# ${{\boldsymbol t}}{{\overline{\boldsymbol t}}}$ Production Cross Section in ${{\boldsymbol p}}{{\overline{\boldsymbol p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV INSPIRE search

Unless otherwise noted the first quoted error is from statistics, the second from systematic uncertainties, and the third from luminosity. If only two errors are quoted the luminosity is included in the systematic uncertainties.
VALUE (pb) DOCUMENT ID TECN  COMMENT
• • • We do not use the following data for averages, fits, limits, etc. • • •
$7.26$ $\pm0.13$ ${}^{+0.57}_{-0.50}$ 1
 2016 F
D0 ${{\mathit \ell}}{{\mathit \ell}}$ , ${{\mathit \ell}}$+jets channels
$8.1$ $\pm2.1$ 2
 2014 A
CDF ${{\mathit \ell}}$ + ${{\mathit \tau}_{{h}}}$ + ${}\geq{}$ 2jets (${}\geq{}1{{\mathit b}}$-tag)
$7.60$ $\pm0.20$ $\pm0.29$ $\pm0.21$ 3
 2014 H
TEVA ${{\mathit \ell}}{{\mathit \ell}}$ , ${{\mathit \ell}}$+jets, all-jets channels
$8.0$ $\pm0.7$ $\pm0.6$ $\pm0.5$ 4
 2014 K
D0 ${{\mathit \ell}}+\not E_T+{}\geq{}$4 jets (${}\geq{}1{{\mathit b}}$-tag)
$7.09$ $\pm0.84$ 5
 2013 AB
CDF ${{\mathit \ell}}{{\mathit \ell}}$ + $\not E_T$ + ${}\geq{}$2 jets
$7.5$ $\pm1.0$ 6
 2013 G
CDF ${{\mathit \ell}}$ + $\not E_T$ + ${}\geq{}$ 3jets (${}\geq{}1{{\mathit b}}$-tag)
$8.8$ $\pm3.3$ $\pm2.2$ 7
 2012 AL
CDF ${{\mathit \tau}_{{h}}}$ + $\not E_T$ +4j (${}\geq{}1{{\mathit b}}$)
$8.5$ $\pm0.6$ $\pm0.7$ 8
 2011 D
CDF ${{\mathit \ell}}$ + $\not E_T$ + jets (${}\geq{}1{{\mathit b}}$-tag)
$7.64$ $\pm0.57$ $\pm0.45$ 9
 2011 W
CDF ${{\mathit \ell}}$ + $\not E_T$ + jets (${}\geq{}1{{\mathit b}}$-tag)
$7.99$ $\pm0.55$ $\pm0.76$ $\pm0.46$ 10
 2011 Y
CDF $\not E_T$ + ${}\geq{}$4jets (0,1,2 ${{\mathit b}}$-tag)
$7.78$ ${}^{+0.77}_{-0.64}$ 11
 2011 E
D0 ${{\mathit \ell}}$ + $\not E_T$ + ${}\geq{}$2 jets
$7.56$ ${}^{+0.63}_{-0.56}$ 12
 2011 Z
D0 Combination
$6.27$ $\pm0.73$ $\pm0.63$ $\pm0.39$ 13
 2010 AA
CDF Repl. by AALTONEN 2013AB
$7.2$ $\pm0.5$ $\pm1.0$ $\pm0.4$ 14
 2010 E
CDF ${}\geq{}$6 jets, vtx ${{\mathit b}}$-tag
$7.8$ $\pm2.4$ $\pm1.6$ $\pm0.5$ 15
 2010 V
CDF ${{\mathit \ell}}$ +${}\geq{}$3 jets, soft-${{\mathit e}}{{\mathit b}}$-tag
$7.70$ $\pm0.52$ 16
 2010 W
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
 2010 I
D0 ${}\geq{}$6 jets with 2 ${{\mathit b}}$-tags
$6.9$ $\pm1.2$ ${}^{+0.8}_{-0.7}$ $\pm0.4$ 18
 2010 Q
D0 ${{\mathit \tau}_{{h}}}$ + 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
 2009 H
CDF ${{\mathit \ell}}$ + ${}\geq{}$3 jets+$\not E_T$/soft ${{\mathit \mu}}{{\mathit b}}$-tag
