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 |
|---|---|---|---|---|---|---|---|---|---|
| 45890 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ \phi_1^4$ | 0.6994 | 0.8663 | 0.8073 | [X:[], M:[0.9428, 0.9428, 0.9428], q:[0.5858, 0.4714], qb:[0.4714, 0.4714], phi:[0.5]] | [X:[], M:[[0, 1, 1], [1, 0, 1], [1, 1, 0]], q:[[-1, -1, -1], [1, 0, 0]], qb:[[0, 1, 0], [0, 0, 1]], phi:[[0, 0, 0]]] | 3 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ q_2\tilde{q}_1$, $ M_2$, $ q_2\tilde{q}_2$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ \phi_1q_2^2$, $ \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$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1q_2$, $ \phi_1q_1^2$, $ M_3^2$, $ M_3q_2\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_2M_3$, $ M_2q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ M_1M_3$, $ M_3\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_2^2$, $ M_2q_2\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ M_1M_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_1^2$, $ M_1\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_3\phi_1^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_2\phi_1^2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_1\phi_1^2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$ | . | -10 | 6*t^2.83 + t^3. + 6*t^4.33 + 3*t^4.67 + t^5.01 + 18*t^5.66 + 6*t^5.83 - 10*t^6. - 3*t^6.34 + 30*t^7.16 + 40*t^8.49 + 33*t^8.66 - 54*t^8.83 - t^4.5/y - (3*t^7.33)/y + (3*t^7.67)/y + (15*t^8.66)/y + (6*t^8.83)/y - t^4.5*y - 3*t^7.33*y + 3*t^7.67*y + 15*t^8.66*y + 6*t^8.83*y | 2*g1*g2*t^2.83 + 2*g1*g3*t^2.83 + 2*g2*g3*t^2.83 + t^3. + g1^2*t^4.33 + g1*g2*t^4.33 + g2^2*t^4.33 + g1*g3*t^4.33 + g2*g3*t^4.33 + g3^2*t^4.33 + t^4.67/(g1*g2) + t^4.67/(g1*g3) + t^4.67/(g2*g3) + t^5.01/(g1^2*g2^2*g3^2) + 3*g1^2*g2^2*t^5.66 + 3*g1^2*g2*g3*t^5.66 + 3*g1*g2^2*g3*t^5.66 + 3*g1^2*g3^2*t^5.66 + 3*g1*g2*g3^2*t^5.66 + 3*g2^2*g3^2*t^5.66 + 2*g1*g2*t^5.83 + 2*g1*g3*t^5.83 + 2*g2*g3*t^5.83 - 4*t^6. - (g1*t^6.)/g2 - (g2*t^6.)/g1 - (g1*t^6.)/g3 - (g2*t^6.)/g3 - (g3*t^6.)/g1 - (g3*t^6.)/g2 - t^6.34/(g1*g2*g3^2) - t^6.34/(g1*g2^2*g3) - t^6.34/(g1^2*g2*g3) + 2*g1^3*g2*t^7.16 + 2*g1^2*g2^2*t^7.16 + 2*g1*g2^3*t^7.16 + 2*g1^3*g3*t^7.16 + 4*g1^2*g2*g3*t^7.16 + 4*g1*g2^2*g3*t^7.16 + 2*g2^3*g3*t^7.16 + 2*g1^2*g3^2*t^7.16 + 4*g1*g2*g3^2*t^7.16 + 2*g2^2*g3^2*t^7.16 + 2*g1*g3^3*t^7.16 + 2*g2*g3^3*t^7.16 + 4*g1^3*g2^3*t^8.49 + 4*g1^3*g2^2*g3*t^8.49 + 4*g1^2*g2^3*g3*t^8.49 + 4*g1^3*g2*g3^2*t^8.49 + 4*g1^2*g2^2*g3^2*t^8.49 + 4*g1*g2^3*g3^2*t^8.49 + 4*g1^3*g3^3*t^8.49 + 4*g1^2*g2*g3^3*t^8.49 + 4*g1*g2^2*g3^3*t^8.49 + 4*g2^3*g3^3*t^8.49 + g1^4*t^8.66 + g1^3*g2*t^8.66 + 4*g1^2*g2^2*t^8.66 + g1*g2^3*t^8.66 + g2^4*t^8.66 + g1^3*g3*t^8.66 + 4*g1^2*g2*g3*t^8.66 + 4*g1*g2^2*g3*t^8.66 + g2^3*g3*t^8.66 + 4*g1^2*g3^2*t^8.66 + 4*g1*g2*g3^2*t^8.66 + 4*g2^2*g3^2*t^8.66 + g1*g3^3*t^8.66 + g2*g3^3*t^8.66 + g3^4*t^8.66 - 4*g1^2*t^8.83 - 10*g1*g2*t^8.83 - 4*g2^2*t^8.83 - (2*g1^2*g2*t^8.83)/g3 - (2*g1*g2^2*t^8.83)/g3 - 10*g1*g3*t^8.83 - (2*g1^2*g3*t^8.83)/g2 - 10*g2*g3*t^8.83 - (2*g2^2*g3*t^8.83)/g1 - 4*g3^2*t^8.83 - (2*g1*g3^2*t^8.83)/g2 - (2*g2*g3^2*t^8.83)/g1 - t^4.5/y - (g1*g2*t^7.33)/y - (g1*g3*t^7.33)/y - (g2*g3*t^7.33)/y + t^7.67/(g1*g2*y) + t^7.67/(g1*g3*y) + t^7.67/(g2*g3*y) + (g1^2*g2^2*t^8.66)/y + (4*g1^2*g2*g3*t^8.66)/y + (4*g1*g2^2*g3*t^8.66)/y + (g1^2*g3^2*t^8.66)/y + (4*g1*g2*g3^2*t^8.66)/y + (g2^2*g3^2*t^8.66)/y + (2*g1*g2*t^8.83)/y + (2*g1*g3*t^8.83)/y + (2*g2*g3*t^8.83)/y - t^4.5*y - g1*g2*t^7.33*y - g1*g3*t^7.33*y - g2*g3*t^7.33*y + (t^7.67*y)/(g1*g2) + (t^7.67*y)/(g1*g3) + (t^7.67*y)/(g2*g3) + g1^2*g2^2*t^8.66*y + 4*g1^2*g2*g3*t^8.66*y + 4*g1*g2^2*g3*t^8.66*y + g1^2*g3^2*t^8.66*y + 4*g1*g2*g3^2*t^8.66*y + g2^2*g3^2*t^8.66*y + 2*g1*g2*t^8.83*y + 2*g1*g3*t^8.83*y + 2*g2*g3*t^8.83*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 |
|---|---|---|---|---|---|---|---|---|---|
| 45843 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ | 0.7577 | 0.9271 | 0.8174 | [X:[], M:[0.7655, 0.7655, 0.7655], q:[0.6539, 0.5806], qb:[0.5806, 0.5806], phi:[0.4011]] | 3*t^2.3 + t^2.41 + 3*t^3.48 + 6*t^4.59 + 6*t^4.69 + 3*t^4.7 + t^4.81 + 3*t^4.91 + t^5.13 + 6*t^5.78 + 3*t^5.89 - 10*t^6. - t^4.2/y - t^4.2*y | detail |