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Role of the interaction between ionizable groups in the folding of bovine alpha-lactalbumin.

Previous studies of the reversible unfolding of alpha-lactalbumin in the acid to neutral pH region have shown that the unfolding transition with guanidine hydrochloride involves a stable intermediate which is similar to a partially unfolded state produced by acid transition. In order to clarify how the interaction of ionizable groups takes part in stabilization of the native structure during the folding of the protein, the transitions were further investigated in the alkaline region in the presence of the denaturant by means of circular dichroism, difference spectra and pH-jump measurements, and the effects of pH on the equilibrium and kinetics of the unfolding in the whole pH region are discussed. The alkaline state is indistinguishable from the acid state in equilibrium and kinetic properties. Thus, as a first approximation, the total unfolding in the whole pH region can be expressed as a three-state mechanism involving the native (N), the intermediate (A), and the fully unfolded (D) states. The strong pH dependence of the N Equilibrium A transition above pH 10 is almost entirely ascribable to the abnormal tyrosines in the N state previously detected by the pH-jump titration method, while the dependence between pH 7 and 10 also suggests the presence of an abnormal alpha-amino group. The normalization of most of the alkaline and the acidic abnormally ionizable groups in the N state occurs simultaneously in the first step of the unfolding pathway, i.e., the forward activation of the N Equilibrium A transition, and the final step of the folding may be associated with the interaction of the ionizable groups. Among the abnormally ionizable groups detected, the tyrosyl and carboxyl groups are most important in view of the large changes in their pK values, suggesting the presence of some interactions, even if only indirect, between these groups. Alignment data of amino acid residues also suggest that at least one such abnormal tyrosyl residue (Tyr 50) and its neighbors are conserved throughout in the alpha-lactalbumin-lysozyme group of proteins. Possible mechanisms of the interaction between the tyrosyl and carboxyl groups are discussed.

Animals↗

Total ionized serum calcium and parathyroid hormone levels in patients with disseminated coccidioidomycosis.

Twenty-one patients with severe coccidioidomycosis, including eight with osseous lesions, were admitted to the University of California, Davis, Medical Center, during a recent epidemic. Transient mild ionized hypercalcemia occurred in only two patients, and a tendency toward low normal ionized calciums was noted. Parathyroid hormone levels appeared to be appropriate for the ionized calcium in these patients. There were no significant differences in ionized calcium levels of parathyroid hormone levels among patients with and without osseous coccidioidomycosis. We conclude that hypercalcemia is rare in coccidioidomycosis, even with extensive bony involvement.

Calcium↗

Effect of hyperventilation on total calcium, ionized calcium, and serum phosphorus in neonates.

The effect of alkalosis (pH greater than 7.55) on total calcium, ionized calcium, and serum phosphorus was studied in seven infants with persistent pulmonary hypertension (PPH) before, during, and after hyperventilation. Hyperventilation-induced alkalosis resulted in marked decreases in total calcium, phosphorus, and ionized calcium. There was an inverse correlation between plasma Ca+2 and pH; a 0.1-unit increase in blood pH decreased Ca+2 by 0.42 mg/dl. Two of the study infants had ionized calcium concentrations less than 2.5 mg/dl during hyperventilation. These disturbing changes in total calcium, ionized calcium, and serum phosphorus could have potentially detrimental effects on neonates with PPH.

Alkalosis↗

Ionized magnesium concentrations in critically ill children.

OBJECTIVE: To test the hypothesis that many critically ill children exhibit ionized hypomagnesemia despite having normal total magnesium (TMg) concentrations. DESIGN: A prospective, observational study with convenience sampling. SETTING: Pediatric and cardiovascular intensive care units of a large children's hospital. PATIENTS: Patients aged 1 day to 21 yrs admitted from January 1 to October 31, 1996. Patients with chronic renal failure or weight <3 kg were excluded. A group of healthy children involved in a school-based nutritional assessment study were also studied. INTERVENTIONS: None. MEASUREMENTS AND MAIN RESULTS: Sixty-seven patients (5.4+/-5.7 [SD] yrs) and 24 healthy children (10.84+/-0.93 yrs, p< .001) were studied. Plasma was assayed for ionized magnesium (IMg) using a blood analyzer. Forty (59%)/67 critically ill subjects had IMg concentrations <0.40 mmol/L, the lowest published normal value and the lowest value observed in our group of healthy children. Of these, 24 (60%)/40 had normal TMg concentrations. IMg was significantly (p=.00) lower in critically ill subjects than in the group of healthy children (0.37+/-0.10 mmol/L vs. 0.46+/-0.03 mmol/L). IMg did not correlate strongly with ionized calcium (r2=0.49), albumin (r2=0.09), or pH (r2=0.18). CONCLUSION: Many critically ill children exhibit ionized hypomagnesemia with normal TMg concentrations. These children would not be recognized as magnesium-deficient based on routine TMg testing. Critically ill children exhibited significantly lower concentrations of IMg than a group of healthy children.

Adolescent↗

Spatial and temporal response characteristics of ionization chambers used in diagnostic radiology for exposure measurements and quality control.

