Emission of energetic protons from relativistic intensity laser interaction with a cone-wire target

Emission of energetic protons (maximum energy ∼18 MeV) from the interaction of relativistic intensity laser with a cone-wire target is experimentally measured and numerically simulated with hybrid particle-in-cell code, lsp [D. R. Welch et al., Phys. Plasmas 13, 063105 (2006)]. The protons originate from the wire attached to the cone after the OMEGA EP laser (670 J, 10 ps, 5 × 10^{18} W/cm^{2}) deposits its energy inside the cone. These protons are accelerated from the contaminant layer on the wire surface, and are measured in the radial direction, i.e., in a direction transverse to the wire length. Simulations show that the radial electric field, responsible for the proton acceleration, is excited by three factors, viz., (i) transverse momentum of the relativistic fast electrons beam entering into the wire, (ii) scattering of electrons inside the wire, and (iii) refluxing of escaped electrons by "fountain effect" at the end of the wire. The underlying physics of radial electric field and acceleration of protons is discussed.

Dynamics of relativistic laser-plasma interaction on solid targets

A novel time-resolved diagnostic is used to record the critical surface motion during picosecond-scale relativistic laser interaction with a solid target. Single-shot measurements of the specular light show a redshift decreasing with time during the interaction, corresponding to a slowing-down of the hole boring process into overdense plasma. On-shot full characterization of the laser pulse enables simulations of the experiment without any free parameters. Two-dimensional particle-in-cell simulations yield redshifts that agree with the data, and support a simple explanation of the slowing-down of the critical surface based on momentum conservation between ions and reflected laser light.

Feasibility and efficacy of transcranial motor-evoked potential monitoring in neuroendovascular surgery

BACKGROUND AND PURPOSE

Neurophysiological monitoring for neuroendovascular procedures typically involves EEG and SSEP monitoring via cutaneous electrodes. MEP monitoring has been used less frequently because, traditionally, this has required subdural electrode placement. With the advent of transcutaneous techniques, MEP monitoring use has increased. However, little has been published regarding the use of this technique in therapeutic neuroendovascular procedures. The purpose of this study was therefore to determine whether TcMEP monitoring is feasible and efficacious in therapeutic neuroendovascular procedures.

MATERIALS AND METHODS

We retrospectively reviewed our data base of therapeutic neuroendovascular procedures performed with the use of TcMEP monitoring. We specifically determined the incidence of TcMEP changes compared with changes in either SSEP or EEG. We then correlated these changes to actual adverse neurologic events.

RESULTS

Although TcMEP monitoring was technically successful in all of the 140 patients in which it was attempted, we observed significant changes in TcMEP signals in only 1 patient. This patient experienced changes involving all 3 monitoring modalities after intraprocedural aneurysm rupture. In contrast, changes in SSEP tracings alone were found in 9 patients. Of these, 2 patients were known to be moribund before their procedures and neither recovered. Among the remaining 7 patients, temporary SSEP changes tended to correlate with temporary neurologic deficits, while permanent changes were associated with permanent or long-lasting deficits.

CONCLUSIONS

These results suggest that TcMEP monitoring is feasible in therapeutic neuroendovascular procedures. However, it appears that the addition of TcMEP monitoring provides no added benefit to SSEP and EEG monitoring alone.

[21-year-old woman with Reye's syndrome after influenza]

HISTORY AND ADMISSION FINDINGS

A 21-year old woman was referred to the hospital because of progressively deteriorating consciousness. Initially agitation and irritability, later confusion and delirium predominated. Previously influenza with high temperature, headache and vomiting had occurred and been treated with acetylsalicylic acid for some days. Non preliminary diseases were reported. CLINICAL INVESTIGATION: Besides of the deterioration in consciousness no clinical or neurological abnormalities were found. Electroencephalography demonstrated general abnormalities of medium range. Cranial magnetic resonance imaging and liquor investigations showed no pathological findings. In laboratory tests a marked increase of transaminases and ammonia were found. The toxicological screening was normal.

TREATMENT AND COURSE

A hepatic encephalopathy due to acute hepatic failure was diagnosed and a detoxication of ammonemia with lactulose was started immediately. Transjugular liver biopsy showed a marked fattening of liver tissue without serological or histological findings for a reason. Because of progressive deterioration in consciousness mechanical ventilation became necessary. Despite of a rapid decline of ammonium serum levels further neurological deterioration occurred. Cranial computed tomography showed oedema of the cerebrum with beginning cerebral occlusion. Despite immediate therapy of cerebral oedema the patient died because of secondary cerebral oedema in hepatic encephalopathy.

CONCLUSION

Reye's syndrome is an acute illness characterized by hepatic encephalopathy and fatty degeneration of the liver. It often occurs after viral infections. After a viral infection that was eventually treated with acetylsalicylic acid Reye's syndrome has to be discussed after exclusion of common causes of hepatic failure.

