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 |
|---|---|---|---|---|---|---|---|---|---|
| 45946 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1^4$ + $ \phi_1\tilde{q}_1^2$ | 0.6467 | 0.8193 | 0.7892 | [X:[], M:[1.1186, 0.8093, 0.8093], q:[0.4407, 0.4407], qb:[0.75, 0.3686], phi:[0.5]] | [X:[], M:[[0, 1], [1, 1], [-1, 0]], q:[[-1, -1], [1, 0]], qb:[[0, 0], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ q_1\tilde{q}_2$, $ M_2$, $ q_2\tilde{q}_2$, $ \phi_1^2$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_1^2$, $ \phi_1q_1q_2$, $ M_3^2$, $ M_3q_1\tilde{q}_2$, $ q_1^2\tilde{q}_2^2$, $ M_2M_3$, $ M_3q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$, $ M_2^2$, $ M_2q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_3\phi_1^2$, $ \phi_1^2q_1\tilde{q}_2$, $ M_2\phi_1^2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_1M_3$, $ M_3\tilde{q}_1\tilde{q}_2$, $ q_1\tilde{q}_1\tilde{q}_2^2$, $ M_1M_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$ | . | -5 | 4*t^2.43 + t^3. + 2*t^3.36 + t^3.71 + 2*t^3.93 + 3*t^4.14 + 10*t^4.86 + 4*t^5.43 + 6*t^5.78 - 5*t^6. + 4*t^6.14 - 2*t^6.22 + 8*t^6.36 + 8*t^6.57 + 3*t^6.71 - 2*t^6.93 + 2*t^7.07 - t^7.14 + 20*t^7.28 + t^7.42 - 2*t^7.5 + 2*t^7.64 - 4*t^7.72 + 12*t^7.86 + 2*t^8.07 + 12*t^8.21 + 5*t^8.29 - 20*t^8.43 + 10*t^8.57 - 8*t^8.64 + 18*t^8.78 - t^4.5/y - (2*t^6.93)/y + t^7.14/y + (5*t^7.86)/y + (2*t^8.07)/y + (4*t^8.43)/y + (8*t^8.78)/y - t^4.5*y - 2*t^6.93*y + t^7.14*y + 5*t^7.86*y + 2*t^8.07*y + 4*t^8.43*y + 8*t^8.78*y | (2*t^2.43)/g1 + 2*g1*g2*t^2.43 + t^3. + 2*g2*t^3.36 + g2^2*t^3.71 + t^3.93/g1 + g1*g2*t^3.93 + g1^2*t^4.14 + t^4.14/(g1^2*g2^2) + t^4.14/g2 + (3*t^4.86)/g1^2 + 4*g2*t^4.86 + 3*g1^2*g2^2*t^4.86 + (2*t^5.43)/g1 + 2*g1*g2*t^5.43 + (3*g2*t^5.78)/g1 + 3*g1*g2^2*t^5.78 - 3*t^6. - t^6./(g1^2*g2) - g1^2*g2*t^6. + (2*g2^2*t^6.14)/g1 + 2*g1*g2^3*t^6.14 - t^6.22/(g1*g2^2) - (g1*t^6.22)/g2 + (2*t^6.36)/g1^2 + 4*g2*t^6.36 + 2*g1^2*g2^2*t^6.36 + 2*g1*t^6.57 + (2*t^6.57)/(g1^3*g2^2) + (2*t^6.57)/(g1*g2) + 2*g1^3*g2*t^6.57 + 3*g2^2*t^6.71 - t^6.93/g1 - g1*g2*t^6.93 + 2*g2^3*t^7.07 - t^7.14/g2 + (4*t^7.28)/g1^3 + (6*g2*t^7.28)/g1 + 6*g1*g2^2*t^7.28 + 4*g1^3*g2^3*t^7.28 + g2^4*t^7.42 - 2*t^7.5 + (g2^2*t^7.64)/g1 + g1*g2^3*t^7.64 - (2*t^7.72)/(g1*g2^2) - (2*g1*t^7.72)/g2 + (4*t^7.86)/g1^2 + 4*g2*t^7.86 + 4*g1^2*g2^2*t^7.86 + t^8.07/(g1^3*g2^2) + g1^3*g2*t^8.07 + (4*g2*t^8.21)/g1^2 + 4*g2^2*t^8.21 + 4*g1^2*g2^3*t^8.21 + g1^4*t^8.29 + t^8.29/(g1^4*g2^4) + t^8.29/(g1^2*g2^3) + t^8.29/g2^2 + (g1^2*t^8.29)/g2 - (8*t^8.43)/g1 - (2*t^8.43)/(g1^3*g2) - 8*g1*g2*t^8.43 - 2*g1^3*g2^2*t^8.43 + (3*g2^2*t^8.57)/g1^2 + 4*g2^3*t^8.57 + 3*g1^2*g2^4*t^8.57 - 2*g1^2*t^8.64 - (2*t^8.64)/(g1^2*g2^2) - (4*t^8.64)/g2 + (3*t^8.78)/g1^3 + (6*g2*t^8.78)/g1 + 6*g1*g2^2*t^8.78 + 3*g1^3*g2^3*t^8.78 - t^4.5/y - t^6.93/(g1*y) - (g1*g2*t^6.93)/y + t^7.14/(g2*y) + t^7.86/(g1^2*y) + (3*g2*t^7.86)/y + (g1^2*g2^2*t^7.86)/y + (g1*t^8.07)/y + t^8.07/(g1*g2*y) + (2*t^8.43)/(g1*y) + (2*g1*g2*t^8.43)/y + (4*g2*t^8.78)/(g1*y) + (4*g1*g2^2*t^8.78)/y - t^4.5*y - (t^6.93*y)/g1 - g1*g2*t^6.93*y + (t^7.14*y)/g2 + (t^7.86*y)/g1^2 + 3*g2*t^7.86*y + g1^2*g2^2*t^7.86*y + g1*t^8.07*y + (t^8.07*y)/(g1*g2) + (2*t^8.43*y)/g1 + 2*g1*g2*t^8.43*y + (4*g2*t^8.78*y)/g1 + 4*g1*g2^2*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 |
|---|---|---|---|---|---|---|---|---|
| 46204 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1^4$ + $ \phi_1\tilde{q}_1^2$ + $ M_4\phi_1\tilde{q}_2^2$ | 0.666 | 0.8535 | 0.7803 | [X:[], M:[1.1382, 0.8191, 0.8191, 0.7236], q:[0.4309, 0.4309], qb:[0.75, 0.3882], phi:[0.5]] | t^2.17 + 4*t^2.46 + t^3. + 2*t^3.41 + 2*t^3.96 + 3*t^4.09 + t^4.34 + 4*t^4.63 + 10*t^4.91 + t^5.17 + 4*t^5.46 + 2*t^5.59 + 6*t^5.87 - 5*t^6. - t^4.5/y - t^4.5*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 |
|---|---|---|---|---|---|---|---|---|---|
| 45906 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_1$ + $ \phi_1^4$ | 0.6988 | 0.8648 | 0.8081 | [X:[], M:[0.9484, 0.9484, 0.9484], q:[0.5258, 0.5258], qb:[0.5258, 0.4226], phi:[0.5]] | 6*t^2.85 + t^3. + t^4.04 + 3*t^4.35 + 6*t^4.65 + 18*t^5.69 + 6*t^5.85 - 10*t^6. - t^4.5/y - t^4.5*y | detail |