pdgLive

2016

${{\mathit \ell}}{{\mathit \ell}}$ , ${{\mathit \ell}}$+jets channels

$8.1$ $\pm2.1$

2014

CDF

${{\mathit \ell}}$ + ${{\mathit \tau}_{{h}}}$ + ${}\geq{}$ 2jets (${}\geq{}1{{\mathit b}}$-tag)

$7.60$ $\pm0.20$ $\pm0.29$ $\pm0.21$

2014

TEVA

${{\mathit \ell}}{{\mathit \ell}}$ , ${{\mathit \ell}}$+jets, all-jets channels

$8.0$ $\pm0.7$ $\pm0.6$ $\pm0.5$

⁴

2014

${{\mathit \ell}}+\not E_T+{}\geq{}$4 jets (${}\geq{}1{{\mathit b}}$-tag)

$7.09$ $\pm0.84$

⁵

2013

CDF

${{\mathit \ell}}{{\mathit \ell}}$ + $\not E_T$ + ${}\geq{}$2 jets

$7.5$ $\pm1.0$

⁶

2013

CDF

${{\mathit \ell}}$ + $\not E_T$ + ${}\geq{}$ 3jets (${}\geq{}1{{\mathit b}}$-tag)

$8.8$ $\pm3.3$ $\pm2.2$

⁷

2012

CDF

${{\mathit \tau}_{{h}}}$ + $\not E_T$ +4j (${}\geq{}1{{\mathit b}}$)

$8.5$ $\pm0.6$ $\pm0.7$

⁸

CDF

${{\mathit \ell}}$ + $\not E_T$ + jets (${}\geq{}1{{\mathit b}}$-tag)

$7.64$ $\pm0.57$ $\pm0.45$

⁹

CDF

${{\mathit \ell}}$ + $\not E_T$ + jets (${}\geq{}1{{\mathit b}}$-tag)

$7.99$ $\pm0.55$ $\pm0.76$ $\pm0.46$

¹⁰

CDF

$\not E_T$ + ${}\geq{}$4jets (0,1,2 ${{\mathit b}}$-tag)

$7.78$ ${}^{+0.77}_{-0.64}$

¹¹

${{\mathit \ell}}$ + $\not E_T$ + ${}\geq{}$2 jets

$7.56$ ${}^{+0.63}_{-0.56}$

¹²

Combination

$6.27$ $\pm0.73$ $\pm0.63$ $\pm0.39$

¹³

CDF

Repl. by AALTONEN 2013AB

$7.2$ $\pm0.5$ $\pm1.0$ $\pm0.4$

¹⁴

CDF

${}\geq{}$6 jets, vtx ${{\mathit b}}$-tag

$7.8$ $\pm2.4$ $\pm1.6$ $\pm0.5$

¹⁵

CDF

${{\mathit \ell}}$ +${}\geq{}$3 jets, soft-${{\mathit e}}{{\mathit b}}$-tag

$7.70$ $\pm0.52$

¹⁶

CDF

${{\mathit \ell}}$ + $\not E_T$ + ${}\geq{}$3 jets + ${{\mathit b}}$-tag, norm. to ${\mathit \sigma (}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{)}_{TH}$

$6.9$ $\pm2.0$

¹⁷

${}\geq{}$6 jets with 2 ${{\mathit b}}$-tags

$6.9$ $\pm1.2$ ${}^{+0.8}_{-0.7}$ $\pm0.4$

¹⁸

${{\mathit \tau}_{{h}}}$ + jets

$9.6$ $\pm1.2$ ${}^{+0.6}_{-0.5}$ $\pm0.6$

¹⁹

CDF

${{\mathit \ell}}{{\mathit \ell}}$ + $\not E_T$ $/$ vtx ${{\mathit b}}$-tag

$9.1$ $\pm1.1$ ${}^{+1.0}_{-0.9}$ $\pm0.6$

²⁰

CDF

${{\mathit \ell}}$ + ${}\geq{}$3 jets+$\not E_T$/soft ${{\mathit \mu}}{{\mathit b}}$-tag

