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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5970 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_5M_6$ + $ M_7q_1\tilde{q}_1$ + $ M_8\phi_1q_2^2$ + $ M_9q_1\tilde{q}_2$ | 0.6351 | 0.8273 | 0.7677 | [X:[], M:[0.9627, 1.112, 1.0373, 0.888, 0.7407, 1.2593, 0.8153, 0.888, 0.8153], q:[0.7407, 0.2966], qb:[0.444, 0.444], phi:[0.5187]] | [X:[], M:[[4], [-12], [-4], [12], [1], [-1], [-7], [12], [-7]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ M_7$, $ M_9$, $ M_4$, $ M_8$, $ M_3$, $ \phi_1^2$, $ M_6$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_1^2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ \phi_1q_1q_2$, $ M_7q_2\tilde{q}_1$, $ M_9q_2\tilde{q}_1$, $ M_7q_2\tilde{q}_2$, $ M_9q_2\tilde{q}_2$, $ M_7^2$, $ M_7M_9$, $ M_9^2$, $ M_4q_2\tilde{q}_1$, $ M_8q_2\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ M_8q_2\tilde{q}_2$, $ M_4M_7$, $ M_7M_8$, $ M_4M_9$, $ M_8M_9$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_4^2$, $ M_4M_8$, $ M_8^2$, $ M_3M_7$, $ M_3M_9$, $ M_7\phi_1^2$, $ M_9\phi_1^2$, $ M_3M_4$, $ M_3M_8$, $ M_4\phi_1^2$, $ M_8\phi_1^2$ | $M_6q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_2$, $ \phi_1q_2^2\tilde{q}_2^2$ | -2 | 2*t^2.22 + 2*t^2.45 + 2*t^2.66 + 2*t^3.11 + 2*t^3.78 + 3*t^4.22 + 3*t^4.44 + 4*t^4.67 + 7*t^4.89 + 4*t^5.11 + 7*t^5.33 + 2*t^5.56 + 3*t^5.78 - 2*t^6. + 5*t^6.22 + 6*t^6.44 + 6*t^6.67 + 6*t^6.88 + 6*t^6.89 + 7*t^7.11 + 9*t^7.33 + 4*t^7.34 + 6*t^7.55 + 7*t^7.56 + 4*t^7.77 + 4*t^7.78 + 4*t^7.99 + 8*t^8. - 4*t^8.22 + 9*t^8.44 - 2*t^8.45 - 3*t^8.66 + 4*t^8.67 + 10*t^8.89 - t^4.56/y - (2*t^7.)/y - t^7.22/y + (2*t^7.44)/y + (3*t^7.67)/y + (6*t^7.89)/y + (6*t^8.11)/y + (5*t^8.33)/y + (4*t^8.56)/y + (4*t^8.78)/y - t^4.56*y - 2*t^7.*y - t^7.22*y + 2*t^7.44*y + 3*t^7.67*y + 6*t^7.89*y + 6*t^8.11*y + 5*t^8.33*y + 4*t^8.56*y + 4*t^8.78*y | 2*g1*t^2.22 + (2*t^2.45)/g1^7 + 2*g1^12*t^2.66 + (2*t^3.11)/g1^4 + (2*t^3.78)/g1 + 3*g1^10*t^4.22 + 3*g1^2*t^4.44 + (4*t^4.67)/g1^6 + (3*t^4.89)/g1^14 + 4*g1^13*t^4.89 + 4*g1^5*t^5.11 + (4*t^5.33)/g1^3 + 3*g1^24*t^5.33 + (2*t^5.56)/g1^11 + 3*g1^8*t^5.78 - 2*t^6. + (5*t^6.22)/g1^8 + 6*g1^11*t^6.44 + 6*g1^3*t^6.67 + 6*g1^22*t^6.88 + (6*t^6.89)/g1^5 + (4*t^7.11)/g1^13 + 3*g1^14*t^7.11 + 9*g1^6*t^7.33 + (4*t^7.34)/g1^21 + 6*g1^25*t^7.55 + (7*t^7.56)/g1^2 + 4*g1^17*t^7.77 + (4*t^7.78)/g1^10 + 4*g1^36*t^7.99 + (2*t^8.)/g1^18 + 6*g1^9*t^8. - 4*g1*t^8.22 + 9*g1^20*t^8.44 - (2*t^8.45)/g1^7 - 3*g1^12*t^8.66 + (4*t^8.67)/g1^15 + 10*g1^4*t^8.89 - t^4.56/(g1^2*y) - (2*t^7.)/(g1^9*y) - (g1^10*t^7.22)/y + (2*g1^2*t^7.44)/y + (3*t^7.67)/(g1^6*y) + (2*t^7.89)/(g1^14*y) + (4*g1^13*t^7.89)/y + (6*g1^5*t^8.11)/y + (4*t^8.33)/(g1^3*y) + (g1^24*t^8.33)/y + (4*t^8.56)/(g1^11*y) + (4*g1^8*t^8.78)/y - (t^4.56*y)/g1^2 - (2*t^7.*y)/g1^9 - g1^10*t^7.22*y + 2*g1^2*t^7.44*y + (3*t^7.67*y)/g1^6 + (2*t^7.89*y)/g1^14 + 4*g1^13*t^7.89*y + 6*g1^5*t^8.11*y + (4*t^8.33*y)/g1^3 + g1^24*t^8.33*y + (4*t^8.56*y)/g1^11 + 4*g1^8*t^8.78*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 |
---|---|---|---|---|---|---|---|---|---|
4471 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\phi_1q_2\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_5M_6$ + $ M_7q_1\tilde{q}_1$ + $ M_8\phi_1q_2^2$ | 0.62 | 0.8023 | 0.7727 | [X:[], M:[0.9554, 1.1337, 1.0446, 0.8663, 0.7389, 1.2611, 0.828, 0.8663], q:[0.7389, 0.3057], qb:[0.4331, 0.4331], phi:[0.5223]] | 2*t^2.22 + t^2.48 + 2*t^2.6 + 2*t^3.13 + t^3.52 + 2*t^3.78 + 3*t^4.17 + 3*t^4.43 + 2*t^4.7 + 4*t^4.82 + t^4.97 + 2*t^5.08 + 3*t^5.2 + 4*t^5.35 + 5*t^5.73 - t^6. - t^4.57/y - t^4.57*y | detail |