Microwave-assisted Rydberg electromagnetically induced transparency: publisher's note.

This publisher's note corrects an error on page 1 in Opt. Lett.43, 1822 (2018).OPLEDP0146-959210.1364/OL.43.001822.

Microwave-assisted Rydberg electromagnetically induced transparency.

We demonstrate electromagnetically induced transparency (EIT) in a four-level cascade-like system, where the two upper levels are Rydberg states coupled by a microwave field. A two-photon transition consisting of an off-resonant microwave field and an off-resonant optical field forms an effective coupling field to induce transparency of the probe light. We characterize the Rabi frequency of the effective coupling field, as well as the EIT microwave spectra. The results show that microwave-assisted EIT allows us to efficiently access Rydberg states with relatively high orbital angular momentum ℓ=3, which is promising for the study of exotic Rydberg molecular states.

Microwave transitions in pairs of Rb Rydberg atoms.

We have observed microwave transitions between pairs of cold Rb atoms, specifically, transitions between the molecular nd(5/2)nd(5/2) and (n+1)d(j)(n-2)f states for 41≤n≤44. (We use the separated atom limits as labels.) The transition is allowed because the dipole-dipole induced configuration interaction between the nd(5/2)nd(5/2) state and the energetically close (n+2)p(3/2)(n-2)f state leads to an admixture of the latter into the former. Such transitions may provide a way of selecting closely spaced pairs of atoms.

Phase-dependent electron-ion recombination in a microwave field.

Using picosecond laser photoionization of Li in a microwave field we have observed phase-dependent reccombination of the photoelectrons with their parent Li+ ions. Recombination occurs at phases of the microwave field such that energy is removed from the photoelectron in the first microwave cycle after excitation, and there are two maxima in the recombination in each microwave cycle. These observations are consistent with observations made using an attosecond pulse train phase locked to an infrared pulse and with the "simpleman's" model, modified to account for the fact that the photoelectrons are produced in a Coulomb potential.

Kilohertz dye laser system for high resolution laser spectroscopy.

We have electro-optically sliced the output light of a commercial Coherent Evolution Nd:YLF laser to pump a kilohertz repetition rate nanosecond dye laser system. Simple and highly adjustable, this laser system can easily be used for initial state preparation for ultrafast systems as well as high resolution spectroscopy.

Nondispersing Bohr wave packets.

Long-lived, nondispersing circular, or Bohr, wave packets are produced starting from Li Rydberg atoms by exposing them first to a linearly polarized microwave field at the orbital frequency, 17.6 GHz at principal quantum number n=72, which locks the electron's motion into an approximately linear orbit in which the electron oscillates in phase with the microwave field. The microwave polarization is changed to circular polarization slowly compared to the orbital frequency, and the electron's motion follows, resulting in a nondispersing Bohr wave packet.

Many-body ionization in a frozen Rydberg gas.

In a dense gas of 300 microK 85Rb atoms of n approximately 50 ionization occurs on a 100 ns time scale, far too fast to be explained by the motion of the atoms or photoionization by 300 K blackbody radiation. Rapid ionization is accompanied by spectral broadening, with the spectrum becoming continuous at n=88 at a density of 5x10(10)cm(-3). The atomic transitions broaden both smoothly and by the emergence of new features, which we attribute to multiple atom absorptions. We attribute the rapid ionization to a sequence of near resonant dipole-dipole transitions through virtual states in this intrinsically many-body system, culminating in the ionization of some of the atoms.

Multiphoton assisted recombination.

We have observed multiphoton assisted recombination in the presence of a 38.8 GHz microwave field. Stimulated emission of up to ten microwave photons results in energy transfer from continuum electrons, enabling recombination. The maximum electron energy loss is far greater than the 2Up predicted by the standard "simpleman's" model. The data are well reproduced by both an approximate analytic expression and numerical simulations in which the combined Coulomb and radiation fields are taken into account.

Coherent population transfer in an atom by multiphoton adiabatic rapid passage.

Coherent population transfer in an atom using a sequence of adiabatic rapid passages through single-photon resonances is well-known, but it requires that the frequency sweep match the changing frequencies of the atomic transitions. The same population transfer can be effected via a single multiphoton adiabatic rapid passage, which requires only a small frequency sweep, if it is possible to select the desired multiphoton transition from the many possible transitions. Here we report the observation of population transfer between Rydberg states by high order multiphoton adiabatic rapid passage.

Dipole-dipole excitation and ionization in an ultracold gas of Rydberg atoms.

In cold dense Rydberg atom samples, the dipole-dipole interaction strength is effectively resonant at the typical interatomic spacing in the sample, and the interaction has a 1/R3 dependence on interatomic spacing R. The dipole-dipole attraction leads to ionizing collisions of initially stationary atoms, which produces hot atoms and ions and initiates the evolution of initially cold samples of neutral Rydberg atoms into plasmas. More generally, the strong dipole-dipole forces lead to motion, which must be considered in proposed applications.

Microwave manipulation of an atomic electron in a classical orbit.

Although an atom is a manifestly quantum mechanical system, the electron in an atom can be made to move in a classical orbit almost indefinitely if it is exposed to a weak microwave field oscillating at its orbital frequency. The field effectively tethers the electron, phase-locking its motion to the oscillating microwave field. By exploiting this phase-locking, we have sped up or slowed down the orbital motion of the electron in excited lithium atoms by increasing or decreasing the microwave frequency between 13 and 19 gigahertz; the binding energy and orbital size change concurrently.

Quantum suppression of microwave ionization of Rydberg atoms at high scaled frequency.

