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 |
|---|---|---|---|---|---|---|---|---|---|
| 6379 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ + ${ }M_{3}M_{8}$ + ${ }M_{1}M_{4}$ + ${ }M_{6}X_{1}$ + ${ }M_{4}M_{9}$ | 0.6519 | 0.8058 | 0.809 | [X:[1.3333], M:[1.1293, 0.7212, 0.9798, 0.8707, 1.1293, 0.6667, 0.8707, 1.0202, 1.1293], q:[0.5101, 0.3606], qb:[0.5101, 0.7687], phi:[0.4626]] | [X:[[0]], M:[[-2], [-6], [-10], [2], [-2], [0], [2], [10], [-2]], q:[[5], [-3]], qb:[[5], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{8}$, ${ }M_{1}$, ${ }M_{9}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }X_{1}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{7}^{2}$, ${ }M_{2}M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{9}$, ${ }\phi_{1}^{4}$, ${ }M_{7}M_{8}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{8}\phi_{1}^{2}$ | ${}M_{1}M_{7}$, ${ }M_{7}M_{9}$ | -2 | t^2.164 + t^2.612 + t^2.776 + t^3.061 + 2*t^3.388 + t^3.552 + t^3.836 + 2*t^4. + t^4.327 + 3*t^4.448 + t^4.776 + t^4.939 + 2*t^5.224 + t^5.388 + t^5.552 + t^5.673 + t^5.715 + t^5.836 - 2*t^6. + t^6.121 + 4*t^6.164 + t^6.327 + t^6.491 + 4*t^6.612 + 2*t^6.776 + t^6.897 + t^6.939 + 3*t^7.061 + 2*t^7.103 + 2*t^7.224 + t^7.388 + 3*t^7.509 + 3*t^7.552 - 2*t^7.673 + t^7.715 + 4*t^7.836 + t^7.879 + 4*t^8. - 3*t^8.164 + 3*t^8.285 + 3*t^8.327 + 3*t^8.448 + t^8.491 - 4*t^8.612 + t^8.655 + t^8.733 + t^8.776 + 6*t^8.897 + 3*t^8.939 - t^4.388/y - t^6.552/y + t^7./y - t^7.164/y + t^7.612/y + t^7.939/y + (2*t^8.224)/y + t^8.388/y + (2*t^8.552)/y + t^8.673/y + t^8.836/y - t^4.388*y - t^6.552*y + t^7.*y - t^7.164*y + t^7.612*y + t^7.939*y + 2*t^8.224*y + t^8.388*y + 2*t^8.552*y + t^8.673*y + t^8.836*y | t^2.164/g1^6 + g1^2*t^2.612 + t^2.776/g1^4 + g1^10*t^3.061 + (2*t^3.388)/g1^2 + t^3.552/g1^8 + g1^6*t^3.836 + 2*t^4. + t^4.327/g1^12 + 3*g1^8*t^4.448 + t^4.776/g1^4 + t^4.939/g1^10 + 2*g1^4*t^5.224 + t^5.388/g1^2 + t^5.552/g1^8 + g1^12*t^5.673 + t^5.715/g1^14 + g1^6*t^5.836 - 2*t^6. + g1^20*t^6.121 + (4*t^6.164)/g1^6 + t^6.327/g1^12 + t^6.491/g1^18 + 4*g1^2*t^6.612 + (2*t^6.776)/g1^4 + g1^16*t^6.897 + t^6.939/g1^10 + 3*g1^10*t^7.061 + (2*t^7.103)/g1^16 + 2*g1^4*t^7.224 + t^7.388/g1^2 + 3*g1^18*t^7.509 + (3*t^7.552)/g1^8 - 2*g1^12*t^7.673 + t^7.715/g1^14 + 4*g1^6*t^7.836 + t^7.879/g1^20 + 4*t^8. - (3*t^8.164)/g1^6 + 3*g1^14*t^8.285 + (3*t^8.327)/g1^12 + 3*g1^8*t^8.448 + t^8.491/g1^18 - 4*g1^2*t^8.612 + t^8.655/g1^24 + g1^22*t^8.733 + t^8.776/g1^4 + 6*g1^16*t^8.897 + (3*t^8.939)/g1^10 - t^4.388/(g1^2*y) - t^6.552/(g1^8*y) + t^7./y - t^7.164/(g1^6*y) + (g1^2*t^7.612)/y + t^7.939/(g1^10*y) + (2*g1^4*t^8.224)/y + t^8.388/(g1^2*y) + (2*t^8.552)/(g1^8*y) + (g1^12*t^8.673)/y + (g1^6*t^8.836)/y - (t^4.388*y)/g1^2 - (t^6.552*y)/g1^8 + t^7.*y - (t^7.164*y)/g1^6 + g1^2*t^7.612*y + (t^7.939*y)/g1^10 + 2*g1^4*t^8.224*y + (t^8.388*y)/g1^2 + (2*t^8.552*y)/g1^8 + g1^12*t^8.673*y + g1^6*t^8.836*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 |
|---|---|---|---|---|---|---|---|---|---|
| 4761 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ + ${ }M_{3}M_{8}$ + ${ }M_{1}M_{4}$ + ${ }M_{6}X_{1}$ | 0.6635 | 0.8258 | 0.8035 | [X:[1.3333], M:[1.1317, 0.7285, 0.992, 0.8683, 1.1317, 0.6667, 0.8683, 1.008], q:[0.504, 0.3643], qb:[0.504, 0.7675], phi:[0.4651]] | t^2.186 + 2*t^2.605 + t^2.79 + t^3.024 + t^3.395 + t^3.581 + t^3.814 + 2*t^4. + t^4.371 + 3*t^4.419 + 2*t^4.79 + t^4.976 + 4*t^5.21 + 2*t^5.395 + 2*t^5.629 + t^5.766 + t^5.814 - 2*t^6. - t^4.395/y - t^4.395*y | detail |