\usepackage or this document’s own macros. Corpus-wide, \bm occurs 327 times, \Perp is defined by no package and spans 10 documents, and 11,088 of 11,624 undefined occurrences are the source document’s own macros. A row that looks wrong here may be correct, and one that looks right here may not compile. The LaTeX report renders through the document’s own preamble and is the surface to judge from.1034 rows
The page, the confidence and the picture of an inline formula are its HOST LINE's --- a formula has none of its own. A line's confidence is not a formula's.
| Identifier | Page | Conf. | LaTeX source | Rendered | Image |
|---|---|---|---|---|---|
| 1510.06699_FO0001 | 1 | 0.755 | { }^{1,2, \mathrm{a}} | | |
| 1510.06699_FO0002 | 1 | 0.755 | { }^{1, \mathrm{~b}} | | |
| 1510.06699_FO0003 | 1 | 0.969 | { }^{1)} | | |
| 1510.06699_FO0004 | 1 | 0.979 | { }^{2)} | | |
| 1510.06699_FO0005 | 1 | 0.947 | { }^{\underline{1}} | | |
| 1510.06699_FO0006 | 1 | 0.998 | \varphi | | |
| 1510.06699_FO0007 | 1 | 0.798 | { }^{\text {a) }} | | |
| 1510.06699_FO0008 | 1 | 0.997 | { }^{\text {b) }} | | |
| 1510.06699_FO0009 | 1 | 1.000 | S_{\mathrm{M}}= | | |
| 1510.06699_FO0010 | 1 | 1.000 | \int L_{\mathrm{M}}\left(\varphi, \partial_{\mu} \varphi\right) d^{4} x | | |
| 1510.06699_FO0011 | 1 | 1.000 | h_{a}{ }^{\mu} | | |
| 1510.06699_FO0012 | 1 | 1.000 | A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0013 | 1 | 0.990 | \mathcal{D}_{a} \varphi | | |
| 1510.06699_FO0014 | 1 | 1.000 | S_{\mathrm{M}}=\int h^{-1} L_{\mathrm{M}}\left(\varphi, \mathcal{D}_{a} \varphi\right) d^{4} x | | |
| 1510.06699_FO0015 | 1 | 1.000 | h \equiv \operatorname{det}\left(h_{a}{ }^{\mu}\right) | | |
| 1510.06699_FO0016 | 2 | 1.000 | \left[\mathcal{D}_{a}, \mathcal{D}_{b}\right] \varphi | | |
| 1510.06699_FO0017 | 2 | 1.000 | \mathcal{R}^{a b}{ }_{c d}(h, A, \partial A) | | |
| 1510.06699_FO0018 | 2 | 0.999 | \mathcal{T}^{a}{ }_{b c}(h, \partial h, A) | | |
| 1510.06699_FO0019 | 2 | 1.000 | S_{\mathrm{G}}=\int h^{-1} L_{\mathrm{G}}\left(\mathcal{R}^{a b}{ }_{c d}, \mathcal{T}^{a}{ }_{b c}\right) d^{4} x | | |
| 1510.06699_FO0020 | 2 | 1.000 | L_{\mathrm{G}} | | |
| 1510.06699_FO0021 | 2 | 1.000 | \tau^{k}{ }_{\mu} \equiv \delta \mathcal{L}_{\mathrm{M}} / \delta h_{a}{ }^{\mu} | | |
| 1510.06699_FO0022 | 2 | 1.000 | \sigma_{a b}{ }^{\mu} \equiv \delta \mathcal{L}_{\mathrm{M}} / \delta A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0023 | 2 | 1.000 | \mathcal{L}_{\mathrm{M}} \equiv h^{-1} L_{\mathrm{M}}\left(\varphi, \mathcal{D}_{a} \varphi\right) | | |
| 1510.06699_FO0024 | 2 | 1.000 | \mathcal{R} \equiv \mathcal{R}^{a b}{ }_{a b} | | |
| 1510.06699_FO0025 | 2 | 1.000 | L_{\mathrm{G}} \propto \mathcal{R} | | |
| 1510.06699_FO0026 | 2 | 0.733 | { }^{\underline{5}} | | |
| 1510.06699_FO0027 | 2 | 1.000 | \delta \varphi \equiv \varphi^{\prime}\left(x^{\prime}\right)-\varphi(x) | | |
| 1510.06699_FO0028 | 2 | 1.000 | \delta_{0} \varphi \equiv \varphi^{\prime}(x)-\varphi(x) | | |
| 1510.06699_FO0029 | 2 | 1.000 | \delta_{0} \varphi | | |
| 1510.06699_FO0030 | 2 | 0.988 | { }^{6,9} | | |
| 1510.06699_FO0031 | 2 | 0.991 | { }^{\underline{10}} | | |
| 1510.06699_FO0032 | 2 | 1.000 | \mathcal{R}^{a b}{ }_{c d} | | |
| 1510.06699_FO0033 | 2 | 1.000 | \mathcal{T}^{a}{ }_{b c} | | |
| 1510.06699_FO0034 | 2 | 1.000 | { }^{11,12} | | |
| 1510.06699_FO0035 | 2 | 1.000 | \kappa=8 \pi G / c^{4} | | |
| 1510.06699_FO0036 | 2 | 1.000 | \Lambda | | |
| 1510.06699_FO0037 | 2 | 1.000 | a | | |
| 1510.06699_FO0038 | 3 | 1.000 | \alpha_{i} | | |
| 1510.06699_FO0039 | 3 | 1.000 | \beta_{i} | | |
| 1510.06699_FO0040 | 3 | 0.362 | { }^{\underline{12,14}-\underline{16}} | | |
| 1510.06699_FO0041 | 3 | 1.000 | \alpha_{1}, \alpha_{3} | | |
| 1510.06699_FO0042 | 3 | 1.000 | \alpha_{6} | | |
| 1510.06699_FO0043 | 3 | 0.999 | c=\hbar=1 | | |
| 1510.06699_FO0044 | 3 | 0.944 | { }^{-4} | | |
| 1510.06699_FO0045 | 3 | 0.944 | S_{\mathrm{G}} | | |
| 1510.06699_FO0046 | 3 | 1.000 | \kappa | | |
| 1510.06699_FO0047 | 3 | 0.986 | { }^{-2} | | |
| 1510.06699_FO0048 | 3 | 0.585 | { }^{19,20} | | |
| 1510.06699_FO0049 | 3 | 1.000 | b^{a}{ }_{\mu} | | |
| 1510.06699_FO0050 | 3 | 1.000 | h | | |
| 1510.06699_FO0051 | 3 | 1.000 | b^{a}{ }_{0} | | |
| 1510.06699_FO0052 | 3 | 1.000 | A^{a b}{ }_{0} | | |
| 1510.06699_FO0053 | 3 | 1.000 | b^{a}{ }_{\alpha} | | |
| 1510.06699_FO0054 | 3 | 1.000 | A^{a b}{ }_{\alpha}(\alpha=1,2,3) | | |
| 1510.06699_FO0055 | 3 | 1.000 | \mathcal{R}+\mathcal{T}^{2} | | |
| 1510.06699_FO0056 | 3 | 1.000 | L_{\mathrm{G}}=\kappa^{-1}\left(a \mathcal{R}+L_{\mathcal{T}^{2}}\right) | | |
| 1510.06699_FO0057 | 3 | 1.000 | A | | |
| 1510.06699_FO0058 | 3 | 1.000 | L_{\mathcal{R}^{2}} | | |
| 1510.06699_FO0059 | 3 | 1.000 | \mathcal{R}+\mathcal{R}^{2} | | |
| 1510.06699_FO0060 | 3 | 0.970 | \mathcal{R}^{2}+\mathcal{T}^{2} | | |
| 1510.06699_FO0061 | 3 | 0.986 | \mathcal{R}+\mathcal{R}^{2}+\mathcal{T}^{2} | | |
| 1510.06699_FO0062 | 3 | 1.000 | \mathcal{R} | | |
| 1510.06699_FO0063 | 3 | 1.000 | \mathcal{T}^{2} | | |
| 1510.06699_FO0064 | 3 | 1.000 | \mathcal{R}^{2} | | |
| 1510.06699_FO0065 | 3 | 1.000 | { }^{\underline{25}} | | |
| 1510.06699_FO0066 | 3 | 0.881 | { }^{\underline{26}} | | |
| 1510.06699_FO0067 | 3 | 0.995 | a, \alpha_{i} | | |
| 1510.06699_FO0068 | 3 | 0.924 | { }^{\underline{27}} | | |
| 1510.06699_FO0069 | 4 | 1.000 | h_{a}^{\mu} | | |
| 1510.06699_FO0070 | 4 | 1.000 | L_{\mathrm{G}}^{(2)} | | |
| 1510.06699_FO0071 | 4 | 1.000 | k | | |
| 1510.06699_FO0072 | 4 | 1.000 | J^{P} | | |
| 1510.06699_FO0073 | 4 | 1.000 | k^{a} | | |
| 1510.06699_FO0074 | 4 | 0.998 | J^{P}=2^{+} | | |
| 1510.06699_FO0075 | 4 | 1.000 | J^{P}=2^{ \pm}, 1^{ \pm}, 0^{ \pm} | | |
| 1510.06699_FO0076 | 4 | 1.000 | 2(5+3+1)=18 | | |
| 1510.06699_FO0077 | 4 | 1.000 | S | | |
| 1510.06699_FO0078 | 4 | 1.000 | k^{2} | | |
| 1510.06699_FO0079 | 4 | 1.000 | -R /\left(k^{2}-m^{2}\right) | | |
| 1510.06699_FO0080 | 4 | 1.000 | R>0 | | |
| 1510.06699_FO0081 | 4 | 1.000 | m^{2} \geq 0 | | |
| 1510.06699_FO0082 | 4 | 1.000 | { }^{18,33} | | |
| 1510.06699_FO0083 | 4 | 1.000 | J^{P}=1^{-} | | |
| 1510.06699_FO0084 | 4 | 1.000 | \sim 1 / k^{4} | | |
| 1510.06699_FO0085 | 4 | 1.000 | \sim 1 / k^{2} | | |
| 1510.06699_FO0086 | 4 | 1.000 | { }^{29,31,35} | | |
| 1510.06699_FO0087 | 4 | 1.000 | 1 / k^{4} | | |
| 1510.06699_FO0088 | 4 | 1.000 | \left(k^{2}-m_{1}^{2}\right)^{-1}\left(k^{2}-m_{2}^{2}\right)^{-1}= | | |
| 1510.06699_FO0089 | 4 | 1.000 | \left(m_{2}^{2}-m_{1}^{2}\right)^{-1}\left[\left(k^{2}-m_{2}^{2}\right)^{-1}-\left(k^{2}-m_{1}^{2}\right)^{-1}\right] | | |
| 1510.06699_FO0090 | 4 | 1.000 | { }^{6,39} | | |
| 1510.06699_FO0091 | 4 | 0.945 | { }^{40,41} | | |
| 1510.06699_FO0092 | 4 | 0.991 | { }^{\underline{31,43}} | | |
| 1510.06699_FO0093 | 4 | 0.566 | { }^{44-46} | | |
| 1510.06699_FO0094 | 4 | 1.000 | m^{2} \neq 0 | | |
| 1510.06699_FO0095 | 4 | 0.838 | \mathrm{C}(1,3)^{\underline{48}-50} | | |
| 1510.06699_FO0096 | 5 | 1.000 | S_{\mathrm{M}}=\int L_{\mathrm{M}}\left(\varphi, \partial_{\mu} \varphi\right) d^{4} x | | |
| 1510.06699_FO0097 | 5 | 1.000 | B_{\mu} | | |
| 1510.06699_FO0098 | 5 | 0.870 | { }^{51-53} | | |
| 1510.06699_FO0099 | 5 | 1.000 | h_{a}{ }^{\mu}, A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0100 | 5 | 0.991 | \mathcal{D}_{a}^{*} \varphi | | |
| 1510.06699_FO0101 | 5 | 1.000 | S_{\mathrm{M}}=\int h^{-1} L_{\mathrm{M}}\left(\varphi, \mathcal{D}_{a}^{*} \varphi\right) d^{4} x | | |
| 1510.06699_FO0102 | 5 | 1.000 | L_{\mathrm{M}} | | |
| 1510.06699_FO0103 | 5 | 1.000 | h^{-1} | | |
| 1510.06699_FO0104 | 5 | 0.788 | w\left(h^{-1}\right)=4 | | |
| 1510.06699_FO0105 | 5 | 1.000 | w\left(L_{\mathrm{G}}\right)=-4 | | |
| 1510.06699_FO0106 | 5 | 1.000 | \left[\mathcal{D}_{a}^{*}, \mathcal{D}_{b}^{*}\right] \varphi | | |
| 1510.06699_FO0107 | 5 | 1.000 | \mathcal{T}^{* a}{ }_{b c}(h, \partial h, A, B) | | |
| 1510.06699_FO0108 | 5 | 1.000 | \mathcal{H}_{a b}(h, \partial B) | | |
| 1510.06699_FO0109 | 5 | 1.000 | S_{\mathrm{G}}= | | |
| 1510.06699_FO0110 | 5 | 0.999 | \int h^{-1} L_{\mathrm{G}}\left(\mathcal{R}^{a b}{ }_{c d}, \mathcal{T}^{* a}{ }_{b c}, \mathcal{H}_{a b}\right) d^{4} x | | |
| 1510.06699_FO0111 | 5 | 1.000 | \zeta^{\mu} \equiv \delta \mathcal{L}_{\mathrm{M}} / \delta B_{\mu} | | |
| 1510.06699_FO0112 | 5 | 1.000 | w\left(\mathcal{R}^{a b}{ }_{c d}\right)=w\left(\mathcal{H}_{a b}\right)=-2 | | |
| 1510.06699_FO0113 | 5 | 1.000 | w\left(\mathcal{T}^{* a}{ }_{b c}\right)=-1 | | |
| 1510.06699_FO0114 | 5 | 1.000 | \mathcal{H}_{a b} | | |
| 1510.06699_FO0115 | 5 | 1.000 | \mathcal{T}^{* a}{ }_{b c} | | |
| 1510.06699_FO0116 | 5 | 1.000 | \mathcal{R}^{2}+\mathcal{H}^{2} | | |
| 1510.06699_FO0117 | 5 | 1.000 | \xi | | |
| 1510.06699_FO0118 | 5 | 1.000 | \mathcal{T}^{* 2} | | |
| 1510.06699_FO0119 | 5 | 1.000 | w=-4 | | |
| 1510.06699_FO0120 | 5 | 0.999 | \phi | | |
| 1510.06699_FO0121 | 5 | 0.999 | w(\phi)=-1 | | |
| 1510.06699_FO0122 | 5 | 0.785 | (\mathrm{s}){ }^{\underline{10}} | | |
| 1510.06699_FO0123 | 5 | 0.803 | \phi^{2} \mathcal{R} | | |
| 1510.06699_FO0124 | 5 | 0.803 | \phi^{2} L_{\mathcal{T}^{* 2}} | | |
| 1510.06699_FO0125 | 5 | 1.000 | { }^{54,55} | | |
| 1510.06699_FO0126 | 5 | 0.999 | \phi^{2} L_{\mathcal{T} * 2} | | |
| 1510.06699_FO0127 | 5 | 0.969 | { }^{56,57} | | |
| 1510.06699_FO0128 | 5 | 1.000 | \psi | | |
| 1510.06699_FO0129 | 5 | 1.000 | w(\psi)=w(\bar{\psi})=-\frac{3}{2} | | |
| 1510.06699_FO0130 | 5 | 1.000 | m \bar{\psi} \psi | | |
| 1510.06699_FO0131 | 5 | 0.983 | { }^{10} \zeta^{\mu} \equiv \delta \mathcal{L}_{\mathrm{M}} / \delta B_{\mu} | | |
| 1510.06699_FO0132 | 6 | 1.000 | m \bar{\psi} \psi \rightarrow \mu \phi \bar{\psi} \psi | | |
| 1510.06699_FO0133 | 6 | 1.000 | \mu | | |
| 1510.06699_FO0134 | 6 | 1.000 | \mu \phi | | |
| 1510.06699_FO0135 | 6 | 1.000 | G | | |
| 1510.06699_FO0136 | 6 | 1.000 | \phi=\phi_{0} | | |
| 1510.06699_FO0137 | 6 | 1.000 | m=\mu \phi_{0} | | |
| 1510.06699_FO0138 | 6 | 1.000 | w | | |
| 1510.06699_FO0139 | 6 | 1.000 | \mathcal{R}_{a b c d} | | |
| 1510.06699_FO0140 | 6 | 1.000 | \mathcal{T}_{a b c} | | |
| 1510.06699_FO0141 | 6 | 0.617 | { }^{59-62,89} | | |
| 1510.06699_FO0142 | 6 | 1.000 | Y_{4} | | |
| 1510.06699_FO0143 | 7 | 1.000 | \widehat{Y}_{4} | | |
| 1510.06699_FO0144 | 7 | 1.000 | \mathcal{M} | | |
| 1510.06699_FO0145 | 7 | 1.000 | x^{\mu} | | |
| 1510.06699_FO0146 | 7 | 1.000 | \varphi(x) | | |
| 1510.06699_FO0147 | 7 | 0.959 | \boldsymbol{e}_{\mu} | | |
| 1510.06699_FO0148 | 7 | 0.997 | \boldsymbol{e}_{\mu} \cdot \boldsymbol{e}_{\nu}=\eta_{\mu \nu} | | |
| 1510.06699_FO0149 | 7 | 1.000 | \eta_{\mu \nu}=\operatorname{diag}(1,-1,-1,-1) | | |
| 1510.06699_FO0150 | 7 | 1.000 | \hat{\boldsymbol{e}}_{a}(x) | | |
