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 |
|---|---|---|---|---|---|---|---|---|---|
| 48230 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_4\phi_1^2$ + $ M_5\phi_1q_2\tilde{q}_2$ | 0.6027 | 0.776 | 0.7767 | [X:[], M:[0.6727, 1.1091, 0.7818, 1.1091, 0.7818], q:[0.7773, 0.55], qb:[0.6682, 0.2227], phi:[0.4455]] | [X:[], M:[[12], [-4], [8], [-4], [8]], q:[[-1], [-11]], qb:[[3], [1]], phi:[[2]]] |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ q_2\tilde{q}_2$, $ M_3$, $ M_5$, $ \phi_1^2$, $ q_1\tilde{q}_2$, $ M_2$, $ M_4$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ q_1\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_1M_3$, $ M_1M_5$, $ \phi_1q_2^2$, $ q_2^2\tilde{q}_2^2$, $ M_3q_2\tilde{q}_2$, $ M_5q_2\tilde{q}_2$, $ M_3^2$, $ M_3M_5$, $ M_5^2$, $ M_1\phi_1^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_2$, $ M_3\phi_1^2$, $ M_5\phi_1^2$, $ \phi_1q_1q_2$, $ q_1q_2\tilde{q}_2^2$, $ M_1M_2$, $ M_1M_4$, $ \phi_1^4$, $ \phi_1\tilde{q}_1^2$, $ M_3q_1\tilde{q}_2$, $ M_5q_1\tilde{q}_2$, $ M_4q_2\tilde{q}_2$, $ M_2M_3$, $ M_3M_4$, $ M_2M_5$, $ M_4M_5$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1^2q_1\tilde{q}_2$ | . | t^2.02 + t^2.32 + 2*t^2.35 + t^2.67 + t^3. + 2*t^3.33 + t^4.01 + t^4.04 + 2*t^4.34 + 2*t^4.36 + 2*t^4.64 + t^4.66 + 4*t^4.69 + 2*t^4.99 + 2*t^5.02 + t^5.32 + 6*t^5.35 + t^5.65 + 4*t^5.67 - 2*t^6. + t^6.03 + t^6.05 + t^6.33 + 2*t^6.35 + 2*t^6.38 + 3*t^6.65 + 3*t^6.68 + 4*t^6.71 + 2*t^6.95 + 3*t^7.01 + 6*t^7.04 + t^7.31 + 2*t^7.34 + 7*t^7.36 + t^7.64 + 3*t^7.66 + 9*t^7.69 + 2*t^7.96 + 5*t^8.02 + t^8.05 + t^8.07 - 2*t^8.32 - 3*t^8.35 + 2*t^8.37 + 2*t^8.4 + 2*t^8.67 + 3*t^8.7 + 4*t^8.73 + t^8.97 - t^4.34/y - t^6.35/y - (2*t^6.68)/y + t^7.01/y + t^7.34/y + (2*t^7.36)/y + t^7.66/y + (2*t^7.69)/y + (3*t^7.99)/y + (3*t^8.02)/y + (2*t^8.32)/y + (4*t^8.35)/y - t^8.37/y + (2*t^8.65)/y + (5*t^8.67)/y - (2*t^8.7)/y - t^4.34*y - t^6.35*y - 2*t^6.68*y + t^7.01*y + t^7.34*y + 2*t^7.36*y + t^7.66*y + 2*t^7.69*y + 3*t^7.99*y + 3*t^8.02*y + 2*t^8.32*y + 4*t^8.35*y - t^8.37*y + 2*t^8.65*y + 5*t^8.67*y - 2*t^8.7*y | g1^12*t^2.02 + t^2.32/g1^10 + 2*g1^8*t^2.35 + g1^4*t^2.67 + t^3. + (2*t^3.33)/g1^4 + g1^6*t^4.01 + g1^24*t^4.04 + 2*g1^2*t^4.34 + 2*g1^20*t^4.36 + (2*t^4.64)/g1^20 + t^4.66/g1^2 + 4*g1^16*t^4.69 + (2*t^4.99)/g1^6 + 2*g1^12*t^5.02 + t^5.32/g1^10 + 6*g1^8*t^5.35 + t^5.65/g1^14 + 4*g1^4*t^5.67 - 2*t^6. + g1^18*t^6.03 + g1^36*t^6.05 + t^6.33/g1^4 + 2*g1^14*t^6.35 + 2*g1^32*t^6.38 + (3*t^6.65)/g1^8 + 3*g1^10*t^6.68 + 4*g1^28*t^6.71 + (2*t^6.95)/g1^30 + 3*g1^6*t^7.01 + 6*g1^24*t^7.04 + t^7.31/g1^16 + 2*g1^2*t^7.34 + 7*g1^20*t^7.36 + t^7.64/g1^20 + (3*t^7.66)/g1^2 + 9*g1^16*t^7.69 + (2*t^7.96)/g1^24 + 5*g1^12*t^8.02 + g1^30*t^8.05 + g1^48*t^8.07 - (2*t^8.32)/g1^10 - 3*g1^8*t^8.35 + 2*g1^26*t^8.37 + 2*g1^44*t^8.4 + 2*g1^4*t^8.67 + 3*g1^22*t^8.7 + 4*g1^40*t^8.73 + t^8.97/g1^18 - (g1^2*t^4.34)/y - (g1^14*t^6.35)/y - (2*g1^10*t^6.68)/y + (g1^6*t^7.01)/y + (g1^2*t^7.34)/y + (2*g1^20*t^7.36)/y + t^7.66/(g1^2*y) + (2*g1^16*t^7.69)/y + (3*t^7.99)/(g1^6*y) + (3*g1^12*t^8.02)/y + (2*t^8.32)/(g1^10*y) + (4*g1^8*t^8.35)/y - (g1^26*t^8.37)/y + (2*t^8.65)/(g1^14*y) + (5*g1^4*t^8.67)/y - (2*g1^22*t^8.7)/y - g1^2*t^4.34*y - g1^14*t^6.35*y - 2*g1^10*t^6.68*y + g1^6*t^7.01*y + g1^2*t^7.34*y + 2*g1^20*t^7.36*y + (t^7.66*y)/g1^2 + 2*g1^16*t^7.69*y + (3*t^7.99*y)/g1^6 + 3*g1^12*t^8.02*y + (2*t^8.32*y)/g1^10 + 4*g1^8*t^8.35*y - g1^26*t^8.37*y + (2*t^8.65*y)/g1^14 + 5*g1^4*t^8.67*y - 2*g1^22*t^8.7*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46779 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1q_1^2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_1$ + $ M_4\phi_1\tilde{q}_2^2$ + $ M_4\phi_1^2$ | 0.5854 | 0.7449 | 0.7859 | [X:[], M:[0.6895, 1.1035, 0.793, 1.1035], q:[0.7759, 0.5346], qb:[0.6724, 0.2241], phi:[0.4483]] | t^2.07 + t^2.28 + t^2.38 + t^2.69 + t^3. + 2*t^3.31 + t^3.62 + t^4.03 + t^4.14 + 2*t^4.34 + t^4.45 + 2*t^4.55 + 2*t^4.76 + 2*t^4.97 + t^5.07 + t^5.28 + 5*t^5.38 + t^5.59 + 3*t^5.69 + t^5.9 - t^6. - t^4.34/y - t^4.34*y | detail |