3,583 research outputs found

    DJpsiFDC: an event generator for the process gg→J/ψJ/ψgg\to J/\psi J/\psi at LHC

    Full text link
    DJpsiFDC is an event generator package for the process gg→J/ψJ/ψgg\to J/\psi J/\psi. It generates events for primary leading-order 2→22\to 2 processes. The package could generate a LHE document and this document could easily be embedded into detector simulation software frameworks. The package is produced in Fortran codes.Comment: 10 pages, 3 figure

    Employment Contract Law in China: Changes and Implications (FLA Stakeholder Forum PowerPoint Presentation)

    Get PDF
    This document is part of a digital collection provided by the Martin P. Catherwood Library, ILR School, Cornell University, pertaining to the effects of globalization on the workplace worldwide.  Special emphasis is placed on labor rights, working conditions, labor market changes, and union organizing.FLA_Qiao_Jian_PPT.pdf: 248 downloads, before Oct. 1, 2020

    Low field phase diagram of spin-Hall effect in the mesoscopic regime

    Get PDF
    When a mesoscopic two dimensional four-terminal Hall cross-bar with Rashba and/or Dresselhaus spin-orbit interaction (SOI) is subjected to a perpendicular uniform magnetic field BB, both integer quantum Hall effect (IQHE) and mesoscopic spin-Hall effect (MSHE) may exist when disorder strength WW in the sample is weak. We have calculated the low field "phase diagram" of MSHE in the (B,W)(B,W) plane for disordered samples in the IQHE regime. For weak disorder, MSHE conductance GsHG_{sH} and its fluctuations rms(GSH)rms(G_{SH}) vanish identically on even numbered IQHE plateaus, they have finite values on those odd numbered plateaus induced by SOI, and they have values GSH=1/2G_{SH}=1/2 and rms(GSH)=0rms(G_{SH})=0 on those odd numbered plateaus induced by Zeeman energy. For moderate disorder, the system crosses over into a regime where both GsHG_{sH} and rms(GSH)rms(G_{SH}) are finite. A larger disorder drives the system into a chaotic regime where GsH=0G_{sH}=0 while rms(GSH)rms(G_{SH}) is finite. Finally at large disorder both GsHG_{sH} and rms(GSH)rms(G_{SH}) vanish. We present the physics behind this ``phase diagram".Comment: 4 page, 3 figure

    In vivo studies of genomic packaging in the dsRNA bacteriophage Φ8

    Get PDF
    BACKGROUND: Φ8 is a bacteriophage containing a genome of three segments of double-stranded RNA inside a polyhedral capsid enveloped in a lipid-containing membrane. Plus strand RNA binds and is packaged by empty procapsids. Whereas Φ6, another member of the Cystoviridae, shows high stringency, serial dependence and precision in its genomic packaging in vitro and in vivo, Φ8 packaging is more flexible. Unique sequences (pac) near the 5' ends of plus strands are necessary and sufficient for Φ6 genomic packaging and the RNA binding sites are located on P1, the major structural protein of the procapsid. RESULTS: In this paper the boundaries of the Φ8 pac sequences have been explored by testing the in vivo packaging efficacy of transcripts containing deletions or changes in the RNA sequences. The pac sequences have been localized to the 5' untranslated regions of the viral transcripts. Major changes in the pac sequences are either tolerated or ameliorated by suppressor mutations in the RNA sequence. Changes in the genomic packaging program can be established as a result of mutations in P1, the major structural protein of the procapsid and the determinant of RNA binding specificity. CONCLUSION: Although Φ8 is distantly related to bacteriophage Φ6, and does not show sequence similarity, it has a similar genomic packaging program. This program, however, is less stringent than that of Φ6
    • …
    corecore