On Thu, 11 May 2017 17:17:55 -0400 Adam Jackson ,ajax at redhat.com, wrote: , C99 isnt enough on its own to get POSIX feature sets defined. , , Signed-off-by: Adam Jackson ,ajax at redhat.com, , --- , include/meson.build , 3 +++ , 1 file changed, 3 insertions(+) , , diff --git a/include/meson.build b/include/meson.build , index 358e04976..2f8882803 100644 , --- a/include/meson.build , +++ b/include/meson.build , @@ -4,7 +4,10 @@ dri_dep = dependency(dri, required: build_dri2 or build_dri3) , conf_data = configuration_data() , conf_data.set(_DIX_CONFIG_H_, 1) , , + , + , conf_data.set(MONOTONIC_CLOCK, cc.compiles( , + #define _POSIX_C_SOURCE 200112L , #include ,time.h, , #include ,unistd.h, , #ifndef CLOCK_MONOTONIC Hi Adam, this indeed fixes the CLOCK_MONOTONIC for me. The whole xserver build succeeds now, just a few screenfuls of compiler warnings, no errors. For both patches: Tested-by: Pekka Paalanen ,pekka.paalanen at collabora.co.uk, Thanks, pq -------------- next part ...

Looking for B meson? Find out information about B meson. An elementary particle with strong nuclear interactions, baryon number B = 0, spin J = 0, positive parity, negative charge parity, isotopic spin I = 1, and... Explanation of B meson

This patchset adds the test/test/test app to the Meson build. In doing so, the test app is improved to allow running a unit test by setting an environment variable. This allows the meson test infrastructure to integrate with the DPDK tests. Some nice improvements from the above integration, including debug aids... Run all autotests: $ meson test Run a specific test: $ meson test ring_perf_autotest Run a specific test multiple times, eg brute-forcing race conditions: $ meson test eventdev_sw_autotest --repeat=3 Run a specific test multiple times in gdb, eg to drop to GDB if race found: $ meson test eventdev_sw_autotest --repeat=3 --gdb Meson also provides various options to wrap the test binary, which can be used for running in eg: Valgrind or other tools. For more information about Meson and its testing capabilities, see here: http://mesonbuild.com/Unit-tests.html Cheers, -Harry Harry van Haaren (2): test: use env variable to run test if set meson: add tests app to build meson.build , 1 + ...

The proposed mechanism should be at work in any generalization of standard model claiming to explain neutrino masses and their mixing without flavor changing neutral currents. If the observed anomaly is different from this prediction, one can start to search for new physics explanations but before this brane constructions in multiverse are not perhaps the best possible strategy. What about the anomalies related to B meson decays? The model that Lubos refers to tries to explain also the anomalies related to semileptonic decays of neutral B meson. Neutrino mixing is certainly not a natural candidate if one wants to explain the 2.5 sigma anomalies reported for the decays of B meson to K meson plus muon pair. Lubos has a nice posting about surprisingly many anomalies related to the leptonic and pion and kaon decays of neutral B meson. Tommaso Dorigo tells about 4-sigma evidence for new physics in rare G boson decays. There is also an anomaly related to the decay of neutral B meson to muon pair ...

Abstract: Exclusive production of $\omega$ mesons was studied at the COMPASS experiment by scattering $160~\mathrm{GeV}/\mathit{c}$ muons off transversely polarised protons. Five single-spin and three double-spin azimuthal asymmetries were measured in the range of photon virtuality $1~(\mathrm{GeV}/\mathit{c})^2 , Q^2 , 10~(\mathrm{GeV}/\mathit{c})^2$, Bjorken scaling variable $0.003 , x_{\mathit{Bj}} , 0.3$ and transverse momentum squared of the $\omega$ meson $0.05~(\mathrm{GeV}/\mathit{c})^2 , p_{T}^{2} , 0.5~(\mathrm{GeV}/\mathit{c})^2$. The measured asymmetries are sensitive to the nucleon helicity-flip Generalised Parton Distributions (GPD) $E$ that are related to the orbital angular momentum of quarks, the chiral-odd GPDs $H_{T}$ that are related to the transversity Parton Distribution Functions, and the sign of the $\pi\omega$ transition form factor. The results are compared to recent calculations of a GPD-based model ...

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Abstract: I discuss the theoretical status of the `soft pomeron and its place in describing generic diffractive processes. The role of perturbative QCD (pQCD) corrections is considered, in particular in the context of quasi-elastic vector meson production at high $Q^2$. In those processes where short distances are dominant, the `hard (pQCD) pomeron is expected to reveal itself, such a process may well be that of diffractive vector meson production at high-$t$ and I discuss this ...

As with any typical buildsystem, correct incremental builds is the most significant speed feature (because all incremental progress is discarded whenever the user is forced to do a clean build). Unlike bare Make, the separate configure step ensures that changes to arguments, environment variables and command output are not partially applied in subsequent builds, which would lead to a stale build. Like Ninja, Meson does not support globbing of source files.[6] By requiring all source files to be listed in the build definition files, the build definition file timestamps are sufficient to determine if the set of source files has changed, thereby ensuring that removed source files are detected. CMake supports globbing, but recommends against it for the same reason.[8] Meson uses ccache automatically if installed. It also detects changes to symbol tables of shared libraries to skip relinking executables against the library when there are no ABI changes. Precompiled headers are supported, but requires ...

We compute the masses of the pseudoscalar mesons π+ , K0 and D+ at finite temperature and baryon chemical potential. The computations are based on a symmetry- preserving Dyson-Schwinger equation treatment of a vector-vector four quark contact interaction. The results found for the temperature dependence of the meson masses are in qualitative agreement with lattice QCD data and QCD sum rules calculations. The chemical potential dependence of the masses provide a novel prediction of the present computation.. ...

books.google.comhttps://books.google.com/books/about/The_spectator_process_in_the_production.html?id=mU1ZAAAAYAAJ&utm_source=gb-gplus-shareThe spectator process in the production of single negative pi mesons from the neutron in deuterium by photons of energy from threshold to 1 bev ...

Meson Atlantico, Tenerife Picture: nice frozen strawberry daiquiri - Check out Tripadvisor members 97 candid photos and videos.

meson (mē´zŏn) [Gr.,=middle (i.e., middleweight)], class of elementary particles [1] whose masses are generally between those of the lepton [2] class of lighter particles and those of the baryon [3] class of heavier particles.

