355 research outputs found
Effects of omeprazole on mechanisms of gastroesophageal reflux in childhood
Prolonged recordings of esophageal motility have shown that dynamic changes of lower esophageal sphincter (LES) pressure such as transient LES relaxation and LES pressure drifts are the most common mechanisms underlying gastroesophageal reflux (GER). The coexistence of a delayed gastric emptying has also been reported in a high proportion of patients with reflux disease. However, not much information is available on the effects of antireflux therapy on the pathogenetic mechanisms of GER. The purpose of this study was to determine in a group of children with severe reflux disease the effect of omeprazole therapy on motor changes of LES underlying GER as well as on gastric emptying time. Twenty-two children (median age: 6.6 years) with GER disease, refractory to combined ranitidine and cisapride administration, entered into an eight-week omeprazole course. Ten subjects with moderate GER disease served as controls (median age: 6.0 years). Before and after omeprazole administration, the following variables were assessed: esophagitis grading, fasting and fed simultaneous prolonged recording of distal esophageal sphincter pressure (with a sleeve catheter) and intraesophageal pH, LES and esophageal peristalsis amplitude, and gastric emptying time of a mixed solid-liquid meal (measured with gastric ultrasound). As compared to controls, patients showed a higher rate of transient LES relaxation and LES pressure drift (P < 0.01), a reduced amplitude of basal sphincter pressure (P < 0.01) and peristalsis (P < 0.05), and a more prolonged gastric emptying time (P < 0.05). After ending omeprazole, there was no significant change in any of the motor abnormalities of the esophagus and in gastric emptying time despite a marked improvement of symptoms and esophagitis in all patients. Sixteen patients were symptomatic when reevaluated on a clinical basis two months after ending therapy. We conclude that in children with severe GER disease, an abnormally high rate of both transient LES relaxation and LES pressure drift and slow gastric emptying are not affected by omperazole treatment, even though esophageal mucosal damage is markedly improved or cured. These abnormalities represent a primary motor disorder and can be implicated in the refractoriness of reflux disease
Comparison of gastric electrical activity and gastric emptying in health and dyspeptic children
Laparoscopic esophagomyotomy for the treatment of achalasia in children - A preliminary report of eight cases
GRB070125: The First Long-Duration Gamma-Ray Burst in a Halo Environment
We present the discovery and high signal-to-noise spectroscopic observations
of the optical afterglow of the long-duration gamma-ray burst GRB070125. Unlike
all previously observed long-duration afterglows in the redshift range 0.5 < z
1.0 A) absorption
features in the wavelength range 4000 - 10000 A. The sole significant feature
is a weak doublet we identify as Mg II 2796 (W = 0.18 +/- 0.02 A), 2803 (W =
0.08 +/- 0.01) at z = 1.5477 +/- 0.0001. The low observed Mg II and inferred H
I column densities are typically observed in galactic halos, far away from the
bulk of massive star formation. Deep ground-based imaging reveals no host
directly underneath the afterglow to a limit of R > 25.4 mag. Either of the two
nearest blue galaxies could host GRB070125; the large offset (d >= 27 kpc)
would naturally explain the low column density. To remain consistent with the
large local (i.e. parsec scale) circum-burst density inferred from broadband
afterglow observations, we speculate GRB070125 may have occurred far away from
the disk of its host in a compact star-forming cluster. Such distant stellar
clusters, typically formed by dynamical galaxy interactions, have been observed
in the nearby universe, and should be more prevalent at z>1 where galaxy
mergers occur more frequently.Comment: 8 pages, accepted in Ap
Dark Bursts in the Swift Era: The Palomar 60 inch-Swift Early Optical Afterglow Catalog
We present multi-color optical observations of long-duration gamma-ray bursts
(GRBs) made over a three year period with the robotic Palomar 60 inch telescope
(P60). Our sample consists of all 29 events discovered by Swift for which P60
began observations less than one hour after the burst trigger. We were able to
recover 80% of the optical afterglows from this prompt sample, and we attribute
this high efficiency to our red coverage. Like Melandri et al. (2008), we find
that a significant fraction (~ 50%) of Swift events show a suppression of the
optical flux with regards to the X-ray emission (so-called "dark" bursts). Our
multi-color photometry demonstrates this is likely due in large part to
extinction in the host galaxy. We argue that previous studies, by selecting
only the brightest and best-sampled optical afterglows, have significantly
underestimated the amount of dust present in typical GRB environments.Comment: 49 pages, including 6 figures and 3 tables (one of which is quite
