388 research outputs found
Conformal Invariance of the Subleading Soft Theorem in Gauge Theory
In this note, I show that the recently proposed subleading soft factor in
massless gauge theory uniquely follows from conformal symmetry of tree-level
gauge theory amplitudes in four dimensions.Comment: v1: 6 pages, no figures, JHEP style; v2: 7 pages, added some
discussion and references; v3: 5 pages, PRD accepted version, minor wording
change
Unsafe but Calculable: Ratios of Angularities in Perturbative QCD
Infrared- and collinear-safe (IRC-safe) observables have finite cross
sections to each fixed-order in perturbative QCD. Generically, ratios of
IRC-safe observables are themselves not IRC safe and do not have a valid
fixed-order expansion. Nevertheless, in this paper we present an explicit
method to calculate the cross section for a ratio observable in perturbative
QCD with the help of resummation. We take the IRC-safe jet angularities as an
example and consider the ratio formed from two angularities with different
angular exponents. While the ratio observable is not IRC safe, it is "Sudakov
safe", meaning that the perturbative Sudakov factor exponentially suppresses
the singular region of phase space. At leading logarithmic (LL) order, the
distribution is finite but has a peculiar expansion in the square root of the
strong coupling constant, a consequence of IRC unsafety. The accuracy of the LL
distribution can be further improved with higher-order resummation and
fixed-order matching. Non-perturbative effects can sometimes give rise to order
one changes in the distribution, but at sufficiently high energies Q, Sudakov
safety leads to non-perturbative corrections that scale like a (fractional)
power of 1/Q, as is familiar for IRC-safe observables. We demonstrate that
Monte Carlo parton showers give reliable predictions for the ratio observable,
and we discuss the prospects for computing other ratio observables using our
method.Comment: 41 pages, 14 figures, 1 table, small changes in v.
How Much Information is in a Jet?
Machine learning techniques are increasingly being applied toward data
analyses at the Large Hadron Collider, especially with applications for
discrimination of jets with different originating particles. Previous studies
of the power of machine learning to jet physics has typically employed image
recognition, natural language processing, or other algorithms that have been
extensively developed in computer science. While these studies have
demonstrated impressive discrimination power, often exceeding that of
widely-used observables, they have been formulated in a non-constructive manner
and it is not clear what additional information the machines are learning. In
this paper, we study machine learning for jet physics constructively,
expressing all of the information in a jet onto sets of observables that
completely and minimally span N-body phase space. For concreteness, we study
the application of machine learning for discrimination of boosted, hadronic
decays of Z bosons from jets initiated by QCD processes. Our results
demonstrate that the information in a jet that is useful for discrimination
power of QCD jets from Z bosons is saturated by only considering observables
that are sensitive to 4-body (8 dimensional) phase space.Comment: 14 pages + appendices, 10 figures; v2: JHEP version, updated neural
network, included deeper network and boosted decision tree result
QCD Analysis of the Scale-Invariance of Jets
Studying the substructure of jets has become a powerful tool for event
discrimination and for studying QCD. Typically, jet substructure studies rely
on Monte Carlo simulation for vetting their usefulness; however, when possible,
it is also important to compute observables with analytic methods. Here, we
present a global next-to-leading-log resummation of the angular correlation
function which measures the contribution to the mass of a jet from constituents
that are within an angle R with respect to one another. For a scale-invariant
jet, the angular correlation function should scale as a power of R. Deviations
from this behavior can be traced to the breaking of scale invariance in QCD. To
do the resummation, we use soft-collinear effective theory relying on the
recent proof of factorization of jet observables at e+ e- colliders.
Non-trivial requirements of factorization of the angular correlation function
are discussed. The calculation is compared to Monte Carlo parton shower and
next-to-leading order results. The different calculations are important in
distinct phase space regions and exhibit that jets in QCD are, to very good
approximation, scale invariant over a wide dynamical range.Comment: Updated to PRD version, added discussion of relative importance of
NLL vs. NLO contribution
Automating the Construction of Jet Observables with Machine Learning
Machine-learning assisted jet substructure tagging techniques have the
potential to significantly improve searches for new particles and Standard
Model measurements in hadronic final states. Techniques with simple analytic
forms are particularly useful for establishing robustness and gaining physical
insight. We introduce a procedure to automate the construction of a large class
of observables that are chosen to completely specify -body phase space. The
procedure is validated on the task of distinguishing
from , where and previous brute-force approaches
to construct an optimal product observable for the -body phase space have
established the baseline performance. We then use the new method to design
tailored observables for the boosted search, where and brute-force
methods are intractable. The new classifiers outperform standard -prong
tagging observables, illustrating the power of the new optimization method for
improving searches and measurement at the LHC and beyond.Comment: 15 pages, 8 tables, 12 figure
Sudakov Safety in Perturbative QCD
Traditional calculations in perturbative quantum chromodynamics (pQCD) are
based on an order-by-order expansion in the strong coupling .
