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 |
|---|---|---|---|---|---|---|---|---|---|
| 1846 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ | 0.6116 | 0.7678 | 0.7965 | [M:[1.0, 1.2202, 0.6698, 0.8899, 0.6698], q:[0.6399, 0.9702], qb:[0.3601, 0.4702], phi:[0.3899]] | [M:[[0], [2], [-3], [-1], [-3]], q:[[-1], [2]], qb:[[1], [2]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{5}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }q_{1}q_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{5}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}$ | -1 | 2*t^2.009 + t^2.491 + t^2.67 + t^3. + t^3.33 + 2*t^3.66 + 3*t^4.019 + t^4.321 + 2*t^4.5 + 2*t^4.679 + t^4.83 + t^4.981 + 2*t^5.009 + t^5.16 + 2*t^5.34 + t^5.491 + 3*t^5.67 + t^5.821 - t^6. + 4*t^6.028 + 2*t^6.151 + 3*t^6.33 + 2*t^6.509 + t^6.66 + 3*t^6.688 + t^6.812 + 3*t^6.991 + 3*t^7.019 + 2*t^7.321 + 3*t^7.349 + t^7.472 + t^7.5 + 4*t^7.679 + t^7.83 + 2*t^7.981 - 2*t^8.009 + 5*t^8.037 + 2*t^8.16 + t^8.312 + 4*t^8.34 - t^8.491 + 2*t^8.519 + 3*t^8.642 - 2*t^8.67 + 4*t^8.698 + t^8.821 - t^4.17/y - (2*t^6.179)/y - t^6.84/y + t^7.019/y + (3*t^7.5)/y + (2*t^7.679)/y + (2*t^8.009)/y + (3*t^8.16)/y - (3*t^8.188)/y + (2*t^8.34)/y + t^8.491/y + (5*t^8.67)/y + t^8.821/y - (2*t^8.849)/y - t^4.17*y - 2*t^6.179*y - t^6.84*y + t^7.019*y + 3*t^7.5*y + 2*t^7.679*y + 2*t^8.009*y + 3*t^8.16*y - 3*t^8.188*y + 2*t^8.34*y + t^8.491*y + 5*t^8.67*y + t^8.821*y - 2*t^8.849*y | (2*t^2.009)/g1^3 + g1^3*t^2.491 + t^2.67/g1 + t^3. + g1*t^3.33 + 2*g1^2*t^3.66 + (3*t^4.019)/g1^6 + g1^4*t^4.321 + 2*t^4.5 + (2*t^4.679)/g1^4 + g1*t^4.83 + g1^6*t^4.981 + (2*t^5.009)/g1^3 + g1^2*t^5.16 + (2*t^5.34)/g1^2 + g1^3*t^5.491 + (3*t^5.67)/g1 + g1^4*t^5.821 - t^6. + (4*t^6.028)/g1^9 + 2*g1^5*t^6.151 + 3*g1*t^6.33 + (2*t^6.509)/g1^3 + g1^2*t^6.66 + (3*t^6.688)/g1^7 + g1^7*t^6.812 + 3*g1^3*t^6.991 + (3*t^7.019)/g1^6 + 2*g1^4*t^7.321 + (3*t^7.349)/g1^5 + g1^9*t^7.472 + t^7.5 + (4*t^7.679)/g1^4 + g1*t^7.83 + 2*g1^6*t^7.981 - (2*t^8.009)/g1^3 + (5*t^8.037)/g1^12 + 2*g1^2*t^8.16 + g1^7*t^8.312 + (4*t^8.34)/g1^2 - g1^3*t^8.491 + (2*t^8.519)/g1^6 + 3*g1^8*t^8.642 - (2*t^8.67)/g1 + (4*t^8.698)/g1^10 + g1^4*t^8.821 - t^4.17/(g1*y) - (2*t^6.179)/(g1^4*y) - t^6.84/(g1^2*y) + t^7.019/(g1^6*y) + (3*t^7.5)/y + (2*t^7.679)/(g1^4*y) + (2*t^8.009)/(g1^3*y) + (3*g1^2*t^8.16)/y - (3*t^8.188)/(g1^7*y) + (2*t^8.34)/(g1^2*y) + (g1^3*t^8.491)/y + (5*t^8.67)/(g1*y) + (g1^4*t^8.821)/y - (2*t^8.849)/(g1^5*y) - (t^4.17*y)/g1 - (2*t^6.179*y)/g1^4 - (t^6.84*y)/g1^2 + (t^7.019*y)/g1^6 + 3*t^7.5*y + (2*t^7.679*y)/g1^4 + (2*t^8.009*y)/g1^3 + 3*g1^2*t^8.16*y - (3*t^8.188*y)/g1^7 + (2*t^8.34*y)/g1^2 + g1^3*t^8.491*y + (5*t^8.67*y)/g1 + g1^4*t^8.821*y - (2*t^8.849*y)/g1^5 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 455 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ | 0.5907 | 0.7264 | 0.8132 | [M:[1.0, 1.2196, 0.6706, 0.8902], q:[0.6402, 0.9696], qb:[0.3598, 0.4696], phi:[0.3902]] | t^2.012 + t^2.488 + t^2.671 + t^3. + t^3.329 + 2*t^3.659 + t^3.988 + t^4.024 + t^4.317 + t^4.5 + t^4.683 + t^4.829 + t^4.976 + t^5.012 + t^5.159 + t^5.341 + t^5.488 + t^5.671 + t^5.817 - t^4.171/y - t^4.171*y | detail |