$8.18$ ${}^{+0.98}_{-0.87}$ 21
 2009 AG
D0 ${{\mathit \ell}}$ + jets, ${{\mathit \ell}}{{\mathit \ell}}$ and ${{\mathit \ell}}{{\mathit \tau}}$ + jets
$7.5$ $\pm1.0$ ${}^{+0.7}_{-0.6}$ ${}^{+0.6}_{-0.5}$ 22
 2009 R
D0 ${{\mathit \ell}}{{\mathit \ell}}$ and ${{\mathit \ell}}{{\mathit \tau}}$ + jets
$8.18$ ${}^{+0.90}_{-0.84}$ $\pm0.50$ 23
 2008 M
D0 ${{\mathit \ell}}$ + n jets with 0,1,2 ${{\mathit b}}$-tag
$7.62$ $\pm0.85$ 24
 2008 N
D0 ${{\mathit \ell}}$ + n jets + ${{\mathit b}}$-tag or kinematics
$8.5$ ${}^{+2.7}_{-2.2}$ 25
 2008
CDF ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$, ${{\mathit \mu}}$)
$8.3$ $\pm1.0$ ${}^{+2.0}_{-1.5}$ $\pm0.5$ 26
 2007 D
CDF ${}\geq{}$6 jets, vtx ${{\mathit b}}$-tag
$7.4$ $\pm1.4$ $\pm1.0$ 27
 2007 O
D0 ${{\mathit \ell}}{{\mathit \ell}}$ + jets, vtx ${{\mathit b}}$-tag
$4.5$ ${}^{+2.0}_{-1.9}$ ${}^{+1.4}_{-1.1}$ $\pm0.3$ 28
 2007 P
D0 ${}\geq{}$6 jets, vtx ${{\mathit b}}$-tag
$6.4$ ${}^{+1.3}_{-1.2}$ $\pm0.7$ $\pm0.4$ 29
 2007 R
D0 ${{\mathit \ell}}$ + ${}\geq{}$4 jets
$6.6$ $\pm0.9$ $\pm0.4$ 30
 2006 X
D0 ${{\mathit \ell}}$ + jets, vtx ${{\mathit b}}$-tag
$8.7$ $\pm0.9$ ${}^{+1.1}_{-0.9}$ 31
 2006 Z
CDF ${{\mathit \ell}}$ + jets, vtx ${{\mathit b}}$-tag
$5.8$ $\pm1.2$ ${}^{+0.9}_{-0.7}$ 32
 2006 C
CDF missing $\mathit E_{T}$ + jets, vtx ${{\mathit b}}$-tag
$7.5$ $\pm2.1$ ${}^{+3.3}_{-2.2}$ ${}^{+0.5}_{-0.4}$ 33
 2006 E
CDF $6 - 8$ jets, ${{\mathit b}}$-tag
$8.9$ $\pm1.0$ ${}^{+1.1}_{-1.0}$ 34
 2006 F
CDF ${{\mathit \ell}}$ +${}\geq{}$3 jets, ${{\mathit b}}$-tag
$8.6$ ${}^{+1.6}_{-1.5}$ $\pm0.6$ 35
 2005 Q
D0 ${{\mathit \ell}}$ + n jets
$8.6 {}^{+3.2}_{-2.7}\pm0.6$ 36
 2005 R
D0 di-lepton + n jets
$6.7$ ${}^{+1.4}_{-1.3}$ ${}^{+1.6}_{-1.1}$ $\pm0.4$ 37
 2005 X
D0 ${{\mathit \ell}}$ + jets $/$ kinematics
$5.3$ $\pm3.3$ ${}^{+1.3}_{-1.0}$ 38
 2005 S
CDF ${{\mathit \ell}}$ + jets $/$ soft ${{\mathit \mu}}{{\mathit b}}$-tag
$6.6$ $\pm1.1$ $\pm1.5$ 39
 2005 T
CDF ${{\mathit \ell}}$ + jets $/$ kinematics
$6.0$ ${}^{+1.5}_{-1.6}$ ${}^{+1.2}_{-1.3}$ 40
 2005 U
CDF ${{\mathit \ell}}$ + jets/kinematics + vtx ${{\mathit b}}$-tag
$5.6$ ${}^{+1.2}_{-1.1}$ ${}^{+0.9}_{-0.6}$ 41
 2005 V
CDF ${{\mathit \ell}}$ + n jets
$7.0$ ${}^{+2.4}_{-2.1}$ ${}^{+1.6}_{-1.1}$ $\pm0.4$ 42
 2004 I
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.
2  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.
3  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.
