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 |
|---|---|---|---|---|---|---|---|---|---|
| 55583 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ | 0.679 | 0.8521 | 0.7969 | [M:[1.1538, 1.0769, 0.8462, 0.7692, 0.6923], q:[0.3846, 0.4615], qb:[0.5385, 0.7692], phi:[0.4615]] | [M:[[0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 459/676, c: 144/169, M1: 15/13, M2: 14/13, M3: 11/13, M4: 10/13, M5: 9/13, q1: 5/13, q2: 6/13, qb1: 7/13, qb2: 10/13, phi1: 6/13} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | ${}q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | 2 | t^2.077 + t^2.308 + t^2.538 + t^2.769 + t^3. + t^3.231 + t^3.462 + t^3.692 + t^3.923 + 3*t^4.154 + 2*t^4.385 + 3*t^4.615 + 2*t^4.846 + 3*t^5.077 + 3*t^5.308 + 3*t^5.538 + 2*t^5.769 + 2*t^6. + 4*t^6.231 + 5*t^6.462 + 6*t^6.692 + 6*t^6.923 + 5*t^7.154 + 6*t^7.385 + 6*t^7.615 + 5*t^7.846 + 4*t^8.077 + 6*t^8.308 + 5*t^8.538 + 8*t^8.769 - t^4.385/y - t^6.462/y - t^6.692/y + t^7.385/y + t^7.615/y + (2*t^7.846)/y + (3*t^8.077)/y + (4*t^8.308)/y + (2*t^8.538)/y + (3*t^8.769)/y - t^4.385*y - t^6.462*y - t^6.692*y + t^7.385*y + t^7.615*y + 2*t^7.846*y + 3*t^8.077*y + 4*t^8.308*y + 2*t^8.538*y + 3*t^8.769*y | t^2.077 + t^2.308 + t^2.538 + t^2.769 + t^3. + t^3.231 + t^3.462 + t^3.692 + t^3.923 + 3*t^4.154 + 2*t^4.385 + 3*t^4.615 + 2*t^4.846 + 3*t^5.077 + 3*t^5.308 + 3*t^5.538 + 2*t^5.769 + 2*t^6. + 4*t^6.231 + 5*t^6.462 + 6*t^6.692 + 6*t^6.923 + 5*t^7.154 + 6*t^7.385 + 6*t^7.615 + 5*t^7.846 + 4*t^8.077 + 6*t^8.308 + 5*t^8.538 + 8*t^8.769 - t^4.385/y - t^6.462/y - t^6.692/y + t^7.385/y + t^7.615/y + (2*t^7.846)/y + (3*t^8.077)/y + (4*t^8.308)/y + (2*t^8.538)/y + (3*t^8.769)/y - t^4.385*y - t^6.462*y - t^6.692*y + t^7.385*y + t^7.615*y + 2*t^7.846*y + 3*t^8.077*y + 4*t^8.308*y + 2*t^8.538*y + 3*t^8.769*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 |
|---|---|---|---|---|---|---|---|---|
| 57252 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6996 | 0.892 | 0.7844 | [M:[1.1538, 1.0769, 0.8462, 0.7692, 0.6923, 0.6923], q:[0.3846, 0.4615], qb:[0.5385, 0.7692], phi:[0.4615]] | 2*t^2.077 + t^2.308 + t^2.538 + t^2.769 + t^3. + t^3.231 + t^3.462 + t^3.692 + 5*t^4.154 + 3*t^4.385 + 4*t^4.615 + 3*t^4.846 + 4*t^5.077 + 4*t^5.308 + 4*t^5.538 + 3*t^5.769 + t^6. - t^4.385/y - t^4.385*y | detail | {a: 12297/17576, c: 15677/17576, M1: 15/13, M2: 14/13, M3: 11/13, M4: 10/13, M5: 9/13, M6: 9/13, q1: 5/13, q2: 6/13, qb1: 7/13, qb2: 10/13, phi1: 6/13} |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 47181 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ | 0.6791 | 0.8522 | 0.7969 | [M:[1.1508, 1.0793, 0.8492, 0.762, 0.6905], q:[0.381, 0.4682], qb:[0.5397, 0.7698], phi:[0.4603]] | t^2.071 + t^2.286 + t^2.548 + t^2.762 + t^3.024 + t^3.238 + t^3.452 + t^3.667 + t^3.929 + 2*t^4.143 + t^4.19 + t^4.357 + t^4.405 + t^4.572 + 2*t^4.619 + 2*t^4.833 + t^5.048 + 2*t^5.095 + 3*t^5.31 + 2*t^5.524 + t^5.571 + t^5.738 + t^5.786 + t^5.953 - t^4.381/y - t^4.381*y | detail |