Measuring the structure and equation of state of polyethylene terephthalate at megabar pressures.

We present structure and equation of state (EOS) measurements of biaxially orientated polyethylene terephthalate (PET, [Formula: see text], also called mylar) shock-compressed to ([Formula: see text]) GPa and ([Formula: see text]) K using in situ X-ray diffraction, Doppler velocimetry, and optical pyrometry. Comparing to density functional theory molecular dynamics (DFT-MD) simulations, we find a highly correlated liquid at conditions differing from predictions by some equations of state tables, which underlines the influence of complex chemical interactions in this regime. EOS calculations from ab initio DFT-MD simulations and shock Hugoniot measurements of density, pressure and temperature confirm the discrepancy to these tables and present an experimentally benchmarked correction to the description of PET as an exemplary material to represent the mixture of light elements at planetary interior conditions.

Novel experimental setup for megahertz X-ray diffraction in a diamond anvil cell at the High Energy Density (HED) instrument of the European X-ray Free-Electron Laser (EuXFEL).

The high-precision X-ray diffraction setup for work with diamond anvil cells (DACs) in interaction chamber 2 (IC2) of the High Energy Density instrument of the European X-ray Free-Electron Laser is described. This includes beamline optics, sample positioning and detector systems located in the multipurpose vacuum chamber. Concepts for pump-probe X-ray diffraction experiments in the DAC are described and their implementation demonstrated during the First User Community Assisted Commissioning experiment. X-ray heating and diffraction of Bi under pressure, obtained using 20 fs X-ray pulses at 17.8 keV and 2.2 MHz repetition, is illustrated through splitting of diffraction peaks, and interpreted employing finite element modeling of the sample chamber in the DAC.

Mirror to measure small angle x-ray scattering signal in high energy density experiments.

Small angle x-ray scattering (SAXS) is a well established technique to detect nanometer scale structures in matter. In a typical setup, this diagnostic uses a detector with a direct line of sight to the scattering target. However, in the harsh environment of high intensity laser interaction, intense secondary radiation and high-energy particles are generated. Such a setup would therefore suffer a significant increase of noise due to this background, which could eventually prevent such measurements. In this paper, we present a novel tool consisting of a mosaic graphite crystal that works as a mirror for the SAXS signal and allows us to position the detector behind appropriate shielding. This paper studies the performance of this mirror both by experiment at the European XFEL (X-Ray Free-Electron Laser Facility) laboratory and by simulations.

Laboratory study of stationary accretion shock relevant to astrophysical systems.

Accretion processes play a crucial role in a wide variety of astrophysical systems. Of particular interest are magnetic cataclysmic variables, where, plasma flow is directed along the star's magnetic field lines onto its poles. A stationary shock is formed, several hundred kilometres above the stellar surface; a distance far too small to be resolved with today's telescopes. Here, we report the results of an analogous laboratory experiment which recreates this astrophysical system. The dynamics of the laboratory system are strongly influenced by the interplay of material, thermal, magnetic and radiative effects, allowing a steady shock to form at a constant distance from a stationary obstacle. Our results demonstrate that a significant amount of plasma is ejected in the lateral direction; a phenomenon that is under-estimated in typical magnetohydrodynamic simulations and often neglected in astrophysical models. This changes the properties of the post-shock region considerably and has important implications for many astrophysical studies.

Evidence for Crystalline Structure in Dynamically-Compressed Polyethylene up to 200 GPa.

We investigated the high-pressure behavior of polyethylene (CH2) by probing dynamically-compressed samples with X-ray diffraction. At pressures up to 200 GPa, comparable to those present inside icy giant planets (Uranus, Neptune), shock-compressed polyethylene retains a polymer crystal structure, from which we infer the presence of significant covalent bonding. The A2/m structure which we observe has previously been seen at significantly lower pressures, and the equation of state measured agrees with our findings. This result appears to contrast with recent data from shock-compressed polystyrene (CH) at higher temperatures, which demonstrated demixing and recrystallization into a diamond lattice, implying the breaking of the original chemical bonds. As such chemical processes have significant implications for the structure and energy transfer within ice giants, our results highlight the need for a deeper understanding of the chemistry of high pressure hydrocarbons, and the importance of better constraining planetary temperature profiles.