$8.18$ ${}^{+0.98}_{-0.87}$

²¹

${{\mathit \ell}}$ + jets, ${{\mathit \ell}}{{\mathit \ell}}$ and ${{\mathit \ell}}{{\mathit \tau}}$ + jets

$7.5$ $\pm1.0$ ${}^{+0.7}_{-0.6}$ ${}^{+0.6}_{-0.5}$

²²

${{\mathit \ell}}{{\mathit \ell}}$ and ${{\mathit \ell}}{{\mathit \tau}}$ + jets

$8.18$ ${}^{+0.90}_{-0.84}$ $\pm0.50$

²³

${{\mathit \ell}}$ + n jets with 0,1,2 ${{\mathit b}}$-tag

$7.62$ $\pm0.85$

²⁴

${{\mathit \ell}}$ + n jets + ${{\mathit b}}$-tag or kinematics

$8.5$ ${}^{+2.7}_{-2.2}$

²⁵

CDF

${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$, ${{\mathit \mu}}$)

$8.3$ $\pm1.0$ ${}^{+2.0}_{-1.5}$ $\pm0.5$

²⁶

CDF

${}\geq{}$6 jets, vtx ${{\mathit b}}$-tag

$7.4$ $\pm1.4$ $\pm1.0$

²⁷

${{\mathit \ell}}{{\mathit \ell}}$ + jets, vtx ${{\mathit b}}$-tag

$4.5$ ${}^{+2.0}_{-1.9}$ ${}^{+1.4}_{-1.1}$ $\pm0.3$

²⁸

${}\geq{}$6 jets, vtx ${{\mathit b}}$-tag

$6.4$ ${}^{+1.3}_{-1.2}$ $\pm0.7$ $\pm0.4$

²⁹

${{\mathit \ell}}$ + ${}\geq{}$4 jets

$6.6$ $\pm0.9$ $\pm0.4$

³⁰

${{\mathit \ell}}$ + jets, vtx ${{\mathit b}}$-tag

$8.7$ $\pm0.9$ ${}^{+1.1}_{-0.9}$

³¹

CDF

${{\mathit \ell}}$ + jets, vtx ${{\mathit b}}$-tag

$5.8$ $\pm1.2$ ${}^{+0.9}_{-0.7}$

³²

CDF

missing $\mathit E_{T}$ + jets, vtx ${{\mathit b}}$-tag

$7.5$ $\pm2.1$ ${}^{+3.3}_{-2.2}$ ${}^{+0.5}_{-0.4}$

³³

CDF

$6 - 8$ jets, ${{\mathit b}}$-tag

$8.9$ $\pm1.0$ ${}^{+1.1}_{-1.0}$

³⁴

CDF

${{\mathit \ell}}$ +${}\geq{}$3 jets, ${{\mathit b}}$-tag

$8.6$ ${}^{+1.6}_{-1.5}$ $\pm0.6$

³⁵

${{\mathit \ell}}$ + n jets

$8.6 {}^{+3.2}_{-2.7}\pm0.6$

³⁶

di-lepton + n jets

$6.7$ ${}^{+1.4}_{-1.3}$ ${}^{+1.6}_{-1.1}$ $\pm0.4$

³⁷

${{\mathit \ell}}$ + jets $/$ kinematics

$5.3$ $\pm3.3$ ${}^{+1.3}_{-1.0}$

³⁸

CDF

${{\mathit \ell}}$ + jets $/$ soft ${{\mathit \mu}}{{\mathit b}}$-tag

$6.6$ $\pm1.1$ $\pm1.5$

³⁹

CDF

${{\mathit \ell}}$ + jets $/$ kinematics

$6.0$ ${}^{+1.5}_{-1.6}$ ${}^{+1.2}_{-1.3}$

⁴⁰

CDF

${{\mathit \ell}}$ + jets/kinematics + vtx ${{\mathit b}}$-tag

$5.6$ ${}^{+1.2}_{-1.1}$ ${}^{+0.9}_{-0.6}$

⁴¹

CDF

${{\mathit \ell}}$ + n jets

$7.0$ ${}^{+2.4}_{-2.1}$ ${}^{+1.6}_{-1.1}$ $\pm0.4$

⁴²

2004

CDF

di-lepton + jets + missing ET

¹	ABAZOV 2016F based on 9.7 fb${}^{-1}$ of data. The result is for ${\mathit m}_{{{\mathit t}}}$ = 172.5 GeV, and the ${\mathit m}_{{{\mathit t}}}$ dependence is shown in Table V and Fig. 9. The result agrees with the NNLO+NNLL SM prediction of $7.35$ ${}^{+0.23}_{-0.27}$ pb.

