5,909 research outputs found
Scalable two- and four-qubit parity measurement with a threshold photon counter
Parity measurement is a central tool to many quantum information processing
tasks. In this Letter, we propose a method to directly measure two- and
four-qubit parity with low overhead in hard- and software, while remaining
robust to experimental imperfections. Our scheme relies on dispersive
qubit-cavity coupling and photon counting that is sensitive only to intensity;
both ingredients are widely realized in many different quantum computing
modalities. For a leading technology in quantum computing, superconducting
integrated circuits, we analyze the measurement contrast and the back action of
the scheme and show that this measurement comes close enough to an ideal parity
measurement to be applicable to quantum error correction.Comment: 5 pages + 7 pages supplementary, 4 figures + 2 figures supplementar
Renormalization group scaling in nonrelativistic QCD
We discuss the matching conditions and renormalization group evolution of
non-relativistic QCD. A variant of the conventional MS-bar scheme is proposed
in which a subtraction velocity nu is used rather than a subtraction scale mu.
We derive a novel renormalization group equation in velocity space which can be
used to sum logarithms of v in the effective theory. We apply our method to
several examples. In particular we show that our formulation correctly
reproduces the two-loop anomalous dimension of the heavy quark production
current near threshold.Comment: (27 pages, revtex
Hadronic Spectral Moments in Semileptonic B Decays With a Lepton Energy Cut
We compute the first two moments of the final hadronic invariant mass in
inclusive semileptonic B decay, in the presence of a cut on the charged lepton
energy. These moments may be measured directly by experiments at the
Upsilon(4S) using the neutrino reconstruction technique, which requires such a
cut. Measurement of these moments will place constraints on the nonperturbative
parameters \bar\Lambda and \lambda_1, which are relevant for extracting the
quark masses m_b and m_c, as well as the CKM angle V_cb. We include terms of
order \alpha_s^2\beta_0 and 1/m_b^3 in the operator product expansion, and use
the latter to estimate the theoretical uncertainty in the extraction of
\bar\Lambda and \lambda_1.Comment: 13 pages, 5 figures, REVTe
Implications of the lepton spectrum for heavy quark physics
The shape of the lepton spectrum in inclusive semileptonic decay is sensitive to matrix elements of the heavy quark
effective theory, and . From CLEO data we extract
GeV and , where
the uncertainty is the statistical error only. Systematic
uncertainties are discussed. These values for and are
used to determine and the bottom and charm quark
masses. We discuss the theoretical uncertainties related to order
effects and higher orders in the perturbative
expansion.Comment: 10 pages revtex + one figure. Corrections from secondary leptons
included, that affect the numerical results. Thus the central values become
and $\lambda_1=-0.19\pm0.10GeV^2
Unconventional Magnetic Ground State in YbTiO
We report low temperature specific heat and muon spin relaxation/rotation
(SR) measurements on both polycrystalline and single crystal samples of
the pyrochlore magnet YbTiO. This system is believed to possess a
spin Hamiltonian supporting a Quantum Spin Ice (QSI) ground state and to
display sample variation in its low temperature heat capacity. Our two samples
exhibit extremes of this sample variation, yet our SR measurements
indicate a similar disordered low temperature state down to 16 mK in both. We
report little temperature dependence to the spin relaxation and no evidence for
ferromagnetic order, in contrast to recent reports by Chang \emph{et al.} (Nat.
Comm. {\bf 3}, 992 (2012)). Transverse field (TF) SR measurements show
changes in the temperature dependence of the muon Knight shift which coincide
with heat capacity anomalies. We are therefore led to propose that
YbTiO enters a hidden order ground state below mK
where the nature of the ordered state is unknown but distinct from simple long
range order.Comment: Accepted for publication in Phys. Rev. B. 5 pages, 4 figure
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