High resolution x-ray Thomson scattering measurements from cryogenic hydrogen jets using the linac coherent light source.

We present the first spectrally resolved measurements of x-rays scattered from cryogenic hydrogen jets in the single photon counting limit. The 120 Hz capabilities of the LCLS, together with a novel hydrogen jet design [J. B. Kim et al., Rev. Sci. Instrum. (these proceedings)], allow for the ability to record a near background free spectrum. Such high-dynamic-range x-ray scattering measurements enable a platform to study ultra-fast, laser-driven, heating dynamics of hydrogen plasmas. This measurement has been achieved using two highly annealed pyrolytic graphite crystal spectrometers to spectrally resolve 5.5 keV x-rays elastically and inelastically scattered from cryogenic hydrogen and focused on Cornell-SLAC pixel array detectors [S. Herrmann et al., Nucl. Instrum. Methods Phys. Res., Sect. A 718, 550 (2013)].

ß-endorphins Plasma Level is Higher in Lean Polycystic Ovary Syndrome (PCOS) Women.

AIM: The evaluation the ß-endorphin plasma levels in lean women with polycystic ovary syndrome as well as in women without this disorder. The associations between ß-endorphins and other laboratory parameters were also investigated. MATERIALS AND METHODS: 31 women lean, defined as women with normal range body mass index, 15 with polycystic ovary syndrome and 16 without this disorder were included to the study. In all the patients the level of ß-endorphins was measured. Also the diagnostic laboratory profile including hormone assessment was made in all patients. RESULTS: There were significant differences in ß-endorphin levels between the 2 groups. The ß-endorphin level was higher in the polycystic ovary syndrome group compared to the healthy controls (15.5±4.37 pg/ml vs. 6.9±2.47 pg/ml, p<0.0001). The ß-endorphin levels positively correlated with cortisol at 8 am (R=0.632, p=0.011) and negatively correlated with sex hormone binding globuline (R=0.518, p=0.0478) in polycystic ovary syndrome group. Increase in ß-endorphin level of 1 pg/ml was associated with an increase of cortisol at 8 am level of 1.134 µg/dl and decrease of sex hormone binding globuline of 0.948 nmol/l in polycystic ovary syndrome group. CONCLUSION: Our study showed that the levels of ß-endorphins were significantly higher in lean patients with polycystic ovary syndrome than in lean controls. Moreover, ß-endorphins levels were found to be correlated with other hormonal parameters. In this respect, ß-endorphins may play a role in polycystic ovary syndrome pathophysiology.

Experimental demonstration of an inertial collimation mechanism in nested outflows.

Interaction between a central outflow and a surrounding wind is common in astrophysical sources powered by accretion. Understanding how the interaction might help to collimate the inner central outflow is of interest for assessing astrophysical jet formation paradigms. In this context, we studied the interaction between two nested supersonic plasma flows generated by focusing a long-pulse high-energy laser beam onto a solid target. A nested geometry was created by shaping the energy distribution at the focal spot with a dedicated phase plate. Optical and x-ray diagnostics were used to study the interacting flows. Experimental results and numerical hydrodynamic simulations indeed show the formation of strongly collimated jets. Our work experimentally confirms the "shock-focused inertial confinement" mechanism proposed in previous theoretical astrophysics investigations.

NAIS: nuclear activation-based imaging spectroscopy.

In recent years, the development of high power laser systems led to focussed intensities of more than 10(22) W/cm(2) at high pulse energies. Furthermore, both, the advanced high power lasers and the development of sophisticated laser particle acceleration mechanisms facilitate the generation of high energetic particle beams at high fluxes. The challenge of imaging detector systems is to acquire the properties of the high flux beam spatially and spectrally resolved. The limitations of most detector systems are saturation effects. These conventional detectors are based on scintillators, semiconductors, or radiation sensitive films. We present a nuclear activation-based imaging spectroscopy method, which is called NAIS, for the characterization of laser accelerated proton beams. The offline detector system is a combination of stacked metal foils and imaging plates (IP). After the irradiation of the stacked foils they become activated by nuclear reactions, emitting gamma decay radiation. In the next step, an autoradiography of the activated foils using IPs and an analysis routine lead to a spectrally and spatially resolved beam profile. In addition, we present an absolute calibration method for IPs.

Energy loss and charge transfer of argon in a laser-generated carbon plasma.