The temporal and spatial (partial volume) response characteristics of ionization chambers used for measuring radiation exposures in x-ray quality control (QC) programs were evaluated. Five ionization chambers were evaluated using a pencil beam scanning x-ray source and a conventional radiographic system. The spatial response was determined by recording the exposure during scanning of the pencil beam or in increments using a slitted lead sheet on a conventional x-ray system. The temporal response was determined by recording x-ray wave forms using the different ionization chambers. The effects of partial volume irradiation of the chambers makes them unsuitable for use under these conditions, except those designed for exposure measurements in computed tomography. The temporal response of many chambers resembles that of a typical resistive-capacitive circuit, making them unsuitable for exposure time measurements or x-ray wave form evaluation. The appropriate ionization chamber must be selected for exposure measurements and quality control in diagnostic radiology.

Equipment Design↗

Plasma ionized calcium monitoring during liver transplantation.

Plasma ionized calcium and citrate concentrations were measured in 11 patients undergoing liver transplantation. During the anhepatic phase of the procedure, ionized calcium concentrations fell to as low as 40% of normal, in spite of calcium supplementation. Simultaneously, citrate concentrations rose to between 20 and 100 times preoperative levels. In two patients low plasma ionized calcium concentrations were associated with hypotension that responded to calcium infusion. Intraoperative monitoring of plasma ionized calcium during liver transplantation is helpful in the rational control of the patient's calcium status.

Calcium↗

Partially ionized hydrogen plasma in strong magnetic fields.

We study the thermodynamic properties of a partially ionized hydrogen plasma in strong magnetic fields, B approximately 10(12)-10(13) G, typical of neutron stars. The properties of the plasma depend significantly on the quantum-mechanical sizes and binding energies of the atoms, which are strongly modified by thermal motion across the field. We use new fitting formulas for the atomic binding energies and sizes, based on accurate numerical calculations and valid for any state of motion of the atom. In particular, we take into account decentered atomic states, neglected in previous studies of thermodynamics of magnetized plasmas. We also employ analytic fits for the thermodynamic functions of nonideal fully ionized electron-ion Coulomb plasmas. This enables us to construct an analytic model of the free energy. An ionization equilibrium equation is derived, taking into account the strong magnetic field effects and the nonideality effects. This equation is solved by an iteration technique. Ionization degrees, occupancies, and the equation of state are calculated.

Journal Article↗

Effects of ionization in single-bubble sonoluminescence.

We studied the effects of ionization in a sonoluminescing (SL) bubble within the hydrodynamic framework. The thermodynamic variables and the degrees of ionization inside the bubble throughout an oscillation cycle are obtained by solving the hydrodynamic equations assuming spherical symmetry. Several models are used to compute the emitted radiation, which are then compared with experimental data. Numerical results show that shock waves are absent in the stable SL regime, and compressional waves are already strong enough to produce moderate temperature and ionization. The degrees of ionization at the bubble center are found to be within 7% to 30%, and Ar+ is the only dominant ion. Moreover, an opacity-corrected blackbody radiation model gives the peak power, pulse widths, and spectra that agree very well with the experimental data.

Journal Article↗

Population kinetics on K alpha lines of partially ionized Cl atoms.

A population kinetics code was developed to analyze K alpha emission from partially ionized chlorine atoms in hydrocarbon plasmas. Atomic processes are solved under collisional-radiative equilibrium for two-temperature plasmas. It is shown that the fast electrons dominantly contribute to ionize the K-shell bound electrons (i.e., inner-shell ionization) and the cold electrons to the outer-shell bound ones. Ratios of K alpha lines of partially ionized atoms are presented as a function of cold-electron temperature. The model was validated by observation of the K alpha lines from a chlorinated plastic target irradiated with 1 TW Ti:sapphire laser pulses at 1.5 x 10(17) W/cm(2), inferring a plasma temperature of about 100 eV on the target surface.

Journal Article↗

Photon acceleration of ultrashort laser pulses by relativistic ionization fronts.

We present experimental results from the collision of weak ultrashort pulses with relativistic ionization fronts in copropagation and counterpropagation. The observed frequency upshifts of the probe pulses provide not only information about the electron density of the ionization front but also reveal the fine structure of the front. The connection between the correlation lengths for copropagation and counterpropagation and the longitudinal and transverse dimensions of the ionization front is also demonstrated thus showing the feasibility of using the frequency upshift experienced by short probe pulses to fully characterize relativistic ionization fronts and other relativistic coherent structures in laser-produced plasmas.

Journal Article↗

Hydrodynamic flow of ions and atoms in partially ionized plasmas.

We have derived the hydrodynamic equations of motion for a partially ionized plasma, when the ionized component and the neutral components have different flow velocities and kinetic temperatures. Starting from the kinetic equations for a gas of ions and a gas of atoms we have considered various processes of encounters between the two species: self-collisions, interspecies collisions, ionization, recombination, and charge exchange. Our results were obtained by developing a general approach for the hydrodynamics of a gas in a binary mixture, in particular when the components drift with respect to each other. This was applied to a partially ionized plasma, when the neutral-species gas and the charged-species gas have separate velocities. We have further suggested a generalized version of the relaxation time approximation and obtained the contributions of the interspecies encounters to the transport equations.

