Abstract

We consider extensions of the standard model based on open strings ending on D-branes, with gauge bosons due to strings attached to stacks of D-branes and chiral matter due to strings stretching between intersecting D-branes. Assuming that the fundamental string mass scale ${M}_{s}$ is in the TeV range and that the theory is weakly coupled, we discuss possible signals of string physics at the upcoming HL-LHC run (integrated $\mathrm{luminosity}=3000\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$) with a center-of-mass energy of $\sqrt{s}=14\text{ }\text{ }\mathrm{TeV}$ and at potential future $pp$ colliders, HE-LHC and VLHC, operating at $\sqrt{s}=33$ and 100 TeV, respectively (with the same integrated luminosity). In such D-brane constructions, the dominant contributions to full-fledged string amplitudes for all the common QCD parton subprocesses leading to dijets and $\ensuremath{\gamma}+\mathrm{jet}$ are completely independent of the details of compactification and can be evaluated in a parameter-free manner. We make use of these amplitudes evaluated near the first $(n=1)$ and second $(n=2)$ resonant poles to determine the discovery potential for Regge excitations of the quark, the gluon, and the color singlet living on the QCD stack. We show that for string scales as large as 7.1 TeV (6.1 TeV) lowest massive Regge excitations are open to discovery at the $\ensuremath{\ge}5\ensuremath{\sigma}$ in dijet ($\ensuremath{\gamma}+\mathrm{jet}$) HL-LHC data. We also show that for $n=1$ the dijet discovery potential at HE-LHC and VLHC exceedingly improves: up to 15 TeV and 41 TeV, respectively. To compute the signal-to-noise ratio for $n=2$ resonances, we first carry out a complete calculation of all relevant decay widths of the second massive level string states (including decays into massless particles and a massive $n=1$ and a massless particle), where we rely on factorization and conformal field theory techniques. Helicity wave functions of arbitrary higher spin massive bosons are also constructed. We demonstrate that for string scales ${M}_{s}\ensuremath{\lesssim}10.5\text{ }\text{ }\mathrm{TeV}$ (${M}_{s}\ensuremath{\lesssim}28\text{ }\text{ }\mathrm{TeV}$) detection of $n=2$ Regge recurrences at HE-LHC (VLHC) would become the smoking gun for D-brane string compactifications. Our calculations have been performed using a semianalytic parton model approach which is cross checked against an original software package. The string event generator interfaces with HERWIG and Pythia through BlackMax. The source code is publicly available in the hepforge repository.

Highlights

  • One of the most challenging problems in high-energy physics today is to find out what is the underlying theory that completes the standard model (SM)

  • The hierarchy implies a severe finetuning of the fundamental parameters in more than 30 decimal places in order to keep the masses of elementary particles at their observed values

  • The reason is that quantum radiative corrections to all masses generated by the Higgs vacuum expectation value (VEV) are proportional to the ultraviolet cutoff which in the presence of gravity is fixed by the Planck mass

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Summary

INTRODUCTION

One of the most challenging problems in high-energy physics today is to find out what is the underlying theory that completes the standard model (SM). Two quarks, are independent of the details of the compactification, such as the configuration of branes, the geometry of the extra dimensions, and whether SUSY is broken or not.2 This model independence makes it possible to compute the string corrections to γ þ jet and dijet signals at the LHC, which, if traced to low-mass-scale string tpheffiffiory, could with 100 fb−1 of integrated luminosity (at s 1⁄4 14 TeV) probe deviations from SM physics at a 5σ significance for Ms as large as 6.8 TeV [5,8]. A point worth noting at this juncture is that the tensor-toscalar ratio (r 1⁄4 0.20þ−00..0057) inferred from the excess B-mode power observed by the Background Imaging of Cosmic Extragalactic Polarization (BICEP2) experiment suggests in simple slow-roll models an era of inflation with energy densities of order ð1016 GeVÞ4, not far below the Planck density [40] This presumably suggests that low-mass-scale string compactifications in connection with large extra dimension are quite hard to realize. One should keep in mind that there is an ongoing controversy concerning the effect of background on the BICEP2 result [41,42]

INTERSECTING D-BRANE STRING COMPACTIFICATIONS
Mass mixing effect
OTiaAa: a ð2:4Þ
SM from D-brane constructs
LOWEST MASSIVE REGGE EXCITATIONS OF OPEN STRINGS
Amplitudes and factorization
Excited quarks decay to SUð2Þ gauge bosons
Massive string states decaying to anomalous Uð1Þ’s
Comments on how to realize right-handed quarks in intersecting brane models
STRING COMPUTATION OF PARTIAL DECAY WIDTHS
Vertex operators of the second massive level universal string states
Helicity wave functions for higher spin massive fields
Review of helicity wave functions for spin-1 and spin-2 bosonic fields
Building helicity wave functions for higher spin massive bosons
Decay of the second massive level string states
Partial decay widths of the spin-3 state σμνρ
Partial decay width of the spin-2 state πμν
Bump hunting
Angular distributions
VIII. CONCLUSIONS
Helicity wave functions for massless spin-12 fermions
Helicity wave functions for massless spin-1 gauge boson
Massive spin-32 fermions wave functions
Standalone mode
LHAPDF
Findings
LHAPDF with simultaneous Pythia hadronization
Full Text
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