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 |
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56950 | 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}_2^2$ + $ M_5\phi_1q_1q_2$ + $ M_5q_2\tilde{q}_1$ + $ M_1M_6$ + $ M_7q_2\tilde{q}_1$ | 0.6921 | 0.8823 | 0.7845 | [X:[], M:[1.1575, 0.885, 0.8425, 0.715, 0.7575, 0.8425, 0.7575], q:[0.3575, 0.485], qb:[0.7575, 0.8], phi:[0.4]] | [X:[], M:[[1], [-2], [-1], [2], [1], [-1], [1]], q:[[1], [-2]], qb:[[1], [0]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_4$, $ M_5$, $ M_7$, $ \phi_1^2$, $ M_3$, $ M_6$, $ M_2$, $ \phi_1q_1^2$, $ \phi_1q_2^2$, $ M_4^2$, $ M_4M_5$, $ M_4M_7$, $ M_5^2$, $ M_5M_7$, $ M_7^2$, $ M_4\phi_1^2$, $ \phi_1q_1\tilde{q}_1$, $ M_3M_4$, $ M_4M_6$, $ M_5\phi_1^2$, $ M_7\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ M_2M_4$, $ M_3M_5$, $ M_5M_6$, $ M_3M_7$, $ M_6M_7$, $ \phi_1^4$, $ M_2M_5$, $ M_2M_7$, $ M_3\phi_1^2$, $ M_6\phi_1^2$, $ \phi_1q_2\tilde{q}_1$, $ M_3^2$, $ M_3M_6$, $ M_6^2$, $ M_2\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_2M_3$, $ M_2M_6$, $ M_2^2$, $ M_4\phi_1q_1^2$, $ M_5\phi_1q_1^2$, $ M_7\phi_1q_1^2$, $ \phi_1^3q_1^2$, $ \phi_1\tilde{q}_1^2$, $ M_6\phi_1q_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$ | . | -3 | t^2.15 + 2*t^2.27 + t^2.4 + 2*t^2.53 + t^2.65 + t^3.35 + t^4.11 + t^4.29 + 2*t^4.42 + 5*t^4.55 + 5*t^4.67 + 5*t^4.8 + 5*t^4.93 + 4*t^5.05 + t^5.18 + t^5.31 + t^5.49 + t^5.62 + 2*t^5.75 + t^5.87 - 3*t^6. - t^6.13 + t^6.44 + t^6.51 + 2*t^6.56 + 2*t^6.64 + 6*t^6.69 + t^6.76 + 9*t^6.82 + 9*t^6.95 + 12*t^7.07 + 11*t^7.2 + 9*t^7.33 + 8*t^7.45 + 6*t^7.58 + t^7.64 + t^7.71 + t^7.76 + t^7.84 + 4*t^7.89 + t^7.96 + 3*t^8.02 - 3*t^8.15 + t^8.22 - 6*t^8.27 - 6*t^8.4 - 10*t^8.53 + t^8.58 - 5*t^8.65 + 2*t^8.71 - t^8.78 + 6*t^8.84 + t^8.91 + 10*t^8.96 - t^4.2/y - t^6.35/y - (2*t^6.47)/y - t^6.6/y - t^6.73/y - t^6.85/y + (2*t^7.42)/y + (3*t^7.55)/y + (5*t^7.67)/y + (6*t^7.8)/y + (6*t^7.93)/y + (3*t^8.05)/y + (2*t^8.18)/y - (3*t^8.75)/y - t^8.87/y - t^4.2*y - t^6.35*y - 2*t^6.47*y - t^6.6*y - t^6.73*y - t^6.85*y + 2*t^7.42*y + 3*t^7.55*y + 5*t^7.67*y + 6*t^7.8*y + 6*t^7.93*y + 3*t^8.05*y + 2*t^8.18*y - 3*t^8.75*y - t^8.87*y | g1^2*t^2.15 + 2*g1*t^2.27 + t^2.4 + (2*t^2.53)/g1 + t^2.65/g1^2 + g1^2*t^3.35 + t^4.11/g1^4 + g1^4*t^4.29 + 2*g1^3*t^4.42 + 5*g1^2*t^4.55 + 5*g1*t^4.67 + 5*t^4.8 + (5*t^4.93)/g1 + (4*t^5.05)/g1^2 + t^5.18/g1^3 + t^5.31/g1^4 + g1^4*t^5.49 + g1^3*t^5.62 + 2*g1^2*t^5.75 + g1*t^5.87 - 3*t^6. - t^6.13/g1 + g1^6*t^6.44 + t^6.51/g1^4 + 2*g1^5*t^6.56 + (2*t^6.64)/g1^5 + 6*g1^4*t^6.69 + t^6.76/g1^6 + 9*g1^3*t^6.82 + 9*g1^2*t^6.95 + 12*g1*t^7.07 + 11*t^7.2 + (9*t^7.33)/g1 + (8*t^7.45)/g1^2 + (6*t^7.58)/g1^3 + g1^6*t^7.64 + t^7.71/g1^4 + g1^5*t^7.76 + t^7.84/g1^5 + 4*g1^4*t^7.89 + t^7.96/g1^6 + 3*g1^3*t^8.02 - 3*g1^2*t^8.15 + t^8.22/g1^8 - 6*g1*t^8.27 - 6*t^8.4 - (10*t^8.53)/g1 + g1^8*t^8.58 - (5*t^8.65)/g1^2 + 2*g1^7*t^8.71 - t^8.78/g1^3 + 6*g1^6*t^8.84 + t^8.91/g1^4 + 10*g1^5*t^8.96 - t^4.2/y - (g1^2*t^6.35)/y - (2*g1*t^6.47)/y - t^6.6/y - t^6.73/(g1*y) - t^6.85/(g1^2*y) + (2*g1^3*t^7.42)/y + (3*g1^2*t^7.55)/y + (5*g1*t^7.67)/y + (6*t^7.8)/y + (6*t^7.93)/(g1*y) + (3*t^8.05)/(g1^2*y) + (2*t^8.18)/(g1^3*y) - (3*g1^2*t^8.75)/y - (g1*t^8.87)/y - t^4.2*y - g1^2*t^6.35*y - 2*g1*t^6.47*y - t^6.6*y - (t^6.73*y)/g1 - (t^6.85*y)/g1^2 + 2*g1^3*t^7.42*y + 3*g1^2*t^7.55*y + 5*g1*t^7.67*y + 6*t^7.8*y + (6*t^7.93*y)/g1 + (3*t^8.05*y)/g1^2 + (2*t^8.18*y)/g1^3 - 3*g1^2*t^8.75*y - g1*t^8.87*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 |
---|---|---|---|---|---|---|---|---|---|
55347 | 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}_2^2$ + $ M_5\phi_1q_1q_2$ + $ M_5q_2\tilde{q}_1$ + $ M_1M_6$ | 0.6735 | 0.8485 | 0.7937 | [X:[], M:[1.1608, 0.8784, 0.8392, 0.7216, 0.7608, 0.8392], q:[0.3608, 0.4784], qb:[0.7608, 0.8], phi:[0.4]] | t^2.16 + t^2.28 + t^2.4 + 2*t^2.52 + t^2.64 + t^3.36 + t^3.72 + t^4.07 + t^4.33 + t^4.45 + 3*t^4.56 + 4*t^4.68 + 3*t^4.8 + 4*t^4.92 + 4*t^5.04 + t^5.15 + t^5.27 + t^5.53 + 2*t^5.76 + 2*t^5.88 - 2*t^6. - t^4.2/y - t^4.2*y | detail |