The extended TeV gamma-ray source ARGO J2031+4157 (or MGRO J2031+41) is positionally consistent with the Cygnus Cocoon discovered by Fermi-LAT at GeV energies in the Cygnus superbubble. Reanalyzing the ARGO-YBJ data collected from 2007 November to 2013 January, the angular extension and energy spectrum of ARGO J2031+4157 are evaluated. After subtracting the contribution of the overlapping TeV sources, the ARGO-YBJ excess map is fitted with a two-dimensional Gaussian function in a square region of 10 • × 10 • , finding a source extension σ ext = 1. • 8 ± 0. • 5. The observed differential energy spectrum is dN/dE = (2.5 ± 0.4) × 10 −11 (E/1 TeV) −2.6±0.3 photons cm −2 s −1 TeV −1 , in the energy range 0.2-10 TeV. The angular extension is consistent with that of the Cygnus Cocoon as measured by Fermi-LAT and the spectrum also shows a good connection with the one measured in the 1-100 GeV energy range. These features suggest to identify ARGO J2031+4157 as the counterpart of the Cygnus Cocoon at TeV energies. The Cygnus Cocoon, located in the star-forming region of Cygnus X, is interpreted as a cocoon of freshly accelerated cosmic rays related to the Cygnus superbubble. The spectral similarity with supernova remnants (SNRs) indicates that the particle acceleration inside a superbubble is similar to that in an SNR. The spectral measurements from 1 GeV to 10 TeV allows for the first time to determine the possible spectrum slope of the underlying particle distribution. A hadronic model is adopted to explain the spectral energy distribution.

The engagement of the 4‐1BB (CD137) co‐stimulatory pathway promotes the activation and proliferation of conventional CD4+ T and CD8+ T cells, but the role of 4‐1BB co‐stimulation in CD4+ CD25+ regulatory T cells (Treg) is less clear. In particular, whether 4‐1BB stimulation affects the expression of Foxp3, a master gene for Treg, is unknown. This study demonstrates that co‐stimulation of 4‐1BB engaged by an agonistic antibody promotes the proliferation of Treg in a dependent manner of low‐concentration interleukin‐2 in vitro. The 4‐1BB‐expanded Treg maintain Foxp3 expression and their ability to suppress conventional CD4+ T cells and their feature to produce no interleukin‐2. However, the 4‐1BB‐expanded Treg produce increased levels of interferon‐γ, whose significance is unknown. Thus, 4‐1BB co‐stimulation plays a role in the expansion of functional CD4+ CD25+ Treg cells without adversely affecting their suppressive activity.

The inter-grain exchange-coupling interactions, effective anisotropy, and coercivity in nanocomposite Nd2Fe14B/α−Fe magnets were investigated. The effective anisotropy of nanocomposite magnets has been calculated starting from the statistics of boundaries between magnetically hard-hard, hard-soft, and soft-soft grains. The result shows that the effective anisotropy decreases with reduction in grain size and/or increase in soft phase components. When grain sizes reduce to 4–5 nm, Keff decreases to 1/3−1/4 of the ordinary value of K. The coercivity in nanocomposite magnets demonstrates a similar behavior. The decrement of coercivity is mainly due to the reduction of effective anisotropy. Considering the opposite varying trend the remanence demonstrates with respect to the effective anisotropy and the coercivity, we conclude that the mean grain size should be in the range of 10–15 nm and the volume fraction of soft phase should be less than 50% in order to achieve high energy product magnets.

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High-spin states of ll5In have been studied using the ll4Cd (7Li, a2n) reaction at a beam energy of 48 MeV. A total of 13 new transitions have been observed and added to the level scheme of ll5In. Most ol the states in ll5In can be interpreted in terms of the weak coupling of a g9/2 proton hole to the core states ol 1 l('Sn or a g1/2 proton to the core states of ll4Cd. A A / = 1 band with the 7r(^9/2)_1 ® v(h l:/2)2 configuration was suggested as an oblate band built on the "stapler" mechanism with the aid of the tilted axis cranking model based on covariant density functional theory,