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 |
|---|---|---|---|---|---|---|---|---|---|
| 46259 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ \phi_1\tilde{q}_1^2$ + $ M_4q_1\tilde{q}_2$ | 0.6617 | 0.8086 | 0.8182 | [X:[], M:[1.1019, 0.6944, 1.1019, 0.9956], q:[0.4743, 0.4239], qb:[0.7755, 0.5301], phi:[0.4491]] | [X:[], M:[[0, 4], [0, -12], [0, 4], [1, -7]], q:[[-1, -4], [1, 0]], qb:[[0, 1], [0, 11]], phi:[[0, -2]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ q_2\tilde{q}_2$, $ M_4$, $ M_1$, $ M_3$, $ q_2\tilde{q}_1$, $ q_1\tilde{q}_1$, $ \phi_1q_2^2$, $ \phi_1q_1q_2$, $ M_2^2$, $ \phi_1q_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_1$, $ M_2M_4$, $ M_1M_2$, $ M_2M_3$, $ q_2^2\tilde{q}_2^2$, $ M_4^2$, $ M_2\phi_1q_2^2$ | . | -3 | t^2.08 + t^2.86 + t^2.99 + 2*t^3.31 + t^3.6 + t^3.75 + t^3.89 + t^4.04 + t^4.17 + t^4.19 + t^4.21 + t^4.36 + t^4.53 + t^4.95 + t^5.07 + 2*t^5.39 + t^5.72 + 2*t^5.97 - 3*t^6. + t^6.12 - t^6.15 + t^6.17 + t^6.25 + t^6.28 + 2*t^6.29 - t^6.32 + t^6.46 + t^6.58 + 3*t^6.61 + t^6.75 + t^6.88 + t^6.9 + t^7.03 + t^7.05 + t^7.07 + t^7.15 + 2*t^7.2 + t^7.35 + t^7.39 + 2*t^7.47 + t^7.49 + t^7.5 + t^7.51 + t^7.64 + t^7.78 + t^7.79 + t^7.81 + t^7.83 + t^7.93 + t^7.94 + 2*t^8.06 - 2*t^8.08 + t^8.1 + t^8.21 + t^8.25 + t^8.33 + t^8.36 + 2*t^8.38 + t^8.39 - t^8.4 + t^8.42 + t^8.55 + t^8.59 + 2*t^8.69 + t^8.72 + t^8.74 + t^8.84 - 3*t^8.86 + t^8.89 + 2*t^8.96 - 3*t^8.99 - t^4.35/y - t^6.43/y + t^7.04/y - t^7.33/y + t^7.36/y - t^7.65/y + t^7.95/y + t^8.07/y + t^8.26/y + (2*t^8.39)/y - t^8.51/y + t^8.68/y + t^8.83/y + t^8.85/y + t^8.97/y - t^4.35*y - t^6.43*y + t^7.04*y - t^7.33*y + t^7.36*y - t^7.65*y + t^7.95*y + t^8.07*y + t^8.26*y + 2*t^8.39*y - t^8.51*y + t^8.68*y + t^8.83*y + t^8.85*y + t^8.97*y | t^2.08/g2^12 + g1*g2^11*t^2.86 + (g1*t^2.99)/g2^7 + 2*g2^4*t^3.31 + g1*g2*t^3.6 + t^3.75/(g1*g2^3) + (g1^2*t^3.89)/g2^2 + t^4.04/g2^6 + t^4.17/g2^24 + t^4.19/(g1^2*g2^10) + g1*g2^9*t^4.21 + (g2^5*t^4.36)/g1 + g2^20*t^4.53 + (g1*t^4.95)/g2 + (g1*t^5.07)/g2^19 + (2*t^5.39)/g2^8 + g1^2*g2^22*t^5.72 + (2*g1^2*t^5.97)/g2^14 - 