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o2_model [2021/04/27 20:24] Scott Lawrence [Operator content] |
o2_model [2022/12/21 04:46] (current) Rajeev S. Erramilli [Operator content] |
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===== Operator content ===== | ===== Operator content ===== | ||
- | There are two relevant | + | Three of the leading |
\[ | \[ | ||
- | \Delta_\phi = 0.51926(32) \text{ and } \Delta_s = 1.5117(25) | + | \Delta_\phi = 0.519088(\mathbf{22}),~\Delta_s = 1.51136(\mathbf{22}),~\Delta_t = 1.23629(\mathbf{11}). |
\] | \] | ||
- | while the nonvanishing | + | Four of OPE coefficients |
\[ | \[ | ||
- | \lambda_{sss} = 0.8286(60) \text{ and } \lambda_{\phi\phi | + | \lambda_{\phi\phi s} = 0.687126(27),~\lambda_{s s s} = 0.830914(32), |
- | \text. | + | |
\] | \] | ||
- | These data are from the bootstrap, computed here: [[https:// | + | Additionally, |
+ | |||
+ | \[ | ||
+ | C_J / C_J^{\text {free}}=0.904395(28), | ||
+ | \] | ||
+ | |||
+ | Finally, four additional scalar operators: $s'$ (the next-to-leading singlet), $t'$ (the next-to-leading charge 2 operator), and the leading charge 3 and charge 4 operators, have been determined nonrigorously: | ||
+ | |||
+ | \[ | ||
+ | \Delta_{s' | ||
+ | \] | ||
+ | |||
+ | These data are from the bootstrap, computed here: [[https:// | ||
===== Physical realizations ===== | ===== Physical realizations ===== | ||