| 1510.06699_FO0151 | 7 | 1.000 | \hat{\boldsymbol{e}}_{a} \cdot \hat{\boldsymbol{e}}_{b}=\eta_{a b} | | |
| 1510.06699_FO0152 | 7 | 1.000 | \boldsymbol{e}_{\mu}(x) | | |
| 1510.06699_FO0153 | 7 | 1.000 | \hat{\boldsymbol{e}}_{a}=\delta_{a}^{\mu} \boldsymbol{e}_{\mu} | | |
| 1510.06699_FO0154 | 7 | 1.000 | \operatorname{SO}(3,1) | | |
| 1510.06699_FO0155 | 7 | 1.000 | \operatorname{SL}(2, C) | | |
| 1510.06699_FO0156 | 7 | 1.000 | \left\{\varphi^{a}(x)\right\} | | |
| 1510.06699_FO0157 | 8 | 0.999 | \mathrm{S}(\Lambda) | | |
| 1510.06699_FO0158 | 8 | 1.000 | \Lambda^{\mu}{ }_{\nu}=\delta_{\nu}^{\mu} | | |
| 1510.06699_FO0159 | 8 | 1.000 | a^{\mu}=0 | | |
| 1510.06699_FO0160 | 8 | 1.000 | e^{\rho} | | |
| 1510.06699_FO0161 | 8 | 0.999 | d s^{2}=\eta_{\mu \nu} d x^{\mu} d x^{\nu} | | |
| 1510.06699_FO0162 | 8 | 1.000 | \eta_{\mu \nu} \rightarrow \gamma_{\mu \nu}=e^{2 \rho} \eta_{\mu \nu} | | |
| 1510.06699_FO0163 | 8 | 1.000 | w=2 | | |
| 1510.06699_FO0164 | 8 | 1.000 | x^{\prime \mu}=e^{\rho} x^{\mu} | | |
| 1510.06699_FO0165 | 8 | 1.000 | \gamma_{\mu \nu}^{\prime}=e^{-2 \rho} \gamma_{\mu \nu}=\eta_{\mu \nu} | | |
| 1510.06699_FO0166 | 8 | 1.000 | e^{4 \rho} | | |
| 1510.06699_FO0167 | 8 | 1.000 | m | | |
| 1510.06699_FO0168 | 8 | 1.000 | m=0 | | |
| 1510.06699_FO0169 | 8 | 1.000 | \bar{\psi} \psi | | |
| 1510.06699_FO0170 | 8 | 1.000 | A_{\mu} | | |
| 1510.06699_FO0171 | 8 | 1.000 | F_{\mu \nu} \equiv \partial_{\mu} A_{\nu}-\partial_{\nu} A_{\mu} | | |
| 1510.06699_FO0172 | 8 | 1.000 | J^{\mu} | | |
| 1510.06699_FO0173 | 8 | 1.000 | w_{J} | | |
| 1510.06699_FO0174 | 8 | 1.000 | J_{\mu} | | |
| 1510.06699_FO0175 | 8 | 1.000 | w\left(A_{\mu}\right)=-1 | | |
| 1510.06699_FO0176 | 8 | 1.000 | w\left(J_{\mu}\right)=-3 | | |
| 1510.06699_FO0177 | 8 | 1.000 | J^{\mu} \equiv \bar{\psi} \gamma^{\mu} \psi | | |
| 1510.06699_FO0178 | 9 | 1.000 | a^{\mu} | | |
| 1510.06699_FO0179 | 9 | 1.000 | \rho | | |
| 1510.06699_FO0180 | 9 | 1.000 | x | | |
| 1510.06699_FO0181 | 9 | 1.000 | x^{\prime} | | |
| 1510.06699_FO0182 | 9 | 1.000 | \Lambda(x) | | |
| 1510.06699_FO0183 | 9 | 0.997 | \rho(x) | | |
| 1510.06699_FO0184 | 9 | 1.000 | \Lambda^{a}{ }_{b}(x) | | |
| 1510.06699_FO0185 | 9 | 1.000 | \partial_{\mu} \varphi | | |
| 1510.06699_FO0186 | 9 | 1.000 | \eta_{a b}=\eta^{a b}=\operatorname{diag}(1,-1,-1,-1) | | |
| 1510.06699_FO0187 | 9 | 1.000 | \gamma_{\mu \nu}=\boldsymbol{e}_{\mu} \cdot \boldsymbol{e}_{\nu} | | |
| 1510.06699_FO0188 | 9 | 1.000 | \gamma^{\mu \nu} | | |
| 1510.06699_FO0189 | 9 | 1.000 | \hat{\boldsymbol{e}}^{a}=\eta^{a b} \hat{\boldsymbol{e}}_{b} | | |
| 1510.06699_FO0190 | 9 | 1.000 | \boldsymbol{e}^{\mu}=\gamma^{\mu \nu} \boldsymbol{e}_{\nu} | | |
| 1510.06699_FO0191 | 9 | 1.000 | \gamma_{\mu \nu} | | |
| 1510.06699_FO0192 | 9 | 1.000 | (\Lambda, \rho) | | |
| 1510.06699_FO0193 | 9 | 1.000 | D_{\mu} \varphi(x) | | |
| 1510.06699_FO0194 | 9 | 1.000 | A^{a b}{ }_{\mu}(x) | | |
| 1510.06699_FO0195 | 9 | 1.000 | B_{\mu}(x) | | |
| 1510.06699_FO0196 | 9 | 1.000 | \Sigma_{a b}=-\Sigma_{a b} | | |
| 1510.06699_FO0197 | 9 | 0.483 | (2, C) | | |
| 1510.06699_FO0198 | 9 | 0.483 | (\Lambda) | | |
| 1510.06699_FO0199 | 9 | 1.000 | \Sigma_{a b} | | |
| 1510.06699_FO0200 | 9 | 1.000 | A^{a b}{ }_{\mu}= | | |
| 1510.06699_FO0201 | 9 | 0.890 | -A^{b a}{ }_{\mu} | | |
| 1510.06699_FO0202 | 9 | 0.890 | B | | |
| 1510.06699_FO0203 | 9 | 1.000 | w=0 | | |
| 1510.06699_FO0204 | 10 | 1.000 | \partial_{\mu}^{*} \varphi(x) | | |
| 1510.06699_FO0205 | 10 | 0.999 | D_{\mu}^{*} \varphi | | |
| 1510.06699_FO0206 | 10 | 1.000 | h_{a}{ }^{\mu}(x) | | |
| 1510.06699_FO0207 | 10 | 1.000 | w=-1 | | |
| 1510.06699_FO0208 | 10 | 1.000 | b^{a}{ }_{\mu}(x) | | |
| 1510.06699_FO0209 | 10 | 1.000 | w=1 | | |
| 1510.06699_FO0210 | 10 | 1.000 | \partial \varphi | | |
| 1510.06699_FO0211 | 10 | 1.000 | x \rightarrow x^{\prime} | | |
| 1510.06699_FO0212 | 10 | 0.997 | L_{\mathrm{M}}\left(\varphi ; \mathcal{D}^{*} \varphi\right) | | |
| 1510.06699_FO0213 | 10 | 1.000 | w=4 | | |
| 1510.06699_FO0214 | 10 | 1.000 | \mathcal{L}_{\mathrm{M}} \equiv h^{-1} L_{\mathrm{M}}\left(\varphi, \mathcal{D}_{a}^{*} \varphi\right) | | |
| 1510.06699_FO0215 | 10 | 0.999 | h, A | | |
| 1510.06699_FO0216 | 10 | 0.613 | L_{\mathcal{T} * 2} | | |
| 1510.06699_FO0217 | 10 | 0.999 | D_{\mu}^{*} | | |
| 1510.06699_FO0218 | 10 | 1.000 | \left(\Sigma_{c d}^{1}\right)^{a}{ }_{b}=\left(\delta_{c}^{a} \eta_{d b}-\delta_{d}^{a} \eta_{c b}\right) | | |
| 1510.06699_FO0219 | 10 | 0.509 | C | | |
| 1510.06699_FO0220 | 11 | 1.000 | { }^{0} \nabla_{\mu}^{*} \equiv{ }^{0} \nabla_{\mu}+w B_{\mu},{ }^{0} \Gamma^{\lambda}{ }_{\mu \nu} \equiv \frac{1}{2} \gamma^{\lambda \rho}\left(\partial_{\mu} \gamma_{\nu \rho}+\partial_{\nu} \gamma_{\mu \rho}-\right. | | |
| 1510.06699_FO0221 | 11 | 0.709 | \partial_{\rho} \gamma_{\mu \nu} | | |
| 1510.06699_FO0222 | 11 | 0.991 | \mathrm{X}^{\rho}{ }_{\sigma} | | |
| 1510.06699_FO0223 | 11 | 0.991 | \operatorname{GL}(4, R) | | |
| 1510.06699_FO0224 | 11 | 1.000 | { }^{0} \Gamma^{\sigma}{ }_{\rho \mu} | | |
| 1510.06699_FO0225 | 11 | 1.000 | { }^{0} \nabla_{\mu} | | |
| 1510.06699_FO0226 | 11 | 1.000 | { }^{0} \nabla_{\nu} | | |
| 1510.06699_FO0227 | 11 | 1.000 | \boldsymbol{h} | | |
| 1510.06699_FO0228 | 11 | 1.000 | h_{a}{ }^{\mu} \equiv \boldsymbol{h}\left(\hat{\boldsymbol{e}}_{a}, \boldsymbol{e}^{\mu}\right) | | |
| 1510.06699_FO0229 | 11 | 1.000 | \boldsymbol{b} | | |
| 1510.06699_FO0230 | 11 | 1.000 | b^{a}{ }_{\mu} \equiv \boldsymbol{b}\left(\hat{\boldsymbol{e}}^{a}, \boldsymbol{e}_{\mu}\right) | | |
| 1510.06699_FO0231 | 11 | 1.000 | \boldsymbol{J} | | |
| 1510.06699_FO0232 | 11 | 1.000 | \boldsymbol{J}=J^{\mu} \boldsymbol{e}_{\mu}=J_{\mu} \boldsymbol{e}^{\mu} | | |
| 1510.06699_FO0233 | 11 | 1.000 | \mathcal{J}_{a} \equiv h_{a}{ }^{\mu} J_{\mu}=h_{a \mu} J^{\mu} | | |
| 1510.06699_FO0234 | 11 | 1.000 | \mathcal{J}^{a} \equiv h^{a}{ }_{\mu} J^{\mu}=h^{a \mu} J_{\mu} | | |
| 1510.06699_FO0235 | 11 | 0.967 | \mathcal{J}=\boldsymbol{h}(\cdot, \boldsymbol{J})^{67} | | |
| 1510.06699_FO0236 | 11 | 0.820 | \boldsymbol{h}(\mathcal{J}, \cdot) | | |
| 1510.06699_FO0237 | 11 | 1.000 | h_{a}{ }^{\mu} \mathcal{J}^{a} | | |
| 1510.06699_FO0238 | 11 | 1.000 | \mathcal{J} | | |
| 1510.06699_FO0239 | 11 | 0.690 | \boldsymbol{J}=\boldsymbol{b}(\boldsymbol{\mathcal { J }}, \cdot) | | |
| 1510.06699_FO0240 | 11 | 1.000 | b^{a}{ }_{\mu} \mathcal{J}_{a}=J_{\mu} | | |
| 1510.06699_FO0241 | 11 | 1.000 | J_{\mu}=b_{a \mu} \mathcal{J}^{a} | | |
| 1510.06699_FO0242 | 11 | 1.000 | J^{\mu}=b_{a}{ }^{\mu} \mathcal{J}^{a}=b^{a \mu} \mathcal{J}_{a} | | |
| 1510.06699_FO0243 | 11 | 1.000 | \boldsymbol{b}(\cdot, \boldsymbol{J}) | | |
| 1510.06699_FO0244 | 11 | 1.000 | b^{a}{ }_{\mu} J^{\mu} | | |
| 1510.06699_FO0245 | 11 | 1.000 | \mathcal{J}^{a} | | |
| 1510.06699_FO0246 | 11 | 0.999 | \boldsymbol{T} | | |
| 1510.06699_FO0247 | 11 | 0.968 | \mathcal{T} | | |
| 1510.06699_FO0248 | 11 | 1.000 | \mathcal{T}_{a b}= | | |
| 1510.06699_FO0249 | 11 | 1.000 | h_{a}{ }^{\mu} h_{b}{ }^{\nu} T_{\mu \nu} | | |
| 1510.06699_FO0250 | 11 | 1.000 | T_{\mu \nu}=b^{a}{ }_{\mu} b^{b}{ }_{\nu} \mathcal{T}_{a b} | | |
| 1510.06699_FO0251 | 11 | 0.999 | \hat{\boldsymbol{e}}_{a} | | |
| 1510.06699_FO0252 | 11 | 0.999 | h_{a}{ }^{\mu} J_{\mu} | | |
| 1510.06699_FO0253 | 11 | 1.000 | J_{a} | | |
| 1510.06699_FO0254 | 12 | 1.000 | R^{a b}{ }_{\mu \nu} | | |
| 1510.06699_FO0255 | 12 | 1.000 | H_{\mu \nu} | | |
| 1510.06699_FO0256 | 12 | 1.000 | \mathcal{D}_{a}^{*} \varphi= | | |
| 1510.06699_FO0257 | 12 | 1.000 | h_{a}{ }^{\mu} D_{\mu}^{*} \varphi | | |
| 1510.06699_FO0258 | 12 | 1.000 | \mathcal{R}^{a b}{ }_{c d} \equiv h_{a}{ }^{\mu} h_{b}{ }^{\nu} R^{a b}{ }_{\mu \nu} | | |
| 1510.06699_FO0259 | 12 | 1.000 | \mathcal{H}_{c d}=h_{c}{ }^{\mu} h_{d}{ }^{\nu} H_{\mu \nu} | | |
| 1510.06699_FO0260 | 12 | 0.669 | \mathcal{B}_{a}=h_{a}{ }^{\mu} B_{\mu} | | |
| 1510.06699_FO0261 | 12 | 0.669 | \mathcal{T}_{b}^{*} \equiv | | |
| 1510.06699_FO0262 | 12 | 1.000 | \mathcal{T}^{* a}{ }_{b a}=\mathcal{T}_{b}+3 \mathcal{B}_{b} | | |
| 1510.06699_FO0263 | 12 | 1.000 | \mathcal{T}_{b} | | |
| 1510.06699_FO0264 | 12 | 1.000 | \mathcal{R}^{a b}{ }_{c d}, \mathcal{H}_{c d} | | |
| 1510.06699_FO0265 | 12 | 1.000 | \mathcal{T}^{* a}{ }_{c d} | | |
| 1510.06699_FO0266 | 12 | 1.000 | w\left(\mathcal{R}^{a b}{ }_{c d}\right)=w\left(\mathcal{H}_{c d}\right)=-2 | | |
| 1510.06699_FO0267 | 12 | 1.000 | w\left(\mathcal{T}^{* a}{ }_{c d}\right)=-1 | | |
| 1510.06699_FO0268 | 12 | 1.000 | \mathcal{R}^{a b}{ }_{c d}, \mathcal{H}_{a b} | | |
| 1510.06699_FO0269 | 12 | 1.000 | A_{a b \mu}= | | |
| 1510.06699_FO0270 | 12 | 1.000 | b^{c}{ }_{\mu} \mathcal{A}_{a b c} | | |
| 1510.06699_FO0271 | 12 | 1.000 | \mathcal{T}_{a b c}^{*} | | |
| 1510.06699_FO0272 | 12 | 1.000 | \mathcal{A}_{a b c} | | |
| 1510.06699_FO0273 | 12 | 1.000 | { }^{0} \mathcal{A}_{a b c}^{*} \equiv \frac{1}{2}\left(c_{a b c}^{*}+\right. | | |
| 1510.06699_FO0274 | 12 | 0.506 | \left.c_{b c a}^{*}-c_{c a b}^{*}\right) | | |
| 1510.06699_FO0275 | 12 | 1.000 | \mathcal{K}_{a b c}^{*} \equiv-\frac{1}{2}\left(\mathcal{T}_{a b c}^{*}+\mathcal{T}_{b c a}^{*}-\mathcal{T}_{c a b}^{*}\right) | | |
| 1510.06699_FO0276 | 12 | 0.982 | { }^{0} \mathcal{A}_{a b c}^{*} | | |
| 1510.06699_FO0277 | 12 | 0.982 | \mathcal{K}_{a b c}^{*} | | |
| 1510.06699_FO0278 | 12 | 0.991 | \mathcal{A}_{a b c}^{*} | | |
| 1510.06699_FO0279 | 12 | 0.961 | { }^{0} \mathcal{D}_{a}^{*} \equiv h_{a}{ }^{\mu}{ }^{0} D_{\mu}^{*} | | |
| 1510.06699_FO0280 | 12 | 1.000 | \mathcal{D}_{a}^{*} | | |
| 1510.06699_FO0281 | 12 | 1.000 | { }^{0} \mathcal{D}_{a}^{*} | | |
| 1510.06699_FO0282 | 12 | 1.000 | \mathcal{R}^{a b}{ }_{c d}, \mathcal{T}^{* a}{ }_{b c} | | |
| 1510.06699_FO0283 | 13 | 0.947 | \mathcal{T}_{a b c}^{*}= | | |
| 1510.06699_FO0284 | 13 | 0.990 | \epsilon_{a b c d} t^{d} | | |
| 1510.06699_FO0285 | 13 | 0.990 | t^{d} | | |
| 1510.06699_FO0286 | 13 | 0.999 | d | | |
| 1510.06699_FO0287 | 13 | 1.000 | b | | |
| 1510.06699_FO0288 | 13 | 1.000 | e | | |
| 1510.06699_FO0289 | 13 | 0.770 | \mathcal{T}_{a}^{*} | | |
| 1510.06699_FO0290 | 13 | 1.000 | \mathcal{H} | | |
| 1510.06699_FO0291 | 13 | 1.000 | \mathcal{R}_{a b c d}, \mathcal{T}_{a b c}^{*} | | |
| 1510.06699_FO0292 | 13 | 1.000 | \mathcal{L}_{\mathrm{G}} \equiv h^{-1} L_{\mathrm{G}} | | |
| 1510.06699_FO0293 | 13 | 1.000 | \mathcal{R}_{a b c d}, \mathcal{H}_{a b} | | |
| 1510.06699_FO0294 | 13 | 1.000 | w\left(\mathcal{R}_{a b c d}\right)=w\left(\mathcal{H}_{a b}\right)=-2 | | |
| 1510.06699_FO0295 | 13 | 1.000 | w\left(\mathcal{T}_{a b c}^{*}\right)=-1 | | |
| 1510.06699_FO0296 | 13 | 0.988 | { }^{\underline{70}} | | |
| 1510.06699_FO0297 | 13 | 0.994 | L_{\mathcal{H}^{2}} | | |
| 1510.06699_FO0298 | 13 | 1.000 | D \leq 4 | | |