long). Re-submitted to ApJ following referee report. Comments welcome. v2:
Corrected minor typo
Swift-UVOT Observations of the X-Ray Flash 050406
We present Swift-UVOT data on the optical afterglow of the X-ray flash of
2005 April 6 (XRF 050406) from 88s to \sim 10^5s after the initial prompt
gamma-ray emission. Our observations in the V, B and U bands are the earliest
that have been taken of an XRF optical counterpart. Combining the early -time
optical temporal and spectral properties with \gamma- and simultaneous X-ray
data taken with the BAT and XRT telescopes on-board Swift, we are able to
constrain possible origins of the XRF. The prompt emission had a FRED profile
(fast-rise, exponential decay) with a duration of T_90 = 5.7\pm 0.2s, putting
it at the short end of the long-burst duration distribution. The absence of
photoelectric absorption red-ward of 4000 \AA in the UV/optical spectrum
provides a firm upper limit of z\leq 3.1 on the redshift, thus excluding a high
redshift as the sole reason for the soft spectrum. The optical light curve is
consistent with a power-law decay with slope alpha = -0.75\pm 0.26
(F_{\nu}\propto t^{\alpha}), and a maximum occurring in the first 200s after
the initial gamma-ray emission. The softness of the prompt emission is well
described by an off-axis structured jet model, which is able to account for the
early peak flux and shallow decay observed in the optical and X-ray bands.Comment: 14 pages, 4 figures, accepted for publication in ApJ; typos corrected
and upper limits in table 1 changed from background subtracted count rate in
extraction region to the error associated with thi
The central engine of GRB 130831A and the energy breakdown of a relativistic explosion
Gamma-ray bursts (GRBs) are the most luminous explosions in the universe, yet
the nature and physical properties of their energy sources are far from
understood. Very important clues, however, can be inferred by studying the
afterglows of these events. We present optical and X-ray observations of GRB
130831A obtained by Swift, Chandra, Skynet, RATIR, Maidanak, ISON, NOT, LT and
GTC. This burst shows a steep drop in the X-ray light-curve at s
after the trigger, with a power-law decay index of . Such a rare
behaviour cannot be explained by the standard forward shock (FS) model and
indicates that the emission, up to the fast decay at s, must be of
"internal origin", produced by a dissipation process within an
ultrarelativistic outflow. We propose that the source of such an outflow, which
must produce the X-ray flux for day in the cosmological rest frame,
is a newly born magnetar or black hole. After the drop, the faint X-ray
afterglow continues with a much shallower decay. The optical emission, on the
other hand, shows no break across the X-ray steep decrease, and the late-time
decays of both the X-ray and optical are consistent. Using both the X-ray and
optical data, we show that the emission after s can be explained
well by the FS model. We model our data to derive the kinetic energy of the
ejecta and thus measure the efficiency of the central engine of a GRB with
emission of internal origin visible for a long time. Furthermore, we break down
the energy budget of this GRB into the prompt emission, the late internal
dissipation, the kinetic energy of the relativistic ejecta, and compare it with
the energy of the associated supernova, SN 2013fu.Comment: Accepted for publication by MNRAS. 21 pages, 3 figures, 8 tables.
Extra table with magnitudes in the sourc
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A Photometric Redshift of z ~ 9.4 for GRB 090429B
Gamma-ray bursts (GRBs) serve as powerful probes of the early universe, with their luminous afterglows revealing the locations and physical properties of star-forming galaxies at the highest redshifts, and potentially locating first-generation (Population III) stars. Since GRB afterglows have intrinsically very simple spectra, they allow robust redshifts from low signal-to-noise spectroscopy, or photometry. Here we present a photometric redshift of z ~ 9.4 for the Swift detected GRB 090429B based on deep observations with Gemini-North, the Very Large Telescope, and the GRB Optical and Near-infrared Detector. Assuming a Small Magellanic Cloud dust law (which has been found in a majority of GRB sight lines), the 90% likelihood range for the redshift is 9.06 7. The non-detection of the host galaxy to deep limits (Y(AB) ~ 28, which would correspond roughly to 0.001L* at z = 1) in our late-time optical and infrared observations with the Hubble Space Telescope strongly supports the extreme-redshift origin of GRB 090429B, since we would expect to have detected any low-z galaxy, even if it were highly dusty. Finally, the energetics of GRB 090429B are comparable to those of other GRBs and suggest that its progenitor is not greatly different from those of lower redshift bursts
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