Based on 9 fb${}^{-1}$ of data. The measurement is in the channel ${{\mathit t}}$ ${{\overline{\mathit t}}}$ $\rightarrow$ ( ${{\mathit b}}{{\mathit \ell}}{{\mathit \nu}}$) ( ${{\mathit b}}{{\mathit \tau}}{{\mathit \nu}}$), where ${{\mathit \tau}}$ decays into hadrons (${{\mathit \tau}_{{h}}}$), and ${{\mathit \ell}}$ (${{\mathit e}}$ or ${{\mathit \mu}}$) include ${{\mathit \ell}}$ from ${{\mathit \tau}}$ decays (${{\mathit \tau}_{{{{\mathit \ell}}}}}$). The result is for ${\mathit m}_{{{\mathit t}}}$ = 173 GeV.

Based on 8.8 fb${}^{-1}$ of data. Combination of CDF and D0 measurements given, respectively, by ${\mathit \sigma (}{{\mathit t}}{{\overline{\mathit t}}}$; CDF${)}$ = $7.63$ $\pm0.31$ $\pm0.36$ $\pm0.16$ pb, ${\mathit \sigma (}{{\mathit t}}{{\overline{\mathit t}}}$; D0${)}$ = $7.56$ $\pm0.20$ $\pm0.32$ $\pm0.46$ pb. All the results are for ${\mathit m}_{{{\mathit t}}}$ = 172.5 GeV. The ${\mathit m}_{{{\mathit t}}}$ dependence of the mean value is parametrized in eq. (1) and shown in Fig. 2.

⁴	Based on 9.7 fb${}^{-1}$ of data. Differential cross sections with respect to , $\vert {{\mathit y}}$(top)$\vert $, $\mathit E_{T}$(top) are shown in Figs. 9, 10, 11, respectively, and are compared to the predictions of MC models.

⁵	Based on 8.8 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV.

⁶

Based on 8.7 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV. Measure the ${{\mathit t}}{{\overline{\mathit t}}}$ cross section simultaneously with the fraction of ${{\mathit t}}$ $\rightarrow$ ${{\mathit W}}{{\mathit b}}$ decays. The correlation coefficient between those two measurements is $-0.434$. Assume unitarity of the 3${\times }$3 CKM matrix and set $\vert \mathit V_{\mathit tb}\vert $ $>$ 0.89 at 95$\%$ CL.

⁷	Based on 2.2 fb${}^{-1}$ of data in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at 1.96 TeV. The result assumes the acceptance for ${\mathit m}_{{{\mathit t}}}$ = 172.5 GeV.

⁸

Based on 1.12 fb${}^{-1}$ and assumes ${\mathit m}_{{{\mathit t}}}$ = 175 GeV, where the cross section changes by $\pm0.1$ pb for every $\mp{}$1 GeV shift in ${\mathit m}_{{{\mathit t}}}$. AALTONEN 2011D fits simultaneously the ${{\mathit t}}{{\overline{\mathit t}}}$ production cross section and the ${{\mathit b}}$-tagging efficiency and find improvements in both measurements.

⁹

Based on 2.7 fb${}^{-1}$. The first error is from statistics and systematics, the second is from luminosity. The result is for ${\mathit m}_{{{\mathit t}}}$ = 175 GeV. AALTONEN 2011W fits simultaneously a jet flavor discriminator between ${{\mathit b}}$-, ${{\mathit c}}$-, and light-quarks, and find significant reduction in the systematic error.