| 1510.06699_FO0299 | 13 | 0.994 | \mathcal{T}_{a b c} \rightarrow \mathcal{T}_{a b c}^{*} | | |
| 1510.06699_FO0300 | 13 | 1.000 | \mathcal{L}_{\mathrm{G}} | | |
| 1510.06699_FO0301 | 13 | 1.000 | L_{\mathrm{G}}=L_{\mathcal{H}^{2}} | | |
| 1510.06699_FO0302 | 13 | 1.000 | S_{\mathrm{T}} | | |
| 1510.06699_FO0303 | 13 | 1.000 | h, A, \partial A | | |
| 1510.06699_FO0304 | 13 | 1.000 | \partial B | | |
| 1510.06699_FO0305 | 13 | 1.000 | \varphi, \partial \varphi, h, A | | |
| 1510.06699_FO0306 | 13 | 1.000 | \partial A | | |
| 1510.06699_FO0307 | 13 | 0.901 | \phi^{2} L_{\mathcal{\mathcal { T } _ { * 2 }}} | | |
| 1510.06699_FO0308 | 13 | 1.000 | \partial h | | |
| 1510.06699_FO0309 | 14 | 1.000 | \mathcal{L}_{\mathrm{T}} | | |
| 1510.06699_FO0310 | 14 | 1.000 | \mathcal{R}_{a b c d}(h, A, \partial A), \mathcal{T}_{a b c}^{*}(h, \partial h, A, B) | | |
| 1510.06699_FO0311 | 14 | 1.000 | t^{a}{ }_{\mu} \equiv | | |
| 1510.06699_FO0312 | 14 | 0.999 | \delta \mathcal{L}_{\mathrm{G}} / \delta h_{a}{ }^{\mu}=\partial \mathcal{L}_{\mathrm{G}} / \partial h_{a}{ }^{\mu}, s_{a b}{ }^{\mu} \equiv \delta \mathcal{L}_{\mathrm{G}} / \delta A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0313 | 14 | 1.000 | j^{\mu} \equiv \delta \mathcal{L}_{\mathrm{G}} / \delta B_{\mu} | | |
| 1510.06699_FO0314 | 14 | 1.000 | \tau^{a}{ }_{\mu} \equiv \delta \mathcal{L}_{\mathrm{M}} / \delta h_{a}{ }^{\mu} | | |
| 1510.06699_FO0315 | 14 | 0.692 | \zeta^{\mu} \equiv \delta \mathcal{L}_{\mathrm{M}} / \delta B_{\mu}=\partial \mathcal{L}_{\mathrm{M}} / \partial B_{\mu} | | |
| 1510.06699_FO0316 | 14 | 0.692 | { }^{\underline{72}} | | |
| 1510.06699_FO0317 | 14 | 1.000 | w=1, w=0 | | |
| 1510.06699_FO0318 | 14 | 1.000 | t^{a}{ }_{b} \equiv t^{a}{ }_{\mu} h_{b}{ }^{\mu}, s_{a b}{ }^{c} \equiv s_{a b}{ }^{\mu} b^{c}{ }_{\mu} | | |
| 1510.06699_FO0319 | 14 | 1.000 | j^{a} \equiv j^{\mu} b^{a}{ }_{\mu} | | |
| 1510.06699_FO0320 | 14 | 0.992 | \bar{\partial} \mathcal{L}_{\mathrm{M}} / \partial \varphi \equiv\left[\partial \mathcal{L}_{\mathrm{M}}\left(\varphi, \mathcal{D}_{\mu}^{*} u, \ldots\right) / \partial \varphi\right]_{u=\varphi} | | |
| 1510.06699_FO0321 | 14 | 1.000 | \mathcal{D}_{\mu}^{*} \varphi | | |
| 1510.06699_FO0322 | 14 | 1.000 | \mathcal{L}_{\mathrm{M}}=h^{-1} L_{\mathrm{M}} | | |
| 1510.06699_FO0323 | 14 | 1.000 | \bar{\partial} L_{\mathrm{M}} / \partial \varphi \equiv | | |
| 1510.06699_FO0324 | 14 | 0.974 | \left[\partial L_{\mathrm{M}}\left(\varphi, \mathcal{D}_{a}^{*} u, \ldots\right) / \partial \varphi\right]_{u=\varphi} | | |
| 1510.06699_FO0325 | 14 | 1.000 | S_{\mathrm{M}} | | |
| 1510.06699_FO0326 | 14 | 0.999 | { }^{9,74} | | |
| 1510.06699_FO0327 | 14 | 0.963 | 2, C | | |
| 1510.06699_FO0329 | 15 | 1.000 | w=-\frac{3}{2} | | |
| 1510.06699_FO0330 | 15 | 1.000 | \psi \rightarrow \psi e^{i \alpha} | | |
| 1510.06699_FO0331 | 15 | 1.000 | \gamma | | |
| 1510.06699_FO0332 | 15 | 1.000 | \bar{\psi} | | |
| 1510.06699_FO0333 | 15 | 1.000 | \mathcal{D}_{a} | | |
| 1510.06699_FO0334 | 15 | 1.000 | \mathcal{D}_{a}^{*} \psi | | |
| 1510.06699_FO0335 | 15 | 1.000 | w=-\frac{5}{2} | | |
| 1510.06699_FO0336 | 15 | 1.000 | \mathcal{D}_{a} \psi=\mathcal{D}_{a}^{*} \psi+\frac{3}{2} \mathcal{B}_{a} \psi | | |
| 1510.06699_FO0337 | 15 | 1.000 | \mathcal{T}_{a}= | | |
| 1510.06699_FO0338 | 15 | 1.000 | \mathcal{T}_{a}^{*}-3 \mathcal{B}_{a} | | |
| 1510.06699_FO0339 | 16 | 1.000 | \mathcal{T}_{a} | | |
| 1510.06699_FO0340 | 16 | 1.000 | \Sigma_{a b}=\frac{1}{4}\left[\gamma_{a}, \gamma_{b}\right] | | |
| 1510.06699_FO0341 | 16 | 0.945 | \mathcal{T}_{[a b c]}^{*}=0 | | |
| 1510.06699_FO0342 | 16 | 1.000 | \tau=h^{-1} \mu \phi \bar{\psi} \psi | | |
| 1510.06699_FO0343 | 16 | 1.000 | \sigma_{a b c}=\sigma_{[a b c]} | | |
| 1510.06699_FO0344 | 16 | 1.000 | \mathcal{D}_{a} \rightarrow \mathcal{D}_{a}^{*} | | |
| 1510.06699_FO0345 | 16 | 1.000 | \mu, \nu, \lambda | | |
| 1510.06699_FO0346 | 16 | 0.669 | \beta_{1}, \beta_{2} | | |
| 1510.06699_FO0347 | 16 | 0.669 | \beta_{3} | | |
| 1510.06699_FO0348 | 16 | 1.000 | F_{\mu \nu} \equiv | | |
| 1510.06699_FO0349 | 16 | 1.000 | \partial_{\mu} A_{\nu}-\partial_{\nu} A_{\mu} | | |
| 1510.06699_FO0350 | 16 | 1.000 | A_{\mu} \rightarrow A_{\mu}+\partial_{\mu} \chi | | |
| 1510.06699_FO0351 | 16 | 1.000 | \chi | | |
| 1510.06699_FO0352 | 16 | 1.000 | \partial_{\mu} J^{\mu}=0 | | |
| 1510.06699_FO0353 | 16 | 1.000 | \mathcal{A}_{a}=h_{a}{ }^{\mu} A_{\mu} | | |
| 1510.06699_FO0354 | 16 | 1.000 | \mathcal{J}_{a}=h_{a}{ }^{\mu} J_{\mu} | | |
| 1510.06699_FO0355 | 16 | 1.000 | w\left(\mathcal{A}_{a}\right)=-1 | | |
| 1510.06699_FO0356 | 16 | 1.000 | w\left(\mathcal{J}_{a}\right)=-3 | | |
| 1510.06699_FO0357 | 16 | 1.000 | w\left(A_{\mu}\right)=0 | | |
| 1510.06699_FO0358 | 16 | 1.000 | w\left(J_{\mu}\right)=-2 | | |
| 1510.06699_FO0359 | 16 | 1.000 | \widehat{\mathcal{F}}_{a b}^{*} \equiv \mathcal{D}_{a}^{*} \mathcal{A}_{b}-\mathcal{D}_{b}^{*} \mathcal{A}_{a} | | |
| 1510.06699_FO0360 | 16 | 1.000 | w\left(\widehat{\mathcal{F}}_{a b}^{*}\right)=-2, \mathcal{L}_{\mathrm{M}} | | |
| 1510.06699_FO0361 | 17 | 1.000 | \mathcal{F}_{a b} \equiv h_{a}{ }^{\mu} h_{b}{ }^{\nu} F_{\mu \nu} | | |
| 1510.06699_FO0362 | 17 | 1.000 | F_{\mu \nu} \equiv D_{\mu}^{*} A_{\nu}-D_{\nu}^{*} A_{\mu}=\partial_{\mu} A_{\nu}-\partial_{\nu} A_{\mu} | | |
| 1510.06699_FO0363 | 17 | 1.000 | \mathcal{T}^{* c}{ }_{a b} | | |
| 1510.06699_FO0364 | 17 | 1.000 | \mathcal{F}_{a b} | | |
| 1510.06699_FO0365 | 17 | 1.000 | F_{\mu \nu} | | |
| 1510.06699_FO0366 | 17 | 1.000 | \widehat{\mathcal{F}}_{a b}^{*} | | |
| 1510.06699_FO0367 | 17 | 1.000 | w\left(\mathcal{F}_{a b}\right)=-2 | | |
| 1510.06699_FO0368 | 17 | 1.000 | \mathcal{L}_{\mathrm{M}} | | |
| 1510.06699_FO0369 | 17 | 0.999 | \delta \mathcal{L}_{\mathrm{EM}} / \delta A_{\mu}=0 | | |
| 1510.06699_FO0370 | 17 | 0.997 | \delta \mathcal{L}_{\mathrm{EM}} / \delta \mathcal{A}_{a}=0 | | |
| 1510.06699_FO0371 | 17 | 1.000 | \mathcal{D}_{a} \mathcal{F}^{a c}=\left(\mathcal{D}_{a}^{*}+\right. | | |
| 1510.06699_FO0372 | 17 | 1.000 | \left.2 \mathcal{B}_{a}\right) \mathcal{F}^{a c} | | |
| 1510.06699_FO0373 | 17 | 1.000 | \mathcal{T}_{a}=\mathcal{T}^{*}{ }_{a}-3 \mathcal{B}_{a} | | |
| 1510.06699_FO0374 | 17 | 1.000 | \mathcal{J}^{a}=0 | | |
| 1510.06699_FO0375 | 17 | 1.000 | \sigma_{a b}{ }^{c}=0 | | |
| 1510.06699_FO0376 | 17 | 1.000 | \tau^{a}{ }_{b} | | |
| 1510.06699_FO0377 | 17 | 1.000 | \tau_{a b} | | |
| 1510.06699_FO0378 | 17 | 1.000 | \mathcal{J}^{a}=q \bar{\psi} \gamma^{a} \psi | | |
| 1510.06699_FO0379 | 17 | 1.000 | w\left(\mathcal{J}^{a}\right)=-3 | | |
| 1510.06699_FO0380 | 17 | 1.000 | \phi \neq 0 | | |
| 1510.06699_FO0381 | 17 | 1.000 | \phi(x)=1 | | |
| 1510.06699_FO0382 | 17 | 1.000 | \phi(x)=\phi_{0} | | |
| 1510.06699_FO0383 | 17 | 1.000 | \phi_{0} | | |
| 1510.06699_FO0385 | 18 | 1.000 | \widehat{\mathcal{A}}^{a b}{ }_{c} \equiv \widehat{h}_{a}{ }^{\mu} \widehat{A}^{a b}{ }_{\mu} | | |
| 1510.06699_FO0386 | 18 | 1.000 | \widehat{\mathcal{B}}_{a} \equiv \widehat{h}_{a}{ }^{\mu} \widehat{B}_{\mu} | | |
| 1510.06699_FO0387 | 18 | 1.000 | \mathcal{D}_{a}^{*} \phi=-\left(\phi^{2} / \phi_{0}\right) \widehat{\mathcal{B}}_{a} | | |
| 1510.06699_FO0388 | 18 | 1.000 | \widehat{\chi}=\left(\phi / \phi_{0}\right)^{-w} \chi | | |
| 1510.06699_FO0389 | 18 | 0.996 | \widehat{\mathcal{D}}_{a} \equiv \widehat{h}_{a}{ }^{\mu} D_{\mu} | | |
| 1510.06699_FO0390 | 18 | 0.996 | \widehat{\mathcal{D}}_{a}^{*}=\widehat{\mathcal{D}}_{a}+w \widehat{\mathcal{B}}_{a} | | |
| 1510.06699_FO0391 | 18 | 1.000 | \left(\phi / \phi_{0}\right)^{1-w} | | |
| 1510.06699_FO0392 | 18 | 1.000 | \widehat{\mathcal{D}}_{a}^{*} \widehat{\chi} | | |
| 1510.06699_FO0393 | 18 | 1.000 | \widehat{\chi} | | |
| 1510.06699_FO0394 | 18 | 0.999 | \widehat{h}_{a}{ }^{\mu}, \widehat{A}^{a b}{ }_{\mu} | | |
| 1510.06699_FO0395 | 18 | 0.999 | \widehat{B}_{\mu} | | |
| 1510.06699_FO0396 | 18 | 0.999 | \mathcal{D}_{a}^{*} \chi | | |
| 1510.06699_FO0397 | 18 | 0.999 | \chi, h_{a}{ }^{\mu} | | |
| 1510.06699_FO0398 | 18 | 1.000 | \mathcal{R}^{a b}{ }_{c d}=\left(\phi / \phi_{0}\right)^{2} \widehat{\mathcal{R}}^{a b}{ }_{c d}, \mathcal{T}^{* a}{ }_{b c}=\left(\phi / \phi_{0}\right) \widehat{\mathcal{T}}^{* a}{ }_{b c} | | |
| 1510.06699_FO0399 | 18 | 1.000 | \mathcal{H}_{a b}=\left(\phi / \phi_{0}\right)^{2} \widehat{\mathcal{H}}_{a b} | | |
| 1510.06699_FO0400 | 18 | 1.000 | h^{-1}=\left(\phi / \phi_{0}\right)^{-4} \widehat{h}^{-1} | | |
| 1510.06699_FO0401 | 18 | 1.000 | \varphi, h_{a}{ }^{\mu}, A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0402 | 18 | 1.000 | \delta \mathcal{L}_{\mathrm{T}} / \delta \widehat{\chi}=0 | | |
| 1510.06699_FO0403 | 18 | 1.000 | \delta \mathcal{L}_{\mathrm{T}} /\left.\delta \chi\right|_{\phi=\phi_{0}}=0 | | |
| 1510.06699_FO0404 | 18 | 1.000 | \delta \mathcal{L}_{\mathrm{T}} / \delta \phi=\delta \mathcal{L}_{\mathrm{M}} / \delta \phi | | |
| 1510.06699_FO0405 | 18 | 1.000 | \delta \mathcal{L}_{\mathrm{T}} / \delta \varphi=\delta \mathcal{L}_{\mathrm{M}} / \delta \varphi=0 | | |
| 1510.06699_FO0406 | 18 | 1.000 | \partial \mathcal{L}_{\mathrm{M}} / \partial \widehat{B}_{\mu} | | |
| 1510.06699_FO0407 | 18 | 1.000 | \delta \mathcal{L}_{\mathrm{M}} / \delta \widehat{B}_{\mu} | | |
| 1510.06699_FO0408 | 19 | 1.000 | m \rightarrow \mu \phi | | |
| 1510.06699_FO0409 | 19 | 1.000 | \frac{1}{2} | | |
| 1510.06699_FO0410 | 19 | 1.000 | p_{\mu} \rightarrow p_{a} \equiv h_{a}{ }^{\mu} p_{\mu} | | |
| 1510.06699_FO0411 | 19 | 1.000 | \dot{x}^{\mu} \rightarrow v^{a} \equiv b^{a}{ }_{\mu} \dot{x}^{\mu} | | |
| 1510.06699_FO0412 | 19 | 1.000 | p^{a}(\lambda) | | |
| 1510.06699_FO0413 | 19 | 1.000 | v^{a}(\lambda) | | |
| 1510.06699_FO0414 | 19 | 1.000 | e(\lambda) | | |
| 1510.06699_FO0415 | 19 | 1.000 | \lambda | | |
| 1510.06699_FO0416 | 19 | 1.000 | w\left(p^{a}\right)=-1, w\left(v^{a}\right)=0, w(e)=1, w(\lambda)=1 | | |
| 1510.06699_FO0417 | 19 | 1.000 | p^{2} \equiv p_{a} p^{a} | | |
| 1510.06699_FO0418 | 19 | 1.000 | c^{c}{ }_{a b} | | |
| 1510.06699_FO0419 | 19 | 1.000 | { }^{0} \mathcal{D}_{c}^{*} | | |
| 1510.06699_FO0420 | 19 | 1.000 | e=1 /(\mu \phi) | | |
| 1510.06699_FO0421 | 19 | 1.000 | v^{2}=1 | | |
| 1510.06699_FO0422 | 19 | 1.000 | \tau | | |
| 1510.06699_FO0423 | 19 | 0.348 | { }^{\mathbf{7 6 - 7 8}} | | |
| 1510.06699_FO0424 | 19 | 0.996 | { }^{0} A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0425 | 19 | 0.996 | { }^{0} \mathcal{D}_{b} | | |
| 1510.06699_FO0426 | 19 | 0.906 | v^{b} \mathcal{D}_{b} v_{a}=0 | | |
| 1510.06699_FO0427 | 19 | 1.000 | { }^{79,80} | | |
| 1510.06699_FO0428 | 19 | 1.000 | \left(q_{\mathrm{W}} / m\right) \mathcal{H}_{a b} v^{b} | | |
| 1510.06699_FO0429 | 19 | 1.000 | q_{\mathrm{W}} | | |
| 1510.06699_FO0430 | 19 | 1.000 | \mu=0 | | |
