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Searches for Higgs boson pair production in the hh →bbττ, γγWW∗, γγbb, bbbb channels with the ATLAS detector
Searches for both resonant and nonresonant Higgs boson pair production are performed in the hh→bbττ, γγWW∗ final states using 20.3  fb−1 of pp collision data at a center-of-mass energy of 8 TeVExpand
Detection of a crack-like conduit beneath the active crater at Aso Volcano Japan
To constrain the source of long period tremors (LPTs), we deployed a very dense broadband seismic network consisting of totally twenty-four stations around the active crater of Aso volcano in Kyushu,Expand
Systematic study of the electronic state in θ-type BEDT-TTF organic conductors by changing the electronic correlation
The behavior of the phase transitions is mapped out as a function of the dihedral angle (\ensuremath{\theta}) or the transfer integral $(t)$ between donor columns for \ensuremath{\theta}-typeExpand
The Intermolecular Interaction of Tetrathiafulvalene and Bis(ethylenedithio)tetrathiafulvalene in Organic Metals. Calculation of Orbital Overlaps and Models of Energy-band Structures
Based on the extended Huckel molecular orbital calculations, the relation between the anisotropy of the band structure and the arrangement of the organic molecules is investigated for two organicExpand
Estimation of πd-Interactions in Organic Conductors Including Magnetic Anions
Magnetic interactions in organic conductors including magnetic anions, such as λ-(BETS) 2 FeCl 4 and κ-(BETS) 2 FeX 4 [X = Cl and Br], are estimated from intermolecular overlap integrals; theExpand
Study of B-→D**0π-(D**0→D(*)+π-) decays
We report the results of a study of charged B decays to the D(+/-)pi(-/+)pi(-/+) and D(*+/-)pi(-/+)pi(-/+) final states using complete D-(*) reconstruction. The contributions of two-body B-->D**piExpand
Effect of UV scattering on SO2 emission rate measurements
We report the quantitative evaluation of the UV scattering effect on the SO 2 emission rate measurement by the compact UV spectrometer system. Plume spectra were obtained simultaneously at threeExpand
BAND STRUCTURES OF TWO TYPES OF (BEDT-TTF)2I3
On the basis of the extended Huckel molecular orbital calculation, the intermolecular overlaps of the highest occupied molecular orbitals are calculated for α-(BEDT-TTF)2I3 reported by Bender et al.,Expand
Crystal and electronic structures of (BEDT-TTF)2(MHg(SCN)4)(M=K and NH4).
The crystal structures of (BEDT–TTF)2[MHg(SCN)4] (M=K at 298 and 104 K and M=NH4 at 298 K) were determined by X-ray analyses. A donor layer and an anion sheet stack alternately along the b-axis. TheExpand
Metallization of magnetite (Fe3O4) under high pressure
Electrical resistivity measurements have been made on a good qualified single crystalline magnetite (Fe3O4) at temperatures from 300 down to 3.0 K under pressure up to 10 GPa. A steep change inExpand
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