Journal Article↗

Recombination and population inversion in plasmas generated by tunneling ionization.

Above-threshold ionization (ATI) ionization by linearly polarized light has been proposed by several authors as a means of driving recombination lasers in the soft x-ray spectral region. The pump radiation generates a cold electron plasma with ions in a single ionization stage, which is an ideal starting condition for strong recombination. Population inversions form during the recombination cascade to the ground state of the next ionization stage. In the absence of any relaxation the electron distribution is strongly peaked near zero energy. However, a number of different processes all heat the cold electrons towards Maxwellian, and may thereby reduce the recombination rate in the higher levels. Using numerical models we investigate these relaxation processes and their effect on recombination. We show that the recombination can be well described by the standard cascade model, provided an appropriate temperature is used. We examine two cases in detail, hydrogen-like lithium where the inversion is with respect to the ground state, and lithium-like nitrogen where it is with the first excited state. The two cases differ markedly in the degree of relaxation achieved, and in the duration of the population inversion.

Journal Article↗

Femtosecond interferometry of propagation of a laminar ionization front in a gas.

We use optical interferometry to investigate ultrafast ionization induced by an intense, ultrashort laser pulse propagating in a helium gas. Besides standard phase shift information, our interferograms show a localized region of fringe visibility depletion (FVD) that moves along the laser propagation axis at luminal velocity. We find that such a loss of visibility can be quantitatively explained by the ultrafast change of refractive index due to the field ionization of the gas in the laser pulse width. We demonstrate that by combining the post facto phase shift distribution with the probe pulse transit effect in the ionizing region, the analysis of the observed FVD yields significant information on the ultrafast dynamics of propagation of the ionization front in the gas.

Journal Article↗

Multielectron effects on single-electron strong field ionization

An apparently simple phenomenon of single-electron strong field ionization involves subtle factors related to multielectron effects. A single electron in an atom or molecule can feel a distinctly different screening strength when exposed to strong fields as opposed to weak fields, and this electron screening due to multielectron motion influences single-electron ionization. The concept and a corresponding model developed in the paper allow a generalization of the Ammosov-Delone-Krainov model for predicting strong field ionization rates of more complicated atoms and molecules. This general approach explains the recently observed anomalous low single ionization rate in O2.

Journal Article↗

Observation of direct dissociative ionization in molecular hydrogen.

Direct dissociative ionization is the simplest three-body breakup process in H2. We describe the experimental verification of direct dissociative ionization to the repulsive A2Sigma(+)(u) state by resolving the kinetic energy and angular distributions of the formed protons. A (2+1) resonant enhanced multiphoton ionization process via the isotropic E,F (1)Sigma(+)(g)(v = 6,J = 0) level is employed. The structure in the kinetic energy spectrum is well described by a projection of the vibrational wave function of the E,F (1)Sigma(+)(g)(v = 6,J = 0) state onto the repulsive ionic state. The electronic character of the ionization continuum is revealed by the proton angular distribution.

Journal Article↗

Total, partial, and electron-capture cross sections for ionization of water vapor by 20-150 keV protons.

We present experimental results for proton ionization of water molecules based on a novel event by event analysis of the different ions produced (and lost). We are able to obtain mass analyzed product ion signals (e.g., H2O+, OH+, O+, O++, H+) in coincidence with the projectile analyzed after the collision, i.e., either being H+, neutral H after single electron capture during the ionization event, or H- after double electron capture. After proper calibration we are thus able to determine a complete set of cross sections for the ionization of a molecular target by protons including the total and the partial cross sections and in addition also the direct ionization and the electron capture cross sections.

Journal Article↗

Separation of recollision mechanisms in nonsequential strong field double ionization of Ar: the role of excitation tunneling.

Vector momentum distributions of two electrons created in double ionization of Ar by 25 fs, 0.25 PW/cm(2) laser pulses at 795 nm have been measured using a "reaction microscope." At this intensity, where nonsequential ionization dominates, distinct correlation patterns are observed in the two-electron momentum distributions. A kinematical analysis of these spectra within the classical "recollision model" revealed an (e,2e)-like process and excitation with subsequent tunneling of the second electron as two different ionization mechanisms. This allows a qualitative separation of the two mechanisms demonstrating that excitation-tunneling is the dominant contribution to the total double ionization yield.

Journal Article↗

Quantum interference in double ionization and fragmentation of C(6)H(6) in intense laser fields.

During tunnel ionization of atoms or molecules by strong laser fields, the electron acquires a transverse velocity which is characteristic of the ionization process. Ellipticity measurements identify nonsequential double ionization as due to recollision in C(6)H(6) and simultaneously measure the transverse velocity distribution of the electron wave packet. We observe signatures of quantum interference of different tunneling trajectories and find identical dependence of nonsequential double ionization and fragmentation of C(6)H(6) on the ellipticity of the laser polarization. This identifies electron recollision as the dominant source of fragmentation at 1.4 microm.

Journal Article↗