| 1510.06699_FO0431 | 19 | 1.000 | e=1 | | |
| 1510.06699_FO0432 | 19 | 1.000 | v^{2}=0 | | |
| 1510.06699_FO0433 | 20 | 1.000 | \widehat{p}_{a}, \widehat{v}^{a} | | |
| 1510.06699_FO0434 | 20 | 1.000 | \widehat{e} | | |
| 1510.06699_FO0435 | 20 | 0.990 | \widehat{\lambda} | | |
| 1510.06699_FO0436 | 20 | 0.990 | \widehat{p}_{a}(\widehat{\lambda}) \equiv \widehat{h}_{a}{ }^{\mu} p_{\mu}(\lambda(\widehat{\lambda})) | | |
| 1510.06699_FO0437 | 20 | 1.000 | \widehat{\epsilon}=\left[1-\widehat{\lambda}\left(d x^{\mu} / d \widehat{\lambda}\right) \partial_{\mu} \ln \left(\phi / \phi_{0}\right)\right] \widehat{e} | | |
| 1510.06699_FO0438 | 20 | 1.000 | \widehat{\lambda}, \widehat{p}_{a}, \widehat{v}^{a} | | |
| 1510.06699_FO0439 | 20 | 1.000 | \widehat{\epsilon} | | |
| 1510.06699_FO0440 | 20 | 1.000 | \lambda, p_{a}, v^{a} | | |
| 1510.06699_FO0441 | 20 | 0.999 | \widehat{h}_{a}{ }^{\mu} | | |
| 1510.06699_FO0442 | 20 | 0.999 | \widehat{b}^{a}{ }_{\mu} | | |
| 1510.06699_FO0443 | 20 | 1.000 | { }^{0} \widehat{\mathcal{D}}_{a} \equiv | | |
| 1510.06699_FO0444 | 20 | 0.977 | \widehat{h}_{a}{ }^{\mu 0} \mathcal{D}_{\mu} | | |
| 1510.06699_FO0445 | 20 | 1.000 | { }^{0} D_{\mu}^{*} | | |
| 1510.06699_FO0446 | 20 | 0.837 | \mathcal{T}_{a b c}^{*} \equiv 0 | | |
| 1510.06699_FO0447 | 20 | 1.000 | { }^{0} R^{* a b}{ }_{\mu \nu}\left(h, \partial h, \partial^{2} h, B, \partial B\right) | | |
| 1510.06699_FO0448 | 20 | 1.000 | { }^{0} A^{* a b}{ }_{\mu} | | |
| 1510.06699_FO0449 | 20 | 0.998 | { }^{0} \mathcal{R}^{* a b}{ }_{c d}=h_{c}{ }^{\mu} h_{d}{ }^{\mu}{ }^{0} R^{* a b}{ }_{\mu \nu} | | |
| 1510.06699_FO0450 | 20 | 1.000 | { }^{0} \mathcal{T}^{* a}{ }_{b c} \equiv | | |
| 1510.06699_FO0451 | 20 | 1.000 | h_{b}{ }^{\mu} h_{c}{ }^{\nu}\left({ }^{0} D_{\mu}^{*} b^{a}{ }_{\nu}-{ }^{0} D_{\nu}^{*} b^{a}{ }_{\mu}\right)=0 | | |
| 1510.06699_FO0452 | 20 | 0.913 | \mathcal{D}_{a}^{*} \rightarrow^{0} \mathcal{D}_{a}^{*}, \mathcal{R}_{a b c d} \rightarrow{ }^{0} \mathcal{R}_{a b c d}^{*} | | |
| 1510.06699_FO0453 | 20 | 0.982 | \mathcal{T}_{a b c}^{*} \rightarrow{ }^{0} \mathcal{T}_{a b c}^{*} \equiv 0 | | |
| 1510.06699_FO0454 | 20 | 1.000 | { }^{0} \mathcal{R}^{* a b}{ }_{c d} | | |
| 1510.06699_FO0455 | 20 | 1.000 | \mathcal{L}_{\mathrm{G}}=h^{-1} L_{\mathrm{G}} | | |
| 1510.06699_FO0456 | 21 | 0.516 | { }^{0} \mathcal{R}_{\text {abcd }}^{*} | | |
| 1510.06699_FO0457 | 21 | 0.999 | \mathcal{R}_{a b c d} \rightarrow{ }^{0} \mathcal{R}_{a b c d}^{*} | | |
| 1510.06699_FO0458 | 21 | 0.996 | \mathcal{D}_{a}^{*} \rightarrow{ }^{0} \mathcal{D}_{a}^{*} | | |
| 1510.06699_FO0459 | 21 | 0.996 | \mathcal{T}_{a}^{*} \rightarrow{ }^{0} \mathcal{T}_{a}^{*} \equiv 0 | | |
| 1510.06699_FO0460 | 21 | 0.756 | \mathcal{D}_{a}^{*} \rightarrow^{0} \mathcal{D}_{a}^{*}, \mathcal{T}_{a b c}^{*} \rightarrow{ }^{0} \mathcal{T}_{a b c}^{*} \equiv 0 | | |
| 1510.06699_FO0461 | 21 | 1.000 | s_{a b c} \equiv 0 \equiv \sigma_{a b c} | | |
| 1510.06699_FO0462 | 21 | 0.975 | \mathcal{T}_{a b c}^{*}=0 | | |
| 1510.06699_FO0463 | 21 | 1.000 | { }^{82-84} | | |
| 1510.06699_FO0464 | 21 | 1.000 | D=4 | | |
| 1510.06699_FO0465 | 21 | 0.741 | { }^{\underline{85}} | | |
| 1510.06699_FO0466 | 21 | 0.968 | \hat{\boldsymbol{e}}^{a}(x) | | |
| 1510.06699_FO0467 | 21 | 0.968 | \boldsymbol{e}^{\mu}(x) | | |
| 1510.06699_FO0468 | 21 | 0.769 | J_{\mu} \boldsymbol{e}^{\mu} | | |
| 1510.06699_FO0469 | 21 | 1.000 | J_{a}=h_{a}{ }^{\mu} J_{\mu} | | |
| 1510.06699_FO0470 | 21 | 1.000 | h_{a}{ }^{\mu} J^{a}=J^{\mu} | | |
| 1510.06699_FO0471 | 21 | 1.000 | b^{a}{ }_{\mu} J^{\mu}=J^{a} | | |
| 1510.06699_FO0472 | 21 | 1.000 | g_{\mu \nu} | | |
| 1510.06699_FO0473 | 21 | 1.000 | h^{-1}=\sqrt{-g} | | |
| 1510.06699_FO0474 | 22 | 1.000 | w\left(g_{\mu \nu}\right)=2 | | |
| 1510.06699_FO0475 | 22 | 1.000 | w\left(h_{a}{ }^{\mu}\right)=-1 | | |
| 1510.06699_FO0476 | 22 | 1.000 | w\left(\eta_{a b}\right)=0 | | |
| 1510.06699_FO0477 | 22 | 1.000 | e_{a}{ }^{\mu} | | |
| 1510.06699_FO0478 | 22 | 1.000 | e^{a}{ }_{\mu} | | |
| 1510.06699_FO0479 | 22 | 1.000 | x+\delta x | | |
| 1510.06699_FO0480 | 22 | 1.000 | J^{a} | | |
| 1510.06699_FO0481 | 22 | 1.000 | J^{a}(x) | | |
| 1510.06699_FO0482 | 22 | 1.000 | J^{a}(x+\delta x) | | |
| 1510.06699_FO0483 | 22 | 1.000 | \hat{\boldsymbol{e}}_{a}(x+\delta x) | | |
| 1510.06699_FO0484 | 22 | 1.000 | \partial_{\mu}^{*} | | |
| 1510.06699_FO0485 | 22 | 1.000 | \eta_{a b} | | |
| 1510.06699_FO0486 | 22 | 1.000 | A^{a b}{ }_{\mu}=-A^{b a}{ }_{\mu} | | |
| 1510.06699_FO0487 | 22 | 0.528 | \nabla_{\mu}^{*}=\partial_{\mu}^{*}+\Gamma^{\sigma}{ }_{\rho \mu} \mathrm{X}^{\rho}{ }_{\sigma} | | |
| 1510.06699_FO0488 | 22 | 1.000 | \Delta_{\mu}^{*} | | |
| 1510.06699_FO0489 | 22 | 1.000 | \nabla_{\mu}^{*} \psi=\partial_{\mu}^{*} \psi | | |
| 1510.06699_FO0490 | 22 | 1.000 | \Delta_{\mu}^{*} \psi=D_{\mu}^{*} \psi | | |
| 1510.06699_FO0491 | 22 | 1.000 | D_{\mu}^{*} \psi=\partial_{\mu}^{*} \psi | | |
| 1510.06699_FO0492 | 22 | 1.000 | \Delta_{\mu}^{*} \psi=\nabla_{\mu}^{*} \psi | | |
| 1510.06699_FO0493 | 22 | 1.000 | \Gamma^{\sigma}{ }_{\rho \mu} | | |
| 1510.06699_FO0494 | 22 | 1.000 | J^{a}+\delta J^{a} | | |
| 1510.06699_FO0495 | 22 | 1.000 | \Gamma | | |
| 1510.06699_FO0496 | 22 | 1.000 | w\left(\Gamma^{\sigma}{ }_{\nu \mu}\right)=0 | | |
| 1510.06699_FO0497 | 22 | 1.000 | \nabla_{\sigma}^{*} g_{\mu \nu}=0 | | |
| 1510.06699_FO0498 | 22 | 1.000 | T^{* a}{ }_{\mu \nu} | | |
| 1510.06699_FO0499 | 22 | 1.000 | R^{\rho}{ }_{\sigma \mu \nu}=e_{a}{ }^{\rho} e^{b}{ }_{\sigma} R^{a}{ }_{b \mu \nu} | | |
| 1510.06699_FO0500 | 22 | 1.000 | T^{* \lambda}{ }_{\mu \nu}=e_{a}{ }^{\lambda} T^{* a}{ }_{\mu \nu} | | |
| 1510.06699_FO0501 | 22 | 1.000 | T^{* \lambda}{ }_{\mu \nu} | | |
| 1510.06699_FO0502 | 22 | 1.000 | R^{\rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0503 | 22 | 1.000 | \widetilde{R}_{\rho \sigma \mu \nu} | | |
| 1510.06699_FO0504 | 22 | 0.774 | \mu, \nu | | |
| 1510.06699_FO0505 | 22 | 0.774 | \rho, \sigma | | |
| 1510.06699_FO0506 | 22 | 0.764 | \widetilde{R}_{(\rho \sigma) \mu \nu}=g_{\rho \sigma} H_{\mu \nu} | | |
| 1510.06699_FO0507 | 22 | 1.000 | V_{4} | | |
| 1510.06699_FO0508 | 22 | 1.000 | \widetilde{R}^{\rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0509 | 22 | 1.000 | \widetilde{R}_{\mu \nu} \equiv \widetilde{R}_{\mu \lambda \nu}{ }^{\lambda}=R_{\mu \nu}-H_{\mu \nu} | | |
| 1510.06699_FO0510 | 22 | 1.000 | \widetilde{R} \equiv \widetilde{R}^{\mu}{ }_{\mu}=R | | |
| 1510.06699_FO0511 | 23 | 1.000 | J^{\rho} | | |
| 1510.06699_FO0512 | 23 | 1.000 | { }^{0} \Gamma^{\lambda}{ }_{\mu \nu} \equiv \frac{1}{2} g^{\lambda \rho}\left(\partial_{\mu} g_{\nu \rho}+\partial_{\nu} g_{\mu \rho}-\partial_{\rho} g_{\mu \nu}\right) | | |
| 1510.06699_FO0513 | 23 | 1.000 | K^{* \lambda}{ }_{\mu \nu} | | |
| 1510.06699_FO0514 | 23 | 1.000 | K_{\lambda \mu \nu}^{*}=-K_{\mu \lambda \nu}^{*} | | |
| 1510.06699_FO0515 | 23 | 1.000 | { }^{0} \Gamma^{* \sigma}{ }_{\rho \mu} | | |
| 1510.06699_FO0516 | 23 | 0.661 | \Gamma^{\sigma}{ }_{\nu \mu} \rightarrow^{0} \Gamma^{* \sigma}{ }_{\nu \mu} | | |
| 1510.06699_FO0517 | 23 | 1.000 | A^{a}{ }_{b \mu} \rightarrow{ }^{0} A^{* a}{ }_{b \mu} | | |
| 1510.06699_FO0518 | 23 | 1.000 | { }^{0} \nabla_{\sigma}^{*} g_{\mu \nu}=0 | | |
| 1510.06699_FO0519 | 23 | 0.983 | R^{\rho}{ }_{\sigma \mu \nu} \rightarrow{ }^{0} R^{* \rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0520 | 23 | 0.983 | \Gamma^{\sigma}{ }_{\nu \mu} \rightarrow{ }^{0} \Gamma^{* \sigma}{ }_{\nu \mu} | | |
| 1510.06699_FO0521 | 23 | 1.000 | { }^{0} T^{* \lambda}{ }_{\mu \nu}=0 | | |
| 1510.06699_FO0522 | 23 | 0.941 | \nabla_{\mu}^{*} \rightarrow{ }^{0} \nabla_{\mu}^{*}, R^{\rho}{ }_{\sigma \mu \nu} \rightarrow{ }^{0} R^{* \rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0523 | 23 | 0.976 | T^{* \sigma}{ }_{\mu \nu} \rightarrow{ }^{0} T^{* \sigma}{ }_{\mu \nu}=0 | | |
| 1510.06699_FO0524 | 23 | 1.000 | P_{\nu} \equiv \partial_{\nu} \rho, \mathcal{P}_{a} \equiv h_{a}{ }^{\nu} P_{\nu} | | |
| 1510.06699_FO0525 | 23 | 1.000 | \theta | | |
| 1510.06699_FO0526 | 23 | 1.000 | w=-2 | | |
| 1510.06699_FO0527 | 24 | 1.000 | \mathcal{T}^{a}{ }_{b c}=0 | | |
| 1510.06699_FO0528 | 24 | 1.000 | \mathcal{T}^{\prime a}{ }_{b c} \neq 0 | | |
| 1510.06699_FO0529 | 24 | 1.000 | \mathcal{T}^{\dagger a}{ }_{b c} | | |
| 1510.06699_FO0530 | 24 | 1.000 | \theta=0 | | |
| 1510.06699_FO0531 | 24 | 1.000 | \theta=1 | | |
| 1510.06699_FO0532 | 24 | 1.000 | { }^{0} \mathcal{R}^{a b}{ }_{c d} | | |
| 1510.06699_FO0533 | 24 | 0.971 | { }^{0} \mathcal{T}^{a}{ }_{b c} | | |
| 1510.06699_FO0534 | 24 | 1.000 | D_{\mu}^{\dagger} \varphi | | |
| 1510.06699_FO0535 | 24 | 1.000 | V_{\mu} | | |
| 1510.06699_FO0536 | 24 | 0.999 | \mathcal{V}_{a}=h_{a}{ }^{\mu} V_{\mu} | | |
| 1510.06699_FO0537 | 24 | 0.999 | A^{\dagger a b}{ }_{\mu} | | |
| 1510.06699_FO0538 | 24 | 1.000 | \partial_{\mu} \varphi^{\prime} | | |
| 1510.06699_FO0539 | 24 | 1.000 | T_{\mu}= | | |
| 1510.06699_FO0540 | 24 | 0.999 | b^{a}{ }_{\mu} \mathcal{T}_{a} | | |
| 1510.06699_FO0541 | 24 | 1.000 | T_{\mu} | | |
| 1510.06699_FO0542 | 24 | 1.000 | T_{\mu}^{\prime}=T_{\mu}+3(1-\theta) P_{\mu} | | |
| 1510.06699_FO0543 | 24 | 0.898 | A^{\dagger a b}{ }_{\mu}=A^{\dagger a b}{ }_{\mu} | | |
| 1510.06699_FO0544 | 24 | 1.000 | V | | |
| 1510.06699_FO0545 | 25 | 1.000 | V_{\mu}=0 | | |
| 1510.06699_FO0546 | 25 | 1.000 | A^{\dagger a b}{ }_{\mu}=A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0547 | 25 | 1.000 | \left.D_{\mu}^{\dagger} \varphi\right|_{\theta=0}=\left(D_{\mu}-\frac{1}{3} w T_{\mu}\right) \varphi | | |
| 1510.06699_FO0548 | 25 | 1.000 | T_{\mu}=0 | | |
| 1510.06699_FO0549 | 25 | 1.000 | \left.D_{\mu}^{\dagger} \varphi\right|_{\theta=1} \equiv\left(\partial_{\mu}+\frac{1}{2} A^{\dagger a b}{ }_{\mu} \Sigma_{a b}-w V_{\mu}\right) \varphi | | |
| 1510.06699_FO0550 | 25 | 1.000 | \partial_{\mu}^{\dagger} \varphi(x) | | |
| 1510.06699_FO0551 | 25 | 1.000 | w-1 | | |
| 1510.06699_FO0552 | 25 | 0.999 | \mathcal{L}_{\mathrm{M}} \equiv h^{-1} L_{\mathrm{M}}\left(\varphi, \mathcal{D}^{\dagger} \varphi\right) | | |
| 1510.06699_FO0553 | 25 | 1.000 | \phi^{2} \mathcal{R}^{\dagger} | | |
| 1510.06699_FO0554 | 25 | 1.000 | \phi^{2} L_{\mathcal{T}^{\dagger 2}} | | |
| 1510.06699_FO0555 | 25 | 0.968 | \operatorname{SU}(2,2) | | |
| 1510.06699_FO0556 | 25 | 0.968 | \mathrm{O}(4,2) | | |
| 1510.06699_FO0557 | 26 | 1.000 | e_{b \mu} b_{a}-e_{a \mu} b_{b} | | |
| 1510.06699_FO0558 | 26 | 1.000 | \omega_{\mu a b} | | |
| 1510.06699_FO0559 | 26 | 0.999 | \mathcal{V} | | |
| 1510.06699_FO0560 | 26 | 0.999 | e_{a \mu} | | |
| 1510.06699_FO0561 | 26 | 1.000 | c_{b \mu} x_{a}-c_{a \mu} x_{b} | | |
| 1510.06699_FO0562 | 26 | 1.000 | c_{a \mu} | | |
| 1510.06699_FO0563 | 26 | 1.000 | x_{a} | | |
