We examine in a model-independent manner the measurements that can be
performed at B-factories with sensitivity to dark matter. If a singlet scalar,
pseudo-scalar, or vector is present and mediates the Standard Model - dark
matter interaction, it can mediate invisible decays of quarkonium states such
as the \$\Upsilon\$, \$J/\Psi\$, and \$\eta\$. Such scenarios have arisen in the
context of supersymmetry, extended Higgs sectors, solutions the supersymmetric
\$\mu\$ problem, and extra U(1) gauge groups from grand unified theories and
string theory. Existing B-factories running at the \$\Upsilon(4S)\$ can produce
lower \$\Upsilon\$ resonances by emitting an Initial State Radiation (ISR)
photon. Using a combination of ISR and radiative decays, the initial state of
an invisibly decaying quarkonium resonance can be tagged, giving sensitivity to
the spin and CP-nature of the particle that mediates standard model-dark matter
interactions. These measurements can discover or place strong constraints on
dark matter scenarios where the dark matter is approximately lighter than the
\$b\$-quark. For the decay chains \$\Upsilon(nS) \pi^+ \pi^- \Upsilon(1S)\$
(n=2,3) we analyze the dominant backgrounds and determine that with \$400
fb^-1\$ collected at the \$\Upsilon(4S)\$, the B-factories can limit
\$BR(\Upsilon(1S) invisible) 0.1\%\$.
%0 Journal Article
%1 McElrath2005Invisible
%A McElrath, Bob
%D 2005
%K bsm, upsilon
%T Invisible Quarkonium Decays as a Sensitive Probe of Dark Matter
%U http://arxiv.org/abs/hep-ph/0506151
%X We examine in a model-independent manner the measurements that can be
performed at B-factories with sensitivity to dark matter. If a singlet scalar,
pseudo-scalar, or vector is present and mediates the Standard Model - dark
matter interaction, it can mediate invisible decays of quarkonium states such
as the \$\Upsilon\$, \$J/\Psi\$, and \$\eta\$. Such scenarios have arisen in the
context of supersymmetry, extended Higgs sectors, solutions the supersymmetric
\$\mu\$ problem, and extra U(1) gauge groups from grand unified theories and
string theory. Existing B-factories running at the \$\Upsilon(4S)\$ can produce
lower \$\Upsilon\$ resonances by emitting an Initial State Radiation (ISR)
photon. Using a combination of ISR and radiative decays, the initial state of
an invisibly decaying quarkonium resonance can be tagged, giving sensitivity to
the spin and CP-nature of the particle that mediates standard model-dark matter
interactions. These measurements can discover or place strong constraints on
dark matter scenarios where the dark matter is approximately lighter than the
\$b\$-quark. For the decay chains \$\Upsilon(nS) \pi^+ \pi^- \Upsilon(1S)\$
(n=2,3) we analyze the dominant backgrounds and determine that with \$400
fb^-1\$ collected at the \$\Upsilon(4S)\$, the B-factories can limit
\$BR(\Upsilon(1S) invisible) 0.1\%\$.
@article{McElrath2005Invisible,
abstract = {We examine in a model-independent manner the measurements that can be
performed at B-factories with sensitivity to dark matter. If a singlet scalar,
pseudo-scalar, or vector is present and mediates the Standard Model - dark
matter interaction, it can mediate invisible decays of quarkonium states such
as the \$\Upsilon\$, \$J/\Psi\$, and \$\eta\$. Such scenarios have arisen in the
context of supersymmetry, extended Higgs sectors, solutions the supersymmetric
\$\mu\$ problem, and extra U(1) gauge groups from grand unified theories and
string theory. Existing B-factories running at the \$\Upsilon(4S)\$ can produce
lower \$\Upsilon\$ resonances by emitting an Initial State Radiation (ISR)
photon. Using a combination of ISR and radiative decays, the initial state of
an invisibly decaying quarkonium resonance can be tagged, giving sensitivity to
the spin and CP-nature of the particle that mediates standard model-dark matter
interactions. These measurements can discover or place strong constraints on
dark matter scenarios where the dark matter is approximately lighter than the
\$b\$-quark. For the decay chains \$\Upsilon(nS) \to \pi^+ \pi^- \Upsilon(1S)\$
(n=2,3) we analyze the dominant backgrounds and determine that with \$400
fb^{-1}\$ collected at the \$\Upsilon(4S)\$, the B-factories can limit
\$BR(\Upsilon(1S) \to invisible) \lsim 0.1\%\$.},
added-at = {2019-02-23T22:09:48.000+0100},
archiveprefix = {arXiv},
author = {McElrath, Bob},
biburl = {https://www.bibsonomy.org/bibtex/22b794185b8956076b5355ff46e9cfa7d/cmcneile},
citeulike-article-id = {7923700},
citeulike-linkout-0 = {http://arxiv.org/abs/hep-ph/0506151},
citeulike-linkout-1 = {http://arxiv.org/pdf/hep-ph/0506151},
day = 25,
eprint = {hep-ph/0506151},
interhash = {5674a0f8bf9b10371d25ee2bcba51e48},
intrahash = {2b794185b8956076b5355ff46e9cfa7d},
keywords = {bsm, upsilon},
month = sep,
posted-at = {2010-09-29 13:13:30},
priority = {2},
timestamp = {2019-02-23T22:15:27.000+0100},
title = {{Invisible Quarkonium Decays as a Sensitive Probe of Dark Matter}},
url = {http://arxiv.org/abs/hep-ph/0506151},
year = 2005
}