CRYRING at the LSR at FLAIR

FLAIR will be the next-generation facility for physics with low-energy antiprotons, providing antiprotons at energies from tens of MeV down to rest. It will also offer unique possibilities for physics with highly charged ions at very low energies. The FLAIR facility will have two deceleration rings, the LSR which will decelerate antiprotons to 300 keV and the USR which will bring them down further to 20 keV. The LSR will consist of the present CRYRING at the Manne Siegbahn Laboratory. During the next few years, CRYRING will be modified with respect to injection and extraction, to allow injection of 30 MeV antiprotons and to provide it with both fast (single-turn) and slow (resonant) extraction at a variable energy. We here describe plans and preparations for the transfer of CRYRING to FLAIR, giving, in particular, an overview of new components for injection and extraction.     

PVDIS at 12 GeV at JLab

In 1956 Lee and Yang suggested that parity might be violated and, if nature were so, they further described a recipe on how to exploit that broken symmetry to measure the muon??s magnetic moment. Of course parity violation was very soon confirmed in the weak interactions and many generations of experiments since then have led to a determination of ?? _?? to better than part-per-billion precision. A new experiment proposed for Fermilab is planned to push this precision further still, being motivated by the sensitive comparison of measurement to exquisite theory. We report on the current comparison, which exceeds three standard deviations, and the plans and promise for the future experimental effort.     

Polarized proton collisions at 205 GeV at RHIC

The Brookhaven Relativistic Heavy Ion Collider (RHIC) has been providing collisions of polarized protons at a beam energy of 100 GeV since 2001. Equipped with two full Siberian snakes in each ring, polarization is preserved during acceleration from injection to 100 GeV. However, the intrinsic spin resonances beyond 100 GeV are about a factor of 2 stronger than those below 100 GeV making it important to examine the impact of these strong intrinsic spin resonances on polarization survival and the tolerance for vertical orbit distortions. Polarized protons were first accelerated to the record energy of 205 GeV in RHIC with a significant polarization measured at top energy in 2005. This Letter presents the results and discusses the sensitivity of the polarization survival to orbit distortions.     

Multi-lepton production at high transverse momentum at HERA

A search for events containing two or more high-transverse-momentum isolated leptons has been performed in ep collisions with the ZEUS detector at HERA using the full collected data sample, corresponding to an integrated luminosity of 480 pb⁻¹. The number of observed events has been compared with the prediction from the Standard Model, searching for possible deviations, especially for multi-lepton events with invariant mass larger than 100 GeV. Good agreement with the Standard Model has been observed. Total and differential cross sections for di-lepton production have been measured in a restricted phase space dominated by photon–photon collisions.     

Atomic Physics Studies at the Gamma Factory at CERN

The Gamma Factory initiative proposes to develop novel research tools at CERN by producing, accelerating, and storing highly relativistic, partially stripped ion beams in the SPS and LHC storage rings. By exciting the electronic degrees of freedom of the stored ions with lasers, high-energy narrow-band photon beams will be produced by properly collimating the secondary radiation that is peaked in the direction of ions' propagation. Their intensities, up to 10¹⁷ photons per second, will be several orders of magnitude higher than those of the presently operating light sources in the particularly interesting γ–ray energy domain reaching up to 400 MeV. This article reviews opportunities that may be afforded by utilizing the primary beams for spectroscopy of partially stripped ions circulating in the storage ring, as well as the atomic-physics opportunities made possible by the use of the secondary high-energy photon beams. The Gamma Factory will enable ground-breaking experiments in spectroscopy and novel ways of testing fundamental symmetries of nature.     

New look at thermodynamics of gas and at clusterization

In the paper, by using the example of a rigorous formulation and rigorous proof of the Maxwell distribution, estimates for the distribution in dependence of the parameter N (the number of particles) are established. Further, the problem concerning the creation of dimers in classical gas is regarded as an analog of Bose condensation, and estimates for the lower level of the analog of Bose condensation are proved. The relationship between this level and the theory of “capture” in the scattering problem corresponding to interaction in the form of Lennard-Jones potential is clarified. The equation of state of a nonideal gas as a result of pairwise interaction of particles in the Lennard-Jones and Kihara models is derived. New quantum equations for the transfer of neutral gas consisting of particles with evenly and oddly many neutrons in capillaries and nanotubes are also presented. To the memory of my teacher in number theory, Professor Anatolii Karatsuba     

Graphite at high pressures: Pseudomelting at 44 GPa

Abstract

The Raman spectra comparative study of graphite-like modifications of carbon: monocrystalline graphite, pyrolytic graphite and amorphous (glassy) carbon was performed at high pressures and room temperature. At P = 44 GPa an abrupt broadening of Raman bands of pyrolytic graphite and glassy carbon was observed. The same process in monocrystalline graphite occures continuously from 23 to 44 GPa and for higher pressures the Raman spectra of all three substances under study become practically indistinguishable from one another and from that of amorphous carbon (a-C) at the same pressure. This result is ascribed to the formation at these pressures of the dence amorphous carbon modification.     