| 1510.06699_FO0564 | 26 | 1.000 | \mathcal{V}_{a} | | |
| 1510.06699_FO0565 | 26 | 1.000 | x \cdot \nabla | | |
| 1510.06699_FO0566 | 26 | 1.000 | { }^{0} \nabla_{\mu}^{\dagger} \equiv{ }^{0} \nabla_{\mu}-w\left(V_{\mu}+\frac{1}{3} T_{\mu}\right),{ }^{0} \Gamma^{\lambda}{ }_{\mu \nu} \equiv \frac{1}{2} \gamma^{\lambda \rho}\left(\partial_{\mu} \gamma_{\nu \rho}+\right. | | |
| 1510.06699_FO0567 | 26 | 0.817 | \partial_{\nu} \gamma_{\mu \rho}-\partial_{\rho} \gamma_{\mu \nu} | | |
| 1510.06699_FO0568 | 26 | 0.801 | D \mu | | |
| 1510.06699_FO0569 | 26 | 1.000 | T^{a}{ }_{\mu \nu} | | |
| 1510.06699_FO0570 | 26 | 1.000 | D_{\mu} | | |
| 1510.06699_FO0571 | 26 | 1.000 | R^{\dagger a b}{ }_{\mu \nu} | | |
| 1510.06699_FO0572 | 26 | 1.000 | H_{\mu \nu}^{\dagger} | | |
| 1510.06699_FO0573 | 26 | 1.000 | \mathcal{R}^{\dagger a b}{ }_{c d}=h_{c}{ }^{\mu} h_{d}{ }^{\nu} R^{\dagger a b}{ }_{\mu \nu} | | |
| 1510.06699_FO0574 | 26 | 1.000 | \mathcal{H}_{c d}^{\dagger}=h_{c}{ }^{\mu} h_{d}{ }^{\nu} H_{\mu \nu}^{\dagger} | | |
| 1510.06699_FO0575 | 27 | 1.000 | \mathcal{R}^{\dagger a b}{ }_{c d}, \mathcal{H}_{c d}^{\dagger} | | |
| 1510.06699_FO0576 | 27 | 1.000 | \mathcal{T}^{\dagger a}{ }_{c d} | | |
| 1510.06699_FO0577 | 27 | 1.000 | w\left(\mathcal{R}^{\dagger a b}{ }_{c d}\right)=w\left(\mathcal{H}_{c d}^{\dagger}\right)=-2 | | |
| 1510.06699_FO0578 | 27 | 0.999 | w\left(\mathcal{T}^{\dagger a}{ }_{c d}\right)=-1 | | |
| 1510.06699_FO0579 | 27 | 1.000 | \mathcal{R}^{\dagger a b}{ }_{c d} | | |
| 1510.06699_FO0580 | 27 | 1.000 | \mathcal{H}_{a b}^{\dagger} | | |
| 1510.06699_FO0581 | 27 | 0.725 | \mathcal{R}^{\dagger a b}{ }_{c d}(h, A, \partial A, V, \partial V), \mathcal{T}^{\dagger a}{ }_{b c}(h, \partial h, A) | | |
| 1510.06699_FO0582 | 27 | 1.000 | \mathcal{H}_{a b}^{\dagger}\left(h, \partial h, \partial^{2} h, A, \partial A, \partial V\right) | | |
| 1510.06699_FO0583 | 27 | 1.000 | \partial h, \partial^{2} h, A | | |
| 1510.06699_FO0584 | 27 | 1.000 | \partial^{2} h | | |
| 1510.06699_FO0585 | 27 | 1.000 | { }^{0} \mathcal{A}_{a b c}^{\dagger} \equiv \frac{1}{2}\left(c_{a b c}^{\dagger}+\right. | | |
| 1510.06699_FO0586 | 27 | 0.973 | \left.c_{b c a}^{\dagger}-c_{c a b}^{\dagger}\right) | | |
| 1510.06699_FO0587 | 27 | 0.973 | c^{\dagger c}{ }_{a b} \equiv h_{a}{ }^{\mu} h_{b}{ }^{\nu}\left(\partial_{\mu}^{\dagger} b^{c}{ }_{\nu}-\partial_{\nu}^{\dagger} b^{c}{ }_{\mu}\right) | | |
| 1510.06699_FO0588 | 27 | 0.981 | \mathcal{K}_{a b c}^{\dagger} \equiv-\frac{1}{2}\left(\mathcal{T}_{a b c}^{\dagger}+\mathcal{T}_{b c a}^{\dagger}-\mathcal{T}_{c a b}^{\dagger}\right) | | |
| 1510.06699_FO0589 | 27 | 0.981 | { }^{0} \mathcal{A}_{a b c}^{\dagger} | | |
| 1510.06699_FO0590 | 27 | 0.840 | \mathcal{K}_{a b c}^{\dagger} | | |
| 1510.06699_FO0591 | 27 | 0.568 | { }^{0} \mathcal{A}_{\text {abc }}^{\dagger} | | |
| 1510.06699_FO0592 | 27 | 0.551 | \mathcal{K}_{\text {abc }}^{\dagger} | | |
| 1510.06699_FO0593 | 27 | 0.992 | \mathcal{A}_{a b c}^{\dagger} | | |
| 1510.06699_FO0594 | 27 | 1.000 | { }^{0} D_{\mu}^{\dagger} \varphi | | |
| 1510.06699_FO0595 | 27 | 0.523 | { }^{0} \mathcal{D}_{a}^{\dagger} \equiv h_{a}{ }^{\mu} 0^{0} D_{\mu}^{\dagger} | | |
| 1510.06699_FO0596 | 27 | 1.000 | \mathcal{D}_{a}^{\dagger} | | |
| 1510.06699_FO0597 | 27 | 1.000 | { }^{0} \mathcal{D}_{a}^{\dagger} | | |
| 1510.06699_FO0598 | 27 | 1.000 | \mathcal{R}^{\dagger a b}{ }_{c d}, \mathcal{T}^{\dagger a}{ }_{b c} | | |
| 1510.06699_FO0599 | 28 | 0.999 | \mathcal{T}_{a b c}^{\dagger}=\epsilon_{a b c d} t^{d} | | |
| 1510.06699_FO0600 | 28 | 0.800 | \mathcal{R}_{a b c d}^{\dagger} | | |
| 1510.06699_FO0601 | 28 | 0.899 | \mathcal{T}_{a b c}^{\dagger} | | |
| 1510.06699_FO0602 | 28 | 1.000 | \mathcal{R}^{\dagger} \equiv | | |
| 1510.06699_FO0603 | 28 | 1.000 | \mathcal{R}^{\dagger a b}{ }_{a b} | | |
| 1510.06699_FO0604 | 28 | 1.000 | L_{\mathcal{R}^{\dagger 2}} | | |
| 1510.06699_FO0605 | 28 | 1.000 | L_{\mathcal{H}^{\dagger 2}} | | |
| 1510.06699_FO0606 | 28 | 1.000 | \mathcal{R}_{a b c d} \rightarrow \mathcal{R}_{a b c d}^{\dagger} | | |
| 1510.06699_FO0607 | 28 | 1.000 | \mathcal{H}_{a b} \rightarrow | | |
| 1510.06699_FO0608 | 28 | 0.829 | { }^{\underline{71}} | | |
| 1510.06699_FO0609 | 28 | 0.556 | \phi^{2} L_{\mathcal{T} \dagger^{2}} | | |
| 1510.06699_FO0610 | 28 | 0.556 | L_{\mathcal{T} \dagger^{2}} | | |
| 1510.06699_FO0611 | 28 | 0.999 | \mathcal{T}_{a b c} \rightarrow \mathcal{T}_{a b c}^{\dagger} | | |
| 1510.06699_FO0612 | 28 | 1.000 | \mathcal{H}_{a b}^{\dagger} \mathcal{H}^{\dagger a b} | | |
| 1510.06699_FO0613 | 28 | 1.000 | \varphi, \partial \varphi, h, \partial h, A | | |
| 1510.06699_FO0614 | 28 | 0.998 | \mathcal{D}_{a}^{\dagger} \varphi | | |
| 1510.06699_FO0615 | 28 | 1.000 | \partial V | | |
| 1510.06699_FO0616 | 29 | 0.626 | \mathcal{R}_{a b c d}^{\dagger}(h, A, \partial A, V, \partial V), \mathcal{T}_{a b c}^{\dagger}(h, \partial h, A) | | |
| 1510.06699_FO0617 | 29 | 1.000 | \mathcal{H}^{\dagger a b} \mathcal{H}_{a b}^{\dagger} | | |
| 1510.06699_FO0618 | 29 | 1.000 | t^{a}{ }_{\mu} \equiv \delta \mathcal{L}_{\mathrm{G}} / \delta h_{a}{ }^{\mu}, s_{a b}{ }^{\mu} \equiv \delta \mathcal{L}_{\mathrm{G}} / \delta A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0619 | 29 | 1.000 | j^{\mu} \equiv | | |
| 1510.06699_FO0620 | 29 | 1.000 | \delta \mathcal{L}_{\mathrm{G}} / \delta V_{\mu} | | |
| 1510.06699_FO0621 | 29 | 1.000 | \zeta^{\mu} \equiv \delta \mathcal{L}_{\mathrm{M}} / \delta V_{\mu} | | |
| 1510.06699_FO0622 | 29 | 0.998 | t^{a}{ }_{b} | | |
| 1510.06699_FO0623 | 29 | 1.000 | t^{a}{ }_{a} | | |
| 1510.06699_FO0624 | 29 | 1.000 | \tau^{a}{ }_{a} | | |
| 1510.06699_FO0625 | 29 | 1.000 | t_{a b} | | |
| 1510.06699_FO0626 | 29 | 1.000 | \tau^{\dagger a}{ }_{a}=\tau^{a}{ }_{a} | | |
| 1510.06699_FO0627 | 29 | 0.999 | t_{a b}^{\dagger} | | |
| 1510.06699_FO0628 | 29 | 1.000 | \mathcal{T}_{a}^{\dagger} \equiv 0 | | |
| 1510.06699_FO0629 | 29 | 1.000 | \bar{\partial} L_{\mathrm{M}} / \partial \varphi \equiv\left[\partial L_{\mathrm{M}}\left(\varphi, \mathcal{D}_{a}^{\dagger} u, \phi, \mathcal{D}_{a}^{\dagger} \phi, \ldots\right) / \partial \varphi\right]_{u=\varphi} | | |
| 1510.06699_FO0630 | 30 | 1.000 | H_{a b}^{\dagger} | | |
| 1510.06699_FO0631 | 30 | 1.000 | H_{a b}=h_{a}{ }^{\mu} h_{b}{ }^{\nu}\left(\partial_{\mu} V_{\nu}-\partial_{\nu} V_{\mu}\right) | | |
| 1510.06699_FO0632 | 30 | 1.000 | j^{\dagger a} | | |
| 1510.06699_FO0633 | 30 | 1.000 | j^{a} | | |
| 1510.06699_FO0634 | 30 | 1.000 | \varphi, \phi, h_{a}^{\mu}, A^{a b}{ }_{\mu}, V_{\mu} | | |
| 1510.06699_FO0635 | 30 | 1.000 | \varphi, \phi | | |
| 1510.06699_FO0636 | 30 | 1.000 | h_{a}^{\mu}, A^{\dagger a b}{ }_{\mu}, V_{\mu} | | |
| 1510.06699_FO0637 | 30 | 1.000 | h_{a}^{\mu}, A^{a b}{ }_{\mu}, V_{\mu} | | |
| 1510.06699_FO0638 | 30 | 1.000 | \mathcal{T}_{b}^{\natural} \equiv \mathcal{T}^{\natural a}{ }_{b a} | | |
| 1510.06699_FO0639 | 30 | 1.000 | \mathcal{T}_{b}^{\natural}=\mathcal{T}_{b}+3 \mathcal{V}_{b} | | |
| 1510.06699_FO0640 | 31 | 0.997 | h, \partial h | | |
| 1510.06699_FO0641 | 31 | 1.000 | A^{\dagger} | | |
| 1510.06699_FO0642 | 31 | 0.566 | \quad \mathcal{R}_{a b c d}^{\dagger}\left(h, A^{\dagger}, \partial A^{\dagger}\right), \quad \mathcal{T}_{a b c}^{\dagger}\left(h, \partial h, A^{\dagger}\right) \quad | | |
| 1510.06699_FO0643 | 31 | 1.000 | \mathcal{H}_{a b}^{\dagger}\left(h, \partial h, \partial^{2} h, A^{\dagger}, \partial A^{\dagger}\right) | | |
| 1510.06699_FO0644 | 31 | 1.000 | \mathcal{L} | | |
| 1510.06699_FO0645 | 31 | 1.000 | (\delta \mathcal{L} / \delta \chi)_{\dagger} | | |
| 1510.06699_FO0646 | 31 | 1.000 | \delta \mathcal{L} / \delta \chi | | |
| 1510.06699_FO0647 | 31 | 1.000 | \sigma_{a b}{ }^{\mu} | | |
| 1510.06699_FO0648 | 31 | 1.000 | \zeta^{\dagger \mu}=0 | | |
| 1510.06699_FO0649 | 31 | 1.000 | \phi, h_{a}{ }^{\mu}, A^{a b}{ }_{\mu}, V_{\mu} | | |
| 1510.06699_FO0650 | 32 | 1.000 | \mathcal{D}_{a}^{*} \rightarrow \mathcal{D}_{a}^{\dagger} | | |
| 1510.06699_FO0651 | 32 | 1.000 | \gamma^{a}\left(\mathcal{D}_{a}+\frac{1}{2} \mathcal{T}_{a}\right) \psi=\gamma^{a} \mathcal{D}_{a}^{\dagger} \psi | | |
| 1510.06699_FO0652 | 32 | 1.000 | \gamma^{a} \Sigma_{b a}=\frac{1}{4} \gamma^{a}\left[\gamma_{b}, \gamma_{a}\right]=-\frac{3}{2} \gamma_{b} | | |
| 1510.06699_FO0653 | 32 | 0.997 | \mathcal{T}_{[a b c]}=0 | | |
| 1510.06699_FO0654 | 32 | 1.000 | { }^{0} \mathcal{D}_{a} \rightarrow{ }^{0} \mathcal{D}_{a}^{\dagger} | | |
| 1510.06699_FO0655 | 32 | 1.000 | \mathcal{T}_{[a b c]} \rightarrow \mathcal{T}_{[a b c]}^{\dagger} | | |
| 1510.06699_FO0656 | 32 | 1.000 | \sigma_{a b}{ }^{c} | | |
| 1510.06699_FO0657 | 32 | 1.000 | \sigma_{a b}{ }^{b}=0 | | |
| 1510.06699_FO0658 | 32 | 0.444 | \beta_{1} | | |
| 1510.06699_FO0659 | 32 | 0.444 | \beta_{2} | | |
| 1510.06699_FO0660 | 32 | 0.444 | L_{\mathcal{\mathcal { T } ^ { + } 2}} | | |
| 1510.06699_FO0661 | 32 | 0.998 | \widehat{\mathcal{F}}_{a b}^{*} \rightarrow \widehat{\mathcal{F}}_{a b}^{\dagger}, \mathcal{T}^{* c}{ }_{a b} \rightarrow \mathcal{T}^{\dagger c}{ }_{a b} | | |
| 1510.06699_FO0662 | 33 | 1.000 | \tau^{\dagger a}{ }_{b}=\tau^{a}{ }_{b} | | |
| 1510.06699_FO0663 | 33 | 1.000 | \varphi, \phi, h_{a}^{\mu} | | |
| 1510.06699_FO0664 | 33 | 0.607 | \widehat{\mathcal{A}}^{\dagger a b}{ }_{c} \equiv \widehat{h}_{a}{ }^{\mu} \widehat{A}^{\dagger a b}{ }_{\mu} | | |
| 1510.06699_FO0665 | 33 | 1.000 | \mathcal{D}_{a}^{\dagger} \chi=\left(\mathcal{D}_{a}^{\natural}-\frac{1}{3} w \mathcal{T}_{a}^{\natural}\right) \chi | | |
| 1510.06699_FO0666 | 33 | 1.000 | \mathcal{D}_{a}^{\natural} | | |
| 1510.06699_FO0667 | 33 | 1.000 | \mathcal{T}_{a}^{\natural} | | |
| 1510.06699_FO0668 | 33 | 1.000 | \widehat{\mathcal{D}}_{a}^{\natural} | | |
| 1510.06699_FO0669 | 33 | 1.000 | \widehat{\mathcal{T}}_{a}^{\natural} | | |
| 1510.06699_FO0670 | 33 | 1.000 | \widehat{A}^{\dagger a b}{ }_{\mu} | | |
| 1510.06699_FO0671 | 33 | 1.000 | \widehat{\mathcal{D}}_{a}^{\natural}=\widehat{h}_{a}{ }^{\mu} D_{\mu}^{\natural} | | |
| 1510.06699_FO0672 | 33 | 1.000 | \mathcal{D}_{a}^{\dagger} \phi=\frac{1}{3}\left(\phi^{2} / \phi_{0}\right) \widehat{\mathcal{T}}_{a}^{\natural} | | |
| 1510.06699_FO0673 | 33 | 0.996 | \widehat{\mathcal{D}}_{a}^{\dagger}=\widehat{\mathcal{D}}_{a}^{\natural}-\frac{1}{3} w \widehat{\mathcal{T}}_{a}^{\natural} | | |
| 1510.06699_FO0674 | 33 | 1.000 | \widehat{\mathcal{D}}_{a}^{\dagger} \widehat{\chi} | | |
| 1510.06699_FO0675 | 33 | 1.000 | \widehat{\chi}, \widehat{h}_{a}{ }^{\mu} | | |
| 1510.06699_FO0676 | 33 | 1.000 | \mathcal{D}_{a}^{\dagger} \chi | | |
| 1510.06699_FO0677 | 33 | 0.999 | \mathcal{R}^{\dagger a b}{ }_{c d}=\left(\phi / \phi_{0}\right)^{2} \widehat{\mathcal{R}}^{\dagger a b}{ }_{c d} | | |
