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 |
|---|---|---|---|---|---|---|---|---|---|
| 55330 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{1}M_{4}$ | 0.6989 | 0.8581 | 0.8144 | [M:[0.9422, 0.9037, 1.0193, 1.0578, 1.0, 0.9807], q:[0.5578, 0.5], qb:[0.5385, 0.4422], phi:[0.4904]] | [M:[[6], [10], [-2], [-6], [0], [2]], q:[[-6], [0]], qb:[[-4], [6]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{1}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{4}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$ | ${}$ | -2 | t^2.711 + t^2.827 + 2*t^2.942 + t^3. + t^3.116 + t^3.173 + t^4.124 + t^4.298 + t^4.413 + 2*t^4.471 + t^4.587 + t^4.644 + t^4.702 + t^4.76 + t^4.818 + t^5.422 + t^5.538 + 2*t^5.653 + 2*t^5.769 + 3*t^5.884 + 2*t^5.942 - 2*t^6. + t^6.058 + t^6.116 - t^6.173 + t^6.231 + t^6.835 + t^6.951 + t^7.009 + 2*t^7.067 + 2*t^7.124 + 3*t^7.24 + 2*t^7.298 + t^7.356 + 5*t^7.413 + t^7.529 + 3*t^7.587 + 2*t^7.644 + 2*t^7.702 + t^7.76 + t^7.818 + t^7.933 + t^7.991 + t^8.133 + 2*t^8.249 + 2*t^8.364 + t^8.422 + 2*t^8.48 + 5*t^8.595 - t^8.653 + t^8.711 + 2*t^8.769 + 3*t^8.884 - 3*t^8.942 - t^4.471/y - t^7.182/y - t^7.413/y + t^7.529/y + t^7.76/y + t^8.538/y + (2*t^8.653)/y + t^8.711/y + (2*t^8.769)/y + (2*t^8.827)/y + (2*t^8.884)/y + (3*t^8.942)/y - t^4.471*y - t^7.182*y - t^7.413*y + t^7.529*y + t^7.76*y + t^8.538*y + 2*t^8.653*y + t^8.711*y + 2*t^8.769*y + 2*t^8.827*y + 2*t^8.884*y + 3*t^8.942*y | g1^10*t^2.711 + g1^6*t^2.827 + 2*g1^2*t^2.942 + t^3. + t^3.116/g1^4 + t^3.173/g1^6 + g1^13*t^4.124 + g1^7*t^4.298 + g1^3*t^4.413 + 2*g1*t^4.471 + t^4.587/g1^3 + t^4.644/g1^5 + t^4.702/g1^7 + t^4.76/g1^9 + t^4.818/g1^11 + g1^20*t^5.422 + g1^16*t^5.538 + 2*g1^12*t^5.653 + 2*g1^8*t^5.769 + 3*g1^4*t^5.884 + 2*g1^2*t^5.942 - 2*t^6. + t^6.058/g1^2 + t^6.116/g1^4 - t^6.173/g1^6 + t^6.231/g1^8 + g1^23*t^6.835 + g1^19*t^6.951 + g1^17*t^7.009 + 2*g1^15*t^7.067 + 2*g1^13*t^7.124 + 3*g1^9*t^7.24 + 2*g1^7*t^7.298 + g1^5*t^7.356 + 5*g1^3*t^7.413 + t^7.529/g1 + (3*t^7.587)/g1^3 + (2*t^7.644)/g1^5 + (2*t^7.702)/g1^7 + t^7.76/g1^9 + t^7.818/g1^11 + t^7.933/g1^15 + t^7.991/g1^17 + g1^30*t^8.133 + 2*g1^26*t^8.249 + 2*g1^22*t^8.364 + g1^20*t^8.422 + 2*g1^18*t^8.48 + 5*g1^14*t^8.595 - g1^12*t^8.653 + g1^10*t^8.711 + 2*g1^8*t^8.769 + 3*g1^4*t^8.884 - 3*g1^2*t^8.942 - (g1*t^4.471)/y - (g1^11*t^7.182)/y - (g1^3*t^7.413)/y + t^7.529/(g1*y) + t^7.76/(g1^9*y) + (g1^16*t^8.538)/y + (2*g1^12*t^8.653)/y + (g1^10*t^8.711)/y + (2*g1^8*t^8.769)/y + (2*g1^6*t^8.827)/y + (2*g1^4*t^8.884)/y + (3*g1^2*t^8.942)/y - g1*t^4.471*y - g1^11*t^7.182*y - g1^3*t^7.413*y + (t^7.529*y)/g1 + (t^7.76*y)/g1^9 + g1^16*t^8.538*y + 2*g1^12*t^8.653*y + g1^10*t^8.711*y + 2*g1^8*t^8.769*y + 2*g1^6*t^8.827*y + 2*g1^4*t^8.884*y + 3*g1^2*t^8.942*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46855 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.7172 | 0.8839 | 0.8115 | [M:[0.8005, 0.9418, 1.0665, 0.9252, 1.0, 0.9335], q:[0.5624, 0.6372], qb:[0.4959, 0.4376], phi:[0.4667]] | t^2.401 + t^2.776 + 2*t^2.8 + t^2.825 + t^3. + t^3.399 + t^4.026 + t^4.201 + t^4.375 + t^4.4 + t^4.575 + t^4.625 + t^4.774 + t^4.799 + t^4.803 + t^4.999 + t^5.177 + 2*t^5.202 + t^5.223 + t^5.227 + t^5.551 + t^5.576 + 4*t^5.601 + t^5.626 + t^5.651 + 2*t^5.8 - 3*t^6. - t^4.4/y - t^4.4*y | detail |