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 |
|---|---|---|---|---|---|---|---|---|---|
| 56226 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{2}M_{6}$ + ${ }M_{3}M_{7}$ | 0.6625 | 0.8299 | 0.7983 | [M:[1.1164, 1.1643, 0.8836, 0.6986, 0.8357, 0.8357, 1.1164], q:[0.3493, 0.5343], qb:[0.4864, 0.7671], phi:[0.4657]] | [M:[[-1], [-10], [1], [-6], [10], [10], [-1]], q:[[-3], [4]], qb:[[13], [2]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{4}\phi_{1}q_{1}\tilde{q}_{1}$ | -2 | t^2.096 + 2*t^2.507 + t^2.794 + t^3.062 + 2*t^3.349 + t^3.761 + t^3.904 + t^4.048 + t^4.191 + t^4.316 + t^4.459 + 3*t^4.603 + t^4.89 + 3*t^5.014 + t^5.158 + 2*t^5.301 + t^5.445 + 2*t^5.569 + 5*t^5.856 - 2*t^6. + t^6.124 + t^6.144 + 2*t^6.268 + t^6.287 + 3*t^6.411 + t^6.555 + 4*t^6.699 + 3*t^6.823 - t^6.842 + 2*t^6.966 + 7*t^7.11 + t^7.378 + 2*t^7.397 + 5*t^7.521 + 4*t^7.665 + 2*t^7.809 + 2*t^7.952 + 4*t^8.076 - 2*t^8.096 + 2*t^8.22 + 8*t^8.363 + t^8.383 - 4*t^8.507 + 3*t^8.631 + t^8.651 + 4*t^8.775 + 7*t^8.918 - 2*t^8.938 - t^4.397/y - t^6.493/y - t^6.904/y + t^7.048/y - t^7.191/y + (3*t^7.603)/y - t^7.746/y + (2*t^7.89)/y + t^8.014/y + t^8.158/y + (3*t^8.301)/y + (2*t^8.445)/y + (2*t^8.569)/y - t^8.589/y + (6*t^8.856)/y - t^4.397*y - t^6.493*y - t^6.904*y + t^7.048*y - t^7.191*y + 3*t^7.603*y - t^7.746*y + 2*t^7.89*y + t^8.014*y + t^8.158*y + 3*t^8.301*y + 2*t^8.445*y + 2*t^8.569*y - t^8.589*y + 6*t^8.856*y | t^2.096/g1^6 + 2*g1^10*t^2.507 + t^2.794/g1^8 + g1^17*t^3.062 + (2*t^3.349)/g1 + g1^15*t^3.761 + g1^6*t^3.904 + t^4.048/g1^3 + t^4.191/g1^12 + g1^22*t^4.316 + g1^13*t^4.459 + 3*g1^4*t^4.603 + t^4.89/g1^14 + 3*g1^20*t^5.014 + g1^11*t^5.158 + 2*g1^2*t^5.301 + t^5.445/g1^7 + 2*g1^27*t^5.569 + 5*g1^9*t^5.856 - 2*t^6. + g1^34*t^6.124 + t^6.144/g1^9 + 2*g1^25*t^6.268 + t^6.287/g1^18 + 3*g1^16*t^6.411 + g1^7*t^6.555 + (4*t^6.699)/g1^2 + 3*g1^32*t^6.823 - t^6.842/g1^11 + 2*g1^23*t^6.966 + 7*g1^14*t^7.11 + g1^39*t^7.378 + (2*t^7.397)/g1^4 + 5*g1^30*t^7.521 + 4*g1^21*t^7.665 + 2*g1^12*t^7.809 + 2*g1^3*t^7.952 + 4*g1^37*t^8.076 - (2*t^8.096)/g1^6 + 2*g1^28*t^8.22 + 8*g1^19*t^8.363 + t^8.383/g1^24 - 4*g1^10*t^8.507 + 3*g1^44*t^8.631 + g1*t^8.651 + 4*g1^35*t^8.775 + 7*g1^26*t^8.918 - (2*t^8.938)/g1^17 - t^4.397/(g1^4*y) - t^6.493/(g1^10*y) - (g1^6*t^6.904)/y + t^7.048/(g1^3*y) - t^7.191/(g1^12*y) + (3*g1^4*t^7.603)/y - t^7.746/(g1^5*y) + (2*t^7.89)/(g1^14*y) + (g1^20*t^8.014)/y + (g1^11*t^8.158)/y + (3*g1^2*t^8.301)/y + (2*t^8.445)/(g1^7*y) + (2*g1^27*t^8.569)/y - t^8.589/(g1^16*y) + (6*g1^9*t^8.856)/y - (t^4.397*y)/g1^4 - (t^6.493*y)/g1^10 - g1^6*t^6.904*y + (t^7.048*y)/g1^3 - (t^7.191*y)/g1^12 + 3*g1^4*t^7.603*y - (t^7.746*y)/g1^5 + (2*t^7.89*y)/g1^14 + g1^20*t^8.014*y + g1^11*t^8.158*y + 3*g1^2*t^8.301*y + (2*t^8.445*y)/g1^7 + 2*g1^27*t^8.569*y - (t^8.589*y)/g1^16 + 6*g1^9*t^8.856*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50977 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{2}M_{6}$ | 0.673 | 0.8479 | 0.7937 | [M:[1.1166, 1.1662, 0.8834, 0.6997, 0.8338, 0.8338], q:[0.3499, 0.5335], qb:[0.4839, 0.7668], phi:[0.4665]] | t^2.099 + 2*t^2.501 + t^2.65 + t^2.799 + t^3.052 + t^3.35 + t^3.752 + t^3.901 + t^4.05 + t^4.198 + t^4.303 + t^4.452 + 3*t^4.601 + t^4.749 + t^4.898 + 3*t^5.003 + 3*t^5.152 + 3*t^5.3 + t^5.449 + 2*t^5.554 + t^5.702 + 3*t^5.851 - t^6. - t^4.399/y - t^4.399*y | detail |