3 research outputs found
Broken selection rule in the quantum Rabi model
Understanding the interaction between light and matter is very relevant for fundamental studies of quantum electrodynamics and for the development of quantum technologies. The quantum Rabi model captures the physics of a single atom interacting with a single photon at all regimes of coupling strength. We report the spectroscopic observation of a resonant transition that breaks a selection rule in the quantum Rabi model, implemented using an LC resonator and an artificial atom, a superconducting qubit. The eigenstates of the system consist of a superposition of bare qubit-resonator states with a relative sign. When the qubit-resonator coupling strength is negligible compared to their own frequencies, the matrix element between excited eigenstates of different sign is very small in presence of a resonator drive, establishing a sign-preserving selection rule. Here, our qubit-resonator system operates in the ultrastrong coupling regime, where the coupling strength is 10% of the resonator frequency, allowing sign-changing transitions to be activated and, therefore, detected. This work shows that sign-changing transitions are an unambiguous, distinctive signature of systems operating in the ultrastrong coupling regime of the quantum Rabi model. These results pave the way to further studies of sign-preserving selection rules in multiqubit and multiphoton models.QN/Quantum Transpor
Measurement of the diffractive cross-section in deep inelastic scattering
Diffractive scattering of , where is either a
proton or a nucleonic system with ~GeV has been measured in deep
inelastic scattering (DIS) at HERA. The cross section was determined by a novel
method as a function of the c.m. energy between 60 and 245~GeV
and of the mass of the system up to 15~GeV at average values of
14 and 31~GeV. The diffractive cross section is,
within errors, found to rise linearly with . Parameterizing the
dependence by the form d\sigma^{diff}/dM_X \propto
(W^2)^{(2\overline{\mbox{\alpha_{_{I\hspace{-0.2em}P}}}} -2)} the DIS data
yield for the pomeron trajectory
\overline{\mbox{\alpha_{_{I\hspace{-0.2em}P}}}} = 1.23 \pm 0.02(stat) \pm
0.04 (syst) averaged over in the measured kinematic range assuming the
longitudinal photon contribution to be zero. This value for the pomeron
trajectory is substantially larger than
\overline{\mbox{\alpha_{_{I\hspace{-0.2em}P}}}} extracted from soft
interactions. The value of \overline{\mbox{\alpha_{_{I\hspace{-0.2em}P}}}}
measured in this analysis suggests that a substantial part of the diffractive
DIS cross section originates from processes which can be described by
perturbative QCD. From the measured diffractive cross sections the diffractive
structure function of the proton F^{D(3)}_2(\beta,Q^2,
\mbox{x_{_{I\hspace{-0.2em}P}}}) has been determined, where is the
momentum fraction of the struck quark in the pomeron. The form F^{D(3)}_2 =
constant \cdot (1/ \mbox{x_{_{I\hspace{-0.2em}P}}})^a gives a good fit to
the data in all and intervals with $a = 1.46 \pm 0.04 (stat) \pmComment: 45 pages, including 16 figure