¹⁰	Based on 2.2 fb${}^{-1}$. The result is for ${\mathit m}_{{{\mathit t}}}$ = 172.5 GeV. AALTONEN 2011Y selects multi-jet events with large $\not E_T$, and vetoes identified electrons and muons.

¹¹	Based on 5.3 fb${}^{-1}$. The error is statistical + systematic + luminosity combined. The result is for ${\mathit m}_{{{\mathit t}}}$ = 172.5 GeV. The results for other ${\mathit m}_{{{\mathit t}}}$ values are given in Table XII and eq.(10) of ABAZOV 2011E.

¹²

Combination of a dilepton measurement presented in ABAZOV 2011Z (based on 5.4 fb${}^{-1}$), which yields $7.36$ ${}^{+0.90}_{-0.79}$ (stat+syst) pb, and the lepton + jets measurement of ABAZOV 2011E. The result is for ${\mathit m}_{{{\mathit t}}}$ = 172.5 GeV. The results for other ${\mathit m}_{{{\mathit t}}}$ values is given by eq.(5) of ABAZOV 2011A.

¹³	Based on 2.8 fb${}^{-1}$. The result is for ${\mathit m}_{{{\mathit t}}}$ = 175 GeV.

¹⁴	Based on 2.9 fb${}^{-1}$. Result is obtained from the fraction of signal events in the top quark mass measurement in the all hadronic decay channel.

¹⁵	Based on 1.7 fb${}^{-1}$. The result is for ${\mathit m}_{{{\mathit t}}}$ = 175 GeV. AALTONEN 2010V uses soft electrons from ${{\mathit b}}$-hadron decays to suppress ${{\mathit W}}$+jets background events.

¹⁶

Based on 4.6 fb${}^{-1}$. The result is for ${\mathit m}_{{{\mathit t}}}$ = 172.5 GeV. The ratio ${\mathit \sigma (}$ ${{\mathit t}}$ ${{\overline{\mathit t}}}$ $\rightarrow$ ${{\mathit \ell}}$ +jets${)}$ $/$ ${\mathit \sigma (}$ ${{\mathit Z}}$ $/$ ${{\mathit \gamma}^{*}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{)}$ is measured and then multiplied by the theoretical ${{\mathit Z}}$ $/$ ${{\mathit \gamma}^{*}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}$ cross section of ${\mathit \sigma (}$ ${{\mathit Z}}$ $/$ ${{\mathit \gamma}^{*}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{)}$ = $251.3$ $\pm5.0$ pb, which is free from the luminosity error.

¹⁷

Based on 1 fb${}^{-1}$. The result is for ${\mathit m}_{{{\mathit t}}}$ = 175 GeV. $7.9$ $\pm2.3$ pb is found for ${\mathit m}_{{{\mathit t}}}$ = 170$~$GeV. ABAZOV 2010I uses a likelihood discriminant to separate signal from background, where the background model was created from lower jet-multiplicity data.

¹⁸

Based on 1 fb${}^{-1}$. The result is for ${\mathit m}_{{{\mathit t}}}$ = 170 GeV. For ${\mathit m}_{{{\mathit t}}}$ = 175 GeV, the result is $6.3$ ${}^{+1.2}_{-1.1}$(stat)$\pm0.7$(syst)$\pm0.4$(lumi)$~$pb. Cross section of ${{\mathit t}}{{\overline{\mathit t}}}$ production has been measured in the ${{\mathit t}}$ ${{\overline{\mathit t}}}$ $\rightarrow$ ${{\mathit \tau}_{{h}}}{+}$ jets topology, where ${{\mathit \tau}_{{h}}}$ denotes hadronically decaying ${{\mathit \tau}}$ leptons. The result for the cross section times the branching ratio is ${\mathit \sigma (}$ ${{\mathit t}}{{\overline{\mathit t}}}{)}$ $\cdot{}$ B( ${{\mathit t}}$ ${{\overline{\mathit t}}}$ $\rightarrow$ ${{\mathit \tau}_{{h}}}{+}$ jets) = $0.60$ ${}^{+0.23}_{-0.22}{}^{+0.15}_{-0.14}$ $\pm0.04~$pb for ${\mathit m}_{{{\mathit t}}}$ = 170 GeV.