| 1510.06699_FO0678 | 33 | 1.000 | \mathcal{T}^{\dagger a}{ }_{b c}=\left(\phi / \phi_{0}\right) \widehat{\mathcal{T}}^{\dagger a}{ }_{b c} | | |
| 1510.06699_FO0679 | 33 | 1.000 | \mathcal{H}_{a b}^{\dagger}=\left(\phi / \phi_{0}\right)^{2} \widehat{\mathcal{H}}_{a b}^{\dagger} | | |
| 1510.06699_FO0680 | 33 | 1.000 | \varphi, h_{a}{ }^{\mu} | | |
| 1510.06699_FO0681 | 34 | 1.000 | \varphi, h | | |
| 1510.06699_FO0682 | 34 | 1.000 | \varphi, \phi, h_{a}^{\mu}, A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0683 | 34 | 1.000 | \widehat{V}_{\mu}=\frac{1}{3} \widehat{T}_{\mu}^{\natural} | | |
| 1510.06699_FO0684 | 34 | 1.000 | \widehat{\mathcal{V}}_{a} \equiv \widehat{h}_{a}{ }^{\mu} \widehat{V}_{\mu} | | |
| 1510.06699_FO0685 | 34 | 1.000 | \varphi, h_{a}^{\mu} | | |
| 1510.06699_FO0686 | 34 | 1.000 | V_{\mu}+\frac{1}{3} T_{\mu} | | |
| 1510.06699_FO0687 | 34 | 1.000 | \widehat{\varphi}, \widehat{h}_{a}{ }^{\mu}, \widehat{A}^{\dagger a b}{ }_{\mu} | | |
| 1510.06699_FO0688 | 34 | 1.000 | \widehat{V}_{\mu} | | |
| 1510.06699_FO0689 | 34 | 1.000 | v^{c}\left(\mathcal{D}_{c}^{\dagger} p_{a}-\right. | | |
| 1510.06699_FO0690 | 34 | 0.971 | \left.\mathcal{T}_{\text {cab }}^{\dagger} p^{b}\right)=e \mu^{2} \phi \mathcal{D}_{a}^{\dagger} \phi | | |
| 1510.06699_FO0691 | 34 | 0.997 | v^{c}{ }^{0} \mathcal{D}_{c}^{\dagger} p_{a}=e \mu^{2} \phi^{0} \mathcal{D}_{a}^{\dagger} \phi | | |
| 1510.06699_FO0692 | 34 | 1.000 | { }^{0} D_{\mu}^{\dagger} | | |
| 1510.06699_FO0693 | 34 | 0.718 | \mathcal{T}_{a b c}^{\dagger} \equiv 0 | | |
| 1510.06699_FO0694 | 34 | 0.718 | \left.\mathcal{K}_{a b c}^{\dagger} \equiv 0\right) | | |
| 1510.06699_FO0695 | 35 | 1.000 | { }^{0} R^{\dagger a b}{ }_{\mu \nu}\left(h, \partial h, \partial^{2} h, A, \partial A, V, \partial V\right) | | |
| 1510.06699_FO0696 | 35 | 1.000 | { }^{0} A^{\dagger a b}{ }_{\mu} | | |
| 1510.06699_FO0697 | 35 | 1.000 | { }^{0} R^{\dagger a b}{ }_{\mu \nu} | | |
| 1510.06699_FO0698 | 35 | 1.000 | R^{\dagger a b}{ }_{\mu \nu}(h, A, \partial A, V, \partial V) | | |
| 1510.06699_FO0699 | 35 | 1.000 | { }^{0} \mathcal{R}^{\dagger a b}{ }_{c d}=h_{c}{ }^{\mu} h_{d}{ }^{\mu}{ }^{0} R^{\dagger a b}{ }_{\mu \nu} | | |
| 1510.06699_FO0700 | 35 | 1.000 | { }^{0} \mathcal{T}^{\dagger a}{ }_{b c} \equiv | | |
| 1510.06699_FO0701 | 35 | 1.000 | h_{b}{ }^{\mu} h_{c}{ }^{\nu}\left({ }^{0} D_{\mu}^{\dagger} b^{a}{ }_{\nu}-{ }^{0} D_{\nu}^{\dagger} b^{a}{ }_{\mu}\right)=0 | | |
| 1510.06699_FO0702 | 35 | 0.785 | \mathcal{D}_{a}^{\dagger} \rightarrow^{0} \mathcal{D}_{a}^{\dagger}, \mathcal{R}_{a b c d} \rightarrow{ }^{0} \mathcal{R}_{a b c d}^{\dagger} | | |
| 1510.06699_FO0703 | 35 | 0.831 | \mathcal{T}_{a b c}^{\dagger} \rightarrow{ }^{0} \mathcal{T}_{a b c}^{\dagger}=0 | | |
| 1510.06699_FO0704 | 35 | 1.000 | { }^{0} \mathcal{R}^{a b}{ }_{c d} \rightarrow | | |
| 1510.06699_FO0705 | 35 | 1.000 | { }^{0} \mathcal{R}^{\dagger a b}{ }_{c d},{ }^{0} \mathcal{D}_{a} \rightarrow{ }^{0} \mathcal{D}_{a}^{\dagger}, \mathcal{K}_{a b c} \rightarrow \mathcal{K}_{a b c}^{\dagger} | | |
| 1510.06699_FO0706 | 35 | 1.000 | \mathcal{R}^{a b}{ }_{c d} \rightarrow{ }^{0} \mathcal{R}^{\dagger a b}{ }_{c d} | | |
| 1510.06699_FO0707 | 35 | 1.000 | { }^{0} \mathcal{R}^{\dagger}{ }_{a b} | | |
| 1510.06699_FO0708 | 35 | 0.999 | { }^{0} \mathcal{R}_{a b c d}^{\dagger} | | |
| 1510.06699_FO0709 | 35 | 1.000 | \mathcal{R}_{a b c d} \rightarrow{ }^{0} \mathcal{R}_{a b c d}^{\dagger} | | |
| 1510.06699_FO0710 | 35 | 0.535 | \mathcal{D}_{a}^{\dagger} \rightarrow^{0} \mathcal{D}_{a}^{\dagger} | | |
| 1510.06699_FO0711 | 35 | 0.720 | \phi^{2}{ }^{0} \mathcal{R}^{\dagger} | | |
| 1510.06699_FO0712 | 35 | 0.806 | \mathcal{D}_{a}^{\dagger} \rightarrow{ }^{0} \mathcal{D}_{a}^{\dagger}, \mathcal{R}_{a b c d}^{\dagger} \rightarrow{ }^{0} \mathcal{R}_{a b c d}^{\dagger} | | |
| 1510.06699_FO0713 | 35 | 0.806 | \mathcal{T}_{a b c}^{\dagger} \rightarrow | | |
| 1510.06699_FO0714 | 35 | 0.961 | { }^{0} \mathcal{T}_{a b c}^{\dagger} \equiv 0 | | |
| 1510.06699_FO0715 | 35 | 0.891 | \mathcal{T}_{a b c}^{\dagger}=0 | | |
| 1510.06699_FO0716 | 36 | 1.000 | b^{b}{ }_{\nu} | | |
| 1510.06699_FO0717 | 36 | 1.000 | e^{b}{ }_{\nu} | | |
| 1510.06699_FO0718 | 36 | 1.000 | e_{a}{ }^{\mu}, A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0719 | 36 | 1.000 | \partial_{\mu}^{\dagger} | | |
| 1510.06699_FO0720 | 36 | 1.000 | A^{\dagger a b}{ }_{\mu}=-A^{\dagger b a}{ }_{\mu} | | |
| 1510.06699_FO0721 | 36 | 0.545 | \nabla_{\mu}^{\dagger}=\partial_{\mu}^{\dagger}+\Gamma^{\sigma}{ }_{\rho \mu} \mathrm{X}^{\rho}{ }_{\sigma} | | |
| 1510.06699_FO0722 | 36 | 0.545 | 4, R | | |
| 1510.06699_FO0723 | 36 | 1.000 | \Delta_{\mu}^{\dagger} | | |
| 1510.06699_FO0724 | 36 | 1.000 | \nabla_{\mu}^{\dagger} \psi=\partial_{\mu}^{\dagger} \psi | | |
| 1510.06699_FO0725 | 36 | 1.000 | \Delta_{\mu}^{\dagger} \psi=D_{\mu}^{\dagger} \psi | | |
| 1510.06699_FO0726 | 36 | 1.000 | D_{\mu}^{\dagger} \psi=\partial_{\mu}^{\dagger} \psi | | |
| 1510.06699_FO0727 | 36 | 1.000 | \Delta_{\mu}^{\dagger} \psi=\nabla_{\mu}^{\dagger} \psi | | |
| 1510.06699_FO0728 | 36 | 1.000 | T | | |
| 1510.06699_FO0729 | 36 | 1.000 | \partial_{\mu}^{*} \rightarrow \partial_{\mu}^{\dagger} | | |
| 1510.06699_FO0730 | 36 | 1.000 | A_{\mu}^{a b} \rightarrow A^{\dagger a b}{ }_{\mu} | | |
| 1510.06699_FO0731 | 36 | 1.000 | \nabla_{\sigma}^{\dagger} g_{\mu \nu}=0 | | |
| 1510.06699_FO0732 | 36 | 1.000 | R^{\dagger \rho}{ }_{\sigma \mu \nu}=e_{a}{ }^{\rho} e^{b}{ }_{\sigma} R^{\dagger a}{ }_{b \mu \nu} | | |
| 1510.06699_FO0733 | 36 | 1.000 | T^{\dagger \lambda}{ }_{\mu \nu}=e_{a}{ }^{\lambda} T^{\dagger a}{ }_{\mu \nu} | | |
| 1510.06699_FO0734 | 37 | 1.000 | T^{\dagger \lambda}{ }_{\mu \lambda}=0 | | |
| 1510.06699_FO0735 | 37 | 1.000 | R^{\dagger \rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0736 | 37 | 0.999 | { }^{0} \Gamma^{\dagger \sigma}{ }_{\rho \mu} | | |
| 1510.06699_FO0737 | 37 | 1.000 | \widehat{R}_{\rho \sigma \mu \nu} | | |
| 1510.06699_FO0738 | 37 | 1.000 | \widehat{R}_{(\rho \sigma) \mu \nu}=-g_{\rho \sigma} H_{\mu \nu}^{\dagger} | | |
| 1510.06699_FO0739 | 37 | 1.000 | \widehat{R}^{\rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0740 | 37 | 1.000 | T^{\dagger \lambda}{ }_{\mu \nu} | | |
| 1510.06699_FO0741 | 37 | 1.000 | \widehat{R}_{\mu \nu} \equiv \widehat{R}_{\mu \lambda \nu}{ }^{\lambda}=R_{\mu \nu}^{\dagger}+H_{\mu \nu}^{\dagger} | | |
| 1510.06699_FO0742 | 37 | 1.000 | \widehat{R} \equiv \widehat{R}^{\mu}{ }_{\mu}=R^{\dagger} | | |
| 1510.06699_FO0743 | 37 | 1.000 | { }^{0} \Delta_{\mu}^{\dagger} e^{a}{ }_{\nu} \equiv \partial_{\mu}^{\dagger} e^{a}{ }_{\nu}-{ }^{0} \Gamma^{\dagger \sigma}{ }_{\nu \mu} e^{a}{ }_{\sigma}+{ }^{0} A^{\dagger a}{ }_{b \mu} e^{b}{ }_{\nu}=0 | | |
| 1510.06699_FO0744 | 37 | 0.992 | \partial_{\mu}^{*} \rightarrow \partial_{\mu}^{\dagger}, \Gamma^{\sigma}{ }_{\nu \mu} \rightarrow | | |
| 1510.06699_FO0745 | 37 | 1.000 | { }^{0} \Gamma^{\dagger \sigma}{ }_{\nu \mu} | | |
| 1510.06699_FO0746 | 37 | 1.000 | A^{a}{ }_{b \mu} \rightarrow{ }^{0} A^{\dagger a}{ }_{b \mu} | | |
| 1510.06699_FO0747 | 37 | 1.000 | { }^{0} \nabla_{\sigma}^{\dagger} g_{\mu \nu}=0 | | |
| 1510.06699_FO0748 | 37 | 1.000 | R^{\dagger \rho}{ }_{\sigma \mu \nu} \rightarrow{ }^{0} R^{\dagger \rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0749 | 37 | 0.999 | \Gamma^{\sigma}{ }_{\nu \mu} \rightarrow{ }^{0} \Gamma^{\dagger \sigma}{ }_{\nu \mu} | | |
| 1510.06699_FO0750 | 37 | 1.000 | { }^{0} T^{\dagger \lambda}{ }_{\mu \nu}=0 | | |
| 1510.06699_FO0751 | 37 | 0.986 | \nabla_{\mu}^{\dagger} \rightarrow{ }^{0} \nabla_{\mu}^{\dagger}, R^{\rho}{ }_{\sigma \mu \nu} \rightarrow{ }^{0} R^{\dagger \rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0752 | 37 | 0.986 | T^{\dagger \sigma}{ }_{\mu \nu} \rightarrow{ }^{0} T^{\dagger \sigma}{ }_{\mu \nu}=0 | | |
| 1510.06699_FO0753 | 37 | 1.000 | L_{\mathrm{T}}= | | |
| 1510.06699_FO0754 | 37 | 1.000 | L_{\mathrm{G}}+L_{\mathrm{M}} | | |
| 1510.06699_FO0755 | 37 | 1.000 | { }^{0} \Gamma^{\lambda}{ }_{\mu \nu} | | |
| 1510.06699_FO0756 | 37 | 1.000 | K^{\dagger \lambda}{ }_{\mu \nu} | | |
| 1510.06699_FO0757 | 37 | 1.000 | L_{G}=L_{\mathcal{R}^{\dagger 2}}+L_{\mathcal{H}^{\dagger 2}} | | |
| 1510.06699_FO0758 | 37 | 1.000 | L_{\mathrm{M}}= | | |
| 1510.06699_FO0759 | 38 | 1.000 | \nu, \lambda, a | | |
| 1510.06699_FO0760 | 38 | 1.000 | \nu, \lambda | | |
| 1510.06699_FO0761 | 38 | 1.000 | L_{\varphi} | | |
| 1510.06699_FO0762 | 38 | 1.000 | \left(\tau_{\varphi}^{\dagger}\right)^{a}{ }_{b}=h_{b}{ }^{\mu}\left(\delta L_{\varphi} / \delta h_{a}{ }^{\mu}\right)_{\dagger} | | |
| 1510.06699_FO0763 | 38 | 1.000 | \left(t_{\mathcal{H}^{2}}^{\dagger}\right)^{a}{ }_{b} | | |
| 1510.06699_FO0764 | 39 | 1.000 | \left(\sigma_{\varphi}^{\dagger}\right)_{a b}{ }^{c}= | | |
| 1510.06699_FO0765 | 39 | 1.000 | b^{c}{ }_{\mu} \delta L_{\varphi} / \delta A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0766 | 39 | 0.860 | \left(s_{\mathcal{H}^{2}}\right)_{a b}{ }^{c} | | |
| 1510.06699_FO0767 | 39 | 0.554 | \mathcal{T}_{c a b}^{\dagger}+2 \mathcal{T}_{[a b] c}^{\dagger}-3 \mathcal{T}_{[c a b]}^{\dagger}=0 | | |
| 1510.06699_FO0768 | 39 | 1.000 | \alpha_{4} | | |
| 1510.06699_FO0769 | 39 | 1.000 | \alpha_{5} | | |
| 1510.06699_FO0770 | 39 | 0.606 | \overline{\mathcal{R}}_{a b c d}^{\dagger} \equiv \mathcal{R}_{c d a b}^{\dagger} | | |
| 1510.06699_FO0771 | 39 | 0.606 | \overline{\mathcal{R}}^{\dagger a}{ }_{b}=\mathcal{R}_{b}^{\dagger a} | | |
| 1510.06699_FO0772 | 39 | 1.000 | \alpha_{2} | | |
| 1510.06699_FO0773 | 39 | 1.000 | \alpha_{3} | | |
| 1510.06699_FO0774 | 39 | 1.000 | \alpha_{1} | | |
| 1510.06699_FO0775 | 39 | 1.000 | \overline{\mathcal{R}}^{\dagger}=\mathcal{R}^{\dagger} | | |
| 1510.06699_FO0776 | 39 | 1.000 | \left(\zeta_{\varphi}\right)_{a}= | | |
| 1510.06699_FO0777 | 39 | 1.000 | b_{a \mu} \delta L_{\varphi} / \delta V_{\mu} | | |
| 1510.06699_FO0778 | 39 | 1.000 | c | | |
| 1510.06699_FO0779 | 39 | 1.000 | j_{a}^{\dagger} | | |
| 1510.06699_FO0780 | 39 | 1.000 | \zeta_{a}^{\dagger} | | |
| 1510.06699_FO0781 | 39 | 1.000 | \partial_{\phi} \equiv \partial / \partial \phi | | |
| 1510.06699_FO0782 | 39 | 1.000 | \delta_{\phi} \equiv \delta / \delta \phi | | |
| 1510.06699_FO0783 | 39 | 1.000 | L_{\phi} | | |
| 1510.06699_FO0784 | 40 | 1.000 | -\phi | | |
| 1510.06699_FO0785 | 40 | 0.999 | \delta_{\varphi} L_{\varphi}=0 | | |
| 1510.06699_FO0786 | 40 | 1.000 | \xi=0 | | |
| 1510.06699_FO0787 | 40 | 1.000 | \left.\mathcal{D}_{a}^{\dagger} \phi\right|_{\phi=\phi_{0}}=\phi_{0}\left(\mathcal{V}_{a}+\frac{1}{3} \mathcal{T}_{a}\right) | | |
| 1510.06699_FO0788 | 40 | 1.000 | \widehat{\varphi}, \widehat{h}_{a}{ }^{\mu} | | |
| 1510.06699_FO0789 | 41 | 1.000 | h^{\prime}{ }_{a}{ }^{\mu}=e^{-\rho} h_{a}{ }^{\mu} | | |