Experiments on the study of the deuteron-proton interactions at intermediate energies at Internal Target at Nuclotron

The experimental program on the study of deuteron-proton interaction at Internal Target at Nuclotron is discussed. Recent results obtained for dp-elastic scattering and dp-breakup reactions at intermediate energies are presented. The status of the DSS setup upgrade is reported.     

Elastic Wave Reflection at the Interface at Preset Stresses

Russian Physics Journal - The problem of elastic wave reflection at the interface at preset constant stresses is discussed. Under the conditions where the reflection laws are fulfilled, analytical...     

Gels at interfaces

We discuss the adsorption of polymer gels on flat surfaces. Even in cases of complete wetting where the spreading power S is positive and where an equivalent liquid would spread, the elastic stresses due to the gel deformation upon adsorption oppose the spreading. The competition between elasticity characterized by the bulk shear modulus G and capillarity characterized by the spreading power S defines a typical length scale ℓ = S/G for the deformation in the gel. For loose gels ℓ can be of the order of 1 μm. Macroscopic gels larger than ℓ deform only at their edges over a region of size ℓ. Microscopic gels smaller than ℓ show a finite deformation despite the elastic stresses. The elastic stresses limit the spreading of the polymer, but solvent can be sucked out of a swollen gel by wetting the surface. The thin solvent film can extend rather far from the gel edge and carry solvent. We calculate the kinetics of the solvent film formation and of the solvent transfer from a more swollen gel to a less swollen gel. Received 16 July 2001     

Chains at interfaces

Simha, together with Frisch and Eirich, was among the first to realize that in energetic interaction with a surface a flexible polymer chain would be under a major conformational constraint which could be analyzed by solving a random walk (diffusional) problem near a barrier. These results stimulated more work, and today we have a fairly good knowledge of the factors which determine polymer adsorption from very dilute solution. Conformational problems arise also when more concentrated systems are used and it has become apparent that as concentration increases the surface phase will, more and more, be scaled by the root mean square diameter of the undeformed macromolecule. One can view the presence of an energetically attractive interface as creating a sink for macromolecules. The closer a polymer solution is to its Θ point, the more easily the polymer in solution can enter the sink and the stronger will be the extent of adsorption. The presence of an interface can thus be seen as a means to produce a phase separation in a polymer system which would otherwise be stable. Coatings of adsorbed polymers over colloidal particles create “macromolecular” solutions, where the “macromolecule” is the colloid particle with its adsorbed coat. This causes polymer segment/polymer segment contacts to dominate the encounter energetically. Hence, the solution behavior of the coated colloid becomes reminiscent of the solution behavior of the polymer in the coat. Stabilization by adsorbed polymer layers derives from converting the original solubility characteristics of the colloid, from what they were, essentially to those of the polymer being used.     

Vibrations at surfaces

This special issue is dedicated to the phenomenon of vibrations at surfaces-a topic that was indispensible a couple of decades ago, since it was one of the few phenomena capable of revealing the nature of binding at solid surfaces. For clean surfaces, the frequencies of modes with characteristic displacement patterns revealed how surface geometry, as well as the nature of binding between atoms in the surface layers, could be different from that in the bulk solid. Dispersion of the surface phonons provided further measures of interatomic interactions. For chemisorbed molecules on surfaces, frequencies and dispersion of the vibrational modes were also critical for determining adsorption sites. In other words, vibrations at surfaces served as a reliable means of extracting information about surface structure, chemisorption and overlayer formation. Experimental techniques, such as electron energy loss spectroscopy and helium-atom-surface scattering, coupled with infra-red spectroscopy, were continually refined and their resolutions enhanced to capture subtleties in the dynamics of atoms and molecules at surfaces. Theoretical methods, whether based on empirical and semi-empirical interatomic potential or on ab initio electronic structure calculations, helped decipher experimental observations and provide deeper insights into the nature of the bond between atoms and molecules in regions of reduced symmetry, as encountered on solid surfaces. Vibrations at surfaces were thus an integral part of the set of phenomena that characterized surface science. Dedicated workshops and conferences were held to explore the variety of interesting and puzzling features revealed in experimental and theoretical investigations of surface vibrational modes and their dispersion. One such conference, Vibrations at Surfaces, first organized by Harald Ibach in Juelich in 1980, continues to this day. The 13th International Conference on Vibrations at Surfaces was held at the University of Central Florida, Orlando, in March 2010. Several speakers at this meeting were invited to contribute to the special section in this issue. As is clear from the articles in this special section, the phenomenon of vibrations at surfaces continues to be a dynamic field of investigation. In fact, there is a resurgence of effort because the insights provided by surface dynamics are still fundamental to the development of an understanding of the microscopic factors that control surface structure formation, diffusion, reaction and structural stability. Examination of dynamics at surfaces thus complements and supplements the wealth of information that is obtained from real-space techniques such as scanning tunneling microscopy. Vibrational dynamics is, of course, not limited to surfaces. Surfaces are important since they provide immediate deviation from the bulk. They display how lack of symmetry can lead to new structures, new local atomic environments and new types of dynamical modes. Nanoparticles, large molecules and nanostructures of all types, in all kinds of local environments, provide further examples of regions of reduced symmetry and coordination, and hence display characteristic vibrational modes. Given the tremendous advance in the synthesis of a variety of nanostructures whose functionalization would pave the way for nanotechnology, there is even greater need to engage in experimental and theoretical techniques that help extract their vibrational dynamics. Such knowledge would enable a more complete understanding and characterization of these nanoscale systems than would otherwise be the case. The papers presented here provide excellent examples of the kind of information that is revealed by vibrations at surfaces. Vibrations at surface contents Poisoning and non-poisoning oxygen on Cu(410)L Vattuone, V Venugopal, T Kravchuk, M Smerieri, L Savio and M Rocca Modifying protein adsorption by layers of glutathione pre-adsorbed on Au(111)Anne Vallée, Vincent Humblot, Christophe Méthivier, Paul Dumas and Claire-Marie Pradier Relating temperature dependence of atom scattering spectra to surface corrugationW W Hayes and J R Manson Effects of the commensurability and disorder on friction for the system Xe/CuA Franchini, V Bortolani, G Santoro and K Xheka Switching ability of nitro-spiropyran on Au(111): electronic structure changes as a sensitive probe during a ring-opening reactionChristopher Bronner, Gunnar Schulze, Katharina J Franke, José Ignacio Pascual and Petra Tegeder High-resolution phonon study of the Ag(100) surfaceK L Kostov, S Polzin and W Widdra On the interpretation of IETS spectra of a small organic molecule Karina Morgenstern.     

