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 |
|---|---|---|---|---|---|---|---|---|---|
| 6329 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{8}$ | 0.6242 | 0.8008 | 0.7794 | [M:[0.7826, 0.9565, 1.0, 0.7391, 1.2609, 0.8261, 0.7391, 1.0435], q:[0.7391, 0.4783], qb:[0.2609, 0.7826], phi:[0.4348]] | [M:[[0], [0], [0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 15189/24334, c: 155897/194672, M1: 18/23, M2: 22/23, M3: 1, M4: 17/23, M5: 29/23, M6: 19/23, M7: 17/23, M8: 24/23, q1: 17/23, q2: 11/23, qb1: 6/23, qb2: 18/23, phi1: 10/23} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{8}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{7}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{1}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{8}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$ | ${}$ | -1 | 2*t^2.217 + t^2.348 + t^2.478 + t^2.609 + t^2.87 + t^3. + t^3.13 + t^4.174 + t^4.304 + 3*t^4.435 + 2*t^4.565 + 3*t^4.696 + 3*t^4.826 + 3*t^4.957 + 3*t^5.087 + 3*t^5.217 + 3*t^5.348 + 3*t^5.478 + 2*t^5.609 + 2*t^5.739 - t^6. + t^6.391 + t^6.522 + 3*t^6.652 + 3*t^6.783 + 4*t^6.913 + 6*t^7.043 + 7*t^7.174 + 7*t^7.304 + 7*t^7.435 + 7*t^7.565 + 6*t^7.696 + 6*t^7.826 + 6*t^7.957 + 3*t^8.087 - t^8.217 + t^8.348 - 3*t^8.478 + t^8.609 - t^4.304/y - t^6.522/y - t^6.652/y - t^6.783/y - t^6.913/y + t^7.435/y + (2*t^7.565)/y + (3*t^7.696)/y + (4*t^7.826)/y + (2*t^7.957)/y + (4*t^8.087)/y + (3*t^8.217)/y + (4*t^8.348)/y + (3*t^8.478)/y + (2*t^8.609)/y - t^4.304*y - t^6.522*y - t^6.652*y - t^6.783*y - t^6.913*y + t^7.435*y + 2*t^7.565*y + 3*t^7.696*y + 4*t^7.826*y + 2*t^7.957*y + 4*t^8.087*y + 3*t^8.217*y + 4*t^8.348*y + 3*t^8.478*y + 2*t^8.609*y | 2*t^2.217 + t^2.348 + t^2.478 + t^2.609 + t^2.87 + t^3. + t^3.13 + t^4.174 + t^4.304 + 3*t^4.435 + 2*t^4.565 + 3*t^4.696 + 3*t^4.826 + 3*t^4.957 + 3*t^5.087 + 3*t^5.217 + 3*t^5.348 + 3*t^5.478 + 2*t^5.609 + 2*t^5.739 - t^6. + t^6.391 + t^6.522 + 3*t^6.652 + 3*t^6.783 + 4*t^6.913 + 6*t^7.043 + 7*t^7.174 + 7*t^7.304 + 7*t^7.435 + 7*t^7.565 + 6*t^7.696 + 6*t^7.826 + 6*t^7.957 + 3*t^8.087 - t^8.217 + t^8.348 - 3*t^8.478 + t^8.609 - t^4.304/y - t^6.522/y - t^6.652/y - t^6.783/y - t^6.913/y + t^7.435/y + (2*t^7.565)/y + (3*t^7.696)/y + (4*t^7.826)/y + (2*t^7.957)/y + (4*t^8.087)/y + (3*t^8.217)/y + (4*t^8.348)/y + (3*t^8.478)/y + (2*t^8.609)/y - t^4.304*y - t^6.522*y - t^6.652*y - t^6.783*y - t^6.913*y + t^7.435*y + 2*t^7.565*y + 3*t^7.696*y + 4*t^7.826*y + 2*t^7.957*y + 4*t^8.087*y + 3*t^8.217*y + 4*t^8.348*y + 3*t^8.478*y + 2*t^8.609*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 |
|---|---|---|---|---|---|---|---|---|---|
| 4740 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ | 0.7151 | 0.9177 | 0.7793 | [M:[1.0362, 0.7952, 1.0, 0.8313, 1.1687, 0.7108, 0.8313, 0.6747], q:[0.5663, 0.3976], qb:[0.4337, 0.7711], phi:[0.4578]] | t^2.024 + t^2.133 + t^2.386 + 2*t^2.494 + t^2.747 + t^3. + t^3.108 + t^3.759 + t^4.012 + t^4.048 + t^4.157 + 2*t^4.265 + t^4.373 + t^4.41 + 3*t^4.518 + 2*t^4.627 + 3*t^4.771 + 3*t^4.88 + 3*t^4.988 + t^5.024 + 3*t^5.133 + 3*t^5.241 + t^5.386 + 3*t^5.494 + t^5.602 + t^5.747 + t^5.783 + t^5.855 - 2*t^6. - t^4.373/y - t^4.373*y | detail |