| 1510.06699_FO0790 | 41 | 1.000 | A^{\prime a b}{ }_{\mu}=A^{a b}{ }_{\mu}+ | | |
| 1510.06699_FO0791 | 41 | 1.000 | \theta\left(b^{a}{ }_{\mu} \mathcal{P}^{b}-b^{b}{ }_{\mu} \mathcal{P}^{a}\right) | | |
| 1510.06699_FO0792 | 41 | 1.000 | \mathcal{P}_{a}=h_{a}{ }^{\mu} \partial_{\mu} \rho | | |
| 1510.06699_FO0793 | 41 | 1.000 | \mathcal{P}^{2} \equiv \mathcal{P}_{a} \mathcal{P}^{a} | | |
| 1510.06699_FO0794 | 41 | 1.000 | (\theta=0) | | |
| 1510.06699_FO0795 | 41 | 1.000 | (\theta=1) | | |
| 1510.06699_FO0796 | 41 | 1.000 | \theta \neq 0 | | |
| 1510.06699_FO0797 | 41 | 1.000 | \alpha_{i}=0 | | |
| 1510.06699_FO0798 | 41 | 0.996 | i | | |
| 1510.06699_FO0799 | 41 | 0.998 | L_{\mathcal{T}^{2}} | | |
| 1510.06699_FO0800 | 42 | 0.989 | \mathcal{L}_{\mathrm{M}} \equiv \mathcal{L}_{\psi}+\mathcal{L}_{\phi}+\phi^{2} \mathcal{L}_{\mathcal{R}}+\phi^{2} \mathcal{L}_{\mathcal{T}^{2}} | | |
| 1510.06699_FO0801 | 42 | 0.990 | \mathcal{L}_{\psi} | | |
| 1510.06699_FO0802 | 42 | 1.000 | \nu, a | | |
| 1510.06699_FO0803 | 42 | 1.000 | \beta_{i}(i=1,2,3) | | |
| 1510.06699_FO0804 | 42 | 1.000 | \nu | | |
| 1510.06699_FO0805 | 42 | 1.000 | \nu=0=2 \beta_{1}+\beta_{2}+3 \beta_{3} | | |
| 1510.06699_FO0806 | 42 | 0.997 | \nu=0=a | | |
| 1510.06699_FO0807 | 42 | 1.000 | \nu=\beta_{1}=\beta_{2}=\beta_{3}=0 | | |
| 1510.06699_FO0808 | 42 | 1.000 | 2 \beta_{1}+\beta_{2}+3 \beta_{3}=0 | | |
| 1510.06699_FO0809 | 42 | 0.706 | \mathcal{D}_{a} \phi \rightarrow\left(\mathcal{D}_{a}+\frac{1}{3} \mathcal{T}_{a}\right) \phi | | |
| 1510.06699_FO0810 | 42 | 0.706 | \mathcal{D}^{a} \phi | | |
| 1510.06699_FO0811 | 42 | 1.000 | \frac{1}{2} \nu+6 a=0 | | |
| 1510.06699_FO0812 | 42 | 0.994 | 2 \beta_{1}+\beta_{2}=0 | | |
| 1510.06699_FO0813 | 42 | 0.994 | L_{\mathcal{T}^{+2}} | | |
| 1510.06699_FO0814 | 43 | 1.000 | { }^{0} \mathcal{D}_{a} | | |
| 1510.06699_FO0815 | 43 | 1.000 | { }^{0} \mathcal{T}^{a}{ }_{b c} \equiv h_{b}{ }^{\mu} h_{c}{ }^{\nu}\left({ }^{0} D_{\mu} b^{a}{ }_{\nu}-{ }^{0} D_{\nu} b^{a}{ }_{\mu}\right)=0 | | |
| 1510.06699_FO0816 | 43 | 1.000 | { }^{0} A^{\prime a b}{ }_{\mu}={ }^{0} A^{a b}{ }_{\mu}+b^{a}{ }_{\mu} \mathcal{P}^{b}-b^{b}{ }_{\mu} \mathcal{P}^{a} | | |
| 1510.06699_FO0817 | 43 | 1.000 | { }^{0} A^{a b}{ }_{\mu},{ }^{0} \mathcal{D}_{c} \varphi | | |
| 1510.06699_FO0818 | 43 | 0.999 | A^{a b}{ }_{\mu}, \mathcal{D}_{c} \varphi | | |
| 1510.06699_FO0819 | 43 | 1.000 | \mathcal{D}_{c} \rightarrow{ }^{0} \mathcal{D}_{c} | | |
| 1510.06699_FO0820 | 43 | 1.000 | \mathcal{T}^{a}{ }_{b c} \rightarrow{ }^{0} \mathcal{T}^{a}{ }_{b c} \equiv 0 | | |
| 1510.06699_FO0821 | 43 | 0.915 | L_{G} | | |
| 1510.06699_FO0822 | 43 | 1.000 | 2 \alpha_{3}+\alpha_{2}=0 | | |
| 1510.06699_FO0823 | 43 | 1.000 | 3 \alpha_{1}-\alpha_{3}=0 | | |
| 1510.06699_FO0824 | 43 | 1.000 | \alpha=\alpha_{3} | | |
| 1510.06699_FO0825 | 43 | 1.000 | { }^{0} \mathcal{R}_{a b c d}{ }^{0} \mathcal{R}^{a b c d} | | |
| 1510.06699_FO0826 | 43 | 0.899 | { }^{\underline{101}} | | |
| 1510.06699_FO0827 | 43 | 0.999 | L_{\mathrm{W}}={ }^{0} \mathcal{C}_{a b c d}{ }^{0} \mathcal{C}^{a b c d} | | |
| 1510.06699_FO0828 | 43 | 0.999 | { }^{0} \mathcal{C}_{a b c d} | | |
| 1510.06699_FO0829 | 44 | 1.000 | { }^{0} \mathcal{R}_{a b c d} | | |
| 1510.06699_FO0830 | 44 | 0.988 | { }^{0} \mathcal{C}_{a b c d}^{\prime}=e^{-2 \rho}{ }^{0} \mathcal{C}_{a b c d} | | |
| 1510.06699_FO0831 | 44 | 1.000 | L_{W} | | |
| 1510.06699_FO0832 | 44 | 1.000 | w\left(L_{W}\right)=-4 | | |
| 1510.06699_FO0833 | 44 | 1.000 | { }^{\underline{19}} | | |
| 1510.06699_FO0834 | 44 | 1.000 | \mathcal{D}_{a} \rightarrow{ }^{0} \mathcal{D}_{a} | | |
| 1510.06699_FO0835 | 44 | 0.554 | \mathcal{R} \rightarrow{ }^{0} \mathcal{R} | | |
| 1510.06699_FO0836 | 44 | 0.972 | { }^{\underline{103}} | | |
| 1510.06699_FO0837 | 44 | 1.000 | \frac{1}{2} \nu+ | | |
| 1510.06699_FO0838 | 44 | 1.000 | 6 a=0 | | |
| 1510.06699_FO0839 | 44 | 0.657 | \phi^{20} \mathcal{R} | | |
| 1510.06699_FO0840 | 44 | 1.000 | { }^{0} \mathcal{R}_{a b c d} \rightarrow{ }^{0} \mathcal{R}_{a b c d}^{*} | | |
| 1510.06699_FO0841 | 44 | 1.000 | { }^{0} \mathcal{R}_{a b c d} \rightarrow{ }^{0} \mathcal{R}_{a b c d}^{\dagger} | | |
| 1510.06699_FO0842 | 44 | 1.000 | \frac{1}{2} \nu+6 a= | | |
| 1510.06699_FO0843 | 44 | 0.996 | \mathcal{T}_{a} \equiv 0 | | |
| 1510.06699_FO0844 | 44 | 0.996 | \mathcal{D}_{a}^{\dagger} \rightarrow{ }^{0} \mathcal{D}_{a}^{*} | | |
| 1510.06699_FO0845 | 44 | 1.000 | \mathcal{R}^{\dagger} \rightarrow{ }^{0} \mathcal{R}^{*} \mathcal{T}_{a b c}^{\dagger} \rightarrow{ }^{0} \mathcal{T}_{a b c}^{*} \equiv 0 | | |
| 1510.06699_FO0846 | 44 | 1.000 | \mathcal{D}_{a}^{\dagger} \rightarrow{ }^{0} \mathcal{D}_{a}^{\dagger}, \mathcal{R}^{\dagger} \rightarrow{ }^{0} \mathcal{R}^{\dagger} | | |
| 1510.06699_FO0847 | 44 | 0.996 | \mathcal{T}_{a b c}^{\dagger} \rightarrow{ }^{0} \mathcal{T}_{a b c}^{\dagger} \equiv 0 | | |
| 1510.06699_FO0848 | 45 | 0.997 | w,-1 | | |
| 1510.06699_FO0849 | 45 | 1.000 | \mathcal{R}_{a b c d}^{\dagger}(h, A, \partial A, V, \partial V) | | |
| 1510.06699_FO0850 | 45 | 1.000 | \mathcal{T}_{a b c}^{\dagger}(h, \partial h, A) \quad | | |
| 1510.06699_FO0851 | 45 | 1.000 | \quad \mathcal{H}_{a b}^{\dagger}\left(h, \partial h, \partial^{2} h, A, \partial A, \partial V\right) | | |
| 1510.06699_FO0852 | 45 | 1.000 | \mathcal{T}_{a}^{\dagger} | | |
| 1510.06699_FO0853 | 45 | 0.971 | \tau_{a b}^{\dagger} | | |
| 1510.06699_FO0854 | 45 | 1.000 | A^{\dagger a b}{ }_{\mu} \equiv | | |
| 1510.06699_FO0855 | 45 | 0.932 | A^{a b}{ }_{\mu}+\left(\mathcal{V}^{a} b^{b}{ }_{\mu}-\mathcal{V}^{b} b^{a}{ }_{\mu}\right) | | |
| 1510.06699_FO0856 | 46 | 1.000 | t^{\dagger a}{ }_{a} | | |
| 1510.06699_FO0857 | 46 | 1.000 | \tau^{\dagger a}{ }_{a} | | |
| 1510.06699_FO0858 | 46 | 0.948 | { }^{0} \mathcal{R}_{a b c d}^{\dagger}\left(h, \partial h, \partial^{2} h, A, \partial A, V, \partial V\right) | | |
| 1510.06699_FO0859 | 47 | 1.000 | \not \partial \equiv \gamma^{\mu} \partial_{\mu} | | |
| 1510.06699_FO0860 | 47 | 0.938 | \bar{\psi} / t | | |
| 1510.06699_FO0861 | 47 | 0.938 | J^{\mu}= | | |
| 1510.06699_FO0862 | 47 | 1.000 | \bar{\psi} \gamma^{\mu} \psi | | |
| 1510.06699_FO0863 | 47 | 1.000 | \psi \bar{\psi} | | |
| 1510.06699_FO0864 | 47 | 1.000 | \gamma^{5}=\gamma_{5}=i \gamma^{0} \gamma^{1} \gamma^{2} \gamma^{3} | | |
| 1510.06699_FO0865 | 47 | 1.000 | \sigma^{\nu \rho}=\frac{i}{2}\left[\gamma^{\nu}, \gamma^{\rho}\right] | | |
| 1510.06699_FO0866 | 47 | 1.000 | \rho \equiv \bar{\psi} \psi | | |
| 1510.06699_FO0867 | 47 | 0.671 | \beta \equiv \bar{\psi} i \gamma^{5} \psi | | |
| 1510.06699_FO0868 | 47 | 0.671 | \bar{\psi} / \hbar= | | |
| 1510.06699_FO0869 | 47 | 1.000 | \bar{\psi}\left(\rho+\beta i \gamma^{5}\right) | | |
| 1510.06699_FO0870 | 47 | 1.000 | \left(\rho-\beta i \gamma^{5}\right) | | |
| 1510.06699_FO0871 | 47 | 0.982 | \nexists \not \partial \psi | | |
| 1510.06699_FO0872 | 47 | 1.000 | J^{\mu} \partial_{\mu} \psi | | |
| 1510.06699_FO0873 | 47 | 1.000 | n^{\nu} \equiv-i \sigma^{\mu \nu} J_{\mu} | | |
| 1510.06699_FO0874 | 47 | 1.000 | J_{\nu} n^{\nu}=-i \sigma^{\mu \nu} J_{\mu} J_{\nu}=0 | | |
| 1510.06699_FO0875 | 47 | 1.000 | -i \sigma^{\mu \nu} J_{\mu} \partial_{\nu} \psi | | |
| 1510.06699_FO0876 | 47 | 1.000 | x^{\mu}(\lambda) | | |
| 1510.06699_FO0877 | 47 | 1.000 | R(\lambda) | | |
| 1510.06699_FO0878 | 47 | 1.000 | \bar{R} R=1 | | |
| 1510.06699_FO0879 | 47 | 1.000 | \bar{R} i \gamma^{5} R=0 | | |
| 1510.06699_FO0880 | 47 | 1.000 | R | | |
| 1510.06699_FO0881 | 47 | 1.000 | \dot{x}^{\mu} \equiv d x^{\mu} / d \lambda | | |
| 1510.06699_FO0882 | 47 | 1.000 | \bar{R} \gamma^{\mu} R | | |
| 1510.06699_FO0883 | 47 | 1.000 | p_{\mu}(\lambda) | | |
| 1510.06699_FO0884 | 47 | 1.000 | p_{\mu} | | |
| 1510.06699_FO0885 | 47 | 1.000 | \dot{x}^{\mu} | | |
| 1510.06699_FO0886 | 47 | 0.999 | m e(\lambda) | | |
| 1510.06699_FO0887 | 47 | 1.000 | x^{\mu}(\lambda), R(\lambda), p^{\mu}(\lambda) | | |
| 1510.06699_FO0888 | 47 | 1.000 | p^{\mu} / m | | |
| 1510.06699_FO0889 | 47 | 1.000 | e(\lambda) \rightarrow \frac{1}{2} e(\lambda) | | |
| 1510.06699_FO0890 | 47 | 1.000 | x^{\mu}(\lambda), p^{\mu}(\lambda) | | |
| 1510.06699_FO0891 | 47 | 1.000 | \rho=0 | | |
| 1510.06699_FO0892 | 47 | 1.000 | \rho(x)=0 | | |
| 1510.06699_FO0893 | 48 | 1.000 | D_{\mu} \varphi | | |
| 1510.06699_FO0894 | 48 | 0.981 | \rho(x)=0= | | |
| 1510.06699_FO0895 | 48 | 1.000 | B_{\mu}=0 | | |
| 1510.06699_FO0896 | 48 | 1.000 | H_{\mu \nu}=0 | | |
| 1510.06699_FO0897 | 48 | 0.999 | \mathcal{R} \equiv \mathcal{R}^{a b}{ }_{a b}, \Lambda | | |
| 1510.06699_FO0898 | 48 | 1.000 | a, \Lambda,\left\{\alpha_{i}\right\} | | |
| 1510.06699_FO0899 | 48 | 1.000 | \left\{\beta_{i}\right\} | | |
| 1510.06699_FO0900 | 48 | 1.000 | \varphi, \partial \varphi, h | | |
| 1510.06699_FO0901 | 48 | 0.546 | \mathcal{H}_{a b}, j^{a}, \zeta^{a} | | |
| 1510.06699_FO0902 | 48 | 1.000 | \mu \phi \bar{\psi} \psi \rightarrow m \bar{\psi} \psi | | |
| 1510.06699_FO0903 | 48 | 1.000 | \phi=1 | | |
| 1510.06699_FO0904 | 48 | 0.992 | { }^{0} \mathcal{T}^{a}{ }_{b c} \equiv 0 | | |
| 1510.06699_FO0905 | 48 | 1.000 | { }^{0} \mathcal{R}^{a b}{ }_{c d}\left(h, \partial h, \partial^{2} h\right) | | |
| 1510.06699_FO0906 | 49 | 1.000 | { }^{0} \mathcal{D}_{a} \mathcal{T}^{a}=h \partial_{\mu}\left(h^{-1} h_{a}{ }^{\mu} \mathcal{T}^{a}\right) | | |
| 1510.06699_FO0907 | 49 | 0.980 | { }^{\underline{105}} | | |
| 1510.06699_FO0908 | 49 | 0.935 | L_{0} \mathcal{R}^{2} | | |
| 1510.06699_FO0909 | 49 | 0.606 | L_{0^{\mathcal{R}^{2}}} | | |
| 1510.06699_FO0910 | 49 | 0.999 | \mathcal{R}_{a b c d} \rightarrow{ }^{0} \mathcal{R}_{a b c d} | | |
| 1510.06699_FO0911 | 49 | 1.000 | \alpha_{3}=0 | | |
| 1510.06699_FO0912 | 49 | 0.999 | \alpha_{1}=\alpha_{2}=0 | | |
| 1510.06699_FO0913 | 49 | 1.000 | a=\frac{1}{2} | | |
| 1510.06699_FO0914 | 49 | 0.999 | a=0=\Lambda, \alpha_{1}=-\frac{1}{3} \alpha_{2} | | |
| 1510.06699_FO0915 | 49 | 1.000 | U_{4} | | |
| 1510.06699_FO0916 | 49 | 1.000 | { }^{0} R^{\rho}{ }_{\sigma \mu \nu} | | |
| 1510.06699_FO0917 | 49 | 1.000 | R \equiv R^{\mu \nu}{ }_{\mu \nu} | | |
| 1510.06699_FO0918 | 49 | 0.999 | { }^{0} R \equiv{ }^{0} R^{\mu \nu}{ }_{\mu \nu} | | |
| 1510.06699_FO0919 | 49 | 1.000 | L_{\mathrm{G}}=-R /(2 \kappa) | | |
| 1510.06699_FO0920 | 49 | 1.000 | T_{\mu \nu \sigma} | | |
| 1510.06699_FO0921 | 49 | 1.000 | T_{\mu \nu \lambda} | | |
| 1510.06699_FO0922 | 49 | 1.000 | \mathcal{R}=\mathcal{R}^{a b}{ }_{a b} | | |
| 1510.06699_FO0923 | 49 | 1.000 | \Lambda=\alpha_{i}=\beta_{i}=0 | | |
| 1510.06699_FO0924 | 49 | 0.983 | { }^{\underline{106}} | | |
| 1510.06699_FO0925 | 50 | 1.000 | \mathcal{T}_{a} \equiv \mathcal{T}^{c}{ }_{a c} | | |
