, the best bound was
poly
(
t
)
·
n
due to Brandão–Harrow–Horodecki (Commun Math Phys 346(2):397–434, 2016) for
D
=
1
. We also improve the “scrambling” and “decoupling” bounds for spatially local random circuits due to Brown and Fawzi (Scrambling speed of random quantum circuits, 2012). One consequence of our result is that assuming the polynomial hierarchy (
PH
) is infinite and that certain counting problems are
#
P
-hard “on average”, sampling within total variation distance from these circuits is hard for classical computers. Previously, exact sampling from the outputs of even constant-depth quantum circuits was known to be hard for classical computers under these assumptions. However the standard strategy for extending this hardness result to approximate sampling requires the quantum circuits to have a property called “anti-concentration”, meaning roughly that the output has near-maximal entropy. Unitary 2-designs have the desired anti-concentration property. Our result improves the required depth for this level of anti-concentration from linear depth to a sub-linear value, depending on the geometry of the interactions. This is relevant to a recent experiment by the Google Quantum AI group to perform such a sampling task with 53 qubits on a two-dimensional lattice (Arute in Nature 574(7779):505–510, 2019; Boixo et al. in Nate Phys 14(6):595–600, 2018) (and related experiments by USTC), and confirms their conjecture that
O
(
n
)
depth suffices for anti-concentration. The proof is based on a previous construction of
t
-designs by Brandão et al. (2016), an analysis of how approximate designs behave under composition, and an extension of the quasi-orthogonality of permutation operators developed by Brandão et al. (2016). Different versions of the approximate design condition correspond to different norms, and part of our contribution is to introduce the norm corresponding to anti-concentration and to establish equivalence between these various norms for low-depth circuits. For random circuits with long-range gates, we use different methods to show that anti-concentration happens at circuit size
O
(
n
ln
2
n
)
corresponding to depth
O
(
ln
3
n
)
. We also show a lower bound of
Ω
(
n
ln
n
)
for the size of such circuit in this case. We also prove that anti-concentration is possible in depth
O
(
ln
n
ln
ln
n
)
(size
O
(
n
ln
n
ln
ln
n
)
) using a different model.
Journal Article