Interperson variability but intraperson stability of baseline plasma cortisol concentrations, and its relation to feedback sensitivity of the hypothalamo-pituitary-adrenal axis to a low dose of dexamethasone in elderly individuals

In the present study, we investigated whether the negative feedback action of glucocorticoids (GCs) on the hypothalamo-pituitary-adrenal (HPA) axis changes with age. We performed a 1-mg dexamethasone (DEX) suppression test in 216 healthy elderly individuals. To investigate individual variability of feedback sensitivity in more detail, 2.5 yr later a 0.25-mg DEX suppression test was carried out in 164 of the same individuals. We investigated whether there was an effect of age or gender on both basal and post-DEX cortisol levels, as well as on the concentration of DEX. Furthermore, we examined whether the reactions to the two doses of DEX differed, and whether indications for an intraperson stability of baseline cortisol levels could be found. Neither the pre- nor the post-1-mg DEX plasma cortisol concentrations showed a correlation with age, and there were no differences between men and women. The same was true for the pre- and post-0.25-mg DEX cortisol concentrations. In reaction to 1 mg DEX, over 90% of the subjects investigated showed a cortisol suppression to levels below 50 nmol/L. After the administration of 0.25 mg DEX, there was a much wider range in post-DEX cortisol concentrations. After the administration of 1 mg DEX, there was a significant correlation between liver function parameters and plasma DEX concentrations in males, and there was a correlation between body mass index and plasma DEX concentration in females. Plasma DEX concentrations after the administration of 1 mg and 0.25 mg DEX were closely correlated within subjects (P < 0.001). There was an intraindividual stability of serum cortisol levels determined at an interval of 2.5 yr. Furthermore, the individuals with the highest baseline cortisol concentrations also had the highest post-0.25-mg DEX cortisol concentrations, indicating a close relationship between basal cortisol levels and the feedback sensitivity of the HPA axis to a low dose of DEX. These observations suggest a genetic influence on the set point of the HPA axis. Aging does not seem to lead to a change in HPA activity as measured by early morning total cortisol levels. Also, no changes in the sensitivity of the feedback system to DEX were observed with age. DEX metabolism is influenced by liver function (in males) and by body mass index (in females)

A polymorphism in the glucocorticoid receptor gene may be associated with and increased sensitivity to glucocorticoids in vivo

We investigated whether a polymorphism at nucleotide position 1220, resulting in an asparagine-to-serine change at codon 363 in the glucocorticoid receptor (GR) gene is associated with an altered sensitivity to glucocorticoids. In a group of 216 elderly persons, 13 heterozygotes for the N363S polymorphism were identified by PCR/single strand conformation polymorphism analysis. In 2 dexamethasone (DEX) suppression tests (DSTs), using 1 and 0.25 mg DEX, the circulating cortisol and insulin concentrations were compared between N363S carriers and controls. In the 1-mg DST, there were no differences between N363S carriers and controls, with respect to adrenal suppression, but there was a significantly higher (P < 0.05) insulin response in N363S carriers. In the 0.25-mg DST, a significantly larger (P < 0.05) cortisol suppression and higher (P < 0.05) insulin response were seen in N363S carriers. Comparison of blood pressure, body mass index (BMI), and bone mineral density (BMD) between the N363S carriers and controls showed that N363S carriers had a higher (P < 0.05) BMI but normal blood pressure. There was an obvious trend towards lower age-, BMI-, and sex-adjusted BMD in the lumbar spine in N363S carriers. GR characteristics measured in 41 controls and 9 N363S carriers in peripheral mononuclear leucocytes showed no differences between N363S carriers and controls, with respect to GR number and ligand binding affinity. However, there was a trend towards greater sensitivity to DEX in the carriers' lymphocytes, in a mitogen-induced cell proliferation assay. In transfection assays, the capacity of the codon 363 variant to activate mouse mammary tumor virus promotor-mediated transcription in COS-1 cells was unaltered, when compared with the wild-type GR. We conclude that in 6.0% of our study population, a polymorphism in codon 363 of the GR gene was found. Individuals carrying this polymorphism seemed healthy at clinical examination but had a higher sensitivity to exogenously administered glucocorticoids, with respect to both cortisol suppression and insulin response. Life-long exposure to the mutated allele may be accompanied by an increased BMI and a lowered BMD in the lumbar spine but does not affect blood pressure

An algebraic SU(1,1) solution for the relativistic hydrogen atom

The bound eigenfunctions and spectrum of a Dirac hydrogen atom are found taking advantage of the $SU(1, 1)$ Lie algebra in which the radial part of the problem can be expressed. For defining the algebra we need to add to the description an additional angular variable playing essentially the role of a phase. The operators spanning the algebra are used for defining ladder operators for the radial eigenfunctions of the relativistic hydrogen atom and for evaluating its energy spectrum. The status of the Johnson-Lippman operator in this algebra is also investigated.Comment: to appear in Physics Letters A (2005). We corrected a misprint in page 7, in the paragraph baggining with "With the value of ..." the ground state should be |\lambda, \lambda>, not |\lambda, \lambda+1