Hot electron temperature and coupling efficiency scaling with prepulse for cone-guided fast ignition

The effect of increasing prepulse energy levels on the energy spectrum and coupling into forward-going electrons is evaluated in a cone-guided fast-ignition relevant geometry using cone-wire targets irradiated with a high intensity (10(20) W/cm(2)) laser pulse. Hot electron temperature and flux are inferred from Kα images and yields using hybrid particle-in-cell simulations. A two-temperature distribution of hot electrons was required to fit the full profile, with the ratio of energy in a higher energy (MeV) component increasing with a larger prepulse. As prepulse energies were increased from 8 mJ to 1 J, overall coupling from laser to all hot electrons entering the wire was found to fall from 8.4% to 2.5% while coupling into only the 1-3 MeV electrons dropped from 0.57% to 0.03%.

[32-year-old patient with acute myocardial infarction possibly induced by the appetite suppressant sibutramine]

HISTORY

A 32-year-old, very slightly overweight woman (body mass index of 25) without any cardiovascular risk factors presented with acute chest pain. She reported taking the appetite suppressant sibutramine daily for three months. She was not pregnant and did not remember episodes of serious mental stress or infection during the last few weeks. Physical examination was unsuspicious.

INVESTIGATION

Laboratory results revealed an elevation of serum markers of myocardial ischemia. The electrocardiogram showed ST segment depressions and T wave inversions in leads II, III and aVF, indicating a nontransmural inferior myocardial infarction.

TREATMENT AND COURSE

Coronary angiography showed patent coronary arteries with inferior wall hypokinesia. There were no signs of a coronary dissection. Assuming that the acute coronary syndrome had been induced by coronary spasms, the patient was treated with amlodipine and ramipril.

CONCLUSION

It seemed reasonable to suspect that the intake of sibutramine had induced coronary spasms. However, this is a diagnosis of exclusion. Three case reports have previously been published about acute myocardial infarctions, possibly related to sibutramin intake, in young patients with a negligible cardiovascular risk profile. The European Medicines Agency has questioned the marketing authorisations for sibutramine (January 2010). In patients presenting with acute coronary syndromes which can not be clearly related to cardiovascular risk factors, it is crucial to obtain a complete drug history. Some patients might continue to take sibutramine.

Limitation on prepulse level for cone-guided fast-ignition inertial confinement fusion

The viability of fast-ignition (FI) inertial confinement fusion hinges on the efficient transfer of laser energy to the compressed fuel via multi-MeV electrons. Preformed plasma due to the laser prepulse strongly influences ultraintense laser plasma interactions and hot electron generation in the hollow cone of an FI target. We induced a prepulse and consequent preplasma in copper cone targets and measured the energy deposition zone of the main pulse by imaging the emitted K_{alpha} radiation. Simulation of the radiation hydrodynamics of the preplasma and particle in cell modeling of the main pulse interaction agree well with the measured deposition zones and provide an insight into the energy deposition mechanism and electron distribution. It was demonstrated that a under these conditions a 100 mJ prepulse eliminates the forward going component of approximately 2-4 MeV electrons.

Electron heated target temperature measurements in petawatt laser experiments based on extreme ultraviolet imaging and spectroscopy

Three independent methods (extreme ultraviolet spectroscopy, imaging at 68 and 256 eV) have been used to measure planar target rear surface plasma temperature due to heating by hot electrons. The hot electrons are produced by ultraintense laser-plasma interactions using the 150 J, 0.5 ps Titan laser. Soft x-ray spectroscopy in the 50-400 eV region and imaging at the 68 and 256 eV photon energies give a planar deuterated carbon target rear surface pre-expansion temperature in the 125-150 eV range, with the rear plasma plume averaging a temperature approximately 74 eV.

Diagnostics for fast ignition science (invited)

The ignition concept for electron fast ignition inertial confinement fusion requires sufficient energy be transferred from an approximately 20 ps laser pulse to the compressed fuel via approximately MeV electrons. We have assembled a suite of diagnostics to characterize such transfer, simultaneously fielding absolutely calibrated extreme ultraviolet multilayer imagers at 68 and 256 eV; spherically bent crystal imagers at 4.5 and 8 keV; multi-keV crystal spectrometers; MeV x-ray bremmstrahlung, electron and proton spectrometers (along the same line of sight), and a picosecond optical probe interferometer. These diagnostics allow careful measurement of energy transport and deposition during and following the laser-plasma interactions at extremely high intensities in both planar and conical targets. Together with accurate on-shot laser focal spot and prepulse characterization, these measurements are yielding new insights into energy coupling and are providing critical data for validating numerical particle-in-cell (PIC) and hybrid PIC simulation codes in an area crucial for fast ignition and other applications. Novel aspects of these diagnostics and how they are combined to extract quantitative data on ultrahigh intensity laser-plasma interactions are discussed.

