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  • 5. Tevatron constraints on models of the Higgs boson with exotic spin and parity using decays to bottom-antibottom quark pairs.
    Aaltonen T; Abazov VM; Abbott B; Acharya BS; Adams M; Adams T; Agnew JP; Alexeev GD; Alkhazov G; Alton A; Amerio S; Amidei D; Anastassov A; Annovi A; Antos J; Apollinari G; Appel JA; Arisawa T; Artikov A; Asaadi J; Ashmanskas W; Askew A; Atkins S; Auerbach B; Augsten K; Aurisano A; Avila C; Azfar F; Badaud F; Badgett W; Bae T; Bagby L; Baldin B; Bandurin DV; Banerjee S; Barbaro-Galtieri A; Barberis E; Baringer P; Barnes VE; Barnett BA; Barria P; Bartlett JF; Bartos P; Bassler U; Bauce M; Bazterra V; Bean A; Bedeschi F; Begalli M; Behari S; Bellantoni L; Bellettini G; Bellinger J; Benjamin D; Beretvas A; Beri SB; Bernardi G; Bernhard R; Bertram I; Besançon M; Beuselinck R; Bhat PC; Bhatia S; Bhatnagar V; Bhatti A; Bland KR; Blazey G; Blessing S; Bloom K; Blumenfeld B; Bocci A; Bodek A; Boehnlein A; Boline D; Boos EE; Borissov G; Bortoletto D; Borysova M; Boudreau J; Boveia A; Brandt A; Brandt O; Brigliadori L; Brock R; Bromberg C; Bross A; Brown D; Brucken E; Bu XB; Budagov J; Budd HS; 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  • 6. Broken SU(3) symmetry applied to rotational nuclei: Cylindrical intrinsic states in the interacting boson model.
    Hartmann FX; Sharon YY; Naumann RA
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  • 7. Erratum: Broken SU(3) symmetry applied to rotational nuclei: Cylindrical intrinsic states in the interacting boson model.
    Hartmann FX; Sharon YY; Naumann RA
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  • 8. Probing the strongly driven spin-boson model in a superconducting quantum circuit.
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