The first demonstration of laser spectroscopy of a meson, achieved at PSIs πE5 beamline, opens up new avenues for precision studies of exotic atoms.

diff --git a/meson.build b/meson.build index f42ed16..c0f741e 100644 --- a/meson.build +++ b/meson.build @@ -81 +81 @@ foreach ident : [ - have = cc.has_function(ident[0], prefix : ident[1]) + have = cc.has_function(ident[0], args : -D_GNU_SOURCE, prefix : ident[1]) ...

Our data has the striking feature that the cross section is very small at [...] in the region of the second and third pion nucleon resonances. Also, although the data is not inconsistent with a simple first, second and third resonance model, it appears likely that above the third resonance the pole process consisting of the exchange of a single vector meson is becoming important or even dominant. The evidence at this time mildly suggests that this behaviour is largely due to [...] mesons and under that hypothesis we are able to estimate some [...] meson coupling constants. For example, using a prescription of Gell-Mann and Zachariasen, we estimate the partial width for the decay [...] to be 240 Kev. ...

An invariant differential cross section measure- ment of inclusive π 0 and η meson production at mid-rapidity in pp collisions at √s = 8 TeV was carried out by the ALICE experiment at the LHC. The spectra of π0 and η mesons were measured in transverse momentum ranges of 0.3 , pT , 35GeV/cand0.5 , pT , 35GeV/c, respectively. Next-to-leading order perturbative QCD cal- culations using fragmentation functions DSS14 for the π0 and AESSS for the η overestimate the cross sections of both neutral mesonns, although such calculations agree with the measured η/π0 ratio within uncertainties. The results were also compared with PYTHIA 8.2 predictions for which the Monash 2013 tune yields the best agreement with the mea- sured neutral meson spectra. The measurements confirm a universal behavior of the η/π 0 ratio seen for NA27, PHENIX and ALICE data for pp collisions from √s = 27.5 GeV to √s = 8 TeV within experimental uncertainties. A rela- tion between the π0 and η production cross ...

This thesis has two parts with different topics in particle physics. In part I, we consider various linear sigma models and their applications to scalar mesons. It is shown that the tree amplitude for ππ scattering in the minimal linear sigma model has an exact expression which induces an infinite geometric series in which the pattern for both the I = 0 and I = 2 s-wave scattering lengths to orders $p^2$, $p^4$ and $p^6$ seems to agree with chiral perturbation theory predictions. The model is then gauged to study the mass differences between the vector meson and the axial vector meson as a possibly useful template for the role of a light scalar in QCD as well as for (at a different scale) an effective Higgs sector for some recently proposed walking technicolor models. The model is applied to the s-wave pion-pion scattering in QCD. Both the near threshold region and (with an assumed unitarization) the global region up to about 800 MeV are considered. It is noted that there is a little tension

The measurement of the Bs-, mu mu and Bd-,mu mu decays is one of the flagships of the LHCb experiment, the latest result in combination with CMS has recently been published on Nature. The aim of this project is to study the yields of other decays with a J/Psi in the final state, like B+ -, J/Psi K+ and Bs-, J/Psi Phi, that can be detected triggering on the muons decay products of the J/Psi. These yields are a crucial input to obtain the Bs-, mu mu and Bd-,mu mu decays branching fraction as they provide a relative normalization. Moreover, in order to use Bd decays to normalize the Bs-, mu mu yields we need to measure the relative probabilities for a b quark to hadronize into a Bs (f_s) or a Bd (f_d) meson, that can also be obtained from B+ -, J/Psi K+, Bs-, J/Psi Phi and Bd-, J/Psi K* decays. The ratio f_s/f_d is not a constant and is therefore important to measure it as a function of both the energy in the center of mass of the pp collision and the B mesons kinematics. The combination of ...

A measurement of the Bs0 decay parameters in the Bs0 → J/ψϕ channel using an integrated luminosity of 14.3 fb−1 collected by the ATLAS detector from 8 TeV pp collisions at the LHC is presented. The measured parameters include the CP -violating phase ϕs, the decay width Γs and the width difference between the mass eigenstates ΔΓs. The values measured for the physical parameters are statistically combined with those from 4.9 fb−1 of 7 TeV data, leading to the following ...

The experimental collaboration -- now composed of 70 scientists from Canada, Japan, Russia and the United States, (see: http://www.phy.bnl.gov/E949/, Collaboration List) -- has been conducting the search for the past decade at the Alternating Gradient Synchrotron, a particle accelerator at Brookhaven Lab that produces the world s most intense beams of K mesons. K mesons are elusive particles that exist for only 12 billionths of a second before decaying into other forms. So, to catch the fleeting events and identify the rare decay, the scientists built a state-of-the-art particle detector the size of a small house, capable of examining 1.6 million decays every second. Interesting events get recorded on tape, with several tens of thousands of gigabytes of data stored so far. The physicists then use sophisticated software to pore over the data to find the most interesting events and examine them in exquisite detail ...

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An experimental study of [omega] photoproduction on the proton was conducted by using the Crystal Ball and TAPS multiphoton spectrometers together with the photon tagging facility at the Mainz Microtron MAMI. The [gamma] p [right arrow] [omega] p differential cross sections are measured from threshold to the incident-photon energy E[subscript gamma] = 1.40 GeV (W = 1.87 GeV for the center-of-mass energy) with 15-MeV binning in E[subscript gamma] and full production-angle coverage. The quality of the present data near threshold gives access to a variety of interesting physics aspects. As an example, an estimation of the [omega]N scattering length [alpha subscript omega]p is provided ...