A Bremsstrahlung spectrometer using k-edge and differential filters with image plate dosimeters

A Bremsstrahlung spectrometer using k-edge and differential filtering has been used with image plate dosimeters to measure the x-ray fluence from short-pulse laser/target interactions. An electron spectrometer in front of the Bremsstrahlung spectrometer deflects electrons from the x-ray line of sight and simultaneously measures the electron spectrum. The response functions were modeled with the Monte Carlo code INTEGRATED TIGER SERIES 3.0 and the dosimeters calibrated with radioactive sources. An electron distribution with a slope temperature of 1.3 MeV is inferred from the Bremsstrahlung spectra.

Density measurement of shock compressed foam using two-dimensional x-ray radiography

We have used spherically bent quartz crystal to image a laser-generated shock in a foam medium. The foam targets had a density of 0.16 g/cm(3) and thickness of 150 microm, an aluminum/copper pusher drove the shock. The experiment was performed at the Titan facility at Lawrence Livermore National Laboratory using a 2 ns, 250 J laser pulse to compress the foam target, and a short pulse (10 ps, 350 J) to generate a bright Ti K alpha x-ray source at 4.5 keV to radiograph the shocked target. The crystal used gives a high resolution (approximately 20 microm) monochromatic image of the shock compressed foam.

Determination of electron-heated temperatures of petawatt laser-irradiated foil targets with 256 and 68 eV extreme ultraviolet imaging

Measurements of plasma temperature at the rear surface of foil targets due to heating by hot electrons, which were produced in short pulse high intensity laser matter interactions using the 150 J, 0.5 ps Titan laser, are reported. Extreme ultraviolet (XUV) imaging at 256 and 68 eV energies is used to determine spatially resolved target rear surface temperature patterns by comparing absolute intensities to radiation hydrodynamic modeling. XUV mirrors at these two energies were absolutely calibrated at the Advanced Light Source at the Lawrence Berkeley Laboratory. Temperatures deduced from both imagers are validated against each other within the range of 75-225 eV.

Latency analysis of single auditory evoked M100 responses by spatio-temporal filtering

Appropriate spatial filtering followed by temporal filtering is well suited for the single-trial analysis of multi-channel magnetoencephalogram or electroencephalogram recordings. This is demonstrated by the results of a single-trial latency analysis obtained for auditory evoked M100 responses from nine subjects using two different stimulation frequencies. Spatial filters were derived automatically from the data via noise-adjusted principle component analysis, and single-trial latencies were estimated from the signal phase after complex bandpass filtering. For each of the two stimulation frequencies, estimated single-trial latencies were consistent with results obtained from a standard approach using averaged evoked responses. The quality of the estimated single-trial latencies was additionally assessed by their ability to separate between the two different stimulation frequencies. As a result, more than 80% of the single trials can be classified correctly by their estimated latencies.

Operative Versorgung einer pertrochantären Femurfraktur unmittelbar nach Stent-PTCA eines akuten Myokardinfarkts

Due to the high risk of perioperative adverse events, elective surgery should be suspended for at least 4 weeks after myocardial infarction and coronary stent revascularization, as current guidelines suggest. This report describes the successful management of a patient who underwent urgent surgery for a displaced hip fracture immediately after stent revascularization of an acute myocardial infarction. No new perioperative ischemia was detected. The therapeutic options and the timing of surgical procedures after stent revascularization are discussed.

[Detection of phenol by means of 4-aminophenazone according to Emerson]

In the literature it is reported that 4-(N,N-dimethylamino) phenazone, like 4-amino phenazone, gives a positive Emerson reaction. This, however, is not true and seems to be a misinterpretation due to very similar common names of the substances.

The effect of single-dose naproxen on eicosanoid formation in human gastroduodenal mucosa

BACKGROUND

In animal studies, aspirin and non-aspirin non-steroidal anti-inflammatory drugs contribute to gastroduodenal damage via cyclo-oxygenase inhibition and consecutive leucotriene formation (COX-LOX eicosanoid shunt).

AIM AND METHODS

Ten Helicobacter pylori-negative healthy volunteers received a single dose of 500 mg naproxen to address two questions: (i) is there a crosstalk between eicosanoids before medication in the human gastroduodenal mucosa and (ii) can we demonstrate a COX-LOX shunt following single-dose naproxen?

RESULTS

Significant correlations in the stomach mucosa before medication were obtained between leucotriene B4 (LTB4) and thromboxane B(2) (TxB(2); r = -0.38, P = 0.05), as well as LTB4 and prostaglandin E(2) (PGE(2); r = 0.71, P < 0.0001). In serum, a >90% inhibition of TxB(2) and PGE(2) occurred within 30 min of naproxen administration. In gastric mucosa, a significant decrease of TxB(2) occurred already at 15 min and preferably in the antrum. For LTB4 there was a non-significant trend towards a transient increase. Mucosal PGE(2) was unchanged in all regions; transcript levels of both cyclo-oxygenases/5-lipoxygenase were unaffected (except for a trend of increasing cyclo-oxygenase-2 in the corpus).

CONCLUSIONS

Baseline correlations between LTB4-TxB(2) and LTB4-PGE(2) reflect a crosstalk between these eicosanoids. A COX-LOX shunt; however, cannot be demonstrated following single-dose naproxen in a low-risk population.