Observables that are calculable in this way are known as "safe". Recently, a
class of unsafe observables was discovered that do not have a valid
expansion but are nevertheless calculable in pQCD using all-orders resummation.
These observables are called "Sudakov safe" since singularities at each
order are regulated by an all-orders Sudakov form factor. In this
letter, we give a concrete definition of Sudakov safety based on conditional
probability distributions, and we study a one-parameter family of momentum
sharing observables that interpolate between the safe and unsafe regimes. The
boundary between these regimes is particularly interesting, as the resulting
distribution can be understood as the ultraviolet fixed point of a generalized
fragmentation function, yielding a leading behavior that is independent of
.Comment: 4+5 pages, 4 figures, 1 table. Version accepted for publication in
PR
Non-Global Logarithms, Factorization, and the Soft Substructure of Jets
An outstanding problem in QCD and jet physics is the factorization and
resummation of logarithms that arise due to phase space constraints, so-called
non-global logarithms (NGLs). In this paper, we show that NGLs can be
factorized and resummed down to an unresolved infrared scale by making
sufficiently many measurements on a jet or other restricted phase space region.
Resummation is accomplished by renormalization group evolution of the objects
in the factorization theorem and anomalous dimensions can be calculated to any
perturbative accuracy and with any number of colors. To connect with the NGLs
of more inclusive measurements, we present a novel perturbative expansion which
is controlled by the volume of the allowed phase space for unresolved
emissions. Arbitrary accuracy can be obtained by making more and more
measurements so to resolve lower and lower scales. We find that even a minimal
number of measurements produces agreement with Monte Carlo methods for
leading-logarithmic resummation of NGLs at the sub-percent level over the full
dynamical range relevant for the Large Hadron Collider. We also discuss other
applications of our factorization theorem to soft jet dynamics and how to
extend to higher-order accuracy.Comment: 46 pages + appendices, 10 figures. v2: added current figures 4 and 5,
as well as corrected several typos in appendices. v3: corrected some typos,
added current figure 9, and added more discussion of fixed-order versus
dressed gluon expansions. v4: fixed an error in numerics of two-dressed
gluon; corrected figure 8, modified comparison to BMS. Conclusions unchanged.
v5: fixed minor typ
Factorization and Resummation for Groomed Multi-Prong Jet Shapes
Observables which distinguish boosted topologies from QCD jets are playing an
increasingly important role at the Large Hadron Collider (LHC). These
observables are often used in conjunction with jet grooming algorithms, which
reduce contamination from both theoretical and experimental sources. In this
paper we derive factorization formulae for groomed multi-prong substructure
observables, focusing in particular on the groomed observable, which is
used to identify boosted hadronic decays of electroweak bosons at the LHC. Our
factorization formulae allow systematically improvable calculations of the
perturbative distribution and the resummation of logarithmically enhanced
terms in all regions of phase space using renormalization group evolution. They
include a novel factorization for the production of a soft subjet in the
presence of a grooming algorithm, in which clustering effects enter directly
into the hard matching. We use these factorization formulae to draw robust
conclusions of experimental relevance regarding the universality of the
distribution in both and collisions. In particular, we show that
the only process dependence is carried by the relative quark vs. gluon jet
fraction in the sample, no non-global logarithms from event-wide correlations
are present in the distribution, hadronization corrections are controlled by
the perturbative mass of the jet, and all global color correlations are
completely removed by grooming, making groomed a theoretically clean QCD
observable even in the LHC environment. We compute all ingredients to one-loop
accuracy, and present numerical results at next-to-leading logarithmic accuracy
for collisions, comparing with parton shower Monte Carlo simulations.
Results for collisions, as relevant for phenomenology at the LHC, are
presented in a companion paper.Comment: 66 pages, 18 figure
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