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Test-Label: intel-Performance-Testing Test-Status: SUCCESS http://dpdk.org/patch/48625 _Performance Testing PASS_ Submitter: Gavin Hu ,gavin.hu at arm.com, Date: Tuesday, December 11 2018 03:55:50 DPDK git baseline: Repo:dpdk Branch: master CommitID:b0aa225b45e102a1eba2215e3a75b5683d8435f2 48625 --, performance testing pass Test environment and result as below: Ubuntu 17.10 Kernel: 4.13.0-43-generic GCC: gcc (Ubuntu 7.2.0-8ubuntu3) 7.2.0 NIC: Intel Corporation Ethernet Converged Network Adapter XL710-QDA2 40000 Mbps Target: x86_64-native-linuxapp-gcc Fail/Total: 0/2 Detail performance results: +------------+---------+-------------------------------------+ , frame_size , txd/rxd , throughput difference from expected , +============+=========+=====================================+ , 64 , 512 , -0.221 , +------------+---------+-------------------------------------+ , 64 , 2048 , 0.749 , +------------+---------+-------------------------------------+ Ubuntu 17.10 Kernel: 4.13.0-43-generic GCC: gcc ...

Re: [dpdk-dev] [PATCH v2 3/5] test/hash: add lock free reader writer functional tests 2020-02-05 16:22 ` Honnappa Nagarahalli @ 2020-02-05 16:41 ` David Marchand 2020-02-05 19:34 ` Wang, Yipeng1 0 siblings, 1 reply; 38+ messages in thread From: David Marchand @ 2020-02-05 16:41 UTC (permalink / raw) To: Honnappa Nagarahalli Cc: Amit Gupta, Wang, Yipeng1, Gobriel, Sameh, thomas, dev, nd On Wed, Feb 5, 2020 at 5:22 PM Honnappa Nagarahalli ,[email protected], wrote: , , , , , On Mon, Feb 3, 2020 at 8:49 PM Honnappa Nagarahalli , , ,[email protected], wrote: , , , , , , Add lock-free reader writer concurrency functional tests. , , , These tests will provide the same coverage that non lock-free APIs , , , have. , , , , , , Signed-off-by: Honnappa Nagarahalli ,[email protected], , , , --- , , , app/test/test_hash_readwrite.c , 58 , , , +++++++++++++++++++++------------- , , , 1 file changed, 36 insertions(+), 22 deletions(-) , , , , , , diff --git ...

This test case has the same tests as tests/virtio-blk-test.c except for tests have block_resize. Since vhost-user server can only server one client one time, two instances of vhost-user-blk-server are started by qemu-storage-daemon for the hotplug test. In order to not block scripts/tap-driver.pl, vhost-user-blk-server will send quit command to qemu-storage-daemons QMP monitor. So a function is added to libqtest.c to establish socket connection with socket server. Suggested-by: Thomas Huth ,[email protected], Signed-off-by: Coiby Xu ,[email protected], --- tests/qtest/libqos/libqtest.h , 17 + tests/qtest/libqos/meson.build , 1 + tests/qtest/libqos/vhost-user-blk.c , 129 +++++ tests/qtest/libqos/vhost-user-blk.h , 48 ++ tests/qtest/libqtest.c , 36 +- tests/qtest/meson.build , 4 +- tests/qtest/vhost-user-blk-test.c , 751 ++++++++++++++++++++++++++++ 7 files changed, 983 insertions(+), 3 deletions(-) create mode 100644 tests/qtest/libqos/vhost-user-blk.c create mode 100644 ...

In Archived 2011-10-09 at the Wayback Machine International Journal of Innovation, Management and job-ready) 2( 1), ebook cp violation in bs0 gt jpsiphi decays measured locations, crucial), 119-142, 2011. thousands of tracked book situ . intensities of the National Academy of Sciences of the United States of America. Steven Bird, Ewan Klein, and Edward Loper( 2009). Natural Language Processing with Python. Daniel Jurafsky and James H. Speech and Language Processing, profesional spectrum. Mohamed Zakaria Kurdi( 2016). Natural Language Processing and Computational Linguistics: molecule, click, and harvesting, node 1. Mohamed Zakaria Kurdi( 2017). Natural Language Processing and Computational Linguistics: dynamics, entry, and documents, microscope 2. fraction to Information Retrieval. Cambridge University Press. sure ebook cp violation in bs0 gt jpsiphi decays measured with and chlorophyll processes misguided without Localization. follicles of Statistical Natural Language Processing. Machine ...

The Large High Altitude Air Shower Observatory (LHAASO) will be constructed at 4400 m asl in Daocheng, Sichuan Province, with the aim of discovering sources of ultra-high energy cosmic rays and studying cosmic ray physics. The whole array includes 1171 muon detectors (MDs), constituting the largest muon detector array in the world. The special high altitude and wide-field environment requires simple and stable calibration as well as monitoring method of MDs. In this paper, the muon decay events will be selected for calibrating the charge and monitoring the water level of each MD. In the prototype muon detector, the simulation and experiment results reveal that the charge of the decay electron is approximately 0.147 times that of the vertical equivalent muon for a standard MD, and the QVEM/Qe shows a linear correlation with the water level ...

Number 600 August 1, 2002 by Phillip F. Schewe, Ben Stein, and James Riordon HIGH PRECISION TESTS OF THE STANDARD MODEL have been reported this past week in two areas: CP-violation in B mesons (experiments at the KEK lab in Japan and the SLAC lab in California) and the magnetic moment of the muon (an experiment at the Brookhaven lab in New York). The standard model, trying to explain the forces of nature through the exchange of particles, consists of the electroweak framework (force exchanged by photons and by Z and W bosons) plus the quantum chromodynamic (QCD) framework for quarks (force exchanged by gluons). The model has been highly successful in accounting for the behavior of electrons in atoms (in the case of some transition frequencies, theory and experiment agree at the parts-per-trillion level or better) and does a good job of predicting other phenomena as well, such as CP violation. The model does not include, but can accommodate, neutrino oscillation. Extensions of the standard model, ...

Dr. Kenneth Kiers, Professor of Physics at Taylor University, specializes in [b meson physics, chaos and encryption with electrical circuits, cp violation, extensions of the standard model, higgs physics, left-right model, mathematical methods in physics, multi-higgs models, neutrino physics, particle physics theory, phenomenology, quantum mechanics, supersymmetry, top quark physics].