Kaon Production and Kaon to Pion Ratio in Au+Au Collisions at \snn=130 GeV

Mid-rapidity transverse mass spectra and multiplicity densities of charged and neutral kaons are reported for Au+Au collisions at \snn=130 GeV at RHIC. The spectra are exponential in transverse mass, with an inverse slope of about 280 MeV in central collisions. The multiplicity densities for these particles scale with the negative hadron pseudo-rapidity density. The charged kaon to pion ratios are $K^+/\pi^- = 0.161 \pm 0.002 {\rm (stat)} \pm 0.024 {\rm (syst)}$ and $K^-/\pi^- = 0.146 \pm 0.002 {\rm (stat)} \pm 0.022 {\rm (syst)}$ for the most central collisions. The $K^+/\pi^-$ ratio is lower than the same ratio observed at the SPS while the $K^-/\pi^-$ is higher than the SPS result. Both ratios are enhanced by about 50% relative to p+p and $\bar{\rm p}$+p collision data at similar energies.Comment: 6 pages, 3 figures, 1 tabl

Demonstration of the temporal matter-wave Talbot effect for trapped matter waves

We demonstrate the temporal Talbot effect for trapped matter waves using ultracold atoms in an optical lattice. We investigate the phase evolution of an array of essentially non-interacting matter waves and observe matter-wave collapse and revival in the form of a Talbot interference pattern. By using long expansion times, we image momentum space with sub-recoil resolution, allowing us to observe fractional Talbot fringes up to 10th order.Comment: 17 pages, 7 figure

Azimuthal anisotropy and correlations in p+p, d+Au and Au+Au collisions at 200 GeV

We present the first measurement of directed flow ($v_1$) at RHIC. $v_1$ is found to be consistent with zero at pseudorapidities $\eta$ from -1.2 to 1.2, then rises to the level of a couple of percent over the range $2.4 < |\eta| < 4$. The latter observation is similar to data from NA49 if the SPS rapidities are shifted by the difference in beam rapidity between RHIC and SPS. Back-to-back jets emitted out-of-plane are found to be suppressed more if compared to those emitted in-plane, which is consistent with {\it jet quenching}. Using the scalar product method, we systematically compared azimuthal correlations from p+p, d+Au and Au+Au collisions. Flow and non-flow from these three different collision systems are discussed.Comment: Quark Matter 2004 proceeding, 4 pages, 3 figure

Azimuthal anisotropy: the higher harmonics

We report the first observations of the fourth harmonic (v_4) in the azimuthal distribution of particles at RHIC. The measurement was done taking advantage of the large elliptic flow generated at RHIC. The integrated v_4 is about a factor of 10 smaller than v_2. For the sixth (v_6) and eighth (v_8) harmonics upper limits on the magnitudes are reported.Comment: 4 pages, 6 figures, contribution to the Quark Matter 2004 proceeding

Partonic flow and ϕ\phi-meson production in Au+Au collisions at sNN\sqrt{s_{NN}} = 200 GeV

We present first measurements of the $\phi$-meson elliptic flow ($v_{2}(p_{T})$) and high statistics $p_{T}$ distributions for different centralities from $\sqrt{s_{NN}}$ = 200 GeV Au+Au collisions at RHIC. In minimum bias collisions the $v_{2}$ of the $\phi$ meson is consistent with the trend observed for mesons. The ratio of the yields of the $\Omega$ to those of the $\phi$ as a function of transverse momentum is consistent with a model based on the recombination of thermal $s$ quarks up to $p_{T}\sim 4$ GeV/$c$, but disagrees at higher momenta. The nuclear modification factor ($R_{CP}$) of $\phi$ follows the trend observed in the $K^{0}_{S}$ mesons rather than in $\Lambda$ baryons, supporting baryon-meson scaling. Since $\phi$-mesons are made via coalescence of seemingly thermalized $s$ quarks in central Au+Au collisions, the observations imply hot and dense matter with partonic collectivity has been formed at RHIC.Comment: 6 pages, 4 figures, submit to PR

Plasma Wakefield Acceleration with a Modulated Proton Bunch

The plasma wakefield amplitudes which could be achieved via the modulation of a long proton bunch are investigated. We find that in the limit of long bunches compared to the plasma wavelength, the strength of the accelerating fields is directly proportional to the number of particles in the drive bunch and inversely proportional to the square of the transverse bunch size. The scaling laws were tested and verified in detailed simulations using parameters of existing proton accelerators, and large electric fields were achieved, reaching 1 GV/m for LHC bunches. Energy gains for test electrons beyond 6 TeV were found in this case.Comment: 9 pages, 7 figure