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 |
|---|---|---|---|---|---|---|---|---|---|
| 56574 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}M_{7}$ | 0.7001 | 0.8631 | 0.8111 | [M:[0.9358, 1.0642, 1.0385, 0.9102, 0.9615, 1.0128, 0.9358], q:[0.5064, 0.5578], qb:[0.4294, 0.5321], phi:[0.4936]] | [M:[[-10], [10], [6], [-14], [-6], [2], [-10]], q:[[1], [9]], qb:[[-11], [5]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{1}$, ${ }M_{7}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}^{4}$ | ${}$ | -2 | t^2.73 + 2*t^2.807 + t^2.884 + t^2.961 + t^3.039 + t^3.116 + t^4.057 + t^4.288 + t^4.365 + t^4.442 + t^4.519 + t^4.596 + 2*t^4.673 + t^4.75 + t^4.827 + t^5.461 + 2*t^5.538 + 3*t^5.615 + 2*t^5.692 + 3*t^5.769 + 3*t^5.846 + 2*t^5.923 - 2*t^6. - t^6.077 - t^6.308 - t^6.385 + t^6.788 + 2*t^6.865 + t^6.942 + 2*t^7.019 + 2*t^7.096 + 3*t^7.173 + 3*t^7.25 + 3*t^7.327 + 4*t^7.404 + 3*t^7.481 + 2*t^7.558 + 3*t^7.635 + t^7.712 + t^7.789 - t^7.866 + t^8.114 + t^8.191 + 2*t^8.268 + 4*t^8.345 + 5*t^8.422 + 4*t^8.499 + 5*t^8.576 + 5*t^8.653 + 2*t^8.73 - 3*t^8.807 - 2*t^8.884 - 3*t^8.961 - t^4.481/y - t^7.211/y - t^7.288/y + t^7.673/y + t^7.75/y + (2*t^8.538)/y + (2*t^8.615)/y + (3*t^8.692)/y + (3*t^8.769)/y + (4*t^8.846)/y + (3*t^8.923)/y - t^4.481*y - t^7.211*y - t^7.288*y + t^7.673*y + t^7.75*y + 2*t^8.538*y + 2*t^8.615*y + 3*t^8.692*y + 3*t^8.769*y + 4*t^8.846*y + 3*t^8.923*y | t^2.73/g1^14 + (2*t^2.807)/g1^10 + t^2.884/g1^6 + t^2.961/g1^2 + g1^2*t^3.039 + g1^6*t^3.116 + t^4.057/g1^23 + t^4.288/g1^11 + t^4.365/g1^7 + t^4.442/g1^3 + g1*t^4.519 + g1^5*t^4.596 + 2*g1^9*t^4.673 + g1^13*t^4.75 + g1^17*t^4.827 + t^5.461/g1^28 + (2*t^5.538)/g1^24 + (3*t^5.615)/g1^20 + (2*t^5.692)/g1^16 + (3*t^5.769)/g1^12 + (3*t^5.846)/g1^8 + (2*t^5.923)/g1^4 - 2*t^6. - g1^4*t^6.077 - g1^16*t^6.308 - g1^20*t^6.385 + t^6.788/g1^37 + (2*t^6.865)/g1^33 + t^6.942/g1^29 + (2*t^7.019)/g1^25 + (2*t^7.096)/g1^21 + (3*t^7.173)/g1^17 + (3*t^7.25)/g1^13 + (3*t^7.327)/g1^9 + (4*t^7.404)/g1^5 + (3*t^7.481)/g1 + 2*g1^3*t^7.558 + 3*g1^7*t^7.635 + g1^11*t^7.712 + g1^15*t^7.789 - g1^19*t^7.866 + t^8.114/g1^46 + t^8.191/g1^42 + (2*t^8.268)/g1^38 + (4*t^8.345)/g1^34 + (5*t^8.422)/g1^30 + (4*t^8.499)/g1^26 + (5*t^8.576)/g1^22 + (5*t^8.653)/g1^18 + (2*t^8.73)/g1^14 - (3*t^8.807)/g1^10 - (2*t^8.884)/g1^6 - (3*t^8.961)/g1^2 - t^4.481/(g1*y) - t^7.211/(g1^15*y) - t^7.288/(g1^11*y) + (g1^9*t^7.673)/y + (g1^13*t^7.75)/y + (2*t^8.538)/(g1^24*y) + (2*t^8.615)/(g1^20*y) + (3*t^8.692)/(g1^16*y) + (3*t^8.769)/(g1^12*y) + (4*t^8.846)/(g1^8*y) + (3*t^8.923)/(g1^4*y) - (t^4.481*y)/g1 - (t^7.211*y)/g1^15 - (t^7.288*y)/g1^11 + g1^9*t^7.673*y + g1^13*t^7.75*y + (2*t^8.538*y)/g1^24 + (2*t^8.615*y)/g1^20 + (3*t^8.692*y)/g1^16 + (3*t^8.769*y)/g1^12 + (4*t^8.846*y)/g1^8 + (3*t^8.923*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 54502 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}M_{5}$ | 0.6951 | 0.8532 | 0.8147 | [M:[0.9573, 1.0427, 1.0256, 0.9402, 0.9744, 1.0085], q:[0.5043, 0.5384], qb:[0.453, 0.5214], phi:[0.4957]] | t^2.821 + t^2.872 + t^2.923 + t^2.974 + t^3.026 + t^3.077 + t^3.128 + t^4.205 + t^4.359 + t^4.41 + t^4.462 + t^4.513 + t^4.564 + 2*t^4.615 + t^4.667 + t^4.718 + t^5.641 + t^5.692 + t^5.744 + t^5.795 + 2*t^5.846 + 2*t^5.897 + 2*t^5.949 - t^6. - t^4.487/y - t^4.487*y | detail |