Magnetic ground state and spin fluctuations in MnGe chiral magnet as studied by muon spin rotation N. Martin, M. Deutsch, F. Bert, D. Andreica, A. Amato, P. Bonfa, R. De Renzi, U. K. Roessler, P. Bonville, L. N. Fomicheva, A. V. Tsvyashchenko, and I. Mirebeau Phys. Rev. B 93 (2016) 174405. We have studied by muon spin resonance the helical ground state and fluctuating chiral phase recently observed in the MnGe chiral magnet. At low temperature, the muon polarization shows double-period oscillations at short-time scales. Their analysis, akin to that recently developed for MnSi [A. Amato et al., Phys. Rev. B 89, 184425 (2014)], provides an estimation of the field distribution induced by the Mn helical order at the muon site. The refined muon position agrees nicely with ab initio calculations. With increasing temperature, an inhomogeneous fluctuating chiral phase sets in, characterized by two well-separated frequency ranges which coexist in the sample. Rapid and slow fluctuations, respectively,

Usage of secondary cosmic muons to image the geological structures density distribution significantly developed during the past ten years. Recent applications demonstrate the method interest to monitor magma ascent and volcanic gas movements inside volcanoes. Muon radiography could be used to monitor density variations in aquifers and the critical zone in the near surface. However, the time resolution achievable by muon radiography monitoring remains poorly studied. It is biased by fluctuation sources exterior to the target, and statistically affected by the limited number of particles detected during the experiment. The present study documents these two issues within a simple and well constrained experimental context: a water tower. We use the data to discuss the influence of atmospheric variability that perturbs the signal, and propose correction formulas to extract the muon flux variations related to the water level changes. Statistical developments establish the feasibility domain of muon

Abstract : The NA48 experiment at CERN has performed a new measurement of direct CP violation, based on data taken in 1997 00 qy Z X . by simultaneously collecting K and K decays into pp and pp. The result for the CP violating parameter Re r LS ZZ.Z.. y4 is 18.54.5 stat 5.8 syst =10 . q 1999 Elsevier Science B.V. All rights reserved. 1 Present address: CERN, CH-1211 Geneva 23, Switzerland. 2 Present address: Physics-Astronomy Building, Michigan State University, East Lansing, MI 48824 USA. 3 Present address: NIKHEF, PO Box 41882, 1009 DB Amsterdam, The Netherlands. 4 Present address: Department of Physics, Wayne State University, Detroit, MI 48201, USA. 5 Funded by the UK Particle Physics and Astronomy Research Council. 6 Z. Present address: Universitat Karlsruhe TH , Fakultat fur Physik, and Forschungszentrum Karlsruhe GmbH, Institut fur Kernphysik, D-76128 Karlsruhe. 7 Present address: DSMrDAPNIA - CEA Saclay, F-91191 Gif-sur-Yvette, France. 8 Present address: Dipar ...

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Denier. Yes, sadly human nature is so weak and despicable and what you say holds truth, and yet there are some noble exceptions whose magnanimous souls and angelic nature love truth for its own sake and show unselfish altruism if encouraged. The outputs of LENR are mostly strange matter mesons, pion and muons. Excess heat is not always produced by the LENR reaction. Leif Holmlid, one of those pure and rare souls who has devoted his life to science and the pursuit of truth will attempt to show subatomic particle production this summer by placing a miniaturized version of his experiment inside a full scale particle detector in an attempt to document how a chemical catalyst can produce subatomic particle emissions. One of his associates who is working on downsizing his experiment told me about this effort to be attempted this summer. I have discounted LENR as a viable and egalitarian energy technology. This unregulated and widespread common usage of the LENR reaction seems to be the dream and ...

SECTIONS. 0. OVERVIEW PAPERS and FOUNDATIONS. 1. The UNIFIED FIELD. Newton, Lagrange, Coulomb and Maxwell all gave us UFTs.. 2. RELATIVITY. Relativity is true; many of the equations are not. The muon, lightclock, Minkowski, Friedmann, Pound-Rebka, and the falsification of gamma.. 3. CALCULUS. The calculus works, despite many fudges and cheats.. 4. QUANTUM PHYSICS. Early mistakes, including superposition, entanglement, tunneling, nonlocality, Bohrs equations.. 5. ELECTROMAGNETICS. Solid-state fudging, current, inductance. Also the Sun and planets. Tides. Bodes Law and interplanetary influences.. 6. GRAVITY. Celestial Mechanics, Laplace, Allais, Cavendish, GOCE, BICEP2, plate tectonics, Roche, vacuum catastrophe, black holes.. 7. QED and QCD. The quantum spin equation. Feynman, Higgs, neutrinos, Landau, mesons, fine structure constant. 8. LIGHT and CHARGE, including dark matter, photons, heat, the Rayleigh equation, blackbody radiation, rainbows, diffraction and refraction.. 9. The ATOMIC ...

A study of charged-current muon neutrino scattering on hydrocarbon in which the final state includes a muon, at least one proton, and no pions is presented. Although this signature has the topology of neutrino quasielastic scattering from neutrons, the event sample contains contributions from quasielastic and inelastic processes where pions are absorbed in the nucleus. The analysis accepts events with muon production angles up to 70° and proton kinetic energies greater than 110 MeV. The cross section, when based completely on hadronic kinematics, is well described by a relativistic Fermi gas nuclear model including the neutrino event generator modeling for inelastic processes and particle transportation through the nucleus. This is in contrast to the quasielastic cross section based on muon kinematics, which is best described by an extended model that incorporates multinucleon correlations. As a result, this measurement guides the formulation of a complete description of neutrino-nucleus ...

In this paper we study O(2000) (quenched) lattice configurations from the APE collaboration, for different lattice volumes and for 6.0 \le beta \le 6.4 using both the Wilson and the SW-Clover fermion actions. We determine the light hadronic spectrum and meson decay constants and study the mesonic dispersion relation. We extract the hadronic variable J and the strange quark mass in the continuum at the next-to-leading order obtaining m_s~{MSbar}(mu=2 GeV) = 122 +/- 20 MeV. A study is made of their dependence on lattice spacing. We implement a newly developed technique to extract the inverse lattice spacing using data at the simulated values of the quark mass (i.e. at masses around the strange quark mass ...

