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 |
|---|---|---|---|---|---|---|---|---|---|
| 46288 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_2\phi_1^2$ + $ M_3\phi_1q_2^2$ | 0.6126 | 0.807 | 0.7591 | [X:[], M:[0.9185, 0.9185, 0.7556], q:[0.7296, 0.3518], qb:[0.3518, 0.4038], phi:[0.5407]] | [X:[], M:[[4], [4], [12]], q:[[1], [-5]], qb:[[-5], [17]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2\tilde{q}_1$, $ M_3$, $ q_2\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ M_1$, $ M_2$, $ \phi_1^2$, $ q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_1^2$, $ M_3q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_3^2$, $ M_3q_2\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ \phi_1q_1q_2$, $ \phi_1q_1\tilde{q}_1$, $ M_2q_2\tilde{q}_1$, $ M_1M_3$, $ M_2M_3$, $ \phi_1q_1\tilde{q}_2$, $ M_2q_2\tilde{q}_2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_1^2$, $ M_1M_2$, $ M_2^2$, $ M_3\phi_1^2$, $ \phi_1^2q_2\tilde{q}_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ M_3q_1\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$, $ q_1\tilde{q}_1\tilde{q}_2^2$ | $M_3\phi_1q_2\tilde{q}_1$, $ M_3\phi_1\tilde{q}_1^2$, $ \phi_1q_2^2\tilde{q}_1\tilde{q}_2$, $ 2\phi_1q_2\tilde{q}_1^2\tilde{q}_2$, $ \phi_1\tilde{q}_1^3\tilde{q}_2$ | 3 | t^2.11 + 3*t^2.27 + 2*t^2.76 + t^3.24 + t^3.4 + 2*t^3.73 + 2*t^3.89 + t^4.04 + t^4.22 + 3*t^4.38 + 6*t^4.53 + 2*t^4.87 + 6*t^5.02 + t^5.36 + 6*t^5.51 + 3*t^5.67 + 3*t^6. + 6*t^6.16 + 3*t^6.31 + t^6.33 + 3*t^6.49 + 8*t^6.64 + 12*t^6.8 + t^6.98 + 4*t^7.13 + 13*t^7.29 + t^7.45 + t^7.47 + 2*t^7.62 + 14*t^7.78 + 8*t^7.93 + t^8.09 - 3*t^8.11 + 5*t^8.27 + 12*t^8.42 + t^8.44 + 6*t^8.58 - t^8.6 - 2*t^8.76 + 15*t^8.91 - t^4.62/y - t^6.89/y + (2*t^7.38)/y + (3*t^7.53)/y + (3*t^7.87)/y + (6*t^8.02)/y + (2*t^8.36)/y + (5*t^8.51)/y + (3*t^8.67)/y + (2*t^8.84)/y - t^4.62*y - t^6.89*y + 2*t^7.38*y + 3*t^7.53*y + 3*t^7.87*y + 6*t^8.02*y + 2*t^8.36*y + 5*t^8.51*y + 3*t^8.67*y + 2*t^8.84*y | t^2.11/g1^10 + 3*g1^12*t^2.27 + 2*g1^4*t^2.76 + t^3.24/g1^4 + g1^18*t^3.4 + (2*t^3.73)/g1^12 + 2*g1^10*t^3.89 + g1^32*t^4.04 + t^4.22/g1^20 + 3*g1^2*t^4.38 + 6*g1^24*t^4.53 + (2*t^4.87)/g1^6 + 6*g1^16*t^5.02 + t^5.36/g1^14 + 6*g1^8*t^5.51 + 3*g1^30*t^5.67 + 3*t^6. + 6*g1^22*t^6.16 + 3*g1^44*t^6.31 + t^6.33/g1^30 + (3*t^6.49)/g1^8 + 8*g1^14*t^6.64 + 12*g1^36*t^6.8 + t^6.98/g1^16 + 4*g1^6*t^7.13 + 13*g1^28*t^7.29 + g1^50*t^7.45 + t^7.47/g1^24 + (2*t^7.62)/g1^2 + 14*g1^20*t^7.78 + 8*g1^42*t^7.93 + g1^64*t^8.09 - (3*t^8.11)/g1^10 + 5*g1^12*t^8.27 + 12*g1^34*t^8.42 + t^8.44/g1^40 + 6*g1^56*t^8.58 - t^8.6/g1^18 - 2*g1^4*t^8.76 + 15*g1^26*t^8.91 - t^4.62/(g1^2*y) - (g1^10*t^6.89)/y + (2*g1^2*t^7.38)/y + (3*g1^24*t^7.53)/y + (3*t^7.87)/(g1^6*y) + (6*g1^16*t^8.02)/y + (2*t^8.36)/(g1^14*y) + (5*g1^8*t^8.51)/y + (3*g1^30*t^8.67)/y + (2*t^8.84)/(g1^22*y) - (t^4.62*y)/g1^2 - g1^10*t^6.89*y + 2*g1^2*t^7.38*y + 3*g1^24*t^7.53*y + (3*t^7.87*y)/g1^6 + 6*g1^16*t^8.02*y + (2*t^8.36*y)/g1^14 + 5*g1^8*t^8.51*y + 3*g1^30*t^8.67*y + (2*t^8.84*y)/g1^22 |
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 |
|---|---|---|---|---|---|---|---|---|
| 46548 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_2\phi_1^2$ + $ M_3\phi_1q_2^2$ + $ M_4\phi_1^2$ | 0.6201 | 0.8206 | 0.7557 | [X:[], M:[0.9167, 0.9167, 0.7501, 0.9167], q:[0.7292, 0.3541], qb:[0.3541, 0.396], phi:[0.5416]] | t^2.12 + 3*t^2.25 + 3*t^2.75 + t^3.38 + 2*t^3.75 + 2*t^3.88 + t^4. + t^4.25 + 3*t^4.38 + 6*t^4.5 + 3*t^4.87 + 9*t^5. + 6*t^5.5 + 3*t^5.63 + t^6. - t^4.62/y - t^4.62*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46041 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_2\phi_1^2$ | 0.594 | 0.7723 | 0.7691 | [X:[], M:[0.9215, 0.9215], q:[0.7304, 0.3481], qb:[0.3481, 0.4164], phi:[0.5392]] | t^2.09 + 2*t^2.29 + 2*t^2.76 + t^3.24 + t^3.44 + 3*t^3.71 + 2*t^3.91 + t^4.12 + t^4.18 + 2*t^4.38 + 3*t^4.59 + 2*t^4.85 + 4*t^5.06 + t^5.32 + 5*t^5.53 + 2*t^5.73 + t^5.79 + 3*t^6. - t^4.62/y - t^4.62*y | detail |