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 |
|---|---|---|---|---|---|---|---|---|---|
| 46425 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }q_{1}q_{2}^{2}\tilde{q}_{1}$ | 0.6724 | 0.8714 | 0.7716 | [M:[1.1326, 0.6837, 0.8163, 0.6837], q:[0.75, 0.4337], qb:[0.3826, 0.4337], phi:[0.5]] | [M:[[-2], [1], [-1], [1]], q:[[0], [1]], qb:[[-2], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{4}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | ${}M_{3}q_{1}q_{2}$ | -2 | 2*t^2.051 + 3*t^2.449 + t^3. + 2*t^3.398 + t^3.551 + t^3.795 + 6*t^4.102 + 6*t^4.5 + 6*t^4.898 + 2*t^5.051 + 7*t^5.449 + 2*t^5.602 + 6*t^5.846 - 2*t^6. + 8*t^6.154 + 3*t^6.244 + 15*t^6.551 + 3*t^6.795 + 10*t^6.949 + 3*t^7.102 + 2*t^7.193 + 7*t^7.346 + 10*t^7.5 + t^7.591 + 2*t^7.654 + 16*t^7.898 - 8*t^8.051 + 15*t^8.205 + 12*t^8.295 - 9*t^8.449 + 18*t^8.602 + 6*t^8.693 + 4*t^8.846 - t^4.5/y - (2*t^6.551)/y - t^6.949/y + (2*t^7.102)/y + (6*t^7.5)/y + (2*t^7.898)/y + (3*t^8.051)/y + (9*t^8.449)/y - t^8.602/y + (8*t^8.846)/y - t^4.5*y - 2*t^6.551*y - t^6.949*y + 2*t^7.102*y + 6*t^7.5*y + 2*t^7.898*y + 3*t^8.051*y + 9*t^8.449*y - t^8.602*y + 8*t^8.846*y | 2*g1*t^2.051 + (3*t^2.449)/g1 + t^3. + (2*t^3.398)/g1^2 + g1*t^3.551 + t^3.795/g1^4 + 6*g1^2*t^4.102 + 6*t^4.5 + (6*t^4.898)/g1^2 + 2*g1*t^5.051 + (7*t^5.449)/g1 + 2*g1^2*t^5.602 + (6*t^5.846)/g1^3 - 2*t^6. + 8*g1^3*t^6.154 + (3*t^6.244)/g1^5 + 15*g1*t^6.551 + (3*t^6.795)/g1^4 + (10*t^6.949)/g1 + 3*g1^2*t^7.102 + (2*t^7.193)/g1^6 + (7*t^7.346)/g1^3 + 10*t^7.5 + t^7.591/g1^8 + 2*g1^3*t^7.654 + (16*t^7.898)/g1^2 - 8*g1*t^8.051 + 15*g1^4*t^8.205 + (12*t^8.295)/g1^4 - (9*t^8.449)/g1 + 18*g1^2*t^8.602 + (6*t^8.693)/g1^6 + (4*t^8.846)/g1^3 - t^4.5/y - (2*g1*t^6.551)/y - t^6.949/(g1*y) + (2*g1^2*t^7.102)/y + (6*t^7.5)/y + (2*t^7.898)/(g1^2*y) + (3*g1*t^8.051)/y + (9*t^8.449)/(g1*y) - (g1^2*t^8.602)/y + (8*t^8.846)/(g1^3*y) - t^4.5*y - 2*g1*t^6.551*y - (t^6.949*y)/g1 + 2*g1^2*t^7.102*y + 6*t^7.5*y + (2*t^7.898*y)/g1^2 + 3*g1*t^8.051*y + (9*t^8.449*y)/g1 - g1^2*t^8.602*y + (8*t^8.846*y)/g1^3 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46194 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6728 | 0.8725 | 0.7711 | [M:[1.1331, 0.696, 0.804, 0.6709], q:[0.75, 0.4209], qb:[0.3831, 0.446], phi:[0.5]] | t^2.013 + t^2.088 + 2*t^2.412 + t^2.487 + t^3. + 2*t^3.399 + t^3.513 + t^3.798 + 2*t^4.026 + 2*t^4.101 + 2*t^4.176 + 2*t^4.425 + 3*t^4.5 + t^4.575 + 3*t^4.824 + 2*t^4.899 + t^4.974 + t^5.013 + t^5.088 + 4*t^5.412 + 3*t^5.487 + t^5.526 + t^5.601 + 4*t^5.811 + 2*t^5.886 + t^5.925 - 2*t^6. - t^4.5/y - t^4.5*y | detail |