The Kaos spectrometer with its short design is used to study the structure of hadrons in (e,eK) reactions. An important measurement program on the Kaos spectrometer includes the generation of kaons at forward angles. In another program, φ mesons are to be generated inside atomic nuclei and detected by their decay into two kaons. This study allows conclusions to be drawn about quasi-stationary states in cold nuclei at normal nuclear density. The theoretical description of such a system of strongly interacting particles takes up models of the internal structure of hadrons, as well as far-reaching questions about the formation of nuclear structures. For the medium-term future, the scientific program of the project also includes the kaon-associated production of atomic nuclei in which a nucleon has been replaced by a hyperon. The study of these so-called hyperons can shed light on structures that remain hidden in conventional nuclear matter; the hyperon opens up the possibility of selectively ...

We present measurements of the photon beam asymmetry Σ for the reaction γp-,K+Σ0(1193) using the GlueX experiment in Jefferson Labs Hall D. Data were collected using a linearly polarized photon beam with energy range 8.2-8.8 GeV incident on a liquid hydrogen target. Asymmetries are measured as functions of Mandelstam variables t and u. These are the first exclusive measurements of the photon beam asymmetry Σ in this reaction at high energies. In the t-channel, results show that the reaction is dominated by the natural-parity exchange of presumably the K*(892) meson, as predicted by theoretical models. Results obtained for the u-channel are consistent with an intermediate baryon exchange mechanism predicted by theoretical models ...

We present an analysis of the gamma-ray data obtained with the Large Area Telescope (LAT) on board the Fermi Gamma-ray Space Telescope in the direction of SNR W49B (G43.3-0.2). A bright unresolved gamma-ray source detected at a significance of 38 sigma is found to coincide with SNR W49B. The energy spectrum in the 0.2-200 GeV range gradually steepens toward high energies. The luminosity is estimated to be 1.5 x 10(36) (D/8 kpc)(2) erg s(-1) in this energy range. There is no indication that the gamma-ray emission comes from a pulsar. Assuming that the supernova remnant (SNR) shell is the site of gamma-ray production, the observed spectrum can be explained either by the decay of neutral pi mesons produced through the proton-proton collisions or by electron bremsstrahlung. The calculated energy density of relativistic particles responsible for the LAT flux is estimated to be remarkably large, U-e,U-p , 10(4) eV cm(-3), for either gamma-ray production mechanism.. ...

S) (n = 1, two, 3) transitions with partial widths of 300 - 400 keV [1116]. Recently Belle S) (n = 1, two, three) transitions with partial widths of 300 - 400 keV [1116]. Recently Belle reported preliminary outcomes around the observation of (5S) (1S, 2S) and (5S) + - (1D) with anomalously significant prices [985]. Its proposed that these anomalies are because of rescatterings [1123,1124]. The big branching fraction from the (4S) (1S) decay observed in 2010 by BaBar could have a similar origin [1125]. The mechanism can be regarded as either as a rescatter??ing on the D D or B B mesons, or as a http://www.tongji.org/members/shadow2pantry/activity/516070/ contribution of the molecular component towards the quarkonium wave function. ?The model in which Y (4260) is really a D1 (2420) D molecule naturally explains the high probability of the intermediate molecular resonance within the Y (4260) + - J/ transitions [1126,1127] and predicts the Y (4260) X (3872) transitions with high prices [1128]. Such ...

Konstantina graduated from the University of Warwick in 2016 with a master degree in Mathematics and Physics. During her final year she completed a project in particle physics under the supervision of professor Tim Gershon which resulted in the discovery of a new B meson decay mode with the CERN LHCb experiment. She also represented Warwick at iGEM (The International Genetically Engineered Machine Competition) 2016 in Boston as part of a team where the software she developed received a nomination for Best Software Tool and the team received a silver medal. She became interested in quantum engineering recently so she is keen to explore as many aspects of it as possible. As a person with mostly theoretical background she is also excited to spend time in the lab. In her spare time she practices aerial and pole dance with her highest achievement being bronze medal in the IUPDC (Inter-University Pole Dance Competition) 2015, individual intermediate category ...

In hadron physics, experiments using hadronic probes may shed light on open questions on the structure of hadrons, their interactions that are subject to the strong force and on the symmetries of nature. Therefore a major focus of the physics program studied at the COoler SYnchrotron COSY of the Forschungszentrum Juelich is the production of mesons and hyperons in hadron- hadron scattering with the aim to investigate relevant production processes, interactions of the participating particles as well as symmetries and symmetry breaking. The COoler SYnchrotron COSY at Juelich accelerates protons and deuterons with momenta up to 3.7 GeV/c covering hadron physics in the light quark sector. The availability of the beam cooling systems allow precision measurements, using polarized proton and deuteron beams in combination with polarized Hydrogen or Deuterium targets. Due to the excellent experimental conditions at COSY single- and double-polarization measurements can be performed with high reaction ...

Study of parity nonconservation (PNC) in heavy atoms provides atomic-physics test of the electroweak Standard Model and led to a first measurement of the nuclear anapole moment. The PNC interaction leads to a non-zero amplitude for transitions otherwize forbidden by the parity selection rule, such as the 6s-7s transition in cesium. Combining experimental measurements and theoretical calculations of the PNC amplitude permits one to infer the value of the weak charge and compare it with the value predicted by the Standard Model. In this talk, I will give an overview of the status of the parity nonconservation studies in heavy atoms. I will specifically focus on the calculation of the Cs PNC amplitude and the resulting analysis which yielded the value of the weak charge. The PNC experiment in Cs, combined with the calculation of the spin-depended PNC amplitude, also yielded the value of the nuclear anapole moment and allowed us to place constraints on PNC meson coupling constants which were found ...

The SIDDHARTA experiment was performed at the DAFNE an electron-positron collider, tuned in that way to produce very efficient φ mesons at rest, which decay into back-to-back K+K− pairs with a branching ratio of about 49 %. The monochromatic low-energy kaons are stopped efficiently in a gaseous target to produce kaonic hydrogen atoms. The SIDDHARTA setup consists of a cryogenic gaseous hydrogen target working with a pressure 0.1 MPa at a temperature 23 K, resulting in a hydrogen density of 1.3 × 10−3 g/cm3. The cryogenic target cell is surrounded by 144 silicon drift detectors (SDDs), each having an effective area of 1 cm2 and a thickness of 450 µm, developed within a European research project devoted to this experiment. The SDDs have an energy resolution of ∼ 170 eV (FWHM) at 8 keV and timing resolution below 1μsec. ...

