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 |
|---|---|---|---|---|---|---|---|---|---|
| 5718 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{8}^{2}$ | 0.6231 | 0.7883 | 0.7905 | [X:[1.3929], M:[0.8929, 1.25, 1.1071, 0.6071, 0.75, 0.7857, 0.8929, 1.0], q:[0.7679, 0.4821], qb:[0.625, 0.2679], phi:[0.4643]] | [X:[[0]], M:[[0], [0], [0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 27357/43904, c: 34609/43904, X1: 39/28, M1: 25/28, M2: 5/4, M3: 31/28, M4: 17/28, M5: 3/4, M6: 11/14, M7: 25/28, M8: 1, q1: 43/56, q2: 27/56, qb1: 5/8, qb2: 15/56, phi1: 13/28} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{8}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{7}q_{1}\tilde{q}_{2}$ | ${}$ | -1 | t^2.25 + t^2.357 + 2*t^2.679 + t^2.786 + t^3. + t^3.107 + t^3.75 + t^4.071 + t^4.179 + t^4.286 + t^4.5 + t^4.607 + 2*t^4.714 + t^4.929 + 3*t^5.036 + 2*t^5.143 + t^5.25 + 4*t^5.357 + 3*t^5.464 + 2*t^5.679 + 3*t^5.786 - t^6. + 2*t^6.107 - t^6.321 + t^6.429 + 2*t^6.536 + 2*t^6.75 + 3*t^6.857 + 2*t^6.964 + 3*t^7.071 + 2*t^7.179 + 2*t^7.286 + 3*t^7.393 + 3*t^7.5 + 2*t^7.607 + 4*t^7.714 + 4*t^7.821 + 2*t^7.929 + 6*t^8.036 + 6*t^8.143 + t^8.25 + t^8.357 + 6*t^8.464 + t^8.571 - 5*t^8.679 + t^8.786 + 2*t^8.893 - t^4.393/y - t^6.75/y - t^7.071/y - t^7.179/y + (2*t^7.607)/y + t^7.714/y + (2*t^7.929)/y + (4*t^8.036)/y + t^8.143/y + t^8.25/y + (3*t^8.357)/y + (3*t^8.464)/y + (2*t^8.679)/y + (3*t^8.786)/y + t^8.893/y - t^4.393*y - t^6.75*y - t^7.071*y - t^7.179*y + 2*t^7.607*y + t^7.714*y + 2*t^7.929*y + 4*t^8.036*y + t^8.143*y + t^8.25*y + 3*t^8.357*y + 3*t^8.464*y + 2*t^8.679*y + 3*t^8.786*y + t^8.893*y | t^2.25 + t^2.357 + 2*t^2.679 + t^2.786 + t^3. + t^3.107 + t^3.75 + t^4.071 + t^4.179 + t^4.286 + t^4.5 + t^4.607 + 2*t^4.714 + t^4.929 + 3*t^5.036 + 2*t^5.143 + t^5.25 + 4*t^5.357 + 3*t^5.464 + 2*t^5.679 + 3*t^5.786 - t^6. + 2*t^6.107 - t^6.321 + t^6.429 + 2*t^6.536 + 2*t^6.75 + 3*t^6.857 + 2*t^6.964 + 3*t^7.071 + 2*t^7.179 + 2*t^7.286 + 3*t^7.393 + 3*t^7.5 + 2*t^7.607 + 4*t^7.714 + 4*t^7.821 + 2*t^7.929 + 6*t^8.036 + 6*t^8.143 + t^8.25 + t^8.357 + 6*t^8.464 + t^8.571 - 5*t^8.679 + t^8.786 + 2*t^8.893 - t^4.393/y - t^6.75/y - t^7.071/y - t^7.179/y + (2*t^7.607)/y + t^7.714/y + (2*t^7.929)/y + (4*t^8.036)/y + t^8.143/y + t^8.25/y + (3*t^8.357)/y + (3*t^8.464)/y + (2*t^8.679)/y + (3*t^8.786)/y + t^8.893/y - t^4.393*y - t^6.75*y - t^7.071*y - t^7.179*y + 2*t^7.607*y + t^7.714*y + 2*t^7.929*y + 4*t^8.036*y + t^8.143*y + t^8.25*y + 3*t^8.357*y + 3*t^8.464*y + 2*t^8.679*y + 3*t^8.786*y + t^8.893*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 |
|---|---|---|---|---|---|---|---|---|---|
| 4236 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{2}^{2}$ | 0.6845 | 0.8629 | 0.7932 | [X:[1.3574], M:[1.0228, 1.1673, 0.9772, 0.6426, 0.8327, 0.7148, 1.0228, 0.6693], q:[0.7738, 0.3936], qb:[0.5837, 0.4391], phi:[0.4525]] | t^2.008 + t^2.145 + t^2.498 + t^2.715 + 2*t^3.068 + t^3.502 + t^3.639 + t^3.719 + t^4.016 + t^4.072 + t^4.152 + 2*t^4.289 + t^4.426 + t^4.506 + t^4.643 + t^4.723 + 2*t^4.859 + t^4.996 + 2*t^5.076 + 3*t^5.213 + t^5.51 + t^5.566 + 2*t^5.646 + t^5.727 + 3*t^5.783 - 2*t^6. - t^4.357/y - t^4.357*y | detail |