Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
---|---|---|---|---|---|---|---|---|---|
47080 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ q_2\tilde{q}_1$ + $ M_2X_1$ + $ \phi_1^2X_2$ + $ M_3M_5$ | 0.4697 | 0.5539 | 0.8481 | [X:[1.6534, 1.4286], M:[0.8571, 0.3466, 1.1429, 0.7962, 0.8571], q:[0.3981, 0.7447], qb:[1.2553, 0.459], phi:[0.2857]] | [X:[[2], [0]], M:[[0], [-2], [0], [2], [0]], q:[[1], [-1]], qb:[[1], [-1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
$M_4$, $ M_1$, $ M_5$, $ \phi_1q_1^2$, $ \phi_1q_1q_2$, $ X_2$, $ M_4^2$, $ M_1M_4$, $ M_4M_5$, $ X_1$, $ M_1^2$, $ M_1M_5$, $ M_5^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_4\phi_1q_1^2$, $ M_5\phi_1q_1^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4\phi_1q_1\tilde{q}_2$ | $M_5\phi_1q_1\tilde{q}_2$, $ M_4\phi_1\tilde{q}_2^2$ | -2 | t^2.39 + 2*t^2.57 + t^3.25 + t^4.29 + t^4.78 + 2*t^4.96 + 3*t^5.14 + t^5.63 + t^5.82 - 2*t^6. - t^6.18 + t^6.49 - t^7.04 + t^7.17 + 2*t^7.35 + 3*t^7.53 + 3*t^7.71 - t^7.9 + t^8.02 + t^8.21 - t^8.39 - 4*t^8.57 - 2*t^8.75 + t^8.88 - t^3.86/y - t^6.25/y - t^6.43/y + t^7.29/y + t^7.47/y + (2*t^7.96)/y + t^8.14/y + t^8.82/y - t^3.86*y - t^6.25*y - t^6.43*y + t^7.29*y + t^7.47*y + 2*t^7.96*y + t^8.14*y + t^8.82*y | g1^2*t^2.39 + 2*t^2.57 + g1^2*t^3.25 + t^4.29 + g1^4*t^4.78 + 2*g1^2*t^4.96 + 3*t^5.14 + g1^4*t^5.63 + g1^2*t^5.82 - 2*t^6. - t^6.18/g1^2 + g1^4*t^6.49 - t^7.04/g1^2 + g1^6*t^7.17 + 2*g1^4*t^7.35 + 3*g1^2*t^7.53 + 3*t^7.71 - t^7.9/g1^2 + g1^6*t^8.02 + g1^4*t^8.21 - g1^2*t^8.39 - 4*t^8.57 - (2*t^8.75)/g1^2 + g1^6*t^8.88 - t^3.86/y - (g1^2*t^6.25)/y - t^6.43/y + t^7.29/y + t^7.47/(g1^2*y) + (2*g1^2*t^7.96)/y + t^8.14/y + (g1^2*t^8.82)/y - t^3.86*y - g1^2*t^6.25*y - t^6.43*y + t^7.29*y + (t^7.47*y)/g1^2 + 2*g1^2*t^7.96*y + t^8.14*y + g1^2*t^8.82*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
46635 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_1\tilde{q}_2$ + $ q_2\tilde{q}_1$ + $ M_2X_1$ + $ \phi_1^2X_2$ | 0.4572 | 0.5324 | 0.8587 | [X:[1.6534, 1.4286], M:[0.8571, 0.3466, 1.1429, 0.7962], q:[0.3981, 0.7447], qb:[1.2553, 0.459], phi:[0.2857]] | t^2.39 + t^2.57 + t^3.25 + t^3.43 + t^4.29 + t^4.78 + t^4.96 + t^5.14 + t^5.63 + t^5.82 - t^6. - t^3.86/y - t^3.86*y | detail |