Exotics at PANDA

One highlight in the field of hadron spectroscopy is the recent discovery of unexpected charmonium-like X, Y, Z resonances. The nature of most of these states is still controversial and emphasizes the discussion on exotic states with gluonic degrees of freedom. The PANDA experiment, a core project of the future Facility for Antiproton and Ion Research (FAIR) at GSI in Darmstadt, will investigate antiproton annihilations with the aim to explore fundamental questions in the nonperturbative region of QCD. The PANDA detector, equipped with a fixed target and provided with a high quality antiproton beam in the momentum range between 1.5 and 15 GeV/c, is optimized for high precision measurements of hadrons with masses up to 5 GeV/c ² and in particular of resonances in the charmonium and open charm region. Due to the gluon-rich antiproton annihilation process, it is expected to observe exotic states and therefore to answer fundamental questions in this field. The physics program for the search for exotics is outlined and detailed feasibility studies are presented. Furthermore, strategies for the unambiguous determination of the quantum numbers of these states are discussed.     

Hadron production at forward rapidity in nuclear collisions at RHIC

The main experimental results obtained by the BRAHMS experiment at Relativistic Heavy Ion Collider (RHIC) for Au+Au collisions at \(\sqrt {s_{NN} } \) =62.4, 200 GeV and d+Au collisions at \(\sqrt {s_{NN} } \) = 200GeV are presented. The m _T spectra and the Gaussian-like rapidity densities of produced pions and kaons in Au+Au central collisions at \(\sqrt {s_{NN} } \) = 200 are GeV shown, and their rapidity densities are compared with results from models. The net-proton yield in the same system is compared with that from AGS and SPS energies to study the high energy collision scenario-transparency and stopping. The rapidity, energy and centrality dependence of the nuclear modification factors in both systems are compared with models to differentiate between the initial and final state effect.     

Experiments at COSY

At the COSY cooler synchrotron several experimental facilities are in operation at internal and external target stations. The combination of a high quality low emittance proton beam with high acceptance detector systems allows precise and complete experiments. The momentum range of the COSY beam from 300 MeV/c up to about 3.5 GeV/c opens a large field of experimental studies. One main topic of the present experiments is strangeness production with emphasis to the threshold region.     

Measurement of dijet photoproduction at high transverse energies at HERA

The cross section for dijet photoproduction at high transverse energies is presented as a function of the transverse energies and the pseudorapidities of the jets. The measurement is performed using a sample of ep-interactions corresponding to an integrated luminosity of 6.3 pb, recorded by the ZEUS detector. Jets are defined by applying a -clustering algorithm to the hadrons observed in the final state. The measured cross sections are compared to next-to-leading order QCD calculations. In a kinematic regime where theoretical uncertainties are expected to be small, the measured cross sections are higher than these calculations. Received: 18 May 1999 / Published online: 14 October 1999     

DVCS at HERMES

This talk explores the impact that the Hermes experiment has had regarding knowledge of the Deeply Virtual Compton Scattering process. We discuss the various measurements that HERMES has contributed to the library of DVCS knowledge [1–3], with focus in particular on the recent high-precision beam spin and charge asymmetries [4].