This Letter reports on the measurement of the energy loss and the projectile charge states of argon ions at an energy of 4 MeV/u penetrating a fully ionized carbon plasma. The plasma of n(e)≈10(20) cm(-3) and T(e)≈180 eV is created by two laser beams at λ(Las)=532 nm incident from opposite sides on a thin carbon foil. The resulting plasma is spatially homogenous and allows us to record precise experimental data. The data show an increase of a factor of 2 in the stopping power which is in very good agreement with a specifically developed Monte Carlo code, that allows the calculation of the heavy ion beam's charge state distribution and its energy loss in the plasma.

Development of a Nomarski-type multi-frame interferometer as a time and space resolving diagnostics for the free electron density of laser-generated plasma.

This article reports on the development and set-up of a Nomarski-type multi-frame interferometer as a time and space resolving diagnostics of the free electron density in laser-generated plasma. The interferometer allows the recording of a series of 4 images within 6 ns of a single laser-plasma interaction. For the setup presented here, the minimal accessible free electron density is 5 × 10(18) cm(-3), the maximal one is 2 × 10(20) cm(-3). Furthermore, it provides a resolution of the electron density in space of 50 µm and in time of 0.5 ns for one image with a customizable magnification in space for each of the 4 images. The electron density was evaluated from the interferograms using an Abel inversion algorithm. The functionality of the system was proven during first experiments and the experimental results are presented and discussed. A ray tracing procedure was realized to verify the interferometry pictures taken. In particular, the experimental results are compared to simulations and show excellent agreement, providing a conclusive picture of the evolution of the electron density distribution.

Energy loss of argon in a laser-generated carbon plasma.

The experimental data presented in this paper address the energy loss determination for argon at 4 MeV/u projectile energy in laser-generated carbon plasma covering a huge parameter range in density and temperature. Furthermore, a consistent theoretical description of the projectile charge state evolution via a Monte Carlo code is combined with an improved version of the CasP code that allows us to calculate the contributions to the stopping power of bound and free electrons for each projectile charge state. This approach gets rid of any effective charge description of the stopping power. Comparison of experimental data and theoretical results allows us to judge the influence of different plasma parameters.

Ultrafast melting of carbon induced by intense proton beams.

Laser-produced proton beams have been used to achieve ultrafast volumetric heating of carbon samples at solid density. The isochoric melting of carbon was probed by a scattering of x rays from a secondary laser-produced plasma. From the scattering signal, we have deduced the fraction of the material that was melted by the inhomogeneous heating. The results are compared to different theoretical approaches for the equation of state which suggests modifications from standard models.

Evolution of elastic x-ray scattering in laser-shocked warm dense lithium.

We have studied the dynamics of warm dense Li with near-elastic x-ray scattering. Li foils were heated and compressed using shock waves driven by 4-ns-long laser pulses. Separate 1-ns-long laser pulses were used to generate a bright source of 2.96 keV Cl Ly- alpha photons for x-ray scattering, and the spectrum of scattered photons was recorded at a scattering angle of 120 degrees using a highly oriented pyrolytic graphite crystal operated in the von Hamos geometry. A variable delay between the heater and backlighter laser beams measured the scattering time evolution. Comparison with radiation-hydrodynamics simulations shows that the plasma is highly coupled during the first several nanoseconds, then relaxes to a moderate coupling state at later times. Near-elastic scattering amplitudes have been successfully simulated using the screened one-component plasma model. Our main finding is that the near-elastic scattering amplitudes are quite sensitive to the mean ionization state Z[over ] and by extension to the choice of ionization model in the radiation-hydrodynamics simulations used to predict plasma properties within the shocked Li.

Measurements of ionic structure in shock compressed lithium hydride from ultrafast x-ray Thomson scattering.

We present the first ultrafast temporally, spectrally, and angularly resolved x-ray scattering measurements from shock-compressed matter. The experimental spectra yield the absolute elastic and inelastic scattering intensities from the measured density of free electrons. Laser-compressed lithium-hydride samples are well characterized by inelastic Compton and plasmon scattering of a K-alpha x-ray probe providing independent measurements of temperature and density. The data show excellent agreement with the total intensity and structure when using the two-species form factor and accounting for the screening of ion-ion interactions.