Our work in HEP over the last 20 years has proven direct technical and commercial relevance in biotechnology and biomedicine, in environmental sensing and in renewable energy with award-winning innovations, significant sales and strong adoption across many sectors.. This depicts the real-time pollution sensing from the GUSTO team, using algorithms developed for heavy meson decay and recently augmented by Machine Learning and advanced computing systems. The tools have proven applicability in Toxic Industrial Chemicals (over 50 units sold bringing in £ms of revenue), in Chemical Warfare Agent detection (our tools we used in the 2012 London Olympics) an in Air Quality Monitoring (as shown above: over 8m people a year die from pollution, and over 20% of London school children have pollution-related asthma.) We showed for the first time the concept of Representativeness: you can measure pollution successfully only if you have a mobile system, excellent geographical and spatial accuracy and time ...

The Proton Treatment Facility is located on the lower level of meson hall, next to the cyclotron vault. Protons, accelerated by the cyclotron, are first tuned by the main control room before being used in the treatment of the eye tumour.. The facility is operated in conjunction with the British Columbia Cancer Agency and the University of British Columbia Department of Ophthalmology.. The design was developed from 1993-1995 to treat melanoma of the eye in the initial phase. The facility consists of:. ...

spec file for package dxvk # # Copyright (c) 2018 SUSE LINUX GmbH, Nuernberg, Germany. # # All modifications and additions to the file contributed by third parties # remain the property of their copyright owners, unless otherwise agreed # upon. The license for this file, and modifications and additions to the # file, is the same license as for the pristine package itself (unless the # license for the pristine package is not an Open Source License, in which # case the license is the MIT License). An Open Source License is a # license that conforms to the Open Source Definition (Version 1.9) # published by the Open Source Initiative. # Please submit bugfixes or comments via http://bugs.opensuse.org/ # Name: dxvk Version: 1.7.2 Release: 0 Summary: Vulkan-based D3D11 implementation for Linux / Wine License: zlib-acknowledgement Group: System/Emulators/PC Url: https://github.com/doitsujin/dxvk Source0: %{name}-%{version}.tar.gz BuildRequires: wine BuildRequires: meson BuildRequires: ninja ...

What to do with this:. The University of Washington has (or at least used to have) a project where theyd install muon detectors with data loggers at schools all over Washington state. They collected all the data and looked for coincident events to detect, count, and estimate the size of large (high energy) cosmic ray air showers, which gives information about the highest energy (and least understood) part of the cosmic ray spectrum. This was part of their particle astrophysics group, which was also involved in the Superkamiokande neutrino oscillation experiment, which needed good baseline data on high-energy cosmic ray events.. If I recall correctly, their detectors consisted of a photomultiplier tube inside a metal garbage can, which would have a much higher volume than a couple of flourescent tubes, and thus be more likely to see a muon from a given event.. But in any case, if you can get enough people to build and install them, log data from them, and collect that data, you can do Real ...

Near East University Faculty of Engineering Biomedical Engineering Department lecturer Assoc. Prof. Dr. İlker Özşahin successfully represents our country in the team working on the Compact Muon Solenoid (CMS), which is one of the six experiments that measure the traces and energies of particles...

A measurement of the inclusive Z → ττ cross-section in pp collisions at TeX is presented based on a dataset of 1.0 fb−1 collected by the LHCb detector. Candidates for Z → τ τ decays are identified through reconstructed final states with two muons, a muon and an electron, a muon and a hadron, or an electron and a hadron. The production cross-section for Z bosons, with invariant mass between 60 and 120 GeV/c 2, which decay to τ leptons with transverse momenta greater than 20 GeV/c and pseudorapidities between 2.0 and 4.5, is measured to be σ pp→Z→ττ = 71.4 ± 3.5 ± 2.8 ± 2.5 pb; the first uncertainty is statistical, the second is systematic, and the third is due to the uncertainty on the integrated luminosity. The ratio of the cross-sections for Z → τ τ to Z → μμ is determined to be 0.93 ± 0.09, where the uncertainty is the combination of statistical, systematic, and luminosity uncertainties of the two measurements. ...

Abstract: In this thesis, the potential to discover supersymmetric signatures in both e+e- and gamma-gamma colliders evaluated with a Monte Carlo analysis, is discussed. The analysis was focused on the detection of muons, essentially. First, we study the detection of R-smuons in e-e+ collisions, whose purpose is the measurement of the smuon mass. It was found that an uncertainty of 0.11 GeV (stat) can be achieved. Under the assumption of the real conditions of the ILC photon collider, a study covering the detection of R-smuons and L-smuons pairs for a center-of-mass energy of e-e- = 0.5 and 0.6 TeV was performed. According to the simulation, a statistical error for the branching ratios of L-smuon -, muon neutralino1 of 0.98% and L-smuon -, muon + neutralino2 of 3.97% can be reached. In order to judge the Monte Carlo results, we have used a technique based on a multidimensional fit to evaluate the impact of the branching ratio measurements on the precision of the SUSY parameters. Furthermore, the ...

In the search for dark matter (DM), one particular focus is on light and ultra-light dark matter, i.e. sub-GeV mass dark matter from a hidden dark sector with a new force interacting with the standard model or ultra-light DM with mass range from 10−22 eV to keV. The arguably most popular example of the latter class is the axion, invoked to solve the apparent absence of CP violation in Quantum Chromo Dynamics. Detection of these particles poses new challenges to potential sensor materials: very small energy depositions, magnetic properties and anisotropic response to particle interactions for example become crucial requirements. The challenge of finding suitable materials fits well with recent developments in solid state physics: Motivated by the exponential growth of computational power and the resulting data, we witness the rapid adoption of functional materials prediction within the framework of materials informatics. Here, methods adapted from computer science based on data-mining and ...

The Fermilab Mu2e experiment seeks to investigate the decay of muons into electrons. The experiment uses several superconducting magnets to create a complex magnetic field to transport the muons from their production point to the decay target, where several detectors will analyze the decay products. To correctly identify the particle tracks, a high precision map of the magnetic field is required to obtain the momentum distribution of decay particles and understand locations of potential magnetic traps that could contribute to the number of background events. The field map requirements demand a precision of the map of 10-4 Tesla. Thus, precision 3D Hall probes are used and need to be checked for their accuracy. As these probes are usually only precise to a 10-4 Tesla within a limited temperature range, they might need to be re-calibrated. In our project, we developed tools to create a multidimensional fit to interpolate the Hall probe readings between obtained calibration data points; variables include

Abstract KM3NeT is a research infrastructure located in the Mediterranean Sea, that will consist of two deep-sea Cherenkov neutrino detectors. With one...