¹⁹

Based on 1.1 fb${}^{-1}$. The result is for B( ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ ) = 10.8$\%$ and ${\mathit m}_{{{\mathit t}}}$ = 175 GeV; the mean value is 9.8 for ${\mathit m}_{{{\mathit t}}}$ = 172.5 GeV and 10.1 for ${\mathit m}_{{{\mathit t}}}$ = 170 GeV. AALTONEN 2009AD used high $p_T$ ${{\mathit e}}$ or ${{\mathit \mu}}$ with an isolated track to select ${{\mathit t}}{{\overline{\mathit t}}}$ decays into dileptons including ${{\mathit \ell}}$ = ${{\mathit \tau}}$. The result is based on the candidate event samples with and without vertex ${{\mathit b}}$-tag.

²⁰	Based on 2 fb${}^{-1}$. The result is for ${\mathit m}_{{{\mathit t}}}$ = 175 GeV; the mean value is 3$\%$ higher for ${\mathit m}_{{{\mathit t}}}$ = 170 GeV and 4$\%$ lower for ${\mathit m}_{{{\mathit t}}}$ = 180 GeV.

²¹

Result is based on 1 fb${}^{-1}$ of data. The result is for ${\mathit m}_{{{\mathit t}}}$ = 170 GeV, and the mean value decreases with increasing ${\mathit m}_{{{\mathit t}}}$; see their Fig. 2. The result is obtained after combining ${{\mathit \ell}}$ + jets, ${{\mathit \ell}}{{\mathit \ell}}$ , and ${{\mathit \ell}}{{\mathit \tau}}$ final states, and the ratios of the extracted cross sections are R${}^{ {{\mathit \ell}} {{\mathit \ell}} / {{\mathit \ell}} {{\mathit j}} }$ = $0.86$ ${}^{+0.19}_{-0.17}$ and R${}^{ {{\mathit \ell}} {{\mathit \tau}} / {{\mathit \ell}} {{\mathit \ell}} {{\mathit \ell}} {{\mathit j}} }$ = $0.97$ ${}^{+0.32}_{-0.29}$, consistent with the SM expectation of R = 1. This leads to the upper bound of B( ${{\mathit t}}$ $\rightarrow$ ${{\mathit b}}{{\mathit H}^{+}}$ ) as a function of ${\mathit m}_{{{\mathit H}^{+}}}$. Results are shown in their Fig. 1 for B( ${{\mathit H}^{+}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \nu}}$ ) = 1 and B( ${{\mathit H}^{+}}$ ${{\overline{\mathit s}}}$ ) = 1 cases. Comparison of the ${\mathit m}_{{{\mathit t}}}$ dependence of the extracted cross section and a partial NNLO prediction gives ${\mathit m}_{{{\mathit t}}}$ = $169.1$ ${}^{+5.9}_{-5.2}$ GeV.

²²

Result is based on 1 fb${}^{-1}$ of data. The result is for ${\mathit m}_{{{\mathit t}}}$ = 170 GeV, and the mean value changes by $-0.07$ [${\mathit m}_{{{\mathit t}}}$(GeV)$−$170] pb near the reference ${\mathit m}_{{{\mathit t}}}$ value. Comparison of the ${\mathit m}_{{{\mathit t}}}$ dependence of the extracted cross section and a partial NNLO QCD prediction gives ${\mathit m}_{{{\mathit t}}}$ = $171.5$ ${}^{+9.9}_{-8.8}$ GeV. The ${{\mathit \ell}}{{\mathit \tau}}$ channel alone gives $7.6$ ${}^{+4.9}_{-4.3}{}^{+3.5}_{-3.4}{}^{+1.4}_{-0.9}$ pb and the ${{\mathit \ell}}{{\mathit \ell}}$ channel gives $7.5$ ${}^{+1.2}_{-1.1}{}^{+0.7}_{-0.6}{}^{+0.7}_{-0.5}$ pb.