Effects of irradiation on development of Theiler's murine encephalomyelitis virus (TMEV)-induced demyelinating disease in genetically resistant mice.

Theiler's murine encephalomyelitis virus-induced demyelinating disease (TMEV-IDD), a model for multiple sclerosis, is a chronic T cell-mediated disease. Development of clinical symptoms in susceptible mouse strains generally correlates with TMEV-specific delayed-type hypersensitivity (DTH) responses. These responses, minimal or absent in resistant mouse strains, have been proposed as the pathogenic basis for the central nervous system inflammation and demyelination characterizing the disease. We demonstrate here that normally resistant (C57BL/6 x DBA/2)F1 hybrid mice develop clinical symptoms and DTH responses against TMEV after low doses of gamma-irradiation. Parental C57BL/6 animals remain resistant after similar pretreatment. Thus low-dose irradiation elicits a "latent" susceptibility to TMEV-IDD in some, but not all, resistant mice. Adoptively transferred spleen cells from syngeneic, unirradiated donors reconfer resistance on irradiated, infected B6D2F1 hybrids and reduce DTH responsiveness against TMEV, suggesting a protective role for a radiation-sensitive splenic population(s). The closely related C57BL/6 and C57BL/10 strains differ with respect to intrinsic and latent susceptibility.

Induction of Theiler's murine encephalomyelitis virus (TMEV)-induced demyelinating disease in genetically resistant mice.

Theiler's murine encephalomyelitis virus-induced demyelinating disease, a murine model for multiple sclerosis, is the result of persistent infection which leads to a T cell-mediated immunopathology. Susceptible strains develop virus-specific DTH responses while resistant strains do not, and this response has been proposed as the basis for inflammation and demyelination. (C57BL/6 x DBA/2)F1 hybrid animals, normally resistant to TMEV-induced demyelinating disease, become susceptible when treated in vivo prior to infection with low dose cyclophosphamide. Comparable pretreatment of other resistant animals, C57BL/6 and CB6 (BALB/c x C57BL/6) F1 hybrids, does not render them susceptible (despite the H-2 identity of CB6F1 and B6D2F1 hybrids). Thus the "latent" susceptibility in B6D2F1 hybrids must be attributed to non-H-2 genes from the susceptible D2 parent. Resistance can be restored to CY-treated B6D2F1 animals by the adoptive transfer of splenic cells (including T cell enriched populations) from non-CY-treated donors. Resistance to TMEV-IDD in these animals, therefore, may involve active inhibition of a "latent" disease susceptibility.

Subcutaneous or topical administration of 16,16 dimethyl prostaglandin E2 protects from radiation-induced alopecia in mice.

Alopecia, a common sequel of radiation treatment of brain tumors, increases patient stress to the extent that refusal of treatment may occur. The expectation that loss of hair will be prevented, or that regrowth will occur, is extremely important to patients. To investigate prostaglandin-induced radiation protection against alopecia, the hair of B6D2F1 male mice was plucked from the right thigh and surrounding area to induce anagen. Fourteen days later, mice were injected subcutaneously in the neck with 10 micrograms 16,16 dm PGE2 in 0.2 ml of vehicle, or with the vehicle alone. In another group of previously plucked mice, 16,16 dm PGE2 in the same concentration, or the vehicle was applied topically. One hour later, graded single doses from 6.5 to 12.5 Gy 137Cs gamma irradiation were given to groups of six animals. On day 21 post-plucking, all animals were killed and a portion of the irradiated site was excised. The average hair counts per field in irradiated animals were 85 +/- 4 (6.5 Gy), 25 +/- 5 (8.5 Gy), and 5.5 +/- 0.7 (10 Gy). Animals receiving the prostaglandin systemically had values of 60 +/- 10 (6.5 Gy), 54 +/- 3 (8.5 Gy), 66 +/- 6 (10 Gy), and 30.1 +/- 8 (12.5 Gy). Topical application of the prostaglandin resulted in protection that yielded 52 +/- 3 (8.5 Gy), 34 +/- 4 (10 Gy), and 3.2 +/- 0.9 (12.5 Gy) hairs per field. Both systemic and topical application of 16,16 dm PGE2 protected from some degree of radiation-induced alopecia, which supports the conclusion that prostaglandins may be useful in the protection of hair follicles in patients treated with radiation for brain tumors.