Microwave ionization of Rydberg atoms is well described as the onset of classical chaos when the microwave frequency omega is less than the Kepler frequency 1/n(3). However, when omega>1/n(3), i.e., at high scaled frequency Omega=omegan(3)>1, classical ionization is predicted to be suppressed by quantum interference, an analogue to Anderson localization in a solid. Using 17.55 GHz microwave fields we have observed the ionization of Sr Rydberg atoms in the regime 1

Nondispersing wave packets.

We have formed nondispersing wave packets from atomic Li Rydberg eigenstates by adding a small microwave field approximately resonant with the Deltan=1 transition. The orbital motion of the Rydberg electron in states of 70

Fano line shapes reconsidered: symmetric photoionization peaks from pure continuum excitation.

In a photoionization spectrum in which there is no excitation of the discrete states, but only the underlying continuum, we have observed resonances which appear as symmetric peaks, not the commonly expected window resonances. Furthermore, since the excitation to the unperturbed continuum vanishes, the cross section expected from Fano's configuration interaction theory is identically zero. This shortcoming is removed by the explicit introduction of the phase shifted continuum, which demonstrates that the shape of a resonance, by itself, provides no information about the relative excitation amplitudes to the discrete state and the continuum.

Pyrimidinylimidazole inhibitors of p38: cyclic N-1 imidazole substituents enhance p38 kinase inhibition and oral activity.

Optimization of a series of N-1-cycloalkyl-4-aryl-5-(pyrimidin-4-yl)imidazole inhibitors of p38 kinase is reported. Oral administration of inhibitors possessing a cyclohexan-4-ol or piperidin-4-yl group at N-1 in combination with alkoxy, amino(alkyl), phenoxy and anilino substitution at the 2-position of the pyrimidine was found to potently inhibit LPS-induced TNF in mice and rats. The selectivity of these new inhibitors for p38 kinase versus eight other protein kinases is high and in all cases exceeds that of SB 203580.

Microwave ionization of an atomic electron wave packet.

A short microwave pulse is used to ionize a lithium Rydberg wave packet launched from the core at a well-defined phase of the field. We observe a strong dependence on the relative phase between the motion of the wave packet and the oscillations of the field. This phase dependent ionization is also studied as a function of the relative frequency. Our experimental observations are in good qualitative agreement with a one-dimensional classical model of wave packet ionization.

Phenoxypyrimidine inhibitors of p38alpha kinase: synthesis and statistical evaluation of the p38 inhibitory potencies of a series of 1-(piperidin-4-yl)-4-(4-fluorophenyl)-5-(2-phenoxypyrimidin-4-yl) imidazoles.

As a continuation of our work with 1,4,5 substituted imidazole inhibitors of p38alpha, we report a series of 1-(4-piperidinyl)-4-(4-fluorophenyl)-5-(2-phenoxy-4-pyrimidinyl) imidazoles related to 7. The compounds have IC50's for inhibition of p38alpha ranging from 6.0 to 650nM. Statistical analysis of the p38beta inhibitor potencies shows a correlation of IC50's with the electron donating strength of low molecular weight substituents.

Characterization of auxin-induced ARRO-1 expression in the primary root of Malus domestica.

ARRO-1, a novel 2-oxoacid-dependent dioxygenase (2-ODD) is up-regulated during IBA-induced adventitious root formation in stem discs of Malus domestica. Analysis of ARRO-1's expression profile in the primary root of apple seedlings indicates that it is also highly up-regulated in the root in response to both IAA and IBA, but not 2, 4-D. Auxin-derived evolution of ethylene can be discounted as the source of ARRO-1 induction as ARRO-1 is not induced in the root following treatment with the ethylene precursor ACC. Constitutive expression in the primary root further suggests that ARRO-1's role may be linked to the regulation of natural auxin levels within plant tissues. Significantly, orthologues of ARRO-1 have been identified in Arabidopsis thaliana by means of DNA database analysis which will enable the further molecular characterization of this class of 2-ODD.

The diagnosis of freemartinism in cattle using sex-specific DNA sequences.

The majority of heifers born co-twins to bulls are infertile freemartins. It is important that the condition be diagnosed at an early age as freemartins have no potential for use as replacement stock. A rapid, robust, reliable technique for freemartin diagnosis is described. Three Y-specific polymerase chain reaction (PCR) primer pairs: BOV97M, BRY.1 and AMX/Y were used to detect male cells in the blood of heifers born co-twins to bulls. PCR -based tests have advantages over currently used methods of freemartin diagnosis.

Population pharmacokinetics of glyburide in patients with well-controlled diabetes.

STUDY OBJECTIVES: To investigate glyburide pharmacokinetics in patients with well-controlled noninsulin-dependent diabetes mellitus (NIDDM), and test the hypothesis that intersubject variability in the glyburide dose is due to patient differences in the drug's pharmacokinetics. METHODS: Prospective, open-label study. SETTING: University-affiliated, internal medicine outpatient clinic. PATIENTS: Fifty-one patients with NIDDM (11 women, 40 men, mean age 56.7 +/- 15.3 yrs) receiving oral glyburide and with well-controlled glycohemoglobin levels 10.0% or below. INTERVENTION: After fasting overnight, patients ingested their regular morning dose of glyburide and then ate breakfast. Blood samples were drawn before dosing and between 0.5-2 hours, 2-5 hours, and 5-10 hours after dosing. MEASUREMENTS AND MAIN RESULTS: Serum glyburide was assayed by high-performance liquid chromatography and pharmacokinetics by NONMEM. Glyburide clearance was proportional to weight and greater in older patients (> 60 yrs). CONCLUSION: Variability in the glyburide dose was not primarily due to intersubject differences in the drug's pharmacokinetics.