²³	Result is based on 0.9 fb${}^{-1}$ of data. The first error is from stat + syst, while the latter error is from luminosity. The result is for ${\mathit m}_{{{\mathit t}}}$=175 GeV, and the mean value changes by $-0.09$ pb$\cdot{}[{\mathit m}_{{{\mathit t}}}$(GeV)$−$175].

²⁴

Result is based on 0.9 fb${}^{-1}$ of data. The cross section is obtained from the ${{\mathit \ell}}$ + ${}\geq{}3~$jet event rates with 1 or 2 ${{\mathit b}}$-tag, and also from the kinematical likelihood analysis of the ${{\mathit \ell}}~$+ 3, 4 jet events. The result is for ${\mathit m}_{{{\mathit t}}}$= 172.6 GeV, and its ${\mathit m}_{{{\mathit t}}}$ dependence shown in Fig. 3 leads to the constraint ${\mathit m}_{{{\mathit t}}}$ = $170$ $\pm7$ GeV when compared to the SM prediction.

²⁵

Result is based on 360 pb${}^{-1}$ of data. Events with high $p_T$ oppositely charged dileptons ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$, ${{\mathit \mu}}$) are used to obtain cross sections for ${{\mathit t}}{{\overline{\mathit t}}}$ , ${{\mathit W}^{+}}{{\mathit W}^{-}}$ , and ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ production processes simultaneously. The other cross sections are given in Table IV.

²⁶	Based on 1.02 fb${}^{-1}$ of data. Result is for ${\mathit m}_{{{\mathit t}}}$ = 175 GeV. Secondary vertex ${{\mathit b}}$-tag and neural network selections are used to achieve a signal-to-background ratio of about 1/2.

²⁷	Based on 425 pb${}^{-1}$ of data. Result is for ${\mathit m}_{{{\mathit t}}}$ = 175 GeV. For ${\mathit m}_{{{\mathit t}}}$ = 170.9 GeV, $7.8$ $\pm1.8$(stat + syst) pb is obtained.

²⁸	Based on $405$ $\pm25$ pb${}^{-1}$ of data. Result is for ${\mathit m}_{{{\mathit t}}}$ = 175 GeV. The last error is for luminosity. Secondary vertex ${{\mathit b}}$-tag and neural network are used to separate the signal events from the background.

²⁹	Based on 425 pb${}^{-1}$ of data. Assumes ${\mathit m}_{{{\mathit t}}}$ = 175 GeV.

³⁰	Based on $\sim{}$ 425 pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 175 GeV. The first error is combined statistical and systematic, the second one is luminosity.

³¹

Based on $\sim{}$318 pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 178 GeV. The cross section changes by $\pm0.08$ pb for each $\mp{}$ GeV change in the assumed ${\mathit m}_{{{\mathit t}}}$. Result is for at least one ${{\mathit b}}$-tag. For at least two ${{\mathit b}}$-tagged jets, ${{\mathit t}}{{\overline{\mathit t}}}$ signal of significance greater than 5$\sigma $ is found, and the cross section is $10.1$ ${}^{+1.6}_{-1.4}{}^{+2.0}_{-1.3}$ pb for ${\mathit m}_{{{\mathit t}}}$ = 178 GeV.

³²

Based on $\sim{}$311 pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 178 GeV. For ${\mathit m}_{{{\mathit t}}}$ = 175 GeV, the result is $6.0$ $\pm1.2$ ${}^{+0.9}_{-0.7}$. This is the first CDF measurement without lepton identification, and hence it has sensitivity to the ${{\mathit W}}$ $\rightarrow$ ${{\mathit \tau}}{{\mathit \nu}}$ mode.

