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 |
|---|---|---|---|---|---|---|---|---|---|
| 815 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_5\phi_1q_2\tilde{q}_2$ | 0.6127 | 0.7931 | 0.7725 | [X:[], M:[1.0, 1.1136, 0.7728, 0.7728, 0.6704], q:[0.7784, 0.2216], qb:[0.5623, 0.6648], phi:[0.4432]] | [X:[], M:[[0], [-4], [8], [8], [-6]], q:[[-1], [1]], qb:[[-11], [3]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ M_3$, $ M_4$, $ q_2\tilde{q}_1$, $ \phi_1q_2^2$, $ q_2\tilde{q}_2$, $ M_1$, $ M_2$, $ M_5^2$, $ q_1\tilde{q}_1$, $ M_3M_5$, $ M_4M_5$, $ \phi_1q_1q_2$, $ q_1\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ M_3^2$, $ M_3M_4$, $ M_4^2$, $ M_5\phi_1q_2^2$, $ M_4q_2\tilde{q}_1$, $ M_5q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ M_3\phi_1q_2^2$, $ M_4\phi_1q_2^2$, $ M_4q_2\tilde{q}_2$, $ M_1M_5$, $ \phi_1q_2^3\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_1M_3$, $ M_1M_4$, $ \phi_1^2q_2^4$, $ \phi_1q_2^3\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_2^2$, $ M_2M_5$, $ \phi_1q_1\tilde{q}_1$, $ M_2M_3$, $ M_2M_4$, $ \phi_1q_1\tilde{q}_2$ | . | -2 | t^2.01 + 2*t^2.32 + t^2.35 + 2*t^2.66 + t^3. + t^3.34 + 2*t^4.02 + 3*t^4.33 + t^4.36 + 3*t^4.64 + 3*t^4.67 + 2*t^4.7 + 3*t^4.98 + 4*t^5.01 + 6*t^5.32 + 2*t^5.35 + 3*t^5.66 - 2*t^6. + 2*t^6.03 - 2*t^6.31 + 4*t^6.34 + 2*t^6.37 + 4*t^6.65 + 4*t^6.68 + 2*t^6.71 + 4*t^6.96 + 4*t^6.99 + 5*t^7.02 + 2*t^7.06 + 4*t^7.3 + 6*t^7.33 + 6*t^7.36 + 8*t^7.64 + 7*t^7.67 + t^7.7 + 9*t^7.98 - 2*t^8.01 + 3*t^8.04 - 5*t^8.32 + t^8.35 + 2*t^8.39 - 3*t^8.63 - t^8.66 + 2*t^8.69 + 4*t^8.73 + 2*t^8.97 - t^4.33/y - t^6.34/y - (2*t^6.65)/y + (2*t^7.33)/y + t^7.36/y + t^7.64/y + (4*t^7.67)/y + (4*t^7.98)/y + (5*t^8.01)/y + (4*t^8.32)/y + t^8.35/y + (2*t^8.66)/y + t^8.69/y - (3*t^8.97)/y - t^4.33*y - t^6.34*y - 2*t^6.65*y + 2*t^7.33*y + t^7.36*y + t^7.64*y + 4*t^7.67*y + 4*t^7.98*y + 5*t^8.01*y + 4*t^8.32*y + t^8.35*y + 2*t^8.66*y + t^8.69*y - 3*t^8.97*y | t^2.01/g1^6 + 2*g1^8*t^2.32 + t^2.35/g1^10 + 2*g1^4*t^2.66 + t^3. + t^3.34/g1^4 + (2*t^4.02)/g1^12 + 3*g1^2*t^4.33 + t^4.36/g1^16 + 3*g1^16*t^4.64 + (3*t^4.67)/g1^2 + (2*t^4.7)/g1^20 + 3*g1^12*t^4.98 + (4*t^5.01)/g1^6 + 6*g1^8*t^5.32 + (2*t^5.35)/g1^10 + 3*g1^4*t^5.66 - 2*t^6. + (2*t^6.03)/g1^18 - 2*g1^14*t^6.31 + (4*t^6.34)/g1^4 + (2*t^6.37)/g1^22 + 4*g1^10*t^6.65 + (4*t^6.68)/g1^8 + (2*t^6.71)/g1^26 + 4*g1^24*t^6.96 + 4*g1^6*t^6.99 + (5*t^7.02)/g1^12 + (2*t^7.06)/g1^30 + 4*g1^20*t^7.3 + 6*g1^2*t^7.33 + (6*t^7.36)/g1^16 + 8*g1^16*t^7.64 + (7*t^7.67)/g1^2 + t^7.7/g1^20 + 9*g1^12*t^7.98 - (2*t^8.01)/g1^6 + (3*t^8.04)/g1^24 - 5*g1^8*t^8.32 + t^8.35/g1^10 + (2*t^8.39)/g1^28 - 3*g1^22*t^8.63 - g1^4*t^8.66 + (2*t^8.69)/g1^14 + (4*t^8.73)/g1^32 + 2*g1^18*t^8.97 - (g1^2*t^4.33)/y - t^6.34/(g1^4*y) - (2*g1^10*t^6.65)/y + (2*g1^2*t^7.33)/y + t^7.36/(g1^16*y) + (g1^16*t^7.64)/y + (4*t^7.67)/(g1^2*y) + (4*g1^12*t^7.98)/y + (5*t^8.01)/(g1^6*y) + (4*g1^8*t^8.32)/y + t^8.35/(g1^10*y) + (2*g1^4*t^8.66)/y + t^8.69/(g1^14*y) - (3*g1^18*t^8.97)/y - g1^2*t^4.33*y - (t^6.34*y)/g1^4 - 2*g1^10*t^6.65*y + 2*g1^2*t^7.33*y + (t^7.36*y)/g1^16 + g1^16*t^7.64*y + (4*t^7.67*y)/g1^2 + 4*g1^12*t^7.98*y + (5*t^8.01*y)/g1^6 + 4*g1^8*t^8.32*y + (t^8.35*y)/g1^10 + 2*g1^4*t^8.66*y + (t^8.69*y)/g1^14 - 3*g1^18*t^8.97*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 522 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ | 0.5919 | 0.7517 | 0.7874 | [X:[], M:[1.0, 1.1138, 0.7725, 0.7725], q:[0.7784, 0.2216], qb:[0.5629, 0.6647], phi:[0.4431]] | 2*t^2.32 + t^2.35 + 2*t^2.66 + t^3. + t^3.34 + t^3.99 + t^4.02 + t^4.33 + 3*t^4.63 + t^4.67 + 2*t^4.71 + 3*t^4.98 + 3*t^5.01 + 6*t^5.32 + t^5.35 + 3*t^5.66 - 2*t^6. - t^4.33/y - t^4.33*y | detail |