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 |
|---|---|---|---|---|---|---|---|---|---|
| 45893 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ | 0.6485 | 0.7962 | 0.8145 | [X:[], M:[0.7041, 0.6924], q:[0.4778, 0.8181], qb:[0.8298, 0.4661], phi:[0.352]] | [X:[], M:[[-2, -2], [-5, -1]], q:[[3, 1], [-1, 1]], qb:[[2, 0], [0, 2]], phi:[[-1, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ M_1$, $ \phi_1^2$, $ q_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_1\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_1^2$, $ M_2^2$, $ M_1M_2$, $ M_2\phi_1^2$, $ M_1^2$, $ M_1\phi_1^2$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_1q_2$, $ q_2\tilde{q}_1$, $ \phi_1^2q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_1^2\tilde{q}_2^2$, $ M_2q_2\tilde{q}_2$, $ M_2\phi_1\tilde{q}_2^2$, $ \phi_1q_2^2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ M_1\phi_1\tilde{q}_2^2$, $ \phi_1^3\tilde{q}_2^2$ | $\phi_1^3q_1\tilde{q}_2$, $ M_1\tilde{q}_1\tilde{q}_2$ | 0 | t^2.08 + 2*t^2.11 + t^2.83 + 2*t^3.85 + 2*t^3.89 + t^3.92 + t^4.15 + 2*t^4.19 + 3*t^4.22 + t^4.91 + 3*t^4.94 + t^5.66 + 2*t^5.93 + 4*t^5.96 + t^6.23 + 2*t^6.27 + 3*t^6.3 + 4*t^6.34 + 2*t^6.68 + 2*t^6.72 + t^6.75 + t^6.99 + t^7.02 + t^7.06 - 2*t^7.09 + 3*t^7.71 + 3*t^7.74 + 3*t^7.78 + t^7.85 + 2*t^8.01 + 4*t^8.04 + 2*t^8.08 - 3*t^8.11 - t^8.15 + t^8.31 + 2*t^8.34 + 3*t^8.38 + 4*t^8.41 + 5*t^8.45 + t^8.5 + 2*t^8.76 + 4*t^8.8 - 2*t^8.83 - t^8.87 - t^4.06/y - t^6.13/y - (2*t^6.17)/y + (2*t^7.19)/y + t^7.22/y + t^7.91/y + (4*t^7.94)/y + t^7.98/y - t^8.21/y - (2*t^8.25)/y - (3*t^8.28)/y + (2*t^8.93)/y + (6*t^8.96)/y - t^4.06*y - t^6.13*y - 2*t^6.17*y + 2*t^7.19*y + t^7.22*y + t^7.91*y + 4*t^7.94*y + t^7.98*y - t^8.21*y - 2*t^8.25*y - 3*t^8.28*y + 2*t^8.93*y + 6*t^8.96*y | t^2.08/(g1^5*g2) + (2*t^2.11)/(g1^2*g2^2) + g1^3*g2^3*t^2.83 + (2*g2^3*t^3.85)/g1 + 2*g1^2*g2^2*t^3.89 + g1^5*g2*t^3.92 + t^4.15/(g1^10*g2^2) + (2*t^4.19)/(g1^7*g2^3) + (3*t^4.22)/(g1^4*g2^4) + (g2^2*t^4.91)/g1^2 + 3*g1*g2*t^4.94 + g1^6*g2^6*t^5.66 + (2*g2^2*t^5.93)/g1^6 + (4*g2*t^5.96)/g1^3 + t^6.23/(g1^15*g2^3) + (2*t^6.27)/(g1^12*g2^4) + (3*t^6.3)/(g1^9*g2^5) + (4*t^6.34)/(g1^6*g2^6) + 2*g1^2*g2^6*t^6.68 + 2*g1^5*g2^5*t^6.72 + g1^8*g2^4*t^6.75 + (g2*t^6.99)/g1^7 + t^7.02/g1^4 + t^7.06/(g1*g2) - (2*g1^2*t^7.09)/g2^2 + (3*g2^6*t^7.71)/g1^2 + 3*g1*g2^5*t^7.74 + 3*g1^4*g2^4*t^7.78 + g1^10*g2^2*t^7.85 + (2*g2*t^8.01)/g1^11 + (4*t^8.04)/g1^8 + (2*t^8.08)/(g1^5*g2) - (3*t^8.11)/(g1^2*g2^2) - (g1*t^8.15)/g2^3 + t^8.31/(g1^20*g2^4) + (2*t^8.34)/(g1^17*g2^5) + (3*t^8.38)/(g1^14*g2^6) + (4*t^8.41)/(g1^11*g2^7) + (5*t^8.45)/(g1^8*g2^8) + g1^9*g2^9*t^8.5 + (2*g2^5*t^8.76)/g1^3 + 4*g2^4*t^8.8 - 2*g1^3*g2^3*t^8.83 - g1^6*g2^2*t^8.87 - t^4.06/(g1*g2*y) - t^6.13/(g1^6*g2^2*y) - (2*t^6.17)/(g1^3*g2^3*y) + (2*t^7.19)/(g1^7*g2^3*y) + t^7.22/(g1^4*g2^4*y) + (g2^2*t^7.91)/(g1^2*y) + (4*g1*g2*t^7.94)/y + (g1^4*t^7.98)/y - t^8.21/(g1^11*g2^3*y) - (2*t^8.25)/(g1^8*g2^4*y) - (3*t^8.28)/(g1^5*g2^5*y) + (2*g2^2*t^8.93)/(g1^6*y) + (6*g2*t^8.96)/(g1^3*y) - (t^4.06*y)/(g1*g2) - (t^6.13*y)/(g1^6*g2^2) - (2*t^6.17*y)/(g1^3*g2^3) + (2*t^7.19*y)/(g1^7*g2^3) + (t^7.22*y)/(g1^4*g2^4) + (g2^2*t^7.91*y)/g1^2 + 4*g1*g2*t^7.94*y + g1^4*t^7.98*y - (t^8.21*y)/(g1^11*g2^3) - (2*t^8.25*y)/(g1^8*g2^4) - (3*t^8.28*y)/(g1^5*g2^5) + (2*g2^2*t^8.93*y)/g1^6 + (6*g2*t^8.96*y)/g1^3 |
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 |
|---|---|---|---|---|---|---|---|---|
| 45986 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ | 0.669 | 0.8353 | 0.8009 | [X:[], M:[0.6994, 0.6891, 0.6994], q:[0.4806, 0.82], qb:[0.8303, 0.4703], phi:[0.3497]] | t^2.07 + 3*t^2.1 + t^2.85 + 2*t^3.87 + t^3.9 + t^3.93 + t^4.13 + 3*t^4.17 + 6*t^4.2 + t^4.92 + 4*t^4.95 + t^5.71 + 2*t^5.94 + 5*t^5.97 - t^6. - t^4.05/y - t^4.05*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 45860 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_2\tilde{q}_1$ | 0.6485 | 0.7967 | 0.8141 | [X:[], M:[0.696, 0.696], q:[0.4802, 0.8238], qb:[0.8238, 0.4626], phi:[0.3524]] | 2*t^2.09 + t^2.11 + t^2.83 + t^3.83 + 2*t^3.86 + t^3.89 + t^3.94 + 3*t^4.18 + 2*t^4.2 + t^4.23 + 2*t^4.92 + 2*t^4.94 + t^5.66 + 2*t^5.92 + 4*t^5.95 + 2*t^5.97 - 2*t^6. - t^4.06/y - t^4.06*y | detail |