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 |
|---|---|---|---|---|---|---|---|---|---|
| 46186 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_1q_2$ | 0.6674 | 0.8593 | 0.7766 | [X:[], M:[1.1204, 0.6873, 0.8127, 0.8077], q:[0.75, 0.4423], qb:[0.3704, 0.4373], phi:[0.5]] | [X:[], M:[[1, 0], [0, 1], [0, -1], [1, 1]], q:[[0, 0], [-1, -1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ M_4$, $ \tilde{q}_1\tilde{q}_2$, $ M_3$, $ q_2\tilde{q}_1$, $ \phi_1^2$, $ M_1$, $ q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2^2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2^2$, $ M_2M_4$, $ M_2\tilde{q}_1\tilde{q}_2$, $ M_2M_3$, $ M_2q_2\tilde{q}_1$, $ M_4^2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_3M_4$, $ M_4q_2\tilde{q}_1$, $ M_3\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_3^2$, $ M_3q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_2\phi_1^2$, $ M_1M_2$, $ M_4\phi_1^2$, $ M_2q_1\tilde{q}_1$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ M_3\phi_1^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_1M_4$, $ M_4q_1\tilde{q}_1$, $ M_2\phi_1\tilde{q}_1^2$, $ q_1\tilde{q}_1^2\tilde{q}_2$, $ M_1M_3$, $ M_3q_1\tilde{q}_1$, $ q_1q_2\tilde{q}_1^2$ | . | -3 | t^2.06 + 2*t^2.42 + 2*t^2.44 + t^3. + 2*t^3.36 + t^3.72 + t^3.92 + 2*t^4.12 + t^4.14 + t^4.15 + 2*t^4.48 + 2*t^4.5 + 3*t^4.85 + 4*t^4.86 + 3*t^4.88 + t^5.06 + 4*t^5.42 + 2*t^5.44 + 4*t^5.78 + 3*t^5.8 - 3*t^6. - t^6.02 + 2*t^6.15 + 2*t^6.16 + 2*t^6.19 + 2*t^6.35 + 2*t^6.36 + 4*t^6.55 + 4*t^6.56 + 2*t^6.58 + 2*t^6.59 + 3*t^6.72 + 3*t^6.91 + 3*t^6.92 + t^6.94 + 2*t^7.08 + t^7.12 - t^7.14 + 4*t^7.27 + 6*t^7.28 + 4*t^7.3 + 4*t^7.31 + t^7.45 + 4*t^7.48 + t^7.65 - 2*t^7.7 - 2*t^7.72 + 8*t^7.85 + 6*t^7.86 + 3*t^7.88 + t^8.05 - 4*t^8.06 - 2*t^8.08 + 6*t^8.21 + 6*t^8.22 + 4*t^8.24 + 3*t^8.25 + t^8.26 + t^8.28 + t^8.29 + t^8.31 - 6*t^8.42 - 8*t^8.44 - 2*t^8.45 + 3*t^8.57 + 4*t^8.58 + 3*t^8.6 + 4*t^8.61 + 2*t^8.62 - 2*t^8.64 + 3*t^8.77 + 6*t^8.78 + 2*t^8.8 + 6*t^8.97 + 5*t^8.98 - t^4.5/y - t^6.56/y - t^6.92/y - t^6.94/y + t^7.14/y + (2*t^7.48)/y + (2*t^7.5)/y + t^7.85/y + (3*t^7.86)/y + t^7.88/y + (2*t^8.06)/y + t^8.08/y + (4*t^8.42)/y + (3*t^8.44)/y - t^8.62/y + (5*t^8.78)/y + (4*t^8.8)/y - t^4.5*y - t^6.56*y - t^6.92*y - t^6.94*y + t^7.14*y + 2*t^7.48*y + 2*t^7.5*y + t^7.85*y + 3*t^7.86*y + t^7.88*y + 2*t^8.06*y + t^8.08*y + 4*t^8.42*y + 3*t^8.44*y - t^8.62*y + 5*t^8.78*y + 4*t^8.8*y | g2*t^2.06 + 2*g1*g2*t^2.42 + (2*t^2.44)/g2 + t^3. + 2*g1*t^3.36 + g1^2*t^3.72 + g1*g2*t^3.92 + 2*g2^2*t^4.12 + t^4.14/g1 + t^4.15/(g1^2*g2^2) + 2*g1*g2^2*t^4.48 + 2*t^4.5 + 3*g1^2*g2^2*t^4.85 + 4*g1*t^4.86 + (3*t^4.88)/g2^2 + g2*t^5.06 + 4*g1*g2*t^5.42 + (2*t^5.44)/g2 + 4*g1^2*g2*t^5.78 + (3*g1*t^5.8)/g2 - 3*t^6. - t^6.02/(g1*g2^2) + 2*g1^3*g2*t^6.15 + (2*g1^2*t^6.16)/g2 + 2*g2^3*t^6.19 + 2*g1^2*g2^2*t^6.35 + 2*g1*t^6.36 + 4*g1*g2^3*t^6.55 + 4*g2*t^6.56 + (2*t^6.58)/(g1*g2) + (2*t^6.59)/(g1^2*g2^3) + 3*g1^2*t^6.72 + 3*g1^2*g2^3*t^6.91 + 3*g1*g2*t^6.92 + t^6.94/g2 + 2*g1^3*t^7.08 + g2^2*t^7.12 - t^7.14/g1 + 4*g1^3*g2^3*t^7.27 + 6*g1^2*g2*t^7.28 + (4*g1*t^7.3)/g2 + (4*t^7.31)/g2^3 + g1^4*t^7.45 + 4*g1*g2^2*t^7.48 + g1^3*g2*t^7.65 - (2*g2*t^7.7)/g1 - (2*t^7.72)/(g1^2*g2) + 8*g1^2*g2^2*t^7.85 + 6*g1*t^7.86 + (3*t^7.88)/g2^2 + g1*g2^3*t^8.05 - 4*g2*t^8.06 - (2*t^8.08)/(g1*g2) + 6*g1^3*g2^2*t^8.21 + 6*g1^2*t^8.22 + (4*g1*t^8.24)/g2^2 + 3*g2^4*t^8.25 + (g2^2*t^8.26)/g1 + t^8.28/g1^2 + t^8.29/(g1^3*g2^2) + t^8.31/(g1^4*g2^4) - 6*g1*g2*t^8.42 - (8*t^8.44)/g2 - (2*t^8.45)/(g1*g2^3) + 3*g1^4*g2^2*t^8.57 + 4*g1^3*t^8.58 + (3*g1^2*t^8.6)/g2^2 + 4*g1*g2^4*t^8.61 + 2*g2^2*t^8.62 - (2*t^8.64)/g1 + 3*g1^3*g2^3*t^8.77 + 6*g1^2*g2*t^8.78 + (2*g1*t^8.8)/g2 + 6*g1^2*g2^4*t^8.97 + 5*g1*g2^2*t^8.98 - t^4.5/y - (g2*t^6.56)/y - (g1*g2*t^6.92)/y - t^6.94/(g2*y) + t^7.14/(g1*y) + (2*g1*g2^2*t^7.48)/y + (2*t^7.5)/y + (g1^2*g2^2*t^7.85)/y + (3*g1*t^7.86)/y + t^7.88/(g2^2*y) + (2*g2*t^8.06)/y + t^8.08/(g1*g2*y) + (4*g1*g2*t^8.42)/y + (3*t^8.44)/(g2*y) - (g2^2*t^8.62)/y + (5*g1^2*g2*t^8.78)/y + (4*g1*t^8.8)/(g2*y) - t^4.5*y - g2*t^6.56*y - g1*g2*t^6.92*y - (t^6.94*y)/g2 + (t^7.14*y)/g1 + 2*g1*g2^2*t^7.48*y + 2*t^7.5*y + g1^2*g2^2*t^7.85*y + 3*g1*t^7.86*y + (t^7.88*y)/g2^2 + 2*g2*t^8.06*y + (t^8.08*y)/(g1*g2) + 4*g1*g2*t^8.42*y + (3*t^8.44*y)/g2 - g2^2*t^8.62*y + 5*g1^2*g2*t^8.78*y + (4*g1*t^8.8*y)/g2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46052 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ | 0.652 | 0.8312 | 0.7844 | [X:[], M:[1.1326, 0.6957, 0.8043], q:[0.75, 0.4217], qb:[0.3826, 0.4457], phi:[0.5]] | t^2.09 + 2*t^2.41 + t^2.48 + t^3. + 2*t^3.4 + t^3.52 + t^3.8 + t^3.98 + t^4.03 + t^4.1 + 2*t^4.17 + 2*t^4.5 + t^4.57 + 3*t^4.83 + 2*t^4.9 + t^4.97 + t^5.09 + 2*t^5.41 + 3*t^5.48 + t^5.6 + 3*t^5.81 + 2*t^5.88 + t^5.93 - 2*t^6. - t^4.5/y - t^4.5*y | detail |