t→bH",H'→ ATLAS h→>yand ∫udt=300fb wh/tth.h→>yy Maximal mixing tth,h→bb H→tb ATLAS HA→T TDR →tH,H→ leptons LEP 2000 H→tb A→Zh→‖bb H/A→tt 50100150200250300350400450 DA (Gev) 3. 14: 5 discovery contours for MSSM Higgs boson detection in various channels
ATLAS TDR
40 →bH°,H'→Ty ATLAS ∫Ldt=300fb Wh /th. h ond Maxim h→b H 20 H→tb H/A 098 only detect h the decoupling regime A→Zh→‖bb H/A→t 5010015020025030035040450500 (Gev) 3.14: 5o discovery contours for MSSM Higgs boson detection in various channels
only detect h the
t→bH",H'→ ATLAS 40 ∫udt=300fb h→>yand wh/tth.h→>yy Maximal mixi tth,h→bb BUT depends on good detection capabilities A,H, H for bs and taus signals only detect LEP Il excluded 5010015020025030035040 DA (Gev) 3. 14: 5 discovery contours for MSSM Higgs boson detection in various channels
BUT depends on good detection capabilities for b’s and tau’s only detect h LEP II excluded A, H, H signals
40 H.A→ muons Depends on good detection capabilities for b's and taus only detect -plated LEP Il excluded 5010015020025030035040 DA (Gev) 3. 14: 5 discovery contours for MSSM Higgs boson detection in various channels
Depends on good detection capabilities for b’s and tau’s only detect h H, A muons Gold -plated signal LEP II excluded
阅清华大学 Tsinghua University BUT the preceding does not take into account possible Higgs boson decays into sparticles h.H.A→ x H On the bad side... decays to these channels reduce the rates of SM signal channels On the good side... new signals may be found
清华大学 Tsinghua University the preceding does not take into account possible Higgs boson decays into sparticles 0 0 * , , , , , i j i j h H A 0 , H i j On the bad side… On the good side… decays to these channels reduce the rates of SM signal channels new signals may be found