We study various FCNC involving heavy quarks in the Standard Model (SM) with
a sequential fourth generation. After imposing B→Xsγ, B→Xsl+l− and Z→bbˉ constraints, we find B(Z→sbˉ+sˉb) can be enhanced by an order of magnitude to 10−7,
while t→cZ,cH decays can reach 10−6, which are orders of magnitude
higher than in SM. However,these rates are still not observable for the near
future.With the era of LHC approaching, we focus on FCNC decays involving
fourth generation b′ and t′ quarks. We calculate the rates for
loop induced FCNC decays b′→bZ,bH,bg,bγ, as well as
t^\prime\to tZ,\tH, tg, t\gamma. If ∣Vcb′∣ is of order ∣Vcb∣≃0.04, tree level b′→cW decay would dominate, posing a challenge
since b-tagging is less effective. For ∣Vcb′∣≪∣Vcb∣, b′→tW
would tend to dominate, while b′→t′W∗ could also open for heavier
b′, leading to thepossibility of quadruple-W signals via b′bˉ′→bbˉW+W−W+W−. The FCNC b′→bZ,bH decays could still dominate if
mb′ is just above 200 GeV. For the case of t′, ingeneral t′→bW would be dominant, hence it behaves like a heavy top. For both b′ and
t′, except for the intriguing light b′ case, FCNC decays are in the
10−4−10−2 range, and are quite detectable at the LHC.For a possible
future ILC, we find the associated production of FCNC e+e−→bsˉ,
tcˉ are below sensitivity, while e+e−→b′bˉ
andt′tˉ can be better probed.Tevatron Run-II can still probe the
lighter b′ or t′ scenario. LHC would either discover the fourth generation
and measure the FCNC rates, or rule out the fourth generation conclusively.Comment: 31 pages, 15 eps figures, version to appear in JHE