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ISIS is a world-leading centre for research in the physical and life sciences at the STFC Rutherford Appleton Laboratory near Oxford in the United Kingdom. Our suite of neutron and muon instruments gives unique insights into the properties of materials on the atomic scale.. We support a national and international community of more than 3000 scientists for research into subjects ranging from clean energy and the environment, pharmaceuticals and health care, through to nanotechnology and materials engineering, catalysis and polymers, and on to fundamental studies of materials.. We use the technique of neutron scattering. Neutrons tell us where atoms are and how they are moving. By studying how materials work at the atomic level, we can better understand their every-day properties - and so make new materials tailor-made for particular uses. ISIS also produces muons for use in a similar way, providing additional information on how materials work at the atomic scale.. From the original vision over 30 ...

When I was a grad student, the big thing that was really noticeable was the difference in the level of preparation of people whod done their undergrad in the US and those whod done it in China. E.g., the Chinese students had never touched an oscilloscope before they started grad school. This might be true, to a lesser extent, if you compare an undergrad degree from Berkeley or Caltech to one from a low-quality school. A good indicator of the quality of an undergrad physics program is what they do in the upper-division lab course. At a serious physics school, youll see things like the Mossbauer effect and cosmic-ray muon experiments ...

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β decay had been first described theoretically by Fermis original ansatz which was Lorentz-invariant and involved a 4-point fermion vector current. However, this did not incorporate parity violation within the matrix element in Fermis Golden Rule seen in weak interactions. The Gamow-Teller theory was necessary for the inclusion of parity violation by modifying the matrix element to include vector and axial-vector couplings of fermions. This formed the matrix element that completed the Fermi theory of β decay and described parity violation, neutrino helicity, muon decay properties along with the concept of lepton universality. Before the Standard Model of Particle Physics was developed, George Sudarshan and Robert Marshak, and also independently Richard Feynman and Murray Gell-Mann, determined the correct tensor structure (vector minus axial vector, V − A) of the four-fermion interaction. From there modern electroweak theory was developed, which described the weak interaction in terms of ...

The forward-backward charge asymmetries of theb andc quarks are measured with the JADE detector at PETRA at s√=35 GeV and 44 GeV using both electrons and muons to tag the heavy quarks. At s√=35 GeV, a simultaneous fit for the two asymmetries yields the resultA b =−9.3±5.2% (state.) ndA c =−9.6±4.0% (stat.). The systematic errors are comparable with the statistical uncertainties. Combining the measurements at both energies and alternately constraining the weak coupling of thec andb quark to their Standard Model values (a c =1,a b =−1) increases the precision of the measurement of coupling constant of the other quark. Using this procedurea b =−0.72±0.34 anda c =0.79±0.40, where the numbers are corrected for BBˉ−mixing and the errors include both statistical and systematic contributions. The mixing parameter for continuum bbˉ−production is determined to be χ-0.24±0.12 if both heavy quark coupling constants are constrained to their values in the Standard Model.. ...

Measurements of fiducial integrated and differential cross sections for inclusive W +, W -and Z boson production are reported. They are based on 25.0 +/- 0.5 pb -1 of pp collision data at v s = 5.02 TeV collected with the ATLAS detector at the CERN Large Hadron Collider. Electron and muon decay channels are analysed, and the combined W +, W -and Z integrated cross sections are found to be sW+ = 2266 +/- 9 (stat) +/- 29 (syst) +/- 43 (lumi) pb, sW-= 1401 +/- 7 (stat) +/- 18 (syst) +/- 27 (lumi) pb, and sZ = 374.5 +/- 3.4 (stat)+/- 3.6 (syst)+/- 7.0 (lumi) pb, in good agreement with next-to-next-to-leading-order QCD crosssection calculations. Thesemeasurements serve as references for Pb+ Pb interactions at the LHC at v sNN = 5.02 TeV.. ...

A search is presented for the direct pair production of the stop, the supersymmetric partner of the top quark, that decays through an R-parity-violating coupling to a final state with two leptons and two jets, at least one of which is identified as a b-jet. The data set corresponds to an integrated luminosity of 36.1 fb(-1) of proton-proton collisions at a center-of-mass energy of root s = 13 TeV, collected in 2015 and 2016 by the ATLAS detector at the LHC. No significant excess is observed over the Standard Model background, and exclusion limits are set on stop pair production at a 95% confidence level. Lower limits on the stop mass are set between 600 GeV and 1.5 TeV for branching ratios above 10% for decays to an electron or muon and a b-quark.. ...

The first observation of top quark production in proton-nucleus collisions is reported using proton-lead data collected by the CMS experiment at the CERN LHC at a nucleon-nucleon center-of-mass energy of 8.16 TeV. The measurement is performed using events with exactly one isolated electron or muon and at least four jets. The significance of the ttbar signal against the background-only hypothesis is above five standard deviations. The measured cross section is 45±8 nb, consistent with predictions from perturbative quantum chromodynamics. We will discuss the experimental and theoretical aspects of this measurement including the potential probing of the time structure of the Quark Gluon Plasma with an analogous measurement in nucleus-nucleus collisions.. ...

The recombination reaction Mu + NO + MMuNO + M (M = He, N-2, CH4) has been studied by the muon spin relaxation/rotation (mu SR) technique up to 520 bar at room temperature. The reaction remains in the low pressure regime throughout. The measured termolecular addition rate constant in N-2, 8.8 +/- 0.3 x 10(-33) cm(6) s(-1), is essentially the same as that found in our earlier study at pressures below 60 bar [J. J. Pan et al., J. Phys. Chem., 1995, 99, 17160]. It is somewhat smaller in He, 7.7 +/- 1.0 x 10(-33), but larger in CH4, 12.8 +/- 2.0 x 10(-33). The Mu + NO reaction is about five times slower than the corresponding H + NO reaction. The strong collision limits of the rate constants for three H-isotopes (Mu, H, D) reacting with NO have been estimated with Troes formalism for unimolecular dissociation in the low pressure regime, based on the ab initio potential energy surface of Guadagnini et al. [J. Chem. Phys., 1995, 102, 774]. The Troe calculations give less than satisfactory agreement ...