| 1510.06699_FO0926 | 50 | 0.999 | \mathcal{A}^{a b}{ }_{c}=h_{c}{ }^{\mu} A^{a b}{ }_{\mu} | | |
| 1510.06699_FO0927 | 50 | 1.000 | \sigma_{a b}{ }^{c} \neq 0 | | |
| 1510.06699_FO0928 | 50 | 1.000 | \sigma_{a b c} | | |
| 1510.06699_FO0929 | 50 | 1.000 | \mathcal{T}^{c}{ }_{a b} | | |
| 1510.06699_FO0930 | 50 | 0.997 | \mu \phi \equiv m | | |
| 1510.06699_FO0931 | 50 | 1.000 | \mathcal{T}^{c}{ }_{a b}=2 \kappa h \sigma_{a b}{ }^{c} | | |
| 1510.06699_FO0932 | 50 | 1.000 | R_{\mu \nu} \equiv R^{\lambda}{ }_{\mu \lambda \nu} | | |
| 1510.06699_FO0933 | 50 | 1.000 | R \equiv R^{\mu}{ }_{\mu} | | |
| 1510.06699_FO0934 | 50 | 1.000 | \Gamma^{\lambda}{ }_{\mu \nu} | | |
| 1510.06699_FO0935 | 51 | 1.000 | \tau_{\mu \nu}= | | |
| 1510.06699_FO0936 | 51 | 1.000 | e^{a}{ }_{\mu} e^{b}{ }_{\nu} \tau_{a b} | | |
| 1510.06699_FO0937 | 51 | 1.000 | \sigma_{\mu \nu}{ }^{\lambda}=e^{a}{ }_{\mu} e^{b}{ }_{\nu} e_{c}{ }^{\lambda} \sigma_{a b}{ }^{c} | | |
| 1510.06699_FO0938 | 51 | 1.000 | \sigma_{\mu \nu}{ }^{\lambda} | | |
| 1510.06699_FO0939 | 51 | 1.000 | T^{\lambda}{ }_{\mu \nu} | | |
| 1510.06699_FO0940 | 51 | 1.000 | R_{\mu \nu} | | |
| 1510.06699_FO0941 | 51 | 1.000 | { }^{0} R_{\mu \nu} \equiv R_{\mu \nu}\left(V_{4}\right) | | |
| 1510.06699_FO0942 | 51 | 0.979 | { }^{\underline{108}} | | |
| 1510.06699_FO0943 | 51 | 1.000 | -\frac{1}{4} | | |
| 1510.06699_FO0944 | 51 | 1.000 | \phi^{4} | | |
| 1510.06699_FO0945 | 51 | 1.000 | L_{\varphi}(\varphi, \partial \varphi, h, A, B, \phi) | | |
| 1510.06699_FO0946 | 51 | 1.000 | \mathcal{L}_{T}=h^{-1} L_{T} | | |
| 1510.06699_FO0947 | 51 | 1.000 | L_{T} | | |
| 1510.06699_FO0948 | 51 | 0.993 | (a, \xi, \nu, \lambda) | | |
| 1510.06699_FO0949 | 51 | 1.000 | \phi^{-2} | | |
| 1510.06699_FO0950 | 51 | 0.967 | h_{a}{ }^{\mu}, A^{a b}{ }_{\mu}, B_{\mu} | | |
| 1510.06699_FO0951 | 51 | 1.000 | B_{\mu}, \phi | | |
| 1510.06699_FO0952 | 52 | 1.000 | \left(\tau_{\varphi}\right)^{a}{ }_{b} | | |
| 1510.06699_FO0953 | 52 | 1.000 | \left(\sigma_{\varphi}\right)_{a b}{ }^{c} | | |
| 1510.06699_FO0954 | 52 | 1.000 | \mathcal{D}_{a}^{*} \rightarrow \mathcal{D}_{a}, \mathcal{T}^{* c}{ }_{a b} \rightarrow \mathcal{T}^{c}{ }_{a b} | | |
| 1510.06699_FO0955 | 52 | 1.000 | \mathcal{T}_{a}^{*} \rightarrow \mathcal{T}_{a} | | |
| 1510.06699_FO0956 | 52 | 1.000 | \left(\zeta_{\varphi}\right)^{c} | | |
| 1510.06699_FO0957 | 52 | 1.000 | \left.\mathcal{D}_{a}^{*} \phi\right|_{\phi=\phi_{0}}=-\phi_{0} \mathcal{B}_{a} | | |
| 1510.06699_FO0958 | 52 | 1.000 | a=1 /\left(\kappa \phi_{0}^{2}\right) | | |
| 1510.06699_FO0959 | 52 | 1.000 | \Lambda=\lambda \phi_{0}^{2} / a=\kappa \lambda | | |
| 1510.06699_FO0960 | 52 | 1.000 | m^{2}=\nu \phi_{0}^{2} / \xi | | |
| 1510.06699_FO0961 | 53 | 1.000 | \mathcal{R}^{a b}{ }_{c d}, \mathcal{T}^{a}{ }_{b c}=\mathcal{T}^{* a}{ }_{b c}-\delta_{c}^{a} \mathcal{B}_{b}+\delta_{b}^{a} \mathcal{B}_{c} | | |
| 1510.06699_FO0962 | 53 | 1.000 | \left(\zeta_{\psi}\right)^{\mu}=0 | | |
| 1510.06699_FO0963 | 53 | 1.000 | \mathcal{T}_{a}=0 | | |
| 1510.06699_FO0964 | 53 | 1.000 | \tau_{\psi}=h^{-1} \mu \phi \bar{\psi} \psi | | |
| 1510.06699_FO0965 | 53 | 1.000 | m^{2} \equiv \nu \phi_{0}^{2} / \xi | | |
| 1510.06699_FO0966 | 53 | 1.000 | \mathcal{B}_{a} | | |
| 1510.06699_FO0967 | 53 | 1.000 | D_{\mu}^{*}=D_{\mu}+w B_{\mu} | | |
| 1510.06699_FO0968 | 54 | 1.000 | P_{\mu} \equiv \partial_{\mu} \rho | | |
| 1510.06699_FO0969 | 54 | 1.000 | (w=0) | | |
| 1510.06699_FO0970 | 54 | 1.000 | \mathcal{R}^{\dagger a b}{ }_{c d} \equiv h_{c}{ }^{\mu} h_{d}{ }^{\nu} R^{\dagger a b}{ }_{\mu \nu} | | |
| 1510.06699_FO0971 | 54 | 0.997 | D_{\mu}^{\natural} \varphi | | |
| 1510.06699_FO0972 | 54 | 1.000 | D_{\mu}^{\natural} | | |
| 1510.06699_FO0973 | 54 | 1.000 | \nu=\beta_{1}=\beta_{2}=0 | | |
| 1510.06699_FO0974 | 54 | 0.994 | \xi=\nu=\beta_{1}=\beta_{2}=0 | | |
| 1510.06699_FO0975 | 54 | 1.000 | \mathcal{D}_{a}^{\natural} \chi | | |
| 1510.06699_FO0976 | 54 | 1.000 | \mathcal{D}_{a}^{\dagger} \chi=h_{a}{ }^{\mu} D_{\mu}^{\dagger} \chi | | |
| 1510.06699_FO0977 | 54 | 0.991 | D_{\mu}^{\dagger} | | |
| 1510.06699_FO0978 | 54 | 0.997 | \left(U_{4}\right) | | |
| 1510.06699_FO0979 | 54 | 1.000 | \delta \varphi | | |
| 1510.06699_FO0980 | 54 | 1.000 | \left[\mathcal{D}_{c}, \mathcal{D}_{d}\right] \varphi \equiv \frac{1}{2} \mathcal{R}^{a b}{ }_{c d} \Sigma_{c d} \varphi-\mathcal{T}^{a}{ }_{c d} \mathcal{D}_{a} \varphi, \mathcal{R}^{a}{ }_{b} \equiv \mathcal{R}^{a c}{ }_{b c} | | |
| 1510.06699_FO0981 | 54 | 1.000 | \mathcal{T}_{a} \equiv \mathcal{T}^{b}{ }_{a b} | | |
| 1510.06699_FO0982 | 55 | 1.000 | \widehat{\mathcal{D}}_{a}^{*} | | |
| 1510.06699_FO0983 | 55 | 1.000 | \widehat{\mathcal{R}}^{a b}{ }_{c d} | | |
| 1510.06699_FO0991 | 55 | 0.926 | { }^{\mathrm{a}} | | |
| 1510.06699_FO0993 | 55 | 0.820 | { }^{\mathrm{a}}{ }^{\mathrm{b}} | | |
| 1510.06699_FO0994 | 55 | 0.666 | { }^{\text {b }} | | |
| 1510.06699_FO0995 | 55 | 0.957 | { }^{\mathrm{b}} | | |
| 1510.06699_FO1002 | 55 | 0.957 | \mathcal{T}^{a}{ }_{b c} \equiv 0 | | |
| 1510.06699_FO1003 | 55 | 0.998 | \mathcal{T}^{* a}{ }_{b c} \equiv 0 | | |
| 1510.06699_FO1004 | 55 | 1.000 | \mathcal{T}^{\dagger a}{ }_{b c} \equiv 0 | | |
| 1510.06699_FO1017 | 55 | 0.931 | { }^{\mathrm{c}} | | |
| 1510.06699_FO1018 | 55 | 0.562 | { }^{\text {c }} | | |
| 1510.06699_FO1019 | 55 | 0.999 | \mathcal{R}^{a}{ }_{b} \equiv \mathcal{R}^{a c}{ }_{b c}, \mathcal{R} \equiv \mathcal{R}^{a}{ }_{a} | | |
| 1510.06699_FO1020 | 55 | 0.999 | \mathcal{T}_{a}=\mathcal{T}^{b}{ }_{a b} | | |
| 1510.06699_FO1021 | 56 | 1.000 | S L(2, C) | | |
| 1510.06699_FO1022 | 56 | 1.000 | h^{\mu}{ }_{a} J_{\mu} \neq \mathcal{J}_{a} | | |
| 1510.06699_FO1023 | 56 | 1.000 | { }^{0} \mathcal{A}_{a b c} | | |
| 1510.06699_FO1024 | 56 | 1.000 | \mathcal{K}_{a b c} | | |
| 1510.06699_FO1025 | 56 | 1.000 | { }^{0} \mathcal{A}^{* a b}{ }_{c}= | | |
| 1510.06699_FO1026 | 56 | 1.000 | { }^{0} \mathcal{A}^{a b}{ }_{c}+\delta_{c}^{a} \mathcal{B}^{b}-\delta_{c}^{b} \mathcal{B}^{a} | | |
| 1510.06699_FO1027 | 56 | 1.000 | \mathcal{K}^{* a b}{ }_{c}=\mathcal{K}^{a b}{ }_{c}-\delta_{c}^{a} \mathcal{B}^{b}+\delta_{c}^{b} \mathcal{B}^{a} | | |
| 1510.06699_FO1028 | 56 | 1.000 | t^{a}{ }_{\mu} \equiv h \delta \mathcal{L}_{\mathrm{G}} / \delta h_{a}{ }^{\mu}, s_{a b}{ }^{\mu} \equiv | | |
| 1510.06699_FO1029 | 56 | 1.000 | h \delta \mathcal{L}_{\mathrm{G}} / \delta A^{a b}{ }_{\mu} | | |
| 1510.06699_FO1030 | 56 | 1.000 | j^{\mu} \equiv h \delta \mathcal{L}_{\mathrm{G}} / \delta B_{\mu} | | |
| 1510.06699_FO1031 | 56 | 1.000 | \dot{R} \equiv | | |
| 1510.06699_FO1032 | 56 | 1.000 | \dot{x}^{\mu} \partial_{\mu} R \rightarrow \dot{v}^{a} \mathcal{D}_{a}^{*} R | | |
| 1510.06699_FO1033 | 56 | 0.994 | { }^{77,78} | | |
| 1510.06699_FO1034 | 56 | 0.999 | \bar{\psi} \gamma^{a}{ }^{0} \stackrel{\leftrightarrow}{\mathcal{D}}_{a}^{*} \psi=\bar{\psi} \gamma^{a}{ }^{0} \stackrel{\leftrightarrow}{\mathcal{D}}_{a} \psi | | |
| 1510.06699_FO1035 | 56 | 1.000 | \theta(x) | | |
| 1510.06699_FO1036 | 57 | 1.000 | D_{\mu}^{\dagger} \varphi= | | |
| 1510.06699_FO1037 | 57 | 1.000 | \left[D_{\mu}+\frac{1}{2}\left(\mathcal{V}^{a} b^{b}{ }_{\mu}-\mathcal{V}^{b} b^{a}{ }_{\mu}\right) \Sigma_{a b}-w V_{\mu}-\frac{1}{3} w T_{\mu}\right] \varphi | | |
| 1510.06699_FO1038 | 57 | 1.000 | D_{\mu}^{*} \varphi=\left(D_{\mu}+w B_{\mu}\right) \varphi | | |
| 1510.06699_FO1039 | 57 | 0.995 | { }^{0} \mathcal{A}^{\dagger a b}{ }_{c}={ }^{0} \mathcal{A}^{a b}{ }_{c}-\delta_{c}^{a}\left(\mathcal{V}^{b}+\frac{1}{3} \mathcal{T}^{b}\right)+\delta_{c}^{b}\left(\mathcal{V}^{a}+\right. | | |
| 1510.06699_FO1040 | 57 | 0.600 | \frac{1}{3} \mathcal{T}^{a} | | |
| 1510.06699_FO1041 | 57 | 0.600 | \mathcal{K}^{\dagger a b}{ }_{c}=\mathcal{K}^{a b}{ }_{c}+\frac{1}{3} \delta_{c}^{a} \mathcal{T}^{b}-\frac{1}{3} \delta_{c}^{b} \mathcal{T}^{a} | | |
| 1510.06699_FO1042 | 57 | 0.965 | \bar{\psi} \gamma^{a}{ }^{0} \mathcal{D}_{a}^{\dagger} \psi=\bar{\psi} \gamma^{a}{ }^{0} \stackrel{\leftrightarrow}{\mathcal{D}}_{a} \psi | | |
| 1510.06699_FO1043 | 57 | 1.000 | \nabla_{\sigma} g_{\mu \nu}= | | |
| 1510.06699_FO1044 | 57 | 1.000 | -\frac{1}{2}\left(\Gamma^{\lambda}{ }_{\lambda \sigma}-{ }^{0} \Gamma^{\lambda}{ }_{\lambda \sigma}\right) g_{\mu \nu} | | |
| 1510.06699_FO1045 | 57 | 1.000 | L_{\mathcal{R}^{2}}= | | |
| 1510.06699_FO1046 | 57 | 1.000 | \alpha_{1} \mathcal{R}^{\dagger 2}+\alpha_{2}^{\prime} \mathcal{R}_{(a b)}^{\dagger} \mathcal{R}^{\dagger(a b)}+\alpha_{3}^{\prime} \mathcal{R}_{[a b]}^{\dagger} \mathcal{R}^{\dagger[a b]}+\alpha_{4}^{\prime} \mathcal{R}_{a(b c) d}^{\dagger} \mathcal{R}^{\dagger a(b c) d}+ | | |
| 1510.06699_FO1047 | 57 | 1.000 | \alpha_{5}^{\prime} \mathcal{R}_{a[b c] d}^{\dagger} \mathcal{R}^{\dagger a[b c] d}+\alpha_{6} \mathcal{R}_{a b c d}^{\dagger} \mathcal{R}^{\dagger c d a b} | | |
| 1510.06699_FO1048 | 57 | 0.994 | \alpha_{2}^{\prime}=\alpha_{2}+\alpha_{3}, \alpha_{3}^{\prime}=\alpha_{2}-\alpha_{3}, \alpha_{4}^{\prime}=\alpha_{4}+\alpha_{5} | | |
| 1510.06699_FO1049 | 57 | 0.994 | \alpha_{5}^{\prime}=\alpha_{4}-\alpha_{5} | | |
| 1510.06699_FO1050 | 57 | 1.000 | \alpha_{2}^{\prime}=\alpha_{3}^{\prime} | | |
| 1510.06699_FO1051 | 57 | 0.999 | L_{\mathcal{T}^{2}}=\beta_{1}^{\prime} \mathcal{T}_{(a b) c}^{\dagger} \mathcal{T}^{\dagger(a b) c}+\beta_{2}^{\prime} \mathcal{T}_{[a b] c}^{\dagger} \mathcal{T}^{\dagger[a b] c} | | |
| 1510.06699_FO1052 | 57 | 0.998 | \beta_{1}^{\prime}=\beta_{1}+\beta_{2} | | |
| 1510.06699_FO1053 | 57 | 0.998 | \beta_{2}^{\prime}=\beta_{1}-\beta_{2} | | |
| 1510.06699_FO1054 | 57 | 1.000 | S_{\mathrm{T}}=S_{\mathrm{G}}+S_{\mathrm{M}} | | |
| 1510.06699_FO1055 | 57 | 0.999 | { }^{0} \mathcal{R}^{* a b}{ }_{c d}={ }^{0} \mathcal{R}^{a b}{ }_{c d}-2 \delta_{d}^{[b}\left({ }^{0} \mathcal{D}_{c}-\mathcal{B}_{c}\right) \mathcal{B}^{a]}+ | | |
| 1510.06699_FO1056 | 57 | 1.000 | 2 \delta_{c}^{[b}\left({ }^{0} \mathcal{D}_{d}-\mathcal{B}_{d}\right) \mathcal{B}^{a]}-2 \mathcal{B}^{e} \mathcal{B}_{e} \delta_{c}^{[a} \delta_{d}^{b]} | | |
| 1510.06699_FO1057 | 57 | 1.000 | { }^{0} \mathcal{R}^{* a}{ }_{c}={ }^{0} \mathcal{R}^{a}{ }_{c}-2\left({ }^{0} \mathcal{D}_{c}-\mathcal{B}_{c}\right) \mathcal{B}^{a}- | | |
| 1510.06699_FO1058 | 57 | 1.000 | \left({ }^{0} \mathcal{D}_{e}+2 \mathcal{B}_{e}\right) \mathcal{B}^{e} \delta_{c}^{a} | | |
| 1510.06699_FO1059 | 57 | 1.000 | { }^{0} \mathcal{R}^{*}={ }^{0} \mathcal{R}-6\left({ }^{0} \mathcal{D}_{e}+\mathcal{B}_{e}\right) \mathcal{B}^{e} | | |
| 1510.06699_FO1060 | 57 | 0.996 | { }^{0} \mathcal{R}^{* a b}{ }_{c d} \rightarrow{ }^{0} \mathcal{R}^{\dagger a b}{ }_{c d} | | |
| 1510.06699_FO1061 | 57 | 0.996 | \mathcal{B}_{a} \rightarrow-\left(\mathcal{V}_{a}+\frac{1}{3} \mathcal{T}_{a}\right) | | |
| 1510.06699_FO1062 | 57 | 1.000 | { }^{0} \mathcal{R}^{*} | |