3*t^6. + t^6.12/g2^18 - t^6.15/(g1^2*g2^4) + g1*g2^15*t^6.17 + t^6.25/g2^36 + t^6.28/(g1^2*g2^22) + (2*g1*t^6.29)/g2^3 - (g2^11*t^6.32)/g1 + g1^2*g2^12*t^6.46 + (g1^2*t^6.58)/g2^6 + 3*g2^8*t^6.61 + g1^3*g2^9*t^6.75 + (g1^3*t^6.88)/g2^9 + g1*g2^5*t^6.9 + (g1*t^7.03)/g2^13 + (g2*t^7.05)/g1 + g1^2*g2^20*t^7.07 + (g1*t^7.15)/g2^31 + 2*g1^2*g2^2*t^7.2 + t^7.35/g2^2 + g1*g2^31*t^7.39 + (2*t^7.47)/g2^20 + (g1^3*t^7.49)/g2 + t^7.5/(g1^2*g2^6) + g1*g2^13*t^7.51 + (g1*t^7.64)/g2^5 + (g1^4*t^7.78)/g2^4 + t^7.79/(g1*g2^9) + g1^2*g2^10*t^7.81 + g2^24*t^7.83 + (g1^2*t^7.93)/g2^8 + t^7.94/(g1^3*g2^13) + (2*g1^2*t^8.06)/g2^26 - (2*t^8.08)/g2^12 + g1^3*g2^7*t^8.1 + t^8.21/g2^30 + g1*g2^3*t^8.25 + t^8.33/g2^48 + t^8.36/(g1^2*g2^34) + (2*g1*t^8.38)/g2^15 + t^8.39/(g1^4*g2^20) - t^8.4/(g1*g2) + g1^2*g2^18*t^8.42 + t^8.55/(g1^3*g2^5) + g1^3*g2^33*t^8.59 + (2*t^8.69)/g2^4 + (g2^10*t^8.72)/g1^2 + g1*g2^29*t^8.74 + (g1^3*t^8.84)/g2^3 - 3*g1*g2^11*t^8.86 + (g2^25*t^8.89)/g1 + (2*g1^3*t^8.96)/g2^21 - (3*g1*t^8.99)/g2^7 - t^4.35/(g2^2*y) - t^6.43/(g2^14*y) + t^7.04/(g2^6*y) - (g1*t^7.33)/(g2^9*y) + (g2^5*t^7.36)/(g1*y) - (g2^2*t^7.65)/y + (g1*t^7.95)/(g2*y) + (g1*t^8.07)/(g2^19*y) + (g2^10*t^8.26)/y + (2*t^8.39)/(g2^8*y) - t^8.51/(g2^26*y) + (g1*t^8.68)/(g2^11*y) + t^8.83/(g1*g2^15*y) + (g1^2*g2^4*t^8.85)/y + (g1^2*t^8.97)/(g2^14*y) - (t^4.35*y)/g2^2 - (t^6.43*y)/g2^14 + (t^7.04*y)/g2^6 - (g1*t^7.33*y)/g2^9 + (g2^5*t^7.36*y)/g1 - g2^2*t^7.65*y + (g1*t^7.95*y)/g2 + (g1*t^8.07*y)/g2^19 + g2^10*t^8.26*y + (2*t^8.39*y)/g2^8 - (t^8.51*y)/g2^26 + (g1*t^8.68*y)/g2^11 + (t^8.83*y)/(g1*g2^15) + g1^2*g2^4*t^8.85*y + (g1^2*t^8.97*y)/g2^14 |
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 |
|---|
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46040 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3\phi_1^2$ + $ \phi_1\tilde{q}_1^2$ | 0.6636 | 0.8114 | 0.8179 | [X:[], M:[1.0903, 0.7292, 1.0903], q:[0.4549, 0.4549], qb:[0.7726, 0.4983], phi:[0.4549]] | t^2.19 + 2*t^2.86 + 2*t^3.27 + 2*t^3.68 + 3*t^4.09 + 2*t^4.22 + t^4.35 + t^4.38 + 2*t^5.05 + 2*t^5.46 + 3*t^5.72 - 5*t^6. - t^4.36/y - t^4.36*y | detail |