³³	ABULENCIA,A 2006E measures the ${{\mathit t}}{{\overline{\mathit t}}}$ production cross section in the all hadronic decay mode by selecting events with 6 to 8 jets and at least one b-jet. S/B = 1/5 has been achieved. Based on 311 pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 178 GeV.

³⁴	Based on $\sim{}$318 pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 178 GeV. Result is for at least one ${{\mathit b}}$-tag. For at least two ${{\mathit b}}$-tagged jets, the cross section is $11.1$ ${}^{+2.3}_{-1.9}{}^{+2.5}_{-1.9}~$pb.

³⁵

ABAZOV 2005Q measures the top-quark pair production cross section with $\sim{}$230 pb${}^{-1}$ of data, based on the analysis of ${{\mathit W}}$ plus n-jet events where W decays into ${{\mathit e}}$ or ${{\mathit \mu}}$ plus neutrino, and at least one of the jets is ${{\mathit b}}$-jet like. The first error is statistical and systematic, and the second accounts for the luminosity uncertainty. The result assumes ${\mathit m}_{{{\mathit t}}}$ = 175 GeV; the mean value changes by (175$−{\mathit m}_{{{\mathit t}}}$(GeV)) ${\times }$ 0.06$~$pb in the mass range 160 to 190 GeV.

³⁶

ABAZOV 2005R measures the top-quark pair production cross section with $224 - 243$ pb${}^{-1}$ of data, based on the analysis of events with two charged leptons in the final state. The result assumes ${\mathit m}_{{{\mathit t}}}$ = 175 GeV; the mean value changes by (175$−{\mathit m}_{{{\mathit t}}}$(GeV)) ${\times }$ 0.08$~$pb in the mass range 160 to 190 GeV.

³⁷	Based on 230 pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 175 GeV.

³⁸	Based on 194 pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 175 GeV.

³⁹	Based on $194$ $\pm11$ pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 175 GeV.

⁴⁰	Based on $162$ $\pm10$ pb${}^{-1}$. Assuming ${\mathit m}_{{{\mathit t}}}$ = 175 GeV.

⁴¹

ACOSTA 2005V measures the top-quark pair production cross section with $\sim{}$162 pb${}^{-1}$ data, based on the analysis of ${{\mathit W}}$ plus n-jet events where ${{\mathit W}}$ decays into ${{\mathit e}}$ or ${{\mathit \mu}}$ plus neutrino, and at least one of the jets is ${{\mathit b}}$-jet like. Assumes ${\mathit m}_{{{\mathit t}}}$ = 175 GeV.

⁴²	ACOSTA 2004I measures the top-quark pair production cross section with $197$ $\pm12$ pb${}^{-1}$ data, based on the analysis of events with two charged leptons in the final state. Assumes ${\mathit m}_{{{\mathit t}}}$ = 175 GeV.

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2006F

PR D74 072006

Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$=1.96 TeV using Lepton+Jets Events with Jet Probability ${\mathit {\mathit b}}$-Tagging

2006C

PRL 96 202002

Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV using Missing $\mathit E_{T}$+jets Events with Secondary Vertex ${\mathit {\mathit b}}$ Tagging

2006E

PR D74 072005

Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$=1.96 TeV in the all Hadronic Decay Mode

PL B626 55

PL B626 45

Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96TeV using Kinematic Characteristics of Lepton + Jets Events

2005Q

PL B626 35

Measurement of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV Using Lepton + Jets Events with Lifetime ${\mathit {\mathit b}}$-Tagging

2005U

PR D71 072005

Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$=1.96 TeV using Kinematic Fitting of $\mathit b$-tagged Lepton+Jet Events

2005T

PR D72 052003

Measurement of the Cross Section for ${{\mathit t}}{{\overline{\mathit t}}}$ Production in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions using the Kinematics of Lepton+Jets Events

2005S

PR D72 032002

Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$=1.96 TeV using Lepton plus Jets Events with Semileptonic ${{\mathit B}}$ Decays to Muons

2005V

PR D71 052003

Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$=1.96 TeV using Lepton + Jets Events with Secondary Vertex $\mathit b$-Tagging