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 |
|---|---|---|---|---|---|---|---|---|---|
| 2230 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}q_{1}q_{2}$ + ${ }M_{2}M_{7}$ | 0.6948 | 0.8638 | 0.8044 | [M:[1.0364, 1.1113, 0.9626, 0.7409, 0.9636, 0.8148, 0.8887], q:[0.7778, 0.4074], qb:[0.5562, 0.4813], phi:[0.4443]] | [M:[[32], [-12], [22], [-8], [-32], [2], [12]], q:[[-3], [1]], qb:[[-33], [11]], phi:[[6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}^{2}$ | ${}$ | -2 | t^2.223 + t^2.444 + 2*t^2.666 + t^2.888 + t^2.891 + t^3.777 + t^3.999 + t^4.002 + t^4.221 + t^4.224 + 2*t^4.445 + t^4.667 + t^4.67 + 3*t^4.889 + 3*t^5.11 + t^5.113 + 4*t^5.332 + t^5.335 + t^5.554 + 2*t^5.557 + t^5.781 - 2*t^6. + 3*t^6.443 + t^6.446 + 3*t^6.665 + 4*t^6.668 + 2*t^6.887 + 4*t^6.89 + 2*t^6.893 + 3*t^7.111 + 2*t^7.114 + 2*t^7.333 + 3*t^7.336 + 4*t^7.555 + t^7.561 + 5*t^7.776 + t^7.779 + 6*t^7.998 + 2*t^8.001 + t^8.004 + 2*t^8.22 + t^8.223 + t^8.226 - 4*t^8.444 + 3*t^8.447 + t^8.663 - 4*t^8.666 + 2*t^8.672 - t^8.888 + t^8.894 - t^4.333/y - t^6.556/y - t^6.777/y - t^6.999/y - t^7.221/y + t^7.445/y + (2*t^7.667)/y + (3*t^7.889)/y + (4*t^8.11)/y + t^8.113/y + (2*t^8.332)/y + t^8.335/y + (2*t^8.554)/y + (2*t^8.557)/y - t^4.333*y - t^6.556*y - t^6.777*y - t^6.999*y - t^7.221*y + t^7.445*y + 2*t^7.667*y + 3*t^7.889*y + 4*t^8.11*y + t^8.113*y + 2*t^8.332*y + t^8.335*y + 2*t^8.554*y + 2*t^8.557*y | t^2.223/g1^8 + g1^2*t^2.444 + 2*g1^12*t^2.666 + g1^22*t^2.888 + t^2.891/g1^32 + g1^8*t^3.777 + g1^18*t^3.999 + t^4.002/g1^36 + g1^28*t^4.221 + t^4.224/g1^26 + (2*t^4.445)/g1^16 + t^4.667/g1^6 + t^4.67/g1^60 + 3*g1^4*t^4.889 + 3*g1^14*t^5.11 + t^5.113/g1^40 + 4*g1^24*t^5.332 + t^5.335/g1^30 + g1^34*t^5.554 + (2*t^5.557)/g1^20 + t^5.781/g1^64 - 2*t^6. + 3*g1^20*t^6.443 + t^6.446/g1^34 + 3*g1^30*t^6.665 + (4*t^6.668)/g1^24 + 2*g1^40*t^6.887 + (4*t^6.89)/g1^14 + (2*t^6.893)/g1^68 + (3*t^7.111)/g1^4 + (2*t^7.114)/g1^58 + 2*g1^6*t^7.333 + (3*t^7.336)/g1^48 + 4*g1^16*t^7.555 + t^7.561/g1^92 + 5*g1^26*t^7.776 + t^7.779/g1^28 + 6*g1^36*t^7.998 + (2*t^8.001)/g1^18 + t^8.004/g1^72 + 2*g1^46*t^8.22 + t^8.223/g1^8 + t^8.226/g1^62 - 4*g1^2*t^8.444 + (3*t^8.447)/g1^52 + g1^66*t^8.663 - 4*g1^12*t^8.666 + (2*t^8.672)/g1^96 - g1^22*t^8.888 + t^8.894/g1^86 - (g1^6*t^4.333)/y - t^6.556/(g1^2*y) - (g1^8*t^6.777)/y - (g1^18*t^6.999)/y - (g1^28*t^7.221)/y + t^7.445/(g1^16*y) + (2*t^7.667)/(g1^6*y) + (3*g1^4*t^7.889)/y + (4*g1^14*t^8.11)/y + t^8.113/(g1^40*y) + (2*g1^24*t^8.332)/y + t^8.335/(g1^30*y) + (2*g1^34*t^8.554)/y + (2*t^8.557)/(g1^20*y) - g1^6*t^4.333*y - (t^6.556*y)/g1^2 - g1^8*t^6.777*y - g1^18*t^6.999*y - g1^28*t^7.221*y + (t^7.445*y)/g1^16 + (2*t^7.667*y)/g1^6 + 3*g1^4*t^7.889*y + 4*g1^14*t^8.11*y + (t^8.113*y)/g1^40 + 2*g1^24*t^8.332*y + (t^8.335*y)/g1^30 + 2*g1^34*t^8.554*y + (2*t^8.557*y)/g1^20 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1182 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}q_{1}q_{2}$ | 0.685 | 0.8478 | 0.808 | [M:[1.0524, 1.1054, 0.9735, 0.7369, 0.9476, 0.8158], q:[0.7763, 0.4079], qb:[0.5398, 0.4867], phi:[0.4473]] | t^2.211 + t^2.447 + t^2.684 + t^2.843 + t^2.92 + t^3.316 + t^3.789 + t^3.948 + t^4.026 + t^4.185 + t^4.262 + 2*t^4.421 + t^4.581 + t^4.658 + 2*t^4.895 + t^5.054 + 2*t^5.131 + t^5.29 + 2*t^5.368 + 2*t^5.527 + t^5.686 + t^5.763 - t^6. - t^4.342/y - t^4.342*y | detail |