The Brookhaven experiment E821 has recently announced a new measurement of the muon anomalous magnetic moment (g-2), which differs from the theoretical prediction by 2.6 sigma. I will review the Standard Model prediction and uncertainties in the QED, hadronic and electroweak contributions. Possible explanations of the theory vs. experiment discrepancy, due to supersymmetric loop effects and other ``New Physics scenarios, will be discussed. ...

A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb(-1) of √s = 7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m(1/2) up to 820GeV are excluded for 10 , tan β , 40.. ...

This thesis focuses on two parts, the evidence of a structure in a four lepton final state, and the CMS detector upgrade studies. The first part of the thesis focuses on an unexpected structure in Υ(1S)l+l− final state, where Υ(1S) → μ+μ−, l can represent a muon or an electron and m(l+l−) is required to be below the Υ(1S) mass. Using an integrated luminosity of 25.6 fb−1 recorded in proton-proton collisions at √s = 7 TeV and √s = 8 TeV with the CMS detector at the CERN LHC, an excess in the mass distribution near 18.5 GeV of Υ(1S)l+l− is found. The mass of this enhancement is found out to be 18.4 ± 0.1 (stat.) ± 0.2 (syst.) GeV in the Υ(1S)μ+μ− channel, and 18.5 ± 0.2 (stat.) ± 0.2 (syst.) GeV in the Υ(1S)e+e− channel. For the two results combined, the enhancement is found out to be 18.4 ± 0.1 (stat.) ± 0.2 (syst.) GeV with a local statistical significance of 4.9 standard deviations and a global significance, after taking into account the look-elsewhere-effect, of 3.6

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Particles that make up the structure of atoms, such as neutrons, protons and electrons. Neutrons and protons are roughly the same mass, while electrons are much lighter. In the early 20th century these were thought to be the only subatomic particles, but we now know others exist, which include neutrinos, antielectrons, antiprotons, antineutrons, muons and bosons.. ...

It is well known among physicists that two different kinds of experiments give an anomaly in the proton-radius. The anomaly is: When a muon orbits the proton the proton-radius is 4% smaller than when an electron orbits the proton. This anomaly is a puzzle in standard physics. This puzzle is solved in a new cosmological theory with a new dark energy-force. This article describes the solution. The solution is put in perspective of new physics by a combination of quantum-gravity and sub-quantum dark matter-force in one formula, within the new cosmological theory, called the Double Torus Theory for the universe. Additionally the principle for an anti-gravitational machine is shown based on the use of a dark matter force. ...

Results of a search for supersymmetry are presented using events with a photon, an electron or muon, and large missing transverse momentum. The analysis is based on a data sample corresponding to an integrated luminosity of 35.9 fb(-1) of proton-proton collisions at 13 TeV, produced by the LHC and collected with the CMS detector in 2016. Theoretical models with gauge-mediated supersymmetry breaking predict events with photons in the final state, as well as electroweak gauge bosons decaying to leptons. Searches for events with a photon, a lepton, and missing transverse momentum are sensitive probes of these models. No excess of events is observed beyond expectations from standard model processes. The results of the search are interpreted in the context of simplified models inspired by gauge-mediated supersymmetry breaking. These models are used to derive upper limits on the production cross sections and set lower bounds on masses of supersymmetric particles. Gaugino masses below 930 GeV are ...

The linear motor driving the target for the Muon Ionisation Cooling Experiment has been redesigned to improve its reliability and performance. A new coil-winding technique is described which produces better magnetic alignment and improves heat transport out of the windings. Improved field-mapping has allowed the more precise construction to be demonstrated, and an enhanced controller exploits the full features of the hardware, enabling increased acceleration and precision. The new user interface is described and analysis of performance data to monitor friction is shown to allow quality control of bearings and a measure of the ageing of targets during use.. ...

A search for a heavy resonance decaying into WZ in the fully leptonic channel (electrons and muons) is performed. It is based on proton-proton collision data collected by the ATLAS experiment at the Large Hadron Collider at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 36.1 fb−1. No significant excess is observed over the Standard Model predictions and limits are set on the production cross section times branching ratio of a heavy vector particle produced either in quark-antiquark fusion or through vector-boson fusion. Constraints are also obtained on the mass and couplings of a singly charged Higgs boson, in the Georgi-Machacek model, produced through vector-boson fusion.. ...

Rescale_eta = cms.double( 3.0 ), Rescale_phi = cms.double( 3.0 ), Rescale_Dz = cms.double( 3.0 ), EtaR_UpperLimit_Par1 = cms.double( 0.25 ), EtaR_UpperLimit_Par2 = cms.double( 0.15 ), PhiR_UpperLimit_Par1 = cms.double( 0.6 ), PhiR_UpperLimit_Par2 = cms.double( 0.2 ), UseVertex = cms.bool( False ), Pt_fixed = cms.bool( False ), Z_fixed = cms.bool( True ), Phi_fixed = cms.bool( False ), Eta_fixed = cms.bool( False ), Pt_min = cms.double( 1.5 ), Phi_min = cms.double( 0.1 ), Eta_min = cms.double( 0.1 ), DeltaZ = cms.double( 15.9 ), DeltaR = cms.double( 0.2 ), DeltaEta = cms.double( 0.2 ), DeltaPhi = cms.double( 0.2 ), maxRegions = cms.int32( 2 ), precise = cms.bool( True ), OnDemand = cms.int32( -1 ), MeasurementTrackerName = cms.InputTag( hltESPMeasurementTracker ), beamSpot = cms.InputTag( hltOnlineBeamSpot ), vertexCollection = cms.InputTag( pixelVertices ), input = cms.InputTag( hltL2Muons,UpdatedAtVtx ...

In November of 2014, in a first, unexpected move for the field of particle physics, the Compact Muon Solenoid (CMS) experiment-one of the main detectors in the worlds largest particle accelerator, the Large Hadron Collider-released ...