References:
 ABAZOV 2016F
PR D94 092004 Measurement of the Inclusive ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV and Determination of the Top Quark Pole Mass
 AALTONEN 2014H
PR D89 072001 Combination of Measurements of the Top-Quark Pair Production Cross Section from the Tevatron Collider
 AALTONEN 2014A
PR D89 091101 Study of Top-Quark Production and Decays involving a Tau Lepton at CDF and Limits on a Charged-Higgs Boson Contribution
 ABAZOV 2014K
PR D90 092006 Measurement of differential ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production Cross Sections in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions
 AALTONEN 2013G
PR D87 111101 Measurement of $\mathit R$ = B( ${{\mathit t}}$ $\rightarrow$ ${{\mathit W}}{{\mathit b}}$ )/B( ${{\mathit t}}$ $\rightarrow$ ${{\mathit W}}{{\mathit q}}$ ) in Top$−$quark$−$pair Decays using Lepton+jets Events and the Full CDF Run II Data Set
 AALTONEN 2013AB
PR D88 091103 Measurement of the Top-Quark Pair-Production Cross Section in Events with Two Leptons and Bottom-Quark Jets using the Full CDF Data Set
 AALTONEN 2012AL
PRL 109 192001 Measurements of the Top-Quark Mass and the ${{\mathit t}}{{\overline{\mathit t}}}$ Cross Section in the Hadronic ${{\mathit \tau}}$+jets Decay Channel at $\sqrt {s }$ = 1.96 TeV
 AALTONEN 2011W
PR D84 031101 Measurement of the Top Pair Production Cross Section in the Lepton + Jets Channel Using a Jet Flavor Discriminant
 AALTONEN 2011Y
PR D84 032003 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 Events with Large Missing Transverse Energy and Jets
 AALTONEN 2011D
PR D83 071102 Measurement of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production Cross Section with an $\mathit in~situ$ Calibration of ${\mathit {\mathit b}}$-jet Identification Efficiency
 ABAZOV 2011E
PR D84 012008 Measurement of the Top Quark Pair Production Cross Section in the Lepton+Jets Channel in Proton-Antiproton Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2011Z
PL B704 403 Measurement of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production Cross Section using Dilepton Events in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions
 AALTONEN 2010AA
PR D82 052002 Measurement of the Top Pair Production Cross Section in the Dilepton Decay Channel in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 AALTONEN 2010W
PRL 105 012001 Measurement of the Ratio $\sigma\mathrm {({\mathit {\mathit t}}{\mathit {\overline{\mathit t}}})}$ /$\sigma\mathrm {(Z/ {{\mathit \gamma}^{*}} \rightarrow {{\mathit \ell}} {{\mathit \ell}} )}$ and Precise Extraction of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Cross Section
 AALTONEN 2010V
PR D81 092002 Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collision at $\sqrt {s }$ = 1.96 TeV using Soft Electron ${\mathit {\mathit b}}$-Tagging
 AALTONEN 2010E
PR D81 052011 Measurement of the Top Quark Mass and ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ Cross Section in the All-Hadronic Mode with the CDFII Detector
 ABAZOV 2010Q
PR D82 071102 Measurement of ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production in the ${{\mathit \tau}}$+Jets Topology using ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2010I
PR D82 032002 Measurement of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Cross Section using High-Multiplicity Jet Events
PR D79 112007 Measurement of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96$~$TeV using Dilepton Events with a Lepton Plus Track Selection
 AALTONEN 2009H
PR D79 052007 Measurement of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production Cross Section in 2${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96$~$TeV using Lepton Plus Jets Events with Soft Muon ${\mathit {\mathit b}}$ Tagging
 ABAZOV 2009R
PL B679 177 Measurement of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production Cross Section and Top Quark Mass Extraction using Dilepton Events in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions
 ABAZOV 2009AG
PR D80 071102 Combination of ${{\mathit t}}{{\overline{\mathit t}}}$ Cross Section Measurements and Constraints on the Mass of the Top Quark and Its Decays into Charged Higgs Bosons
 ABAZOV 2008N
PRL 100 192004 Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
 ABAZOV 2008M
PRL 100 192003 Simultaneous Measurement of the Ratio B( ${{\mathit t}}$ $\rightarrow$ ${{\mathit W}}{{\mathit b}}$ )/B( ${{\mathit t}}$ $\rightarrow$ ${{\mathit W}}{{\mathit q}}$ ) and the Top Quark pair Production Cross Section with the ${D0}$ Detector at $\sqrt {s }$ = 1.96 TeV
 ABULENCIA 2008
PR D78 012003 Cross Section Measurements of High-$p_T$ Dilepton Final-State Processes Using a Global Fitting Method
 AALTONEN 2007D
PR D76 072009 Measurement of the ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section and the Top Quark Mass at $\sqrt {s }$ = 1.96 TeV in the All-Hadronic Decay Mode
 ABAZOV 2007O
PR D76 052006 Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions using Dilepton Events
 ABAZOV 2007R
PR D76 092007 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 Characteristics of lepton+jets Events
 ABAZOV 2007P
PR D76 072007 Measurement of the ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ +X Production Cross Section at $\sqrt {s }$ = 1.96 TeV in the Fully Hadronic Decay Channel
 ABAZOV 2006X
PR D74 112004 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 Secondary Vertex ${\mathit {\mathit b}}$ Tagging
 ABULENCIA 2006Z
PRL 97 082004 Measurement of the ${{\mathit t}}{{\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ =1.96 TeV
 ABULENCIA,A 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
 ABULENCIA,A 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
 ABULENCIA,A 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
 ABAZOV 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
 ABAZOV 2005R
PL B626 55 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 in Dilepton Final States
 ABAZOV 2005X
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
 ACOSTA 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
 ACOSTA 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
 ACOSTA 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
 ACOSTA 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
 ACOSTA 